This is only a preview of the January 2022 issue of Silicon Chip. You can view 38 of the 112 pages in the full issue, including the advertisments. For full access, purchase the issue for $10.00 or subscribe for access to the latest issues. Articles in this series:
Items relevant to "Two Classic LED Metronomes":
Articles in this series:
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JANUARY 2022
ISSN 1030-2662
01
The VERY BEST DIY Projects!
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Contents
Vol.35, No.1
January 2022
12 All About Batteries – Part 1
24
Life without batteries would be unthinkable. We’d be stuck with fixed
phones, non-portable computers, and have to crank-start cars. This series
covers everything you need to know about batteries.
By Dr David Maddison
Science
37 Dick Smith Autobiography
Dick Smith – businessman, adventurer, publicity stunt creator, publisher,
food brand, environmentalist and great promoter of Australia. His new
autobiography is a great read for just about anyone.
By Nicholas Vinen
Book review
64
38 Solar Power with Batteries
After collecting data on my solar panels over their lifetime I wanted to see
whether adding batteries to my system would be worthwhile, what type I
should use and how large it should be.
By Dr Alan R. Wilson
96
72 LTDZ Spectrum Analyser
Geekcreit’s low-cost LTDZ V5.0 spectrum analyser can perform analysis over
the range of 35MHz to 4.4GHz. It’s controlled from a PC via USB, and includes
a tracking generator, RF amplifier and more.
By Jim Rowe
Low-cost electronic modules
24 Two Classic LED Metronomes
These two metronomes, one with eight LEDs and the other with 10 LEDs,
simulate the classic pendulum design, with a pointer swinging left-and-right.
They are great projects for beginners due to not requiring any programming.
By Randy Keenan
Musical project
46 Multi-Channel Speaker Protector
This compact Speaker Protector works with up to six amplifier modules and
can operate from the same supply (up to ±40V DC). It perfectly suits the
Hummingbird Amplifier module described last month.
By Phil Prosser
Audio project
64 The PicoMite
The PicoMite is a BASIC interpreter running on the Raspberry Pi Pico
(MMBasic, in fact). It can be easily connected to a variety of displays,
including OLED and e-Ink panels, with extensive support for other peripherals.
By Geoff Graham & Peter Mather
Raspberry Pi project
96 Remote Control Range Extender
Converting your remote control from infrared to UHF will bring its working
range up to 25m with this project! All you need to do is build these two boards,
one goes near the receiving device and the other fits inside the remote.
By John Clarke
Remote control project
2
Editorial Viewpoint
4
Mailbag
11
Subscriptions
52
Product Showcase
61
Circuit Notebook
78
Vintage Radio
89
1. Conway’s Game of Life on Micromite
2. PCB joiner for the MIDI Keyboard
3. Compact reed relay module
The Mysterious Mickey Oz by Ian Batty
Serviceman’s Log
106
Online Shop
108
Ask Silicon Chip
111
Market Centre
112
Advertising Index
112
Notes & Errata
SILICON
SILIC
CHIP
www.siliconchip.com.au
Publisher/Editor
Nicholas Vinen
Technical Editor
John Clarke – B.E.(Elec.)
Technical Staff
Jim Rowe – B.A., B.Sc.
Bao Smith – B.Sc.
Tim Blythman – B.E., B.Sc.
Nicolas Hannekum – Dip.Elec.Tech.
Advertising Enquiries
Glyn Smith
Phone (02) 9939 3295
Mobile 0431 792 293
glyn<at>siliconchip.com.au
Regular Contributors
Allan Linton-Smith
Dave Thompson
David Maddison – B.App.Sc. (Hons 1),
PhD, Grad.Dip.Entr.Innov.
Geoff Graham
Associate Professor Graham Parslow
Dr Hugo Holden – B.H.B, MB.ChB.,
FRANZCO
Ian Batty
Phil Prosser – B.Sc., B.E.(Elec.)
Cartoonist
Brendan Akhurst
Founding Editor (retired)
Leo Simpson – B.Bus., FAICD
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Editorial Viewpoint
Risk aversion stifles innovation
Reading Dick Smith’s autobiography for the review
(p37), I noticed several recurring themes. Two of
them are “surround yourself with capable people” as
a business strategy (good advice!) and the concept of
“responsible risk-taking”. I have felt for a while that the
latter is sorely missing from the Australian landscape,
especially now; clearly, Dick feels the same way.
He’s referring to the concept of being willing to take
risks as long as you judge them to be reasonable, such
as climbing a cliff or flying a helicopter through bad weather. For this to work,
one has to be capable of assessing risk and taking personal responsibility for
one’s own safety (what a quaint concept!).
While I see over-the-top risk aversion all over our modern landscape,
one area in which it is evident within Australia is in the fields of business,
technology and innovation.
Have you noticed how most multi-billion-dollar global juggernaut
companies, especially those which are technology-based, are from the USA (or
sometimes Europe)? Australia has plenty of fine minds, including scientists
and engineers, so why can’t we create success stories like those? ‘Brain drain’
is part of the problem, with many Australians moving overseas to America
(or other places) chasing better prospects (including me, briefly).
A lot of it comes down to risk vs reward, including both ends of that
equation. In terms of risk, American and European investors are more willing
to bet their money by investing in up-and-coming technologies and concepts.
Australians seem to view the stock market as a kind of bank account, especially
now that we have enforced superannuation, and demand low risk (and get
relatively low returns as a result).
Many people turn up their noses at rich people, but it’s the drive to
become one of them that has made so many people work hard to create the
foundations of modern life.
Dick Smith did this when he created Dick Smith Electronics (his ex-senior
manager, the late Gary Johnston, did it again with Jaycar Electronics). Dick
decided to ‘quit while he was ahead’, unlike many others in his position, but
that’s beside the point; his desire for money and success drove him to create
something valuable more than once.
But younger generations (and this includes me) have mostly been raised
in a cocoon, never being allowed to take many risks. I don’t think I’d have
the guts to do what Dick or Gary did. I’m not sure I could have even created
Silicon Chip from scratch like Leo Simpson and Greg Swain back in 1987,
even though I seem to be able to keep the magazine going just fine.
Unless we allow young people to use (and hone) their judgment responsibly
and learn how to weigh up risks and rewards, I don’t see how we can compete
on the global business and technology stage. And that can’t happen if we
don’t allow people to use their judgment.
Innovation and risk-taking are activities that often go hand-in-hand. How
many realise that there is risk in the act of not taking any risks? You miss
many opportunities when you’re laser-focused on the negatives and ignore
the potential positives.
We wouldn’t be where we are today if our ancestors were huddled in caves,
scared to go out into the dangerous world. Some of them took journeys of
thousands of kilometres in small canoes to settle far-off lands; they didn’t even
know if, or when, they would see land again. Imagine having the fortitude
to do that! And we’re pretty much all descended from those brave explorers.
by Nicholas Vinen
24-26 Lilian Fowler Pl, Marrickville 2204
2
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
siliconchip.com.au
Australia's electronics magazine
January 2022 3
MAILBAG
your feedback
Letters and emails should contain complete name, address and daytime phone number. Letters to the Editor are submitted on the condition that
Silicon Chip Publications Pty Ltd had the right to edit, reproduce in electronic form, and communicate these letters. This also applies to submissions to “Ask Silicon Chip”, “Circuit Notebook” and “Serviceman’s Log”.
What to do with historic electronic gear
I have come across an old PMG test
instrument in the family storeroom –
the old Gracemere Station office. It is
an AWA Type R667 Capacity Unbalance Measuring Set. A calibration note
attached to the lid is dated 15/2/68,
but the instrument might be older than
that (see the images below).
I have little idea what it was for; I
presume for improving crosstalk in
either open-wire lines or cables. I have
not opened it, so I don’t know what
is in it. It has a vernier dial reading
Capacity in uuF/nF (I think – not very
clear). It has a battery compartment –
again, I have not opened it, but I suspect it has some active components –
valves, I presume. It also has two mic
earpiece headsets.
I don’t have any idea how it came
into the family. It is in Rockhampton but I live in Brisbane. It is secure
where it is, but there may be a more
appropriate place for it to live, such
as a museum. Do you have any suggestions?
Patrick Durack,
Ashgrove, Qld.
Comments: we aren’t sure what to do
with this device but perhaps one of
our readers has a suggestion.
4
Silicon Chip
USB Cable Tester & SMD Test Tweezers
What a challenge, especially with
soldering the USB-C ports. I completed
the USB Cable Tester (November &
December 2021; siliconchip.com.au/
Series/374) without any soldering
remediation or fault finding, and it will
be useful on my hobby bench.
My soldering skills and techniques
were definitely tested and improved.
This experience highlighted that traditional magnifiers now need to be
supplemented with a digital scope for
quality control, although my phone
camera set to super macro assisted
this time.
The recent SMD Test Tweezers project (October 2021; siliconchip.com.au/
Article/15057) is also a great and useful project and was a fun build.
Barry Hinz,
Charleville, Qld.
Farewell Geoff Nichols
Those who followed ETI Magazine
would have been familiar with Geoff
as a staff member/Project designer.
My good friend Geoff passed away
on the 19th of October, aged 64, of pancreatic cancer.
Craig Laybutt,
North Ryde, NSW.
Australia's electronics magazine
Test Tweezers survived reverse polarity
I am delighted to report that you
can insert the battery the wrong way
and it will still work after correcting
that error!
Horst Leykam,
Dee Why, NSW.
Comment: We believe that it’s possible for a new CR2032 cell to supply
more current (100mA) than the maximum specified for the microcontroller’s clamp diodes (20mA). However, it
may be that components in the OLED
module are also shunting current.
PICs are pretty robust and will generally withstand much higher currents
than the maximum ratings if they are
of limited duration.
Beware of fake solar panel ratings
I bought a solar panel from a toprated seller on eBay. The panel was
rated at 200W, but after receiving it, I
became suspicious that its rating was
incorrect.
I later realised that the panel was
unusually cheap for 200W, a warning
sign I should have paid more attention to.
The panel measures 0.58m2 (820 x
710mm). This is smaller than is physically possible for a 200W panel.
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FEBRUARY 2021
37
Helping to put you in Control
ESP32 Controller
Arduino-compatible ESP32 controller with
2 relay outputs, 2 transistor outputs, 2
opto-isolated inputs, 2 0/4-20 mA analog I/
Os, 2 0-10 VDC analog I/Os and 4 GPIOs.
Interfaces using USB, RS-485 serial, I2C,
Wi-Fi or Bluetooth. DIN rail mountable.
SKU: KTA-332
Price: $251.90 ea
CS Series Closed-Loop Stepper Driver
Closed-loop stepper motor driver with encoder
feedback input and encoder A/B/Z outputs.
Operating at 20-50VDC, max 7A output current.
Suits 2 phase CS Series Closed Loop Stepper
Motors.
SKU: SMC-162
Price: $215.60 ea
Low transformer output mystery solved
Ethernet Closed Loop Stepper Driver
CS3E-D507 is a new Ethercat closed-loop stepper
motor driver with encoder feedback input, operating at
20-50 VDC. Suits 2 phase stepper motors up to 7.0 A.
Has digital inputs and outputs for control such as limit
switch and brake.
SKU: SMC-171
Price: $439.95 ea
CS Series Closed-Loop Stepper Motor
3.0 N·m, 2 Phase NEMA 24 closed loop stepper
motor with 1,000 line encoder for feedback.
Rated at 5.0 A phase current, Nema 17 to
34 sized motors available and 8.0 mm shaft
diameter.
SKU: MOT-162
Price: $202.29 ea
Liquid Level Sensor Detector
A budget priced level sensor for detecting high
and low levels of water in plastic and glass
vessels or tanks.
SKU: HEI-140
Price: $19.20 ea
LogBox Connect WiFi
LogBox Wi-Fi is an IoT device with integrated
data logger and Wi-Fi connectivity. It has three
universal analog inputs one digital input and an
alarm output.
SKU: NOD-012
Price: $604.95 ea
N322-RHT Temperature and RH Controller 230 VAC
Panel mount temperature & relative humidity
controller with sensor probe on 3 metres of
cable. 2 independent relay outputs. 100 to
230 VAC powered.
SKU: CET-109
Price: $290.35 ea
For Wholesale prices
Contact Ocean Controls
Ph: (03) 9708 2390
oceancontrols.com.au
Prices are subjected to change without notice.
6
Silicon Chip
A general figure for solar irradiance at the surface in
Australia is 1100W/m2. The quoted panel efficiency was
17%, which seems reasonable. We can therefore calculate 0.58m2 × 1100W/m2 × 17% = 108W.
Allowing for empty space, this is probably a 100W panel
being incorrectly sold as a 200W panel.
I also made some electrical measurements. The
short-circuit current is 5.84A in peak sunlight. According to the label on the panel, peak power is at 18V. This
means that the panel can generate no more than 105W.
The open-circuit voltage measured 21.7V.
The sticker on the panel does not show the power rating or short-circuit current, which is most unusual.
The situation was somewhat resolved by the seller
refunding half the purchase cost after I presented these
facts. The panel was worth keeping as it seemed to be of
good quality for a no-name panel.
But many purchasers of solar panels would not be aware
they are getting much less than they paid for. I wonder
how common such fraud is.
Dr David Maddison, Toorak, Vic.
I read the Vintage Radio article in the November 2021
issue of Silicon Chip by Graham Parslow with great interest (siliconchip.com.au/Article/15107). Graham writes in a
relaxed yet informative style, easy to read and with plenty
of detailed photos. I always enjoy his articles.
Graham describes the restoration of a Stromberg-
Carlson model 496 autodyne superhet receiver from 1936.
The cabinet looks stunning and the knobs look the part
too. It’s a real shame the electrodynamic speaker was
unable to be repaired; a reality faced by restorers from
time to time.
Graham mentioned the problem experienced with
the 6.3V heater voltage winding running at 4.9V. This
could be explained by the 6V6 heater being connected
to the 6.3V winding. For example, the 6C6 and 6F7 each
draw 0.3A heater current and the two dial lamps draw
0.3A each, for a total specified loading of 1.2A for the
6.3V winding.
Adding the 0.45A heater current required by the 6V6
modification takes the total load on the 6.3V winding to
1.65A, an increase of 37% above the power transformer’s
1.2A load specification. This could explain why the 6.3V
winding voltage has dropped to 4.9V.
Graham mentioned that this particular radio was manufactured before the 6V6 became available, so I presume
it was manufactured with an AL3 output valve, per the
circuit. Graham stated he received the radio with the 6V6
fitted. To improve the originality of the radio, the retrofitted 6V6 and socket could be removed and replaced with
an AL3 and suitable socket.
This would require the AL3 heater to be wired to the
4V winding, which would also remove the additional
loading on the 6.3V winding. That should allow the 6.3V
winding voltage to return closer to the specified 6.3V figure, overcoming the low heater voltage problem Graham
reported, as well as increasing the originality of this very
nicely restored radio.
Graeme Dennes, Bunyip, Vic.
Graham Parslow responds:
I took some measurements of the 6.3V winding with
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8
Silicon Chip
various loads after receiving the suggestion from Graeme
Dennes. Graeme was correct in his analysis; the winding
cannot cope with the load imposed on it with the 6V6
added. I did not consider this initially because most comparable 6.3V windings can handle multiple amps.
In hindsight, looking at the gauge of the winding, it is
thinner wire than usual (this was not immediately evident
due to being sheathed in spaghetti tubing). I measured
a 5.7V output when loaded with just the two 0.3A dial
lamps; the low voltage is no longer a puzzle.
What is padder feedback, really?
In researching radio designs, I have often come across
the term “padder feedback”. There are plenty of references that explain its purpose (to improve local oscillator activity and reliability), but I have not found any good
explanations of its principle of operation.
It looks like the classic Armstrong oscillator, which puts
a feedback transformer between anode and grid. The classic circuit sees one end of each winding (anode and grid)
return to RF ground: the anode winding to decoupled HT,
the oscillator winding to circuit ground.
The only common variant returns the secondary to
ground via the padder. Since this puts the padder in
series with the inductor, its effect is identical to grounding the secondary and connecting the padder between
the secondary’s ‘hot’ end and the oscillator tuning gang
section. This has the advantage of returning one end of
the padder to ground, minimising ‘hand effect’ during
alignment.
But the padder feedback circuit sees the two cold ends
joined (either directly or via a capacitor; C14 in the Astor
Mickey Oz circuit, see page 80 of this issue for example)
and returned to ground via padder capacitor C12.
Whatever this forms, it is not a true Armstrong oscillator. Is it some kind of Hartley oscillator (two inductors, L5
& L6, with mutual coupling), a modified Colpitts (padder
C12 and tuning capacitor C10 with a single inductor L5),
or a pi-filter resonant circuit (padder C12, inductor L5
and capacitor C10), as used in permeability-tuned radios
(essentially a Colpitts oscillator)?
If it is a Colpitts oscillator, why bother with the transformer primary? I trust that someone is less confused
than I am!
Rather than clog the Editor’s inbox, readers who can
explain its principle/s of operation might reply to me at
the email below.
Ian Batty, Rosebud, Vic. – ianbatty311<at>gmail.com
Hydrogen as a storage medium for renewals
As usual, the July, August, and now the September
issues have been worth reading. I was intrigued to see
that you published one of my earlier letters in the September edition. Unfortunately, I have not progressed very
far with the Li-ion battery charging project or any other
projects. It seems that there is almost a limit on how much
a person can do.
It has been almost 40 years since I began experimenting and creating electronic and mechanical devices plus
PC and embedded programs. I have devised many hundreds of circuits, plenty of mechanical devices, and many
hundreds of programs during that time. It seems that the
effort has caught up with me.
Australia's electronics magazine
siliconchip.com.au
Design Contest Win $500+
Dick Smith challenges you
Win $500 by designing a
noughts-and-crosses machine
that can beat 14-year old me!
Dick Smith has described in his new autobiography how one of
the turning points in his life, at age 14, was successfully building a ‘noughts-and-crosses
machine’ (also known as tic-tac-toe) that could play the game as well as anyone. Keep in mind that
this was in 1958, when nobody had computers; it was a purely electromechanical device.
Email Design to Enter
Design your own noughts-andcrosses circuit and send your
submission to compo<at>siliconchip.
com.au including:
a) Your name and address
b) Phone number or email
address (ideally both)
c) A circuit or wiring diagram
which clearly shows how the
device works
d) The display can be anything as
long as it’s understandable
e) Evidence that your device can
always play a perfect game (it
never loses)
f) A video and/or supply images
and text describing it
g) Entries requiring software
must include source code
The deadline for submissions is the
31st of January 2022.
➠
➠ Win $500 + Signed Copy of Dick Smith's Autobiography
➠
Four winners to be decided, one
each for the following categories:
➊ The simplest noughts-andcrosses playing machine
most ingenious noughts➋ The
and-crosses playing machine
youngest constructor to
➌ The
build a working noughts-and-
DICK
SMITH
crosses playing machine
most clever noughts-and➍ The
crosses playing machine not
using any kind of integrated
processor
The entry we judge overall to be
the best will also be featured in
our Circuit Notebook column and
receive an additional $200.
‘Part Bear Grylls, part Bill Gates,
but
Dick is a great innovator, philanth 100% Aussie larrikin.
ropist and adventurer,
who in my eyes can do no wrong.’
PAUL HOGAN
Conditions of entry
Dick Smith writes
1) You must be a resident of
Australia or New Zealand
2) One entry per family (Silicon
Chip staff and their families
are not eligible)
3) Submissions will be confirmed
within 7 days. If you do not
receive a confirmation of your
submission, contact us to
verify that we have received it
4) Chance plays no part in
determining the winner
5) The judges’ decision is final
6) The winners will be decided by
the 3rd of February 2022 and
will be notified immediately
By 1958 I’d advanced from building crystal radio sets to designing
and building what I called a noughts and crosses machine. It really
was an early computer. I used second-hand parts from a telephone
exchange to build it. It would play noughts and crosses against anyone
and no one could beat it.
This was a great boost to me, because while I was no good at rote
learning and theory, I was fine at practical things. The fact that my mind
was capable of working out how to build this complex machine gave
me confidence as I left school. Now I just had to find a job.
Because this was such a turning point in his life and he’s so
enthusiastic about youngsters learning electronics, he’s putting up
$2000 of his own money to award to people who can come up with
a modern version of his noughts-and-crosses machine. Silicon Chip
will judge the entries.
Winners will be announced in the March 2022 issue of Silicon Chip
magazine and will also be contacted directly for payment information.
siliconchip.com.au
Australia's electronics magazine
January 2022 9
I used to wonder why authors of novels would need to
take substantial rest after writing a novel. Now I know.
Currently, I am finding it hard to do anything involving
electronics and/or robotics. Instead, I have been catching
up on home maintenance and seriously overdue home
projects. Hopefully, in the near future, my electronics
drive will return.
On another topic, there is a problem with the storage
of solar energy using batteries of any type, and that problem occurs when the batteries are fully charged. There is
almost certainly more energy available but it cannot be
stored. However, immediate conversion of solar energy
into hydrogen avoids this problem.
Storage tanks are far cheaper than electrochemical cells.
They do not suffer significantly from cycling, nor do they
suffer from over-discharge. More storage is simply changing to a bigger tank or adding more tanks.
Currently, both electricity-to-hydrogen and hydrogen-
to-electricity converters are available off the shelf. Storage tanks almost certainly would be available as well; if
the high leakage of steel can be tolerated, steel tanks are
readily available.
The main reason for bringing this subject to your attention is that solar energy storage via hydrogen is at the
stage where it is feasible for hobbyists to make their own
systems.
Of course, there are safety concerns, and I have no doubt
that our governments’ health and safety departments will
react in their usual “it’s dangerous” manner.
But hydrogen is far safer than LPG with the ability of
hydrogen to rapidly disperse upwards and not lay around
the lower levels of a house. It is unnecessary to store
hydrogen at very high pressures, and a physically large
tank is not a problem like it is for vehicles.
An external installation in a well-ventilated enclosure
should be far safer than any current fuel storage schemes,
except perhaps fuel oil, coal, coke and wood.
George Ramsay, Holland Park, Qld.
Comments: Most city dwellers, even those with a house,
might disagree about your statement that the size of a
hydrogen storage tank is not a concern. Also, safety concerns aside, the round-trip energy efficiency is not likely
to be that great.
Regarding motivation, try working for an electronics
magazine where you have to come up with and complete
four or so project articles per month. Somehow we’re not
only still coming up with new ideas (admittedly, in many
cases, improved versions of previous ideas), but we’re
turning them into working prototypes and documenting
them after all these years.
Article on electric vehicle charging
I recently sent you an email relating to the logistics of
charging multiple electric vehicles (EVs) in a suburban
front yard. I don’t know whether this topic piqued your
interest, but here is a link to an ABC article that relates
to EV charging and the future of service stations: www.
abc.net.au/news/100627312
The broader issue becomes providing the appropriate domestic and public infrastructure to support an EV
based transport sector.
David George,
Montmorency, Vic.
SC
10
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A ll A bout
Part 1:
by Dr David Maddison
batteries
Batteries
Imagine life without batteries. We’d have to crank-start our
cars; we’d be stuck with fixed phones, non-portable computers,
no interactive toys for kids... the list goes on. But you can’t take
batteries for granted either. This series will cover just about
Background Source:
everything you need to know about batteries.
https://unsplash.com/photos/F_EooJ3-uTs
B
atteries are one of our most
important technologies. Today,
nearly everyone carries a smartphone, and its rechargeable battery is
expected to last all day (or sometimes
two or three), even with several hours
of active use. Many people also have an
electronic watch, an electronic key for
their car and possibly even electronic
implants like a heart pacemaker.
Little thought is given to such
devices until the battery inevitably
fails.
Two other important uses for largescale batteries today are electric cars
and storage for intermittent electricity
production.
In this article, we will look at the
history of batteries, how they work,
some interesting or common types and
possible future developments. We will
also look in detail at how some of the
more common battery types from the
past work.
Two following articles will have
more details on lead-acid batteries
and other battery types, information
12
Silicon Chip
on vehicle batteries, battery monitoring and miscellaneous extra facts
about batteries.
in this article. Still, we prefer “cell”
when referring to one cell or “battery”
for multiple.
Terminology
The perfect battery
Any discussion of batteries has to
distinguish between electrochemical
cells and batteries. A cell is the basic
unit of a battery and uses a chemical
reaction to produce electrical energy.
A battery is a collection of multiple
cells connected together, usually in
series, to produce a higher voltage than
an individual cell – see Fig.1.
Cells can also be paralleled to
increase the maximum charge/discharge current and sometimes are
connected in series/parallel to form a
high-voltage, high-current pack.
A typical example of a cell is a standard AA-size alkaline 1.5V cell, often
erroneously referred to as a “battery”.
The 9V batteries used to power smoke
alarms are actual batteries, usually
having six internal 1.5V cells in series.
Given that it is common terminology,
we might use the term battery for cell
A perfect battery might have the following characteristics:
• be made from inexpensive,
non-exotic materials using simple
manufacturing processes
• be non-toxic when disposed of
• be recyclable
• be rechargeable a large number
of times
• provide a useful voltage, not too
high or low
• work consistently over a wide
range of temperatures, including
polar or desert regions as well as
at room temperature
• provide a long life
• be fast to recharge
• be tolerant of high discharge currents
• can be fully discharged safely and
repeatedly
• have low weight
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• be compact for its capacity
• survive a large number of charge
and discharge cycles
• have low self-discharge in storage
• will not leak
• have a relatively stable voltage
during discharge (ie, a small difference between fully charged
and fully discharged voltages)
• will not catch fire or explode even
if misused or badly damaged
Of course, there is no perfect battery. Like all engineering solutions,
every battery type has advantages and
disadvantages and will meet some of
the above criteria, but never all (yet!).
How does a battery work?
A battery (more precisely a galvanic
or voltaic cell) is a device that stores
energy in chemical form and converts
it to electricity via a chemical reaction. There are usually two interfaces
to conductors (ie, anode and cathode),
and a current flow is created due to the
motion of electrons. This is known as
an electrochemical or redox reaction.
Two reactions are involved; one is
called oxidation, the other is called
reduction and there is an external
electron flow. This is different from
ordinary chemical reactions, in which
electrons are also exchanged between
atoms or ions but in a bulk volume,
with no electrodes. In that case, there
is no net flow of electrons or current.
A discharging battery works spontaneously, ie, nothing is required to
start the reaction. The chemical process is known as a spontaneous redox
reaction. Not all electrochemical reactions are spontaneous, so not all can
be used for a battery.
When the battery is discharging, the
positive terminal is called the cathode
and the negative terminal the anode.
The negative terminal is the source of
electrons that flow through an attached
electrical circuit to the positive terminal (see Fig.2).
During oxidation, a chemical species loses one or more electrons,
while in reduction, the chemical species gains one or more electrons. In a
discharging galvanic cell, oxidation
occurs at the anode. That is, electrons
are lost, and this is the source of the
electrons for the negative terminal.
During discharge, reduction also
occurs at the cathode. That is, electrons are gained, and the cathode is
the positive terminal (www.ausetute.
com.au/pbbattery.html).
siliconchip.com.au
Fig.1: a cell (above) is a single
electrochemical cell, generating
something like 1-4V via a chemical
reaction between the anode and
cathode. A battery (right) consists of
two or more cells, usually connected
in series (but sometimes in parallel or
series/parallel), generating a multiple
of the cell voltage.
Fig.2 (below): the electrode
designations, current flow and
electron flow of a secondary cell
during discharging and charging.
Electrons are labelled as “e−”.
Original source: Wikimedia user
Electroche (CC BY-SA 4.0)
An alternative way to state the above
is that oxidation involves the loss of
electrons and always occurs at the
anode, while reduction involves the
gain of electrons and always occurs at
the cathode. The polarity of the anode
and cathode (+ or −) is determined by
which way electrons flow or current
flows during charging and discharging.
Main battery categories
Batteries are classified as either primary or secondary types.
A primary battery can be used
once until it is exhausted and is not
designed to be recharged. The chemical reactions are not generally easily reversible. AA or AAA ‘alkaline’
cells are a typical example. Note,
though, that limited recharging might
be possible, even if not generally
Australia's electronics magazine
recommended. We will discuss that
later.
A secondary battery is designed to
be recharged multiple times; its chemical actions are reversible by applying
a reverse current to recharge the battery. An automotive lead-acid battery
is a typical example. Secondary batteries eventually wear out and have
to be disposed of, recycled or remanufactured because the internal electrodes corrode or the structure of the
cell deteriorates.
Another less-common type of battery is the reserve battery. These are
used in equipment that is stored for a
long time and then has to be suddenly
activated and used, such as certain
types of military equipment like missiles. One way to activate such a battery is to add the electrolyte just before
January 2022 13
Fig.3: the Baghdad Battery with a
disputed interpretation assuming
it was a battery. The ceramic pot is
14cm tall and has an asphalt plug
at the top, a copper cylinder with
an iron rod inside it immersed in
‘electrolyte’. Source: Wikimedia user
Elmar Samizadə (CC BY-SA 4.0)
Fig.4: an early “battery” of Leyden jars.
Today we would call this a capacitor
bank, not a battery. Benjamin Franklin
pioneered this method and is believed
to have owned this example. Source:
American Philosophical Society
use. Sometimes, car batteries are sold
like this as well (dry).
The Baghdad Battery
An ancient artefact called the
Baghdad Battery dates to somewhere
between 150BCE to 650CE (Fig.3).
Some interpreted it to be an ancient
battery (more correctly a cell), but
there is also evidence to suggest that
it wasn’t.
A copy of this artefact can be made
into a workable cell. The TV show
“Mythbusters” looked at this in Episode 29, first broadcast on the 23rd of
March 2005. They were able to make
a replica Baghdad Battery produce
voltage, but only a fraction of a volt;
they got more voltage by sticking metal
fragments into fresh lemons.
Fig.5: Jesse Ramsden’s frictional plate
electrostatic machine of 1768. It was
not a battery but it could produce
an electrical charge. Leyden jars (as
shown in Fig.4) were used as charge
storage devices. Source: gutenberg.
org/files/35092/35092-h/35092-h.htm
14
Silicon Chip
It could have been something other
than a battery. Still, it happens that the
presence of an acidic solution such as
vinegar enables a current to be generated due to the presence of dissimilar metals.
This object disappeared during the
looting of the Iraq Museum in April
2003 and has not been seen since.
Origin of the term “battery”
Benjamin Franklin first used the
term battery, akin to an artillery battery, in 1749 to describe how he had
linked up Leyden jars, an early form
of capacitor, to store electricity from
his static generator (see Fig.4).
The first battery in Australia
Sir Joseph Banks performed
electrical experiments onboard the
HMS Endeavour, the vessel Captain
James Cook used to explore and claim
Australia. Two electrical machines
were carried. One was made by Jesse
Ramsden (Fig.5), a famous instrument
maker, and the other was a machine
belonging to astronomer Charles Green
and made by Francis Watkins.
Banks and some other gentlemen
amused themselves by giving each
other shocks. Both machines appear to
be frictional plate electrostatic generators. The charge from each was stored
in an ‘electrostatic battery’ (basically a
capacitor bank), in what were presumably Leyden jars (see Fig.6). However,
they were not described by Banks by
that name.
Banks noted “the ill success of the
Fig.6: a drawing of a Leyden jar being charged, in 1746. The jar was
independently invented by German Ewald Georg von Kleist in 1745 and
Dutchman Pieter van Musschenbroek of Leiden (Leyden) in 1745-46. Portrayed
in the drawing is a similar experiment to the one performed by Banks, although
the electrostatic generator uses a rotating glass sphere instead of the disc. The
electrical charge produced is stored in the Leyden jar.
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Electrical experiments”, possibly due
to excessive humidity or moisture.
For those interested, an account of
Sir Joseph Banks’ electrical experiments onboard the Endeavour can be
seen in “The Endeavour Journal of
Joseph Banks” at https://setis.library.
usyd.edu.au/ozlit/banks/banksvo1.
pdf (Fig.7). See pages 81 to 93 of the
PDF document (not the diary page
numbers).
Electrical experiments were performed on the 25th of October 1768
(two months after leaving Plymouth,
England) and then again on the 19th
of March and the 23rd of March 1770.
Cook was still charting New Zealand on the March date and did not
leave New Zealand for Australia until
the 31st of March 1770, so the second
battery experiment was performed in
New Zealand waters. However, the
equipment was brought to Australia,
so it can be argued that it was the first
battery in Australia. Cook landed in
Botany Bay on the 29th of April 1770.
Thanks to S. M. of the State Library
of NSW for their assistance in finding some of the source documents on
this topic.
If you want to perform an experiment similar to what Banks would
have, or see the type of spark that
might have been generated (but using
modern materials), see the video
titled “William Gurstelle shows How
to Build an Electrostatic Generator
and a Leyden Jar” at https://youtu.be/
H5wr1Ishmx0
Fig.7: the cover of the 1747 book by
Francis Watkins on his electrical
experiments. He made one of the
machines brought by Banks to
Australia. You can read this book
online at https://books.google.com.au/
books?id=AzRWAAAAcAAJ
Fig.8: one of Volta’s original
voltaic piles, on display at the
Tempio Voltiano in Como, Italy;
see siliconchip.com.au/link/abbp –
Source: Wikimedia user GuidoB (CC
BY-SA 3.0)
The first true battery
Alessandro Giuseppe Antonio
Anastasio Volta invented the first electrochemical battery in 1799, publishing the results in 1800. This is a true
battery in terms of our modern definition of it being an electrochemical
device, not a capacitive charge storage
device like a Leyden jar.
Volta’s original battery or voltaic
pile (shown in Figs.8 & 9) comprised
a column of alternating copper and
zinc discs separated by cloth or cardboard soaked in a brine (saltwater)
electrolyte.
Volta initially misunderstood how
the battery worked. He thought the
electricity was generated by the contact between dissimilar materials.
Later, it became apparent that the corrosion of the zinc discs was related
to the current produced by the battery. Thus, he realised that the battery
siliconchip.com.au
Fig.9: this shows how Volta’s voltaic
pile was constructed. Original source:
Wikimedia user Borbrav, SVG
version by Luigi Chiesa (CC BY-SA
3.0)
Fig.10: a cross-section diagram of the
original Daniell cell. Original source:
Armando-Martin, public domain
worked by an electrochemical process.
Even though the original batteries
produced by Volta were flawed and
only worked for about one hour, they
enabled many new discoveries to be
made.
We will now discuss some of the
more important types of primary batteries, both historical and in current
use. We will look into some of these in
more detail and other types of batteries
in the following article next month.
Batteries after Volta
Primary batteries
Early batteries, including Volta’s,
were primary (non-rechargeable) batteries. Secondary (rechargeable) batteries were developed later.
In 1836, John Frederic Daniell
solved some of the problems with Volta’s battery with the Daniell cell. This
was a copper pot containing copper
Australia's electronics magazine
January 2022 15
Fig.11 (left): the construction of a gravity cell. This particular variant
is called the crowfoot cell due to the shape of the negative terminal.
Original Source: Cyclopedia of Telegraphy and Telephony, 1919
Fig.12 (above): the cross-section of a zinc-carbon battery with
ammonium chloride electrolyte. Original source: Wikimedia user
Mcy jerry (CC BY 2.5)
sulfate into which was immersed a
porous earthenware vessel containing sulfuric acid and a zinc electrode
(see Fig.10).
Ions could pass through the earthenware vessel, but the solutions could
not mix. It produced 1.1V and became
the first practical cell. It was widely
used in the new telegraph networks.
There followed several improvements to the Daniell cell such as Bird’s
cell (1837) by Golding Bird, the Porous
pot cell (1838) by John Dancer and in
the 1860s, the gravity cell by mysterious Frenchman Monsieur Callaud,
whose first name is unknown.
The gravity cell dispensed with the
porous barriers used on Bird’s and
Dancer’s cells, thus giving it a lower
internal resistance and improved current delivery capability.
In the gravity cell, the different electrolytes (zinc sulfate and copper sulfate) are not separated by a barrier but
by gravity due to the different densities of the two electrolytes (see Fig.11).
This gravity separation also renders
the cell unsuitable for mobile applications. Also, a current must be continuously drawn from the cell; otherwise,
the electrolytes will mix.
The gravity cell became standard on
the US and UK telegraph networks and
was in use until the 1950s.
Chromic acid cells were another
type of primary cell developed; one
was the Poggendorff cell. It used zinc
and carbon plates, but the zinc would
16
Silicon Chip
dissolve even when the cell was not
in use, so a mechanism was needed to
lift the zinc out of the electrolyte when
the cell was not in use (see Fig.14).
A further development of the Poggendorff cell was the Fuller cell
(Fig.15). It used mercury to form an
amalgam with zinc to prevent its dissolution.
Later came the Grove cell (1839)
comprising zinc, sulfuric acid, platinum and nitric acid and the Dun cell
(1885) comprising iron, carbon and
a mixture of hydrochloric and nitric
acids. This mixture is known as aqua
regia; it is a very powerful acid that
can dissolve gold or platinum.
The Leclanché cell was invented
in 1866 by Georges Leclanché. It
consisted of a zinc anode, manganese dioxide and carbon cathode and
ammonium chloride as the electrolyte
(Fig.16). It produced 1.4V.
It was used in telegraphy, telephony,
rail signalling and electric bells. One
disadvantage was that the battery current would diminish during long telephone conversations due to increasing
internal resistance.
In 1886, a variant of the Leclanché
cell was produced by Carl Gassner
in which he mixed the liquid ammonium chloride electrolyte along with
zinc chloride (to extend the shelf life
of the electrolyte) with plaster of Paris
to make a ‘dry cell’ producing 1.5V.
In 1896, the National Carbon Company in the USA developed it further,
replacing the plaster with rolled cardboard. The battery could be used in
any orientation and was maintenance-
free. The first battery they made was a
telephone battery (see Fig.13), and in
1898, the company introduced what
later became known as the D-cell or
‘flashlight (torch) battery’.
These became known as zinc-carbon
cells and were the first mass-produced
battery for widespread use, leading to
the development of the battery flashlight (torch). This type of cell is still
common and available today.
Fig.16: a Leclanché cell. This example is a
Samson No.2 brand ammonium chloride,
zinc and manganese dioxide/carbon battery,
c.1906-1916. Such a battery is also featured
in the 25th catalogue of Manhattan Electrical
Supply Co. c.1910. The complete battery sold
for US$1.60 and all parts were replaceable.
Source: Harvard University, The Collection of
Historical Scientific Instruments
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Fig.13: Columbia Gray Label dry cell
telephone batteries of the type first
produced by the National Carbon
Company. It isn’t known when
these were made, but they bear the
Eveready trademark, so they must
have been made after 1917 when
Union Carbide acquired Eveready.
This type of battery was produced
until at least the 1950s.
Source: www.flickr.com/
photos/51764518<at>N02/36670011780
(Creative Commons)
In parallel with these developments, in 1887, another dry battery
based on the Leclanché cell was developed independently by Dane Wilhelm
Hellesen.
Sakizou Yai of Japan also developed
a dry cell in 1887 (said to involve carbon and paraffin), which were used
with great success in the Sino-Japanese
war of 1894-95, earning him the title
“king of the dry battery”. He established a battery factory in 1910.
Improvements were made to the
zinc-carbon cell over the twentieth
century, including about a fourfold
capacity increase. Other improvements were a longer shelf life, better
sealing and the use of less toxic components, such as the elimination of
mercury.
Standard zinc-carbon batteries use
Fig.14: the Poggendorff cell, described
as a “Student’s Plunge Cell”. Source:
25th catalogue of Manhattan
Electrical Supply Co. c.1910, page 176
Fig.15: the Fuller cell, both regular and
high-current versions. Source: 25th
catalogue of Manhattan Electrical
Supply Co. c.1910, page 173
an ammonium chloride electrolyte
with possibly some zinc chloride.
“Heavy-duty” cells use mostly zinc
chloride as the electrolyte. A heavyduty battery has about twice the capacity of a standard battery. However,
zinc-carbon cells have been mostly
replaced these days by the alkaline
variety, which have about eight times
the capacity (see below).
zinc reacts to produce two electrons
and is consumed during discharge.
The electrons flow through the external load to the cathode, where the
manganese dioxide reacts with either
ammonium chloride or zinc chloride
(or both).
The reaction for batteries with an
ammonium chloride electrolyte is:
Chemistry of zinc-carbon cells
A zinc-carbon cell comprises a zinc
‘can’, which constitutes the negative
terminal or anode of the cell and a
carbon rod with manganese dioxide,
which is the positive terminal of the
battery or cathode – see Fig.12. The
electrolyte is either ammonium chloride or zinc chloride (or a mixture).
Regardless of the electrolyte, the
Zn + 2MnO2 + 2NH4Cl ⇌
Mn2O3 + Zn(NH3)2Cl2 + H2O
The reaction for batteries with a zinc
chloride electrolyte is:
Zn + 2MnO2 + ZnCl2 + 2H2O
⇌ 2MnO(OH) + 2Zn(OH)Cl
This type of battery is widely available in the AAA, AA, C, D and PP3
(9V) size formats – see Fig.17. These
batteries have a typical voltage when
Fig.17: a selection of modern disposable consumer batteries. L to R, top to bottom they are: 4.5V (3LR12) battery
(primarily used in Europe), D, C, AA, AAA, AAAA, A23, 9V, LR44 and CR2032. There are many proprietary designations
for battery sizes; the ANSI and the IEC establish standard names. Source: Wikimedia user Lead holder (CC BY-SA 3.0)
siliconchip.com.au
Australia's electronics magazine
January 2022 17
Collecting old batteries
Believe it or not, some people
collect old batteries. For some good
examples, visit www.ericwrobbel.
com/collections/batteries.htm
new of 1.55V to 1.7V and are considered flat when they reach around 0.8V
under load.
Alkaline cells
In alkaline cells, the acidic ammonium chloride or zinc chloride electrolyte of regular zinc-carbon batteries is replaced with zinc powder in
an alkaline potassium hydroxide gel.
A current pickup spike forms the negative electrode (anode). The carbon
electrode is replaced with manganese
dioxide with carbon powder to make
the positive electrode (cathode) – see
Fig.18.
A patent for the modern alkaline cell
based on zinc-manganese dioxide was
filed by Canadian Lewis Urry in 1957,
awarded in 1960. Most of the energy
of these cells is contained within the
zinc electrode. The nominal voltage
is 1.5V. They are direct substitutes
for carbon-zinc batteries in common
appliances and come in the standard
sizes of AAA, AA, C, D etc.
The reaction for alkaline zinc-
manganese dioxide cells is as follows:
Zn(s) + 2MnO2(s)
⇌ ZnO(s) + Mn2O3(s)
Standard alkaline batteries are said
to be rechargeable a few times, with
reduced capacity and some risk of
leakage. This practice is not recommended by manufacturers, although
you can find chargers designed for this
purpose, such as the ReZAP charger
(https://rezap.com/) from an Australian company. It also supports various
other battery chemistries.
Some alkaline cells (known as RAM
or rechargeable alkaline manganese)
have been designed to have limited
rechargeability, up to about 10 times.
They are primarily suitable for lowdrain devices. These days, they might
not be cost-effective due to the low
cost of low-self-discharge NiMH cells,
which are rechargeable hundreds of
times.
acid electrolyte. The original design
was improved in 1881 by Camille
Alphonse Faure, who replaced the
cathode with a lead grid into which
lead dioxide was pressed, allowing
multiple plates to be stacked together.
This basic design is still in use.
The lead-acid battery is heavy and
bulky but is relatively cheap and can
produce a very high current for a short
period, making it ideal as a car starting
battery. It is one of the most recycled
of all products, as virtually all parts
are highly recyclable.
We will discuss lead-acid batteries
more, including describing different
versions like gel cells and AGM batteries, in the article to follow next month.
Secondary (rechargeable)
batteries
Nickel-cadmium cells
Primary batteries have the obvious disadvantage that they must be
replaced (or in early types of primary
batteries, various components had to
be replaced) once they are depleted.
Replacing them with rechargeable batteries would, in the long term, reduce
both cost and waste products.
Lead-acid batteries
The first rechargeable battery was
invented in 1859 by Gaston Planté,
based on lead-acid chemistry. This is
still popular today, used in car starting batteries, backup power systems,
emergency lighting, UPSs, off-grid systems, caravans, boats and more.
These comprise a lead anode and
lead dioxide cathode with a sulfuric
The NiCd, nicad or nickel-cadmium
cell was invented in 1899 by Waldemar
Jungner in Sweden. It was a wet cell
using an alkaline electrolyte of potassium hydroxide and was commercialised in 1910, being introduced in the
USA in 1946. It was originally a competitor to lead-acid batteries.
Later models were made as sealed
dry cells and were available in the
same form factors as zinc-carbon cells
such as AA, C, D etc. The terminal voltage is 1.2V, which remains relatively
constant during discharge. They are
capable of high discharge rates. Nicad
batteries are also robust and tolerant of
deep discharge and can even be stored
in a fully discharged state. They have
a longer life than lead-acid in terms of
lifetime charge and discharge cycles.
Fig.18: a cross-sectional diagram of an alkaline cell, the most
common type of primary cell used today. Original source:
Wikimedia user electrical4u (CC BY 3.0)
Fig.19: a nickel-hydrogen storage battery for space
applications. This model (21HB-7) is from Russia. It weighs
5kg, has a capacity of 7Ah, a working pressure of up to
6.2MPa (900psi) and a service life of five years or 25000
cycles at an operating voltage between 21V and 325V. Source:
https://ueip.org/
18
Silicon Chip
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A common myth surrounding nicad
cells is that they suffer a “memory
effect” where a battery will “remember” an incomplete discharge followed
by a charge and suffer a voltage drop
when the battery is again discharged to
the point of the incomplete discharge.
The authors of the original paper that
claimed this retracted it.
Nicads were once common in
mobile phones, power tools and other
portable devices but were supplanted
by NiMH types (described below),
which themselves have been superseded by lithium-ion cells. Their use
has been decreased dramatically,
partly due to the disposal problems of
toxic cadmium and their higher cost
compared to NiMH cells.
Nickel-hydrogen batteries
The nickel-hydrogen battery was
first patented in 1971 and is a specialised battery primarily suitable for
spacecraft such as the Hubble Space
Telescope. They are now being considered for stationary storage applications. They can be regarded as a
hybrid battery, with elements of both
an electrochemical cell and a fuel cell.
They operate at high pressures
within a vessel, and use nickel as the
positive electrode and a hydrogen fuel
cell as the negative electrode – see
Fig.19. They contain nickel, hydrogen in gaseous form at a pressure of
up to 8.2MPa (1200psi) and potassium
hydroxide as electrolyte.
They have an energy density of
about one-third that of a lithium battery; their main advantage is long service life. They also have a relatively
high self-discharge rate, but this is
not a great concern in space, where
the battery is regularly recharged in
orbit as the solar cells exit the earth
shadow.
As the battery discharges, the hydrogen pressure drops. A single cell has
an open-circuit voltage of 1.55V. The
NiH2 batteries on the Hubble Telescope were replaced after 18 years,
although they were still working with
only some loss of capacity. They were
designed to last just five years.
Nickel-metal-hydride cells
Nickel-metal-hydride cells (NiMH)
are now a common rechargeable type,
replacing nicad cells in consumer
items. They are available in standard
sizes such as AAA, AA, C, D etc. They
are similar to nicads, using a positive
siliconchip.com.au
Fig.20: the structure of a NiMH cell. The electrodes are rolled up in what is
known as a “jelly roll” construction, common in many rechargeable cells such
as 18650s. Source: Radio Shack
nickel electrode, but instead of cadmium for the negative electrode, they
use a hydrogen-absorbing metal (see
Fig.20).
They have two to three times the
energy density of nicad, but still lower
than lithium-ion, and are relatively
non-toxic. Their nominal voltage is
1.2V, and they can typically replace
alkaline cells. They were invented
in 1967 but weren’t released onto the
consumer market until 1989.
The first commercial NiMH batteries had a significant self-discharge
rate of 0.5-4% per day, but in 2005,
Sanyo developed a low-self-discharge
battery under the Eneloop brand that
had a capacity of 70-85% after one
year. The low self-discharge is due to
thicker separators between the positive and negative electrodes, but this
means less room for active materials
and thus lower capacity.
A low self-discharge AA cell might
have a capacity of 2500mAh and a regular one, 2700mAh. Panasonic took
over ownership of Sanyo in 2009, and
FDK Corporation now produces NiMH
batteries for Panasonic.
Before lithium-ion batteries became
commonplace in electric vehicles
(EVs), NiMH cells tended to be used,
such as in the General Motors EV1 and
early Toyota Prius models.
Nickel-iron (Edison) batteries
The nickel-iron or NiFe battery
has nickel(III) oxide-hydroxide positive plates and iron negative plates,
an alkaline electrolyte of potassium
hydroxide, and a nominal cell voltage of 1.2V – see Fig.21. They were
invented by the Swede Waldemar Jungner in 1899, when he substituted the
cadmium in nicad batteries for lower-
cost iron.
The best disposable batteries
Disposable AAA, AAA, C, D and 9V batteries from the “big two” (Duracell
and Energizer) are generally good but don’t ignore batteries and cells from
other sources. We have had success with cells from Aldi or Varta cells from
Bunnings, where 30 AA or AAA cells can be had for less than $10.
Australia's electronics magazine
January 2022 19
Safety warning for lithium button cells
Always store and dispose of lithium button cells correctly, keeping them
away from children and pets. If ingested by children or pets, gastric juices
can corrode the battery case and cause the harmful contents to leak out
and cause chemical burns. Current flowing between the terminals can also
damage internal tissue.
disadvantage, but which may be an
advantage, as we will now discuss.
Proponents of intermittent energy
sources like wind and solar power
are investigating nickel-iron batteries
because they can store energy and produce hydrogen as a byproduct. They
continue safely making it even when
the batteries are fully charged (continued charging would harm most batteries). The hydrogen can be used later
as a fuel – see Fig.22.
Such batteries are called battolysers,
a combination of a battery and an electrolysis cell. A battolyser is better than
an electrolytic cell for making hydrogen because there is minimal cell degradation with the battolyser; in fact,
the battery improves in capacity once
it has been used to produce hydrogen
when fully charged.
He patented the invention but abandoned development because of lower
charging efficiency and excessive
hydrogen production. In the USA,
Thomas Edison patented the NiFe
battery in 1901. He saw it as the ideal
battery for electric vehicles (the preferred type of car in the early 1900s)
and superior to the lead-acid battery.
As internal combustion engines
became popular, Edison was disappointed that his battery was not chosen as the starter battery in such vehicles. At the time, his batteries could
be charged faster and had a higher
energy density than lead-acid batteries. However, they performed poorly
in cold weather and were also more
expensive.
Despite not being adopted in motor
vehicles, Edison batteries (as they were
also known) were produced from 1903
to 1972 by the Edison Storage Battery
Company. They had a wide range of
applications such as in railroads, forklifts and backup power. These batteries
are still available today, made by other
companies, and can be suitable for offgrid power systems, among other uses.
NiFe batteries have the advantages
of cheap materials, long life, durability, high depth-of-discharge (80%), tolerance of overcharging/overdischarging and short circuit resistance. While
somewhat more expensive than leadacid and lithium-ion batteries for the
same total energy storage, they have a
claimed lower cost over their lifetime,
which can be 50 years or more.
Modern NiFe batteries also have a
wide temperature tolerance, working
from -30°C to +60°C.
Due to their high self-discharge rate
(1% per day), it is best to use them in
situations where they are frequently
recharged.
Disadvantages include:
• not being maintenance-free; they
have to be checked and topped up
regularly but do not need to be
‘equalised’ like lead-acid batteries
• lower energy density than leadacid batteries (although the high
depth-of-discharge helps to make
up for this)
• lower charge and discharge rate
due to higher internal resistance
(about five times that of lead-acid)
NiFe batteries produce a lot of
hydrogen during charging, usually a
Fig.21: the Edison nickel-iron battery.
Source: Edison Storage Battery
Company, 1917
Fig.22: the usage scheme for a nickel-iron battolyser. Source: Delft University of
Technology
20
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Australia's electronics magazine
Lithium and Li-ion batteries
At the moment, lithium-ion batteries are in the news more than any
other battery type. They are mostly
standard in consumer devices, phones,
watches, electric cars and many largescale energy storage systems.
Lithium is attractive as an active
material in batteries because of its
low weight, high atomic mobility
(ease of movement through the electrolyte) and its specific electrochemical properties.
Lithium-based primary cells usually contain metallic lithium, while
rechargeable batteries usually contain
siliconchip.com.au
Fig.23: older lithium/iodinepolyvinylpyridine (or Li-I2) batteries,
as used in cardiac pacemakers.
lithium in ion form instead; an important distinction. Lithium primary cells
are sometimes referred to as “lithium metal” to distinguish them from
lithium-ion rechargeable cells. Note
though that rechargeable lithium
metal batteries are being developed
(described next month).
Lithium-based batteries are relatively lightweight, have a high energy
density, low self-discharge, and can
be optimised for either high energy
density (mAh capacity) or high power
density (maximum current that they
can handle). They usually produce no
gas, so they can be fully sealed. However, of all batteries in use, they have
probably been involved in the most
safety incidents.
Lithium-based batteries can be manufactured with a variety of chemistries
and were first commercially produced
in the 1970s as primary cells (non-
rechargeable). Depending on the specific chemistry, their voltage can range
from about 1.5V to 3.7V (or 4.2V fully
charged).
A lithium/iodine-polyvinylpyridine
primary battery was first patented in
1971-72 by James Moser and Alan
Schneider and used in a cardiac pacemaker implanted in 1972. This dramatically improved the life of the device
and reduced its size compared to the
mercury-zinc batteries it replaced (see
Fig.23).
This type of lithium battery is
still in use in pacemakers and other
implanted medical devices today.
They have a terminal voltage of 2.8V
and a high internal resistance of
around 10kW, so they can only be used
for low-current/low-power applications (eg, 1mW), such as pacemakers.
These batteries have outstanding
reliability in their pacemaker application. Battery life is typically 5-15 years,
depending on pacemaker activity.
In the 1980s, there were major
developments towards lithium-based
secondary (rechargeable) batteries. In
1985, Akira Yoshino developed the
siliconchip.com.au
Fig.24: a Panasonic 18650 lithiumion battery taken out of its case. Note
the “jelly roll” construction of the
battery core (green). The 18650 form
factor is very popular in various
applications. Source: Wikimedia user
RudolfSimon (CC BY-SA 3.0)
Fig.25: a lithium-polymer (LiPo)
battery as used in a mobile phone.
Source: Wikimedia user Kristoferb
(CC BY-SA 3.0)
first prototype lithium-ion rechargeable battery based on earlier research
in the 1970s and 1980s by John B.
Goodenough, M. Stanley Whittingham, Rachid Yazami and Koichi
Mizushima.
In 1991, a commercial lithium-ion
battery was then made by Sony and
Asahi Kasei, with a team led by Yoshio
Nishi. In 2019, John B. Goodenough,
M. Stanley Whittingham and Akira
Yoshino received a Nobel Prize for
their work.
In 1997, the first lithium polymer
(LiPo) battery was produced by Sony
and Asahi Kasei. These have a flexible wrapping that can be made in
any desired size and shape rather
than the rigid, typically cylindrical
casing of lithium-ion batteries (see
Figs.24 & 25).
There are numerous lithium-based
battery chemistries, along with a few
common ones (see panel overleaf).
Fig.26 shows the trade-off between
power delivery and cell capacity. The
greater the current delivery, the lower
the capacity.
The negative electrode of a lithium
battery is usually carbon (eg, graphite),
while the positive electrode is a metal
oxide or “polyanion” such as the one
first identified by John Goodenough,
lithium iron phosphate. It is treated
in various ways to make it more electrically conductive. The electrolyte is
a lithium salt in an organic solvent.
For a lithium-ion battery using a
negative carbon (C) electrode and a
positive lithium-cobalt-oxide (LiCoO2)
electrode, the full chemical reaction is
as follows (also see Fig.27). Left to right
Fig.26: the trade-off between energy density and power density for lithium-ion
cells (mostly 18650 size) based upon cathode surface area.
Australia's electronics magazine
January 2022 21
Substituting batteries in old
radios and tape players
Vintage transistor radios and cassette
tape players often need four, six or eight
relatively expensive C or D cells. Modern
AA alkaline cells are usually capable of
powering these devices as well or better
than the C or D cells that were available
in the 1960s or 1970s, when these
devices were designed. All that’s needed
is to buy a “sabot” adaptor, commonly
available online.
Right: this “sabot” adaptor allows a AA cell to be used in place of a C cell.
Other adaptors exist that let you substitute two AA cells for a D cell.
is discharging, right to left is charging.
LiC6 + CoO2 ⇌ C6 + LiCoO2
Because lithium-ion cells can be
easily damaged if overcharged or overdischarged (and in extreme cases can
catch fire or explode), they are generally packaged with protective electronics in each cell or battery. This disconnects them from external circuitry if it
detects a problem such as the voltage
being outside the normal range, high
temperature or excessive current flow
(see Fig.28).
Safety of lithium batteries
Lithium batteries are generally considered safe. Some lithium-ion chemistries, such as LiFePO4 (lithium-ironphosphate), are notably more robust
than others and will withstand abuse
without failing (unless the abuse is
extreme) or catching fire. Regular
lithium-ion and LiPo types are more
sensitive. There have been some notable incidents such as:
September 2010: UPS Airlines
Flight 6, a Boeing 747-400F, crashed
after an onboard fire in a cargo pallet
containing 81,000 lithium batteries
and other material. It is not known
what caused the auto-ignition.
January 2013: there was a problem
with Boeing 787 onboard lithium-ion
batteries catching fire. Fortunately,
no one was hurt, but investigations
revealed a ‘thermal runaway’ event
due to a shorted cell that was attributed
to inadequate quality control at manufacture and inadequate scenario testing by Boeing engineers.
The problem was solved with better
quality control by the battery manufacturer and better thermal and electrical
Fig.28: a battery management circuit,
as used in many lithium cells such
as 18650s, to prevent overcharging,
overdischarging and provide short
circuit protection. Source: Wikimedia
user Oldobelix (public domain)
insulation, along with other changes.
The problem was solved by April 2013,
and the aircraft returned to service.
2016: Samsung Galaxy Note 7
phones were prohibited from being
taken on planes due to a manufacturing fault related to the battery, which
could cause the device to catch fire or
explode after thermal runaway. The
product was recalled, and Samsung
issued software updates that stopped
the phone from being charged at all.
August 2018: Australia’s CASA
(Civil Aviation Safety Authority) has
published a procedure to deal with
lithium battery fires onboard aircraft
– see siliconchip.com.au/link/abbl
July 2021: General Motors
announced a combination of hardware and software alterations to their
Chevrolet Bolt and Bolt EUV cars to
address fire risks. At the same time,
Fig.27: a simplified view of the processes in a lithium-ion battery during charging and discharging.
22
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Common primary
(lithium metal) types:
Figs.29 & 30: Contingency East (emergency services) in Copenhagen developed
this device to contain electric vehicle fires. Source: the Danish Institute of Fire
and Security Technology
they withdrew their previous advice
to park the car more than 15m away
from other vehicles or structures after
12 spontaneous fires in their battery
packs (made by LG). See siliconchip.
com.au/link/abbm
August 2021: there was a large
lithium-ion battery fire in Moorabool,
near Geelong, Victoria, at the Victorian Big Battery (Tesla). It took more
than three days to extinguish. You can
read the report of the investigation by
Energy Safe Victoria at siliconchip.
com.au/link/abbn
The investigation revealed that
“The most likely root cause of the
incident was a leak within the Megapack cooling system that caused a
short circuit that led to a fire in an
electronic component. This resulted
in heating that led to a thermal runaway and fire in an adjacent battery
compartment within one Megapack,
which spread to an adjacent second
Megapack...”
“The supervisory control and data
acquisition (SCADA) system for a
Megapack took 24 hours to ‘map’ to
the control system and provide full
data functionality and oversight to
operators.”
siliconchip.com.au
“The Megapack that caught fire had
been in service for 13 hours before
being switched into an off-line mode
when it was no longer required as part
of the commissioning process. This
prevented the receipt of alarms at the
control facility.”
Container for EV fires
Local emergency services in Copenhagen have developed a container to
place over an electric vehicle in the
event of a battery fire (see Figs.29-30).
A damaged or burning electric car is
lifted into or pushed into the container.
It has nozzles to spray cooling water
and a pump for recirculation.
More on lithium-ion batteries
For more details, see our article
on lithium-ion cells (August 2017;
siliconchip.com.au/Article/10763) &
the article on LiFePO4 cells (June 2013;
siliconchip.com.au/Article/3816).
In the second article in this series,
to be published next month, we’ll
describe quite a few new and upcoming battery chemistries/technologies.
We’ll also have considerably more
detail on lead-acid batteries, which
SC
are still in widespread use.
Australia's electronics magazine
Li-MnO2, 3V
The most common consumer
primary lithium battery
Li-(CF)x, 3V
Used for memory backup and
aerospace applications
Li-FeS2, 1.4V-1.6V
Can replace alkaline consumer
batteries
Li-SOCl2, 3.5V
Works at low temperatures (down
to -55°C), used by militaries,
expensive, hazardous
Li-SO2, 2.85V
Wide temperature range (-55°C to
70°C), used by militaries, toxic,
hazardous
Li-I2, 2.8V
Used for medical implants
Li-Ag2CrO4, 2.6V-3.1V
Used for medical implants
Li-Ag2V4O11 / Li-SVO / Li-CSVO
Medical use, emergency beacons
Li-CuO, 1.5V
Replacement for consumer
alkaline batteries; no longer
popular
Li-Bi2Pb2O5, 1.5V
Replacement for silver-oxide
batteries
Li/Al-MnO2, 3V
Made by Maxell
Common secondary
(lithium-ion) types:
LiCoO2 or LCO (lithium-cobaltoxide), 3.7V
Good overall performance, used
in mobile phones, tablets, laptops,
remote-controlled vehicles etc but
less safe than most other types
NMC (nickel-manganese-cobaltoxide), 3.6V-3.7V
Longer-lived and higher-capacity
compared to LiCoO2; used in
power tools and electric vehicles
NCA (nickel-cobalt-aluminiumoxide), 3.6V-3.7V
Used in electric vehicles (eg. the
Panasonic batteries used by Tesla)
and consumer devices
LiFePO4 (lithium-ironphosphate), 3.0V-3.2V
Robust but lower capacity
density; applications in vehicles,
power tools, backup power
systems etc
January 2022 23
Classic LED
Metronomes
These two Metronome designs simulate
the classic mechanical, invertedpendulum metronome with its batonlike pointer swinging left-and-right,
producing a click at each extreme. Both
designs use only discrete components
and simple logic chips, making them easy
to understand and build. Plus they are
both great projects for a beginner.
By Randy Keenan
I
dislike typical “modern” electronic
metronomes that only click and/or
blink once per beat. I came up with
these designs to better simulate the
mechanical metronomes that I know
and like. Both designs light a series of
LEDs, accompanied by a speaker that
produces beat sounds.
The first design uses eight LEDs and
fits in a standard plastic case, while
the second, slightly more complicated
design has 10 LEDs and uses a custommade timber case. So the latter is a
good project for those readers who
have some woodworking experience.
In both cases, the LEDs are arranged
in an arc and light up in sequence, forward and reverse, to mimic the swing
of an inverted pendulum. A click at
each end of the LED arc further simulates a mechanical metronome. A
typical metronome tempo range is
40-208 beats/minute, a ratio of 5.2 to
one; in these Metronomes, the range
is extended to 36-216 beats/minute, a
ratio of six to one.
Either project is excellent for a
beginner; there are no high-frequency
signals, high voltages or tricky wiring
involved. Nor is there any need to
program a chip with software. However, some measurements and adjustments will be needed to calibrate the
instruments after construction, given
the expected component tolerances.
Two designs
The slightly simpler 8-LED Metronome uses 74HC-series logic ICs
and can be battery-powered, while
the 10-LED Metronome uses CD4000series logic ICs and is intended to be
powered from a plugpack. The two circuits operate similarly: A pulse generator clocks an up/down counter IC at
Fig.1: the 8-LED Metronome is based around three 74HC-series digital logic ICs. The 74HC132 generates pulses at a
selectable frequency. These clock the 74HC191 counter, and its three-bit output drives the eight LEDs via the 74HC137
decoder chip. The remaining three gates in the 74HC132 quad NAND package are used to form a set-reset flip-flop to
reverse the LED chaser’s direction each time it reaches one end, and to generate a pulse from the speaker.
24
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
although it is a different logic chip.
Both versions enable the LEDs at
each end of the arc to flash brighter.
You could also use either of these
circuits anywhere a LED ‘chaser’ is
needed.
LED options
The LED metronome comes in two versions; one with eight LEDs and
another with 10 LEDs (shown in this photo). The case to house it can be as
simple as a small timber frame with a clear plastic panel at the front.
the rate required for the desired tempo.
Another IC decodes the counter value
to light the LEDs sequentially.
A set/reset flip-flop (SR-FF) switches
the counter direction when either end
LED is lit, giving forward and reverse
LED sequences. The click is produced
by ORing the signals to the end LEDs,
followed by a differentiator to shorten
the pulse and a one-transistor amplifier to drive a small loudspeaker.
The block diagrams of the two Metronomes are shown in Figs.1 & 2. In the
8-LED design, the tempo pulse is generated by a Schmitt-trigger NAND gate
(part of a 74HC132). This clocks fourbit up/down counter IC2 (7HC191).
Only three of the four binary outputs
are used to drive 3-to-8-line decoder
IC3 (74HC137) that lights the LEDs in
sequence (eight is the 137’s limit). The
SR-FF is made from two more NAND
gates in the 74HC132.
In the 10-LED design, the pulse is
generated by a CMOS version of the
ubiquitous 555 timer. It clocks fourbit up/down counter IC3 (CD4029)
which drives decoder IC4 (a CD4028)
with 10 outputs. The SR-FF logic is
again provided by two gates from IC1,
There are many options for the LEDs
in these Metronomes. The parts lists
indicate the suggested LEDs, but other
sizes, shapes and colours can be substituted. The two end LEDs could even
be different from the middle LEDs.
However, all LEDs should have
high luminous intensity, ideally at
least 4000mCd (sometimes called
“superbright”). This is to reduce
power consumption. For the 8-LED
Metronome, that maximises battery
life, while in the 10-LED design, it
limits the load on the CD4028 driving IC to a safe level.
Both Metronomes were made using
5mm oval LEDs: green for the 8-LED
version, and red for the 10-LED version. I used oval LEDs because they
glow in a line rather than a dot, providing a more interesting display. 3mm
& 5mm round LEDs are also suitable.
Tinted and diffused lenses look best.
You can use different LEDs from
those specified, but you might need
to adjust some resistor values.
The 8-LED version
The LEDs should be of the same
type and matched; if using different
LEDs at the ends, use matched LEDs
for those two and separately matched
LEDs for the rest. The minimalist circuit is shown in Fig.3 and it works as
follows.
Schmitt-trigger quad NAND gate
IC1d is configured as a pulse generator.
Fig.2: the 10-LED Metronome uses a 555 timer IC instead of a logic-gate-based oscillator as the pulse generator. The
remaining logic ICs are from the 4000-series; a 4029 acts as the up/down counter, while a 4028 is the 4-to-10 decoder that
drives the LEDs. Two of the gates of the 4001 quad NOR IC form the set-reset flip-flop, and the other two gates form the
click pulse.
siliconchip.com.au
Australia's electronics magazine
January 2022 25
The pulse frequency, and thus the
metronome tempo, is determined by
potentiometer VR1, resistors R1 & R2
and capacitors C1-C3.
For an explanation of the operation
of a Schmitt-trigger pulse generator,
see the adjacent panel. Its pulses clock
IC2, an up/down binary counter. IC2’s
outputs are fed to decoder IC3 to light
the eight LEDs in sequence.
The outputs of IC3 and the inputs
of IC1a, IC1b and IC1c use negative
(active-low) logic because IC1 is a
NAND gate rather than a NOR gate
(see the panel on SR-FFs).
The alternative would have been
to use the 74HC7002 Schmitt-trigger
NOR gate with a 74HC237 decoder
and positive logic, but the 74HC7002
is less common and more expensive
than the 74HC132.
When IC3 is counting up, it lights
each LED in sequence, from LED0 to
LED7. When LED7 lights, the low level
at pin 7 of IC3 (Y7) is also applied to
the SR-FF formed by IC1a and IC1b.
This causes pin 6 of IC1b (Q) to go
high, causing IC2 to reverse its direction and count down. Each LED is
now lit in sequence in the opposite
direction. When the first LED, LED0,
is lit, the SR-FF is reset, IC2 reverses
and counts up, and the cycle repeats.
VR2 controls the overall LED brightness. The circuit is designed to make
LED0 and LED7 brighter than the others. The relative brightnesses of the
end-vs-middle LEDs is maintained as
VR2 is adjusted by LED8 or a zener
diode, ZD2. Whenever current is
applied to LED1-LED6, LED8/ZD2 is
in series with that LED, reducing the
voltage across the current-limiting
resistors and thus the LED current.
VR2 could be changed from 500kW
to 1MW to extend the brightness range
down to very dim levels. If you want
VR2 to turn the LEDs completely off
at minimum, fit R3 (300kW), but note
that this creates a large ‘dead zone’ in
the lower range of VR2.
LED8 may be the same type as LED0
through LED7, but for more brightness
contrast between the end and middle
LEDs, use a type with higher forward
voltage such as blue or white, or use a
zener diode of approximately 4.7V. If
you want all LEDs to have equal brightness, fit a wire in place of LED8/ZD2.
Click sounds
When either end LED is lit, the low
level at Y0/Y7 is also sent to IC1c,
which behaves as a NOR gate when
operated in negative logic mode (a low
at either input causes a high output).
Its output is fed to the Click Loudness
control (VR3) and then to a simple
transistor amplifier.
However, the pulse from IC1c is
too long and would cause a click at
the end of the pulse as well as at its
beginning, and the current would be
high during the pulse on-period. To
avoid this, the pulse passes through
C4 and/or C5 to yield a short pulse at
each end of the original pulse, a positive one at the beginning and a negative one at the end.
Diode D1 shunts the negative pulse
so that only the positive pulse is
applied to the base of transistor Q1.
Power supply
This design is powered by a battery
of four AAA cells. 74HC ICs are used
rather than 74HCT or 74LS because
the 74HC series allows a slightly
higher supply voltage, up to 6V. Fresh
standard alkaline AAA cells supply
marginally more than 6V, so the voltage rail for the ICs is limited using
a 47W resistor and a 6V zener diode
(ZD1). Alkaline, dry cell, rechargeable NiMH or Li-ion AAA cells can
be used.
Fig.3: this 8-LED Metronome circuit shows more details than Fig.1. VR2 allows you to set the LED brightness while LED8
or ZD2 reduces the brightness of the middle six LEDs compared to the outer two. Extra capacitors C2-C3 and resistor
R2 allow you to adjust the frequency range to match the beats-per-minute (bpm) range shown on the dial. Additional
capacitor C5 is provided to change how the clicks sound.
26
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Using a Schmitt-trigger gate as a pulse generator
Gate IC1d of the 74HC132 Schmitttrigger input NAND chip generates the
pulses that clock the counter (IC2).
So what is a Schmitt-trigger gate, and
why are we using one?
An ‘ordinary’ non-Schmitt-trigger
gate or inverter is effectively a highgain but mostly linear amplifier. As
a result, the output transition from
high-to-low or low-to-high takes place
over a narrow input voltage range, as
shown in Fig.a, a plot of the output
voltage versus the input voltage.
As a result, the negative-feedback
RC circuit shown in Fig.b will typically
reach equilibrium at some point (E),
with the output ‘stuck’ at an intermediate voltage. If the input were to
increase in voltage, as indicated by
the arrow, the output would respond
by decreasing and would restore the
circuit to point E with a time constant
determined by R and C. The reverse
is true if the input voltage decreases.
You can test this yourself on a
breadboard if you have a spare
74HC00 NAND gate chip. Just
remember to connect all the unused
inputs to one supply rail or the other.
A DVM will show that the voltage at
pin 3 is stable.
In contrast, the Schmitt-trigger version of the gate ensures oscillation
due to its built-in hysteresis and associated positive feedback. This is illustrated in Fig.c, an equivalent plot to
Fig.a but for a gate with Schmitt-trigger inputs.
Once the input voltage increases
above the upper-threshold input voltage (VT+, point U), the output immediately ‘snaps’ to a low level (point
V). It remains there until the input
decreases below the lower-threshold
input voltage (VT−, point L) and the
output ‘snaps’ high (point W).
This can be demonstrated by breadboarding the circuit shown in Fig.d.
Begin with the pot at extreme clockwise (pins 1 & 2 at +6V) and apply
power. The LED should remain off.
Slowly decrease the input voltage via
the pot until the LED goes on; note
the input voltage. Now increase the
input voltage gradually until the LED
goes off. There should be a couple of
volts difference; this is the hysteresis
spread (VT+ − VT−).
You have made one clockwise trip
siliconchip.com.au
Fig.a & b: the transfer function of a standard NOR gate.
The output is low when the input is high and vice versa,
but if the input voltage is intermediate, the output
voltage can be anywhere in between.
Fig.c & d: a Schmitt-trigger inverter has
hysteresis, so once its input voltage is high
enough, the output snaps low and stays low
until the input voltage drops significantly.
Similarly, when the input voltage drops and
the output goes high, it remains high until the
input voltage increases significantly.
Fig.e: the
input & output
waveforms for a
Schmitt-trigger
inverter used as
an oscillator.
around the hysteresis rectangle, as indicated by the arrows in Fig.c.
Because of this, if you substitute
a Schmitt-trigger 74HC132 for the
74HC00 in Fig.b, you will find that it
oscillates, generating a square wave
at the output. The input exhibits an
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exponential pseudo-triangle wave
of amplitude equal to the hysteresis
spread, as shown in Fig.e.
One crucial point to consider is
how the rate of oscillation will vary
with supply voltage (especially in a
battery-powered circuit). As it turns
out, the deceased capacitor charging
current is somewhat compensated by
the decrease in hysteresis spread (as
it is somewhat proportional to the IC’s
supply voltage). Thus, the pulse rate
only changes by a few percent from
6V to 5.5V (an 8% change in voltage).
January 2022 27
The 4700μF and 470μF bulk bypass
capacitors, in combination with the
47W series resistor, reduce the supply
voltage pull-down by the click-pulse
current through the speaker.
As PCB-mounting potentiometers
with built-in switches are rare, a separate power switch is used. A regulated 6V DC plugpack could be used
instead of a battery. Make sure you
verify it is regulated as otherwise, its
output voltage would be too high for
the circuit.
The 10-LED version
The circuit for this version is shown
in Fig.4. It is similar to the 8-LED
version but positive logic is used
throughout. The pulses are generated by CMOS 555 timer IC2. It clocks
IC3, a four-bit up/down counter. IC3’s
outputs are decoded to 10 individual
outputs by IC4, lighting the 10 LEDs
in sequence.
When an end LED (LED0 or LED9)
is lit, the SR-FF formed by IC2a & IC2c
is set or reset, thus switching IC3 into
up or down mode, reversing the LED
sequence.
VR5 controls the LED brightnesses.
Instead of the technique used for the
8-LED design to make the end LEDs
brighter, this version uses a current
mirror comprising Q1 and Q2 with
trimpot VR4, control potentiometer
VR5 and some fixed resistors. VR4
adjusts the brightness of the middle
LEDs relative to the brightness of the
two end LEDs. See the adjacent panel
for an explanation of how this works.
Click generation and circuit variations are the same as for the 8-LED
design. The higher supply voltage of
this version provides a louder click.
Construction
Fig.5 is the PCB layout diagram for
the 8-LED version, while Fig.6 is for
the 10-LED version. Most components
mount on the boards. A few might need
their values tweaked; that is why some
parts do not have an associated value.
Whichever version you are building,
the construction process is initially
similar. Start by fitting all the resistors
with fixed values given, using a DMM
to check the values before soldering
them in place.
Follow with the diode(s), ensuring
their cathode stripes face as shown
Fig.4: the 10-LED Metronome uses a more complicated LED brightness control scheme with PNP transistors Q1 & Q2
forming a current mirror, so the brightnesses of the middle eight and outer two LEDs track over a wide adjustment range.
LED10 lights up the beats-per-minute adjustment dial. Besides these differences, and using a CMOS 555 timer as the pulse
generator, the circuit is quite similar to the 8-LED version.
28
Silicon Chip
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siliconchip.com.au
How a current mirror works
A current mirror circuit is used to match two or possibly
more currents under varying conditions. Fig.f shows a basic
example; similar NPN bipolar transistors Q1 and Q2 have
their bases tied together and set at a control voltage, Vb.
Thus, their emitters will be at equal voltages, approximately
0.6V lower than Vb.
If the emitter resistors, R1 and R2, are of equal resistance, they will conduct equal currents of approximately
Ic = (Vb – 0.6V) ÷ R.
Assuming a sufficiently high current gain (>≈100) for the
transistors, and thus negligible base currents, the collector current of each BJT would be the same as its emitter
current; in other words, the currents through LOAD 1 and
LOAD 2 would be matched. If the base voltage (Vb) is varied,
the emitter and collector currents will vary, but will remain
matched between the two transistors.
Likewise, if one or both loads vary in resistance – within
limits – their currents will still be equal and given by the
equation above.
For the brightness control of the 10-LED Metronome, we
want the current to the middle LEDs to be a fraction of the
current to the end LEDs, and to be the same fraction over
a wide range of currents. If we used the above scheme, the
circuit would be something like Fig.g, with R being a fraction of VR + R, ie, unequal emitter resistors.
However, there is a problem with this: since each group of
LEDs is alternately turned off, that load resistance becomes
extremely high. As a result, the transistor in the off leg of
the circuit has no collector current, and the base current
becomes large because the base-emitter junction is a forward-biased diode. This reduces the base voltage, and thus
the collector current of the other transistor.
For example, Fig.g shows one of the middle LEDs on,
while the end LEDs are both off, resulting in high base current through their transistor (Q2).
To avoid this, I devised a different scheme for the 10-LED
Metronome, shown in Fig.h. This works because the two
loads are, in practice, nearly constant and equal, each consisting of one LED at a time.
The current-mirror circuit is turned on its head, using PNP
transistors rather than NPN. Each group of LEDs is made
part of an emitter circuit, in series with a resistor that will
determine its current and relative brightness.
When lit in sequence, each middle LED is in series with
R1 + VR4, which is made larger than R2 in series with each
end LED. The collector current of Q1 will be a fraction of
that of Q2 (R2 ÷ [R1 + VR4]). This fraction — the ratio of currents — will be maintained over a range of Vb as controlled
by VR5, and thus the brightnesses of the eight middle LEDs
will be a fraction of the brightnesses of the two end LEDs
over a wide range.
This situation will break down if Vb is above 12V − Vled −
0.6V or about 10V. This is avoided by padding the ends of
VR5 with fixed resistors. Trimpot VR4 allows the resistance
ratio R2 ÷ [R1 + VR4] to be set as desired, thus setting the
brightness difference.
Fig.f: a basic current mirror circuit. Since Q1 & Q2
are similar transistors, and thanks to the negative
feedback provided by the emitter resistors, varying
their base voltages using the potentiometer results in
closely matched currents through the two independent
loads.
Fig.g: different emitter resistor values can be used to
make the load currents different, but they keep similar
current ratios when the base voltage is varied.
Fig.h: the circuit shown in Fig.g can suffer from excessive base current problems when the loads can be switched on
and off independently. This circuit solves that by swapping the NPN transistors for PNP and keeping the currentsetting resistor connections at the transistor emitters.
siliconchip.com.au
Australia's electronics magazine
January 2022 29
Fig.5: most of the
8-LED Metronome
components mount
on the PCB, as shown
here. Assembly is
straightforward
but be careful
to orientate the
ICs, LEDs and
diodes as shown.
Also, don’t get the
potentiometers
mixed up as they all
have different values
(check the codes
printed on their
bodies).
in the appropriate overlay diagram
and that you don’t get the different
types mixed up. Remember that for
the 8-LED version, you either fit zener
diode ZD2 or LED8, not both. If using
LED8, push it down onto the board
with the longer lead to the pad marked
A and then solder it in place.
The ICs are next. They can be soldered directly to the PCB or plugged in
via sockets; it’s up to you. Either way,
make sure the pin 1 notches/dots face
as shown and don’t get the two different 16-pin ICs mixed up. Note that
IC3 on the 8-LED board (74HC137) is
oriented opposite to the other two ICs.
Fit the capacitors next, starting
with the smaller non-polarised types
and then moving onto the electrolytic
capacitors, which must be orientated
with their longer positive leads placed
towards the + symbols. The 1000μF
capacitor on the 10-LED board is laid
over as shown before soldering and
trimming its leads. As with the resistors, leave off any that don’t have values indicated as those pads are for
tuning later.
There are no trimpots or discrete
transistors on the 8-LED board. However, on the 10-LED board there are
three trimpots: two 5kW (VR1 & VR3)
and one 100kW (VR4); as well as two
PNP transistors (Q1 & Q2) and one
NPN transistor (Q3). Fit them now,
being careful not to get the different
30
Silicon Chip
types of transistors mixed up. If your
Q3 transistor is taller than the others,
bend its leads so that it is laid over on
its side before soldering to ensure sufficient clearance for the front panel later.
Note that the PCB has footprints to
accommodate different types of transistors from those specified; assuming
you are using the BC558 suggested in
the parts list, they are placed as shown
in Fig.6.
Both boards use a 3-way terminal
block for power, although you can solder wires to its pads instead. If fitting
it, do that next, with the wires entering the front of the board and passing
around to the rear via the notch on the
edge of the board.
Continue by selecting the LEDs you
are going to use. You might wish to
order extras so that you can pick out
a matched set from the larger number.
Fig.7: a drilling
template for the front
panel of the 8-LED
version. Eleven holes
need to be drilled:
eight for the LEDs
(size & shape to suit
the LEDs you are
using, marked “A”)
and three 8mm holes
for the potentiometer
shafts, marked “B”.
The dashed circles
show the positions of
mounting posts within
the specified case; do
not drill those.
While we specify 3mm
diameter holes for “A”,
the size will depend on
what type of LEDs you are
using.
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Fig.6: the 10-LED Metronome is slightly more complicated than the 8-LED version. Note the components laid on their sides
and make sure to place the transistors in the positions shown, unless you are substituting those with a different pinout.
Note that it’s common for their brightnesses to look similar when fairly
bright, but at very low currents (say
around 30μA), they can vary considerably when dim. Try to select the ones
which match best for the middle LEDs.
If you have a bench supply, one
good way to compare the brightness
is to connect several in series, along
with a current-limiting resistor, then
power the entire string from the bench
supply and slowly wind its voltage up.
That way, you can make a direct comparison over a range of brightnesses.
The construction now diverges for
the two versions.
Finishing the
8-LED Metronome
Measure the resistance across VR1’s
track (from one end pin to the other)
and divide the reading by five. This is
the value you should aim for with R1 +
R2. We’ve specified two 10kW resistors
in the parts list because VR1 should
be close to 100kW.
If VR1 does not measure close to
100kW, vary the values of one or both of
those 10kW resistors (eg, changing one
to 9.1kW or 11kW) to get their total as
close as possible to 20% of VR1’s value.
The 8-LED version fits in a Serpac
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131-BK plastic enclosure, but other
enclosures could be used instead. If
using the 131-BK, use the side with
the best appearance as the upper end.
After selecting the LEDs, drill the LED
and potentiometer holes in the front
half of the enclosure. Fig.7 may be used
as a drilling template.
You can print the guide onto card
stock, punch out the mounting holes
to 5mm and temporarily glue the guide
to the inside of the front half of the
enclosure.
If using the recommended oval
LEDs, you will need to carefully elongate the holes after drilling. Note that
the illuminated line from an oval LED
is perpendicular to the larger dimension of the LED body. Decide which
orientation you want and orientate the
LEDs and holes accordingly. When
drilling or adjusting the LED holes,
check that the LEDs fit into the holes
snugly but do not require excessive
insertion force.
Fit the three pots to the PCB without
soldering them, and attach the PCB to
the front of the enclosure. I removed
the small protruding bits on the front
of each pot. To allow space for the components on the PCB, you might need
spacers on the screws. Check the shaft
Australia's electronics magazine
lengths and shorten them as needed
for your knobs.
The shaft-gripping sections of the
knobs that I used were recessed by
several mm. So for pots VR2 and VR3,
I sanded down the backs of the knobs
to about 12.5mm total height to enable
the knobs to grip the shorter pot shafts
adequately.
If the knobs are not tight enough,
the plastic shafts of the potentiometers can be deformed a bit by pinching them with pliers. Solder the three
pots now, after re-checking they have
the correct values.
Now, paying attention to their orientations (see the A & K markings on
the PCB), insert the LED leads into
the board without soldering them. If
using oval LEDs, they will need to be
twisted slightly to conform to the arc.
Again, attach the PCB to the front
half of the enclosure and manoeuvre
each LED into its proper hole in the
front of the enclosure. It’s best to have
them protruding slightly. Check the
LEDs’ appearance and adjust as necessary, then solder the LEDs to the
PCB while it is in place. The LEDs
will probably not be seated on the
PCB but spaced away from it by several millimetres.
January 2022 31
Fig.8 is the tempo dial; this can be
downloaded from the Silicon Chip
website. It is a good idea to print it on
photo paper for a good appearance.
This assumes that VR1 is equivalent
to the type specified in the parts list;
it needs to rotate through a 280° arc.
Align the dial to the tempo pot shaft
and glue it to the front of the enclosure. Fit the knob to the tempo pot
such that its rotation extends equally
beyond the 36 and 216 tempo lines;
this is because pots typically have a
dead zone at each extreme where the
resistance changes very little.
NPN transistor Q1, the 4700μF
capacitor, switch S1, the speaker, and
the battery holder are not mounted on
the PCB but attached to the rear half of
the enclosure (see the photo below).
The speaker holes may be in any pattern. I used a perforated metal sheet,
selected a drill bit of the diameter of its
holes, clamped the sheet to the inside
of the rear half of the enclosure and
used it as a drilling guide.
Attach the slide switch to the panel
using small screws and nuts. The battery holder and speaker are held in
place with clips made from a large,
heavy-duty paper clip.
Q1 and the 4700μF capacitor are
mounted close to the speaker and
wired directly to the speaker terminals to minimise parasitic resistances;
they are not switched by S1, likewise
to reduce parasitic resistance. This can
be important since the supply voltage
is relatively low and speaker impedance is 8W.
When the Metronome is switched
off, there will be only a minuscule
leakage current through these components. However, if the Metronome
is unused for an extended period, it’s
best to remove the cells.
Solder the emitter lead of transistor
Q1, the negative lead of the capacitor,
and a wire to a solder lug before fitting them to the enclosure. Check the
wiring of these components carefully:
a mistake can cause excessive current
and damage Q1 or cook the speaker
coil and cone.
Cut a timber base to suit the enclosure and attach the rear half to it using
screws, giving the enclosure a slight
backward tilt.
Finally, attach the off-PCB parts to
the 3-way terminal block as shown in
the photos. If you don’t want to use
a terminal block, you can solder the
wires directly to the PCB pads.
Adjustments
The tempo and its range will likely
need adjustment. Eight different
74HC132 ICs showed a spread of a
few percent, with one about 7% above
the average. The tempo may not correspond to the dial markings because
of this, plus variations in the timing
capacitors and the resistances of VR1
and R1/R2. Pots can vary by as much
as 20%.
For the LED Metronome, some of
the components such as the speaker
and battery holder are not mounted
on the PCB, but are instead fitted
onto the rear of the enclosure. This
photo shows the 8-LED Metronome
arrangement.
48
44
40
38
36
54 60 72
88
104
120
160
216
50mm
Fig.8: print this dial artwork for the
8-LED version on photo paper, cut it
out and glue it to the front of the case.
The exact diameter is not critical,
but it should be close to 50mm. This
is available to download from our
website as a PDF.
32
Silicon Chip
Australia's electronics magazine
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If you are not happy and want to
bring the tempos into agreement, a
frequency meter is very helpful. The
type built into many low-cost DMMs
is adequate.
Measure the pulse frequency at pin
11 of IC1 or pin 14 of IC2. With VR1 set
at the lowest tempo (aligned with the
marking showing 36 beats/minute),
find a capacitor or paralleled capacitors for C1-C3 that give a pulse frequency of 4.2Hz (see Table 1).
If you don’t have a selection of
capacitors to try out (or want to save
time), calculate the percentage error in
the frequency (actual vs expected) and
measure the capacitance across C1-C3.
Multiply the capacitance reading by
the percentage and divide by 100. This
is how much capacitance you need to
add (if it’s too fast) or subtract (if it’s
too slow).
To subtract capacitance, you’ll need
to replace C1 and/or C2 with lower
value capacitors, then re-check and
possibly add a bit more capacitance by
fitting C3 to get the frequency spot-on.
Assuming you selected R1 & R2
as 1/5th the value of VR1, with VR1
aligned with 216 beats/min, you
should get a frequency reading of
25.2Hz (see Table 1). If this is significantly off, you might want to adjust
those resistor values, reducing the total
to speed it up or increasing them to
slow it down. Calculating the percentage frequency error relative to 25.2Hz
tells you the percentage by which the
total resistance must change.
CON1
3
2
1
Similar to the 8-LED Metronome, the 10-LED metronome also has components
mounted on the rear panel rather than on the PCB, as can be seen in the photo
below, with the wires emanating from the top of this one.
The final result should have all tempos from 36 to 216 (and thus pulse frequencies in Table 1) agreeing with the
dial markings.
Finally, check the click loudness
and timbre. Check that VR3 varies
the click loudness smoothly from zero
to maximum. If it is too soft at maximum, a transistor with a higher hFE
is needed. If the click does not vary
smoothly, replace the 220W resistor
with a higher value until the loudness
variation is satisfactory.
You can vary the timbre of the click
by adding a capacitor at the position marked C5. Adding capacitance
should give a more ‘mellow’ click.
You can also try the speaker in both
polarities as that can affect the sound.
Troubleshooting
If the LEDs don’t light up or behave
Table 1 – Pulse frequency (Hz)
versus tempo (beats/minute)
Tempo
(bpm)
36
38
40
44
48
54
60
66
72
80
88
104
120
160
216
8 LEDs
(Hz)
4.20
4.43
4.67
5.13
5.60
6.30
7.00
7.70
8.40
9.33
10.3
12.1
14.0
18.7
25.2
siliconchip.com.au
10 LEDs
(Hz)
5.40
5.70
6.00
6.60
7.20
8.10
9.00
9.90
10.8
12.0
13.2
15.6
18.0
24.0
32.4
CON1 pin 3
CON1 pin 1
CON1 pin 2
Australia's electronics magazine
January 2022 33
strangely, check the orientation of all
the parts.
Check for solder bridges or poor
joints and that IC pins are not bent.
Check also that there is a pulse at pin
11 of IC1 and pin 14 of IC2.
Finishing the
10-LED Metronome
The mounting holes for VR2 can
accept a 280° pot (matching the others) or a larger 300° pot. While the difference is subtle, the 300° pot allows
the tempo numbers to be spread out
slightly more. Before fitting VR2, measure its resistance, divide by 5.5 and
check that this is close to 18kW. If not,
you might need to replace the 18kW
resistor with a different value that’s
close to this.
If your IC3 is a 4029, fit the solid
red wire link shown in Fig.6. Otherwise, fit the wire link where there is
a dashed red line. You can use a component lead off-cut for either.
Insert LED10 through the PCB from
the back (see the photo on page 33).
Solder its leads on the back of the PCB
to pads “K” and “A”.
Rather than a dial applique as used
in the 8-LED version, the 10-LED
Metronome uses a transparent plastic
disc printed black with clear tempo
numbers (Fig.9). Choose the design
appropriate for your VR2 potentiometer type. If the printed disc is not
sufficiently rigid, a clear backing disc
might be needed.
Glue the disc to the back of a plastic
bushing fitted by friction or glue onto
the shaft of VR2. This bushing can be
made from a cut-down knob. LED10
illuminates the tempo numbers of the
disc to show through the plastic panel.
LED10’s brightness is determined by
the value of resistor R2, specified as
10kW; if you aren’t happy with the
brightness, lower the value of R2 to
make it brighter or increase it to make
it dimmer.
For the 10-LED version, the LEDs do
not protrude through the front panel,
but show through, so holes for the
LEDs are not needed. The holes for the
two lowest potentiometers (VR5/6) can
be 8mm, but VR2 will require a larger
hole to accomodate the bushing holding the tempo dial.
You will need to cut a thin panel on
which to mount the PCB with 15mm
threaded standoffs. This panel will fit
into the back of the timber frame. This
panel also carries the speaker, power
34
Silicon Chip
Parts List – 8-/10-LED Metronome
8-LED Metronome
1 double-sided PCB coded 23111211, 71 x 98mm
1 3-way terminal block (CON1)
1 Serpac 131-BK plastic instrument case, 111 x 82.5 x 38mm
[Mouser 635-131-B, Digi-Key SR131B-ND]
1 timber base, 75 x 90 x 12.5mm (DIY)
4 AAA cells, preferably NiMH rechargeables (BAT1)
1 4xAAA battery holder (BAT1) [Keystone Electronics 2482;
Mouser 534-2482, Digi-Key 36-2482-ND]
1 8W loudspeaker, 36mm diameter (SPK1) [DB Unlimited SM360608-1;
Mouser 497-SM360608-1, Digi-Key 2104-SM260608-1-ND]
1 100kW linear 9mm/10mm vertical potentiometer (VR1)
[Mouser 652-PTV09A4025UB104]
1 500kW linear 9mm/10mm vertical potentiometer (VR2)
[Mouser 652-PTV09A4020UB504]
1 5kW linear 9mm/10mm vertical potentiometer (VR3) [Mouser
652-PTV09A4030UB502, Digi-Key PTV09A4030UB502-ND]
1 SPST or SPDT slide switch (S1) [Alpha SS60012F-0102-4V-NB; Mouser
SS60012F-0102-4V-NB]
1 14-pin DIL IC socket (optional; for IC1)
2 16-pin DIL IC sockets (optional; for IC2 and IC3)
3 knobs to suit VR1-VR3
4 adhesive rubber feet
2 small machine screws and nuts (for mounting slide switch)
1 large, heavy-duty paper clip
8 No.4 x 6mm self-tapping screws
2 small, short (~10mm) panhead wood screws (for mounting case to base)
1 solder lug with ~3.25mm diameter hole
various lengths and colours of light-duty hookup wire
Semiconductors
1 74HC132 quad 2-input Schmitt-trigger NAND gate, DIP-14 (IC1)
1 74HC191 presettable 4-bit binary up/down counter, DIP-16 (IC2)
1 74HC137 or 74HC138 3-to-8 line decoder, DIP-16 (IC3)
1 30V 1A NPN transistor, TO-92 (Q1)
[KSD471ACYTA, KSC2328AYTA or ZTX690B]
8 ‘superbright’ LEDs, round or oval (LED0-LED7)
[Broadcom HLMP-HM74-34CDD (green, oval), Kingbright WP7083ZGD/G
(green, 5mm), Jameco 2169846 (green, 3mm)]
1 6.0V 500mW zener diode (ZD1) [1N5233 or equivalent]
1 blue/white LED or 4.7V zener diode (LED8/ZD2) [1N5231]
1 150mA schottky diode; eg, BAT46/BAT48/BAT85 (D1)
[Jaycar ZR1141, Altronics Z0044, Mouser 511-BAT46]
Capacitors
1 4700μF 6.3V electrolytic [Mouser 667-EEU-FS0J472]
1 470μF 6.3V low-profile electrolytic [Mouser 232-63AX470MEFC8X75]
4 1μF 50V multi-layer ceramic
1 100nF 50V ceramic
1 220pF 50V ceramic
Resistors (1% 1/4W, 1/8W or 1/16W small body metal film unless otherwise stated)
1 300kW (optional)
2 10kW
While we recommend using 1% resistors, you can
1 2.2kW
use 5% resistors if desired. It might need more
2 220W
adjustments to get the tempo range correct.
1 47W
10-LED Metronome
1 double-sided PCB coded 23111212, 108 x 89mm
1 12V DC 100mA+ plugpack
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Table 2: resistor colour codes
1 3-way terminal block (CON1)
1 chassis-mount barrel socket to suit plugpack (CON2)
1 8W loudspeaker, 50mm diameter (SPK1)
[DB Unlimited SM500208-1; Mouser 497-SM500208-1]
2 5kW top-adjust mini trimpots (VR1, VR3)
1 100kW 280° linear 9mm/10mm vertical potentiometer (VR2)
[Mouser 652-PTV09A4025UB104] OR
1 100kW 300° linear 9mm/10mm vertical potentiometer (VR2)
[Mouser 652-PDB12-M4251-104BF] (see text)
1 100kW top-adjust mini trimpot (VR4)
1 20kW linear 9mm/10mm vertical potentiometer (VR5)
[Mouser 652-PTV09A-4030UB203, Digi-Key PTV09A-4030U-B203-ND]
1 5kW linear 9mm/10mm vertical potentiometer (VR6)
[Mouser 652-PTV09A4030UB502, Digi-Key PTV09A4030UB502-ND]
1 SPDT slide switch (S1) [Alpha SS60012F-0102-4V-NB;
Mouser SS60012F-0102-4V-NB]
1 14-pin low-profile DIL IC socket (optional; for IC1)
1 8-pin low-profile DIL IC socket (optional; for IC2)
2 16-pin low-profile DIL IC sockets (optional; for IC3 and IC4)
1 timber base, 75 x 150 x 12mm (DIY)
1 timber frame, 110 x 130 x 40mm (DIY)
1 red-tinted transparent acrylic panel, 100 x 125 x 2.5-3mm (or to fit frame)
3 knobs to suit VR2, VR5 & VR6
1 clear, printable plastic and plastic backing for tempo dial, bushing or cutdown knob for mounting onto VR2
4 M3-tapped 15mm spacers (for mounting PCB to panel)
8 M3 x 6mm panhead machine screws (for mounting PCB to panel)
2 small machine screws and nuts (for mounting slide switch)
2 M3 x 10mm panhead machine screws, flat washers and nuts (for mounting
speaker)
1 large, heavy-duty paper clip
6 small, short (~10mm) panhead wood screws
various lengths and colours of light-duty hookup wire
1 55x55mm square of speaker cloth
Semiconductors
1 CD4001BE quad 2-input NOR gate, DIP-14 (IC1)
1 TLC555IP or LMC555CN CMOS timer, DIP-8 (IC2)
1 CD4029BE, CD4510BE or CD4516BE 4-bit binary up/down counter, DIP-16
(IC3)
1 CD4028BE 4-to-10 binary decoder, DIP-16 (IC4)
2 BC558 30V 100mA PNP transistors, TO-92 (Q1, Q2)
1 30V 2A NPN transistor, TO-92 (Q3) [KSC2328AYTA or ZTX690B]
1 150mA schottky diode; eg, BAT46/BAT48/BAT85 (D1)
[Jaycar ZR1141, Altronics Z0044, Mouser 511-BAT46]
10 ‘superbright’ LEDs, round or oval (LED0-LED9)
[Cree C566D-RFE-CV0X0BB1 (red, oval) recommended]
1 5mm ‘superbright’ red LED (LED10) [Kingbright WP7113SRD/J4
recommended]
Capacitors
1 4700μF 16V electrolytic, 13mm diameter [Mouser 232-16PK4700MEFC125X]
1 1000μF 16V electrolytic, 8mm diameter [Mouser 232-16ZLH1000MEFC8X2]
5 1μF 50V multi-layer ceramic
2 100nF 50V ceramic
Resistors (1% 1/4W, 1/8W or 1/16W small body metal film unless otherwise stated)
1 22kW
1 18kW
2 10kW
1 4.7kW
1 3.3kW
2 390W ½W
4 220W
2 22W
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jack, power switch, 4700µF electrolytic and two 22W resistors (see photo).
Use the correct power socket to match
your plugpack output.
The speaker is held in place by
screws and nuts, with washers that
have been bent down on one side.
You can use hot melt glue or silicone
sealant to secure the large electrolytic
capacitor.
This panel, and thus the PCB, is
secured to the frame by small wood
screws that attach to four approximately 8 x 8 x 12mm pieces of timber glued to the inside corners of the
frame.
There’s nothing extraordinary
about the case; I made mine in the
same manner as a picture frame, with
four 45° mitred timber pieces glued
together. If you don’t like doing
woodwork, you could probably find
a plastic box with a clear lid that’s
large enough to house the PCB and
other components, and drill holes in
the lid for the pots.
Checkout and adjustment
Before applying power, carefully
check the wiring to the off-board components; a mistake here can cause
excessive current and damage Q3 or
cook the speaker coil or cone. Compare your wiring to that shown in our
photos.
Because of variations in components, the tempo will likely need to be
brought into line. A frequency meter
(even a very basic one as found in
many DMMs) or scope is helpful for
adjusting the tempos.
January 2022 35
120
120
50mm
Fig.9: there are two dials for the 10-LED Metronome to suit the larger 300°
potentiometer (left), or the standard 280° potentiometer (right). Unlike the 8-LED
version, these are printed on transparent film and connected to the rotating pot
shaft. Thus LED10 behind can shine through and illuminate the selected tempo.
Set-reset flip-flops (SR-FF)
Both Metronome designs incorporate
a set/reset flip-flop (SR-FF), a logic
circuit with two states: set and reset.
Applying a high level to the S input
while keeping the R input low puts
the flip-flop into the set state, and it
remains there until reset. Similarly,
applying a high level to the R input
while keeping the S input low puts
the SR-FF into the reset state, staying
there until set again.
By today’s naming standards, the
SR-FF is a transparent latch and not
a flip-flop as it has no clock input, but
the traditional term “flip-flop” continues to be used. Another way of thinking of it is as a 1-bit memory store or
a bistable circuit.
An SR-FF is a simple type of sequential logic circuit, which means that its
output depends on its ‘history’; it has a
memory. Compare this to combinatorial logic in which the outputs depend
only on the value of the inputs; there is
no history or memory involved.
An SR-FF can be made from two
NOR gates, as shown in the adjacent
diagram, or you can get dedicated flipflop ICs. In the 10-LED Metronome,
we’re already using NOR gates for
other purposes, so doing it this way
avoids the need for an extra IC.
It works as follows. Imagine that
both the S and R inputs are low. The
circuit can initially be in either state:
set, with Q high and Q low, or reset,
vice versa. Pulsing S high will cause
Q to go low or to stay low, which will
cause Q to go high, which is the set
state. Further pulsing of S will have
36
Silicon Chip
no effect since Q holds the upper
NOR-gate input high, assuming that
R remains low.
Similarly, pulsing R will cause Q to
go low and thus Q to go high, which
is the reset state. Further pulsing of
R will have no effect, assuming that
S remains low.
For the 8-LED Metronome, the
SR-FF is constructed from two NAND
gates rather than NOR gates. All this
means is that the SR-FF uses negative
logic; in negative logic, NAND gates
become NOR gates, and the SR-FF is
set and reset by negative (low) pulses,
specifically, from LED7 (set) and LED0
(reset). The SR-FF Q output is sent to
the 74HC191 counter to change its
counting direction.
The 10-LED Metronome has an
SR-FF, constructed from two NOR
gates in the CD4001. Positive logic
is used, and the SR-FF operates as
described above.
Turn VR2 to the slowest tempo (36
beats/min) and measure the pulse frequency at pin 3 of IC2 or pin 15 of IC3.
Adjust the control voltage (pin 5) of
the timer, IC2, via trimpot VR1 to get
a frequency of 5.4Hz (see Table 1). If
adjusting trimpot VR1 cannot bring the
frequency to 5.4Hz, you need to add
another capacitor in parallel with C1
& C2 (at position C3) to slow it down,
or reduce the value of C1 and/or C2
to speed it up.
Once this frequency is correct, set
the tempo to 216 beats/min and adjust
trimpot VR3 to get 32.4Hz. If VR3 cannot bring the frequency to 32.4Hz,
change the value of its 18kW series
resistor, then repeat the adjustments
for the slowest and fastest tempos.
Finally, adjust trimpot VR4 to
the desired difference in brightness
between the two end LEDs and the
middle LEDs.
Click timbre and loudness can also
be modified for the 10-LED version.
Adjust the value of resistor R1 for
a smooth variation in loudness, as
described for the 8-LED version.
To change the timbre of the click,
experiment with the combined value
of C4-6. A larger capacitance should
produce a more mellow click. The
speaker can also affect the tone, so try
the speaker in both polarities if you
aren’t satisfied with the initial result.
Troubleshooting
If the Metronome is not working,
check the orientation of IC2 and associated parts. Also, check that the IC
pins are all inserted correctly; they
sometimes get bent and don’t go into
the socket or PCB. Check if there is a
pulse at pin 3 of IC2 and pin 15 of IC3.
If the LED sequence is only in one
direction, it is likely that the SR-FF is
not working or not receiving the S and
R pulses from IC4.
Operation
A set-reset flip-flop (SR-FF) made
from two NOR gates. The Q and
Q outputs always have opposite
polarity; Q is brought high when the
S input goes high, while Q goes low
when the R input goes high. Both
inputs must not be high at the same
time.
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The operation of either version is
straightforward. Turn the Metronome
on and adjust the Click Loudness, LED
Brightness and Tempo as desired.
The supply current for the 8-LED
Metronome is about 2-4mA, depending on the LED brightness, click loudness and tempo. AAA cells typically
are rated at about 900mAh. Thus,
assuming it is used for about half an
hour a day, alkaline or rechargeable
cells should power the 8-LED version
for about a month.
SC
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Dick Smith’s Autobiography
Review by
Nicholas Vinen
M
y Adventurous Life
T
he saying “truth is stranger than fiction” is a cliché.
But say you submitted Dick Smith’s autobiography to
an overseas publisher who had never heard of him and
claimed it is an adventure novel. I think they would reject
it as being too unrealistic!
A man who dropped out of high school at 16, became a
successful businessman and flew helicopters and planes
in record-breaking around-the-world flights? Then he set
up a flourishing publishing company with an Australiawide network of shops, plus another business selling
food, while giving away a significant chunk of his money
to charitable causes? Preposterous! Come back with a
more believable story.
A life full of such exploits makes for exciting reading,
and I found myself wanting to go back for more each time
I had to put it down. It helps that the book is well-written
and easy to read. It includes two maps of Mr Smith’s
adventures and several dozen colour photographs which
provide some important context for his words.
One of the things that struck me about this book is
that Dick Smith’s character really comes through. I can’t
pretend to know the man all that well, but he has told me
some of the stories in the book and reading the book gives
much the same experience.
Despite this, he credits three different writers and one
editor at the end. It shows how much effort they all put in
that the final result maintains so much of his personality.
This book is not just for electronics nuts. The story of
Dick Smith Electronics (DSE) takes up only a fairly small
portion of the book. I would have liked more detail in that
area, but I think I would be in the minority of readers.
Saving more pages for the adventures is the right move
for the book to have general appeal.
And I think he has succeeded in that respect. It will
be a great read for just about anyone who has heard of
Dick Smith, and I reckon that’d be most Australians. I
will be passing this copy on to my sister (definitely not
an electronics nut, but loves nature) and my father (a
doctor; I’m sure he will love the story-telling and historical
aspects).
I got into electronics by reading the Fun Way Into
Electronics books (with Dick’s face emblazoned on the
covers). So I was primarily curious about how DSE
became so successful and why Dick sold the business to
Woolworths, when he was clearly making a lot of money
out of it. The book answered my questions, but I ended up
enjoying many other aspects I hadn’t anticipated.
I knew that he is really into flying and went on some
famous adventures, but I didn’t realise the scope of his
achievements until I’d finished reading the book. He had
some close calls, and you can feel his pride in what he
achieved coming through the pages (it doesn’t seem too
boastful, although he drops plenty of names).
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DICK
SMITH
‘Part Bear Grylls, part Bill Gates, but 100% Aussie larrikin.
Dick is a great innovator, philanthropist and adventurer,
who in my eyes can do no wrong.’
PAUL HOGAN
I understand now why he has dedicated so much of his
autobiography to his adventures.
This book is an excellent read for young or old; teenagers
and young adults will not only find his adventures
fascinating, but I think they will learn a great deal about
what Australia was like in the past. It also has some
fantastic lessons about how to be successful in life, have
strong morals and live life to its fullest.
Older readers will no doubt enjoy Dick’s recollections
of Australia of the past. It feels like another world, reading
about what life in Australia was like in the 50s, 60s, 70s
and 80s.
It was a pity that I could not write this review in time
to make the December issue, as this book would be a
great Christmas gift. If someone you know has a birthday
coming up and you have no idea what to get them, this
book would be a good choice due to its broad appeal and
reasonable cost. A quick search finds many shops selling
the hardcover version for well under $30.
Dick Smith – My Adventurous Life (352 pages) is published
by Allen & Unwin and is available from book stores, major
retailers and as an ebook online. The hardcover RRP is
$39.95, while the ebook has an RRP of $29.08.
SC
Australia's electronics magazine
January 2022 37
Solar PV Update
Are batteries worthwhile?
By Dr Alan R. Wilson
Image source: https://pixabay.com/photos/solar-system-roof-power-generation-2939551/
I have had a solar panel array installed for over 10 years now, and I
have a pretty good set of data on how it has performed over those
years. As I suspect the generous feed-in tariff will go away soon, I
have been considering whether it would be worth adding a battery to
the system and, if so, what type and how large. This article describes
how my system has performed and the research I have undertaken.
I
wrote an article detailing my experience with an urban
5kW solar photovoltaic (PV) installation (May 2015;
siliconchip.com.au/Article/8555). My array consists of
27 panels mounted on a north-facing roof with a 5.2kW
inverter. With the system now around 10 years old, it is an
excellent time to revisit the situation and consider adding
batteries to the installation.
To date, the system has performed flawlessly. A contributing factor might be the shade panel I constructed
to shield the inverter from direct sun, mounted on a
north-facing wall.
One problem that I spotted late in 2019 was the growth
of lichen on my solar panels. I caught it early enough
because I could remove it using a long pole, a scraper and
soapy water. Lichen can be a big problem, and there is a
fair amount of ‘chatter’ on the internet about it.
Here’s an example of lichen beginning to form on a solar
panel. You can find more extreme examples online.
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Silicon Chip
It is critical to ensure algae does not grow on the panels
because lichen is a symbiotic partnership of a fungus and
an algae; any hint of green on PV panels and it is time to
clean it off.
The overall performance for the last 10 years is shown in
Fig.1, including the daily (averaged) exported and imported
energy. Clearly, more energy is exported than imported.
There are two points, indicated by the black markers, where
the crossover for these curves drops when circumstances
changed, and the system started to export more energy.
These correspond to when I installed an evacuated tube
solar hot water system (1) and when one of my adult children left the house (2).
Until a couple of years ago, I was not recording the
amount of energy provided by the solar panels themselves.
Doing so gives a greater insight into the pros and cons of
Solar PVs, and this data can be used to determine whether
batteries are a good option or not.
Fig.2 shows the solar PV energy generated, the energy
used by the household (both of these with a cosine curve
fitted to them, see below), and the excess energy which is
available for use by the grid, again presented as daily usage.
The household uses about 11kWh a day in summer and
18kWh in winter. My house has neither electric heating
nor cooling but does have an off-peak electric storage hot
water system. Taking one year within this span, the system generates 6661kWh, with 5028kWh used, giving a net
yearly excess of 1633kWh.
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However, since much of the consumption is overnight, the actual yearly exported energy is 5105kWh with
3471kWh imported. This is currently a good position for
me because I am the lucky recipient of the Victorian Government Premium Feed In Tariff which is significantly
higher than my usage tariff.
My electricity provider (and the taxpayer) pay me rather
than me being faced with a yearly bill of $1609 (5028kWh at
32¢/kWh) if I did not have solar panels. This will change in
the not-too-distant future, and the question is whether it is
worthwhile to install batteries and a new inverter/charger.
A bonus would be the capability of independent operation as insulation against power drop-outs, particularly in
summer. However, how the house would be disconnected
from the grid to allow this is an open question.
Rather than diving directly into consideration of a solar
PV + battery system, first I will assess the performance of
my current PV system, followed by an analysis of commercially available batteries.
Comparison with expected performance
The Bureau of Meteorology provides a large amount of
public data related to many aspects of the climate, including
monthly measured kWh/m2 insolation values – see www.
bom.gov.au/climate/data/index.shtml?bookmark=203
For December 2019 and June 2020, these values were
6.8kWh/m2 and 2.1kWh/m2 respectively (be careful to
select the correct units when looking at the website).
My PV array produced an average of 26kWh and 11kWh
per day during these two months. With an area of approximately 28m2, this equates to conversion efficiencies of 14%
and 19% for December and June respectively. The figure
for December looks low, but it is a good demonstration of
two effects: 1) the sun passes behind the solar panels, and
2) they run hotter and are less efficient in summer.
My north-facing panels can only receive sunlight for
at most 12 hours a day, but the sun is up from 5:55am
to 8:42pm on December 22, nearly 15 hours (see www.
timeanddate.com/sun/australia/melbourne). Considering
Fig.3, sunlight before 6am and after 6pm contributes little to the energy received.
More important is that the panels run hotter in summer.
An increase in temperature from 20°C to 80°C can decrease
performance by up to 30%, and 19 less 30% is about 13,
as observed.
The next parameter I considered was panel placement.
Melbourne is 37.8° South, and my roof has a slope from the
horizontal of about 32° North. This gives an incident angle
to the sun of about 17.6° mid-summer and 29.2° mid-winter
(the tropics are at 23.4°). The question is: should the panels be aimed more at the winter sun to gather more energy
when it is needed?
Fig.4 was obtained at midday a few days before the winter solstice in 2019 for a clear, cloudless sky and a more
typical overcast day with around 80% cloud cover and
the sun covered.
The figure shows the percentage drop from the maximum power received by a small solar cell mounted under
glass as a function of the angle with the northern horizon.
Here, panels on a flat roof correspond to 0°.
The clear day maximum power occurs at 58°. This is very
close to aiming directly at the sun (37.8° + 23.4° = 61.2°),
as expected. 20° either side of this point (38-78°) decreases
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Fig.1: the energy I imported (blue) and exported (red) over
the last 10 years. The two black triangles indicate the
points when circumstances reduced the household’s energy
usage.
Fig.2: the energy generated by the 5kW PV array, the
energy used by the household and the excess energy
available for the grid over a 14-month period. The thin
curves are fitted cosine functions used for my later
modelling. Day d=0 is July 1.
Fig.3: the relative strength of the incoming solar radiant
power collected by flat PV panels as a function of time
of day, at the start of summer (from www.eia.gov/
todayinenergy/detail.php?id=18871).
Australia's electronics magazine
January 2022 39
Fig.4: the percentage drop from the maximum solar energy
detected by a small solar cell as a function of angle (0°
corresponding to facing straight up) close to mid-winter
for a clear day (blue triangles) and during an overcast day
(grey triangles).
Fig.5: the results from a simple model based on realworld experience for a 5kW PV array, showing the energy
generated, day and night power usage, the energy stored
(thin lines) and passing through (dotted lines) a 5kWh,
10kWh and 15kWh battery, and the energy exported and
imported.
the power by less than 2%. However, on an overcast day,
peak power is at 38°.
As the tilt angle increases, the solar cell sees less of the
sky. The clouds scatter a large proportion of the incoming
energy on an overcast day, so less of this is collected as the
angle increases. 20° either side of 38° decreases the power
by 10% in this case.
The two sets of points suggest the optimum mounting
angle is somewhere in the range 30-43°. This angle improves
collection on overcast days but has a minimal effect when
there is little cloud cover, being within the 38-78° range
for a clear day.
Fig.4 gives an idea of how this will affect the operation
in summer. A panel angle of 30° maps to 76.8° in Fig.4 for
a clear sky in summer, resulting in less than a 2% decrease
in power. The figure implies it is best to keep the effective
summer angle to less than 80°, suggesting that the ideal
angle to mount panels facing North is 30-34° (80° - 46.8°).
My panels are at 32°, so I do not need to do anything.
Remember, this is for Melbourne. Further North, I expect
the ideal angle to be lower, with 0° best at the equator. Thus
Brisbane at 27.5° South would have an ideal panel angle
of around 22-25°.
The thin red line in Fig.2 is a good-looking cosine curve
fit to the energy generated: 18.24kWh + 6.79kWh cos(π +
2π × [d + 15] ÷ 365) where d is days from July 1, and the
peak occurs on December 16.
We can use the same approach to give another fit to the
energy used: 13.98kWh + 2.73kWh cos(2π × [d + 4] ÷ 365),
with the peak occurring on June 27.
Determining the total energy used is only half the solution; it must be split into day and night contributions to
assess the flow to/from a battery. Unfortunately, my situation is complicated by the solar evacuated tube hot water
system. In summer it uses no electricity, while in winter
it uses off-peak electricity at night.
It is preferable to divert the day-generated power into the
hot water system before charging the batteries. To include
this in the model requires an estimate of the energy used
by the hot water system.
My summer drop in consumption after the installation
of the solar hot water system is 4.8kWh. But I decreased
the water temperature by 10°C, which in a 250L tank corresponds to 0.7kWh, reducing this to 4.1kWh. Ignoring the
slight offset between the energy generated and energy used,
this leaves 12.6kWh (16.7kWh less 4.1kWh) used in winter compared to the 11.3kWh minimum use mid-summer.
In Melbourne there are 9.5 hours of daylight mid-winter
and 14.5 mid-summer. After removing the contribution by
the hot water heating, the simplest thing to do is apportion
the energy use according to the number of daylight hours.
Yes, lights are on at night and not during the day, you
might object. However, people sleep at night and use other
electrical devices during the day. I am assuming these
roughly balance.
Table 1 shows the expected peak and trough (mid-winter
and mid-summer) energy consumption figures after allowing for the number of daylight hours and shifting hot water
heating to the daytime in winter. Because the model is a
simple sinusoidal wave with a constant offset and known
period and phase, the maximum and minimum are all that
is required to determine the waveform. The estimates in
Table 1 give:
Are batteries worthwhile?
When I lose my Premium Feed In Tariff, I am considering adding batteries to the system. With a battery, I could
store energy during the day and use it at night, rather than
exporting it during the day and importing it at night. But
will that be worthwhile? The model I developed to analyse the financial aspect is based on real-world experience
and can determine the optimal battery for a solar PV array.
To do this, we need to determine how much energy is
generated, how much is used when the sun is up, how
much is drawn overnight from the battery and how much
is imported and exported.
A simplistic model for energy usage over the year is to
assume it is due to the variation of daylight hours, and
use a cosine function with a winter maximum and a summer minimum.
40
Silicon Chip
Australia's electronics magazine
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Fig.6: the modelled yearly operational income (negative is
a cost) versus battery capacity for 1.5kW, 3kW, 5kW and
8kW PV arrays (red lines), and a 6kWh battery against PV
size (blue line, same horizontal axis). It is clear that large
batteries do not pay for themselves, but more PV panels do.
The 0kWh point corresponds to PVs with no battery.
Fig.7: a similar graph to Fig.6 but with air conditioner
(A/C) and heating loads included for 5kW and 8kW PV
arrays. As expected, due to the greater energy use, the
yearly income decreases. The useful battery capacity also
increases due to the larger throughput.
Night use = 6.0kWh + 1.6kWh cos(2π × [d + 4] ÷ 365)
Day use = 7.95kWh + 1.15kWh cos(2π × [d + 4] ÷ 365)
Again, d is days from July 1. The power available to
be stored in the battery is the PV energy less the day use,
plus any not used the previous day, but only up to the battery’s capacity, the rest being exported to the power grid.
The power used overnight is simply the night use figure.
This is most easily calculated using the above expressions in a spreadsheet. We can also use the spreadsheet
to determine the yearly kWh throughput for the battery,
the amount of energy imported and exported and thus the
annual cost of operating the system.
This spreadsheet will be available to download from:
https://alanrwilson.com/solar-batteries/
As a reality check of the model, the predicted total solar
PV energy generated is 6658kWh, within 1% of the measured 6661kWh, and the total night + day consumption is
5092kWh, within 1.5% of the measured 5027kWh.
Fig.5 is an example for a 5kW PV system using the models above. While it looks complicated, it encapsulates the
results from the model and gives some immediate insight
into the effect of battery capacity.
The determined charge at the end of each day (Battery
Charge) and Battery Throughput for 5, 10 and 15kWh batteries show that all the charge is used in winter due to the
low PV energy available, irrespective of battery capacity.
The energy Exported and Imported is only shown for the
10kWh battery; however, the graphs for all battery capacities are essentially the same, with a decrease in the total
annual values of 147kWh exported and 127kWh imported
moving from the 5kWh to the 15kWh battery. The amount
of PV energy available is the governing factor, not the size
of the battery.
The only advantage of a bigger battery is for energy storage in case of blackouts. For my situation with a 5kW PV
array, this suggests that the optimum battery size, including some latitude for estimation errors and a decrease in
capacity, is about 7kWh. That’s assuming such a battery
can deliver the power required.
The ongoing operating costs can be calculated from the
imported and exported energy figures. Fig.6 shows how
the modelled yearly operational income (negative is a
cost) varies with battery capacity for 1.5, 3, 5 and 8kW PV
arrays. These are calculated with a feed-in tariff of 12¢ and
a usage tariff of 32¢.
Clearly, large batteries will not pay for themselves, but
larger PV arrays do. Any battery larger than where the
curves flatten out is not a good financial investment. It is
also apparent that batteries are not helpful with a small
PV installation: there is simply not enough energy to store.
The variation in cost to operate a 6kWh battery with PV
size is also shown (in blue) and more dramatically demonstrates the significant increase in income with a bigger PV
array. Essentially, all the extra capacity of the larger PV
array is generating more revenue in summer.
This is for my situation and does not include heating or
cooling, which is common in many houses. The spreadsheet
can be modified to include both these cases, modelled as a
half-sinewave with a start date and end date (zero to zero).
Fig.7 is like Fig.6 but includes a hypothetical 3kW air
conditioner, operating (cooling) for a peak of 0.6 hours
during the day, 1.4 hours at night, from November 1 to
April 1, using a total of 580kWh and 1590kWh of heating
using a 3kW heat pump for one hour during the day and
2.9 hours at night, from April 1 to October 30.
These figures are based on Law et al., “Energy consumption of 100 Australian residential air conditioners”, Ecolibrium November 2014. What has not been included is
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Table 1 – estimates of energy used to split
between day and night
Winter peak
(12.6kWh total)
Summer trough
(11.3kWh total)
Day
Night
Day
Night
Portion
of use
5.0kWh
7.6kWh
6.8kWh
4.5kWh
Hot water
+4.1kWh
Total
9.1kWh
7.6kWh
6.8kWh
4.4kWh
Energy
used
Australia's electronics magazine
January 2022 41
the possible impact of limited power delivery by the battery, which would result in higher Imported energy costs.
As expected, the operating costs increase, but it again
is apparent that the size of the PV array is the most critical factor. With the extra energy throughput, the point at
which any increased battery capacity has no effect is moved
a little to the right.
All of the operating costs above are well below the $1629
(my house) or $2324 (with heating and cooling) figures for
PV or batteries at 32¢/kWh, and some even generate income.
But what is missing is the up-front cost.
Most systems on the market have a 10-year warranty.
$25,000 spent on a system that fails after 10 years effectively
costs $2500 a year just to cover the purchase price (ignoring
opportunity costs associated with not having that $25,000).
If the system does not generate a positive return, it will be
more expensive than simply pulling power off the grid.
The following sections consider a range of battery technologies, their pros and cons, how much they cost and
whether they will pay for themselves.
Battery choices
Lithium-ion based batteries currently dominate the solar/
renewable energy market; however, one of their claims to
fame (lightness) is not a consideration for static installations. Still, a quick survey of commercially available batteries offered for solar PV installations yielded 36 lithium-ion,
one graphene super capacitor solution, one flow battery and
one lead crystal battery.
The faithful lead-acid battery is not considered in the
race, primarily due to a low cycle lifetime. Nickel-iron
batteries are another old and proven technology. They are
robust and long-lived, but I will not consider them because
they suffer from a number of disadvantages, including the
evolution of hydrogen gas, low efficiency, low charge/discharge rates and a wide operating voltage needing special
inverters.
Irrespective of the type of battery, the parameters I consider important are:
1. It needs to have sufficient capacity for the requirement.
This is rather obvious but beware, usable storage can
be significantly less than nominal storage, and overdischarging a battery can significantly impact its useful
life. The results in Figs.6 & 7 must also be kept in mind
to not needlessly over-specify the battery capacity.
A bank of A602 2V gel cells which is used to store energy
from a 4kW solar array. Source: www.flickr.com/photos/
stephanridgway/14141342129
42
Silicon Chip
2. Many batteries suffer from a drop of capacity with
use. Some warranties are for 10 years but at 60% of
the original capacity.
Other manufacturers using the same base technology make no upfront mention of reduced capacity. It
is worth checking the fine print in the specifications;
it might be that the initial battery capacity must be
over-specified to ensure it is fulfilling the requirements at end-of-life.
3. The ability to deliver the power you need. High capacity does not necessarily mean the battery can deliver
enough power. An 8kWh battery is not as useful if it
can deliver at most 3kW and the household needs 6kW
peak to run, say, an air conditioner (3kW) and cook
dinner (3kW) at the same time.
However, if peak powers are transient, it is worthwhile pulling power from the grid for a short time
rather than installing a big, expensive battery. Off-grid
use requires a big battery and/or a really smart energy
management system that prioritises certain circuits
and/or a lifestyle change.
A small petrol or diesel-powered generator is not
very expensive and could be a solution in these cases,
if low available solar energy is a transient or rare event.
4. Warranted life: do not accept a battery with less than
a 10-year warranty. This is really warranting the construction quality, the ‘nuts and bolts’, not the storage
elements.
5. Warranted throughput: the lifetime warranty is usually expressed as a time or maximum kWh throughput with some capacity drop at the warranted kWh.
Warranted throughput indicates the amount of energy
the battery can store and deliver; it is directly linked
with the gradual degradation of the chemistry/physics of the storage system.
The yearly battery use needs to be determined to
give the expected 10-year kWh input/output required
from the battery. Ideally, the 10 years and the maximum kWh occur at much the same time. With ‘normal’
use, most modern batteries will have enough throughput to last 10 years.
6. Round-trip efficiency: this is an indication of the efficiency of energy storage and retrieval. Lithium batteries are generally in the 95-97% range. Some others are
as low as 80%, which means more solar panels are
required to compensate for the lost energy, but they
may have other beneficial properties.
7. Off-grid capability: if you want it. Standalone batteries can be used anywhere, but some batteries come
with integrated inverters and/or chargers, affecting
how they can be used.
8. Compatibility: batteries and any associated parts of
the system included with them must be compatible
with the other elements of the system.
One area to watch for is the different solar PV panels available. Some (which used to be the norm) are
an array of solar cells connected in series string(s) to
provide a high DC voltage.
Others, which have some advantages, include
micro-inverters that manage the power from each
individual solar panel and generate the AC at the PV
panel itself. These are all connected in parallel and
provide a (nominal) 230V AC.
Australia's electronics magazine
siliconchip.com.au
Table 2 – comparison of four battery types suitable for solar PV storage
Lithium-ion, NMC
(Nickel Manganese
Cobalt)
Lithium, LFP (Iron
Phosphate, LiFePO4)
Flow cell (FC)
Super capacitor
hybrid battery (SC)
Robustness
Fair
Good
Excellent
Very Good
End-of-life Capacity
60%
80%
100%
85%
27-32MWh
32-36MWh
36MWh
36-45MWh
Round trip efficiency
~95%
~95%
80%
>96%
Available power per
10kWh
4-6kW
4-9kW
3kW (5kW peak)
13kW (33kW peak)
Maintenance
Requirement
None
None
Needs period full
discharge.
None
$8-10k
$8-10k
$13k
$12k
Energy density (lower
weight).
Cycle life. End life
capacity. More Robust
than NMC.
Very robust. Full
discharge. No drop in
capacity.
Very robust. Full
discharge. No drop in
capacity. (Projected
long life)
Large capacity drop
over life.
Medium capacity drop
over life.
Low efficiency. Low
power. Mechanical
pumps. Liquids.
Maintenance.
New technology.
Warranted Life:
throughput per
10kWh
Cost per 10kWh
Advantages
Disadvantages
Table 2 has details for two leading lithium-ion battery
technologies and two other more novel technologies. Some
of the figures presented have been factored up or down
from quoted values to compare hypothetical 10kWh batteries. The cost is for a bare battery, and with the fluctuations in exchange rates and the rapid progress being made,
these could very well be wrong by the time this article is
published.
The two common lithium battery technologies are very
similar. Both technologies suffer from a gradual drop in
storage capacity, with the LiFePO4 outperforming the NMC
type. LiFePO4 also has higher lifetime energy storage, may
deliver higher power, is a little more robust (especially if
heavily discharged) and is considered safer.
Both batteries may have prolonged life by reduced discharge, say to 50%, but then a larger capacity battery is
needed to ensure sufficient energy is available for the
requirement. They both offer good power delivery but could
be challenged in an all-electric house over summer with
air conditioning. They are reasonably mature technologies
with a lower price than the other two.
Flow cell (FC) technology is effectively like reversible
electroplating. For instance, zinc-bromide systems plate
out zinc in a reversible process. The FC battery is very
robust, can be discharged entirely and holds its full capacity through life.
Unfortunately, the round trip efficiency is only about
80% (10kWh is required for 8kWh to be later supplied),
and FC has a more complex maintenance regime requiring
a regular full discharge. Along with a low available power
and higher cost than lithium-ion batteries, it is probably
not suited for domestic energy storage.
Super capacitor (SC) hybrid battery technology is much
more interesting with a very high available power and high
efficiency. It is like a hybrid between a super capacitor and
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a lithium battery. Not shown in the table is the high charge
rates that are possible.
Like the FC battery, it is very robust, can be completely
discharged and holds most of its capacity through life. Performance curves suggest 98% after 10 years; however, the
warranty still only guarantees 85% capacity.
It can also provide enough power for pretty much any
domestic use. The only downside is that it is a relatively
new technology. Still, I will keep my eye on it over the
coming years (especially since the company involved is
based in Melbourne).
While more expensive than lithium-ion batteries, the
projected life, as opposed to warranted life, is well beyond
the 10-year warranty, which could make it cheaper in the
long term.
The other costs besides the batteries and solar panels are
the inverter/chargers. Inverter/chargers usually include a
battery management system and load management, making
them more expensive than a grid-tied inverter. For comparison, I am allocating these a cost of $2000/kW.
I decided to investigate 5kW and 8kW PV arrays and
batteries with two primary requirements:
1. At end-of-life (ten years), they must be able to deliver
5kW. The minimum capacity to achieve this is 10kWh
for NMC, 7.7kWh for LFP and 3.8kWh for SC, 3.8kWh.
The NMC and LFP have a quoted spread of values, so
I used the means.
2. The optimum capacities indicated in Fig.6 for my
application, 4kWh for 5kW PV and 6kWh for 8kW PVs.
Based on Fig.7, 7.5kWh must be available at the endof-life for either a 5kW or 8kW system for the inclusion of both air conditioning and heating.
Combined with the first requirement and the capacity
drops specified in Table 2, the relevant batteries for my
theoretical situations are shown in Table 3.
Australia's electronics magazine
January 2022 43
Fig.8 shows the 10-year cost for the 5kW PV array, while
Fig.9 is for the 8kW array. The cost with time is simply
calculated as (up-front cost) + (operating cost) × years. The
results are simple straight lines; however, a visual representation of the slopes and intersections gives a quicker
comparative insight than numbers in tables.
Both figures include the ongoing cost with No PV and the
relevant PV arrays with no battery. The systems are priced
at $1500/kW in the no-battery case due to the cheaper
inverter required.
It is clear from both figures that the most cost-effective
course for the first 10 years is to not use batteries due to
their high up-front cost. Both figures also clearly indicate
that the payback rate is mainly independent of the battery
capacity, with the average cost over time highly dependent on the up-front cost of the system and the size of the
PV array.
Both figures indicate that the PV arrays without a battery
system pay for themselves after ~5-6 years. The batteryinclusive systems would eventually return more than the
no-battery systems; however, this takes at least another
16 years in the best case, well outside warranty periods.
While the 8kW PV array with no battery takes longer to
pay for itself than the 5kW PV array, it pays back more,
becoming superior to the 5kW PV array after about nine
years. Given that the panels should last 20 years, it is better to install the higher capacity in the long run. In both
cases, the payback is earlier with the higher consumption
cooling and heating case simply because more energy is
being used.
If heating and cooling are included, the 5kW array can
never generate income, whereas the 8kW array can.
Throughput
All of the above considers the 10 years life rather than
throughput. The modelled 10-year throughput for the NMC,
LFP and SC batteries are all much the same at 18MWh for
the 5kW array and 28MWh for the 8kW array. These are
likely to be on the low side since it does not consider times
Fig.8: modelled total cost for a 5kW PV array in my
situation (solid lines) and with cooling and heating
included (dashed lines) with the NMC, LFP and SC battery
capacity as indicated. The No PV and No Battery cases are
included to show payback times. A negative slope indicates
income.
44
Silicon Chip
Table 3 – minimum battery capacities for two PV
arrays with and without heating/cooling
5kW,
no AC
5kW,
with AC
8kW,
no AC
8kW,
with AC
NMC
10kWh
12.5kWh
10kWh
12.5kWh
LFP
7.7kWh
9.4kWh
7.7kWh
9.4kWh
SC
4.7kWh
8.8kWh
7.0kWh
8.8kWh
when the PVs become shaded during the day and will provide power from the battery.
However, even allowing for a 33% increase to 24MWh
and 37MWh, all of the batteries should be able to provide
this, although 37MWh exceeds the NMC specification and
is close to the LFP specification.
If throughput is the critical ageing parameter then, provided the other mechanical and electrical systems do not
fail, the lithium batteries for a 5kW PV array could have
another five years or so of useful life left, and the SC around
seven years. This increases the cost-effectiveness of the systems and making them all a sound financial proposition.
For a 10kWh battery, the effect of a battery on imported
and exported energy is shown in Fig.10. The squares are the
results from my 5kW Solar PV with no battery. Doubling
the size of the battery is not helpful, as shown before, and
decreases the imported and exported energy by a miserly
10kWh.
Power grid stability
One of the complaints against solar PV is the wild fluctuations in available energy that can occur when the sun is,
for instance, suddenly shaded by clouds. A smart energy
management system could be implemented whereby stored
battery energy is available to smooth out these fluctuations.
This is the essence of the Virtual Power Plant concept, and
there are some companies already doing this and making
profits by feeding battery stored energy into the grid when
the spot price is high. The Australian Capital Territory is
Fig.9: model results similar to Fig.8 but for an 8kW PV
array.
Australia's electronics magazine
siliconchip.com.au
An example of a solar panel setup, the smaller panel
along the wall is for a solar hot water pump.
planning to implement this strategy in a distributed network of battery storage in the Territory.
Going off-grid
If the desire is to go off-grid then no energy can be
imported. With everything electrical, the model for my
situation indicates a 16kWh battery is required to cover
the nightly use, with a 13kW PV array to fully charge it
in mid-winter. Using the SC battery, this will cost around
$45,000.
That sounds like a lot, but it might not be too bad if you
have to pay $20,000-30,000 to have power cables laid to a
remote location and then have to pay for the connection
costs and electricity.
The combination of battery and PV array assumes there
is always average sunshine and does not allow for cloudy
days. The problem is the daily use is 28kWh; it rapidly
becomes very expensive trying to install enough batteries
to cover the occasional 2-3 day overcast period.
A more cost-effective method is to use a small generator.
Fig.10: imported and exported energy values from the
model calculated with 3kW, 5kW and 8kW PV arrays
and a 10kWh battery. The black and red squares are the
real-world results from my 5kW system with no battery. A
3.8kW PV array is enough to generate all the power for the
household over a year; the problem is moving the excess
energy from summer to winter.
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These are reasonably cheap (3.5kW for around $500) and
can be run long enough to charge the battery when needed.
But personally, I do not like this option in an urban setting.
Conclusions
Investing in Solar PV by itself is definitely worthwhile,
with a suggested payback time of fewer than six years for
the 5kW, north-facing installation considered here. From a
purely financial point of view, batteries are still too expensive, except possibly for the newer SC batteries with their
potentially longer life and their high power-to-capacity ratio
allowing the use of a smaller, cheaper battery.
But adding batteries does reduce the dependence on grid
power and, with the right management systems, should help
reduce power supply fluctuations from renewable energy.
This is something which will need to be considered in the
future. A network with a large number of (highly variable)
solar PV-only generators that simply attempt to deliver as
much power as possible to the grid will become unstable.
The model shows that increasing the allowed household installation of solar PV to 8kW with a suitable battery backing it up can bring a house in Melbourne close
to self-sufficiency. The situation will be even better closer
to the equator.
Keep in mind that some batteries have failed Australian
tests, and some companies have failed too, and are not
around to honour warranties. Doing business with mainstream companies and suppliers in this relatively new
market is probably advisable. Choosing a great-sounding,
cheap deal could very well leave you with expensive boxes
that do not function.
So what battery would I recommend? From a purely
financial point of view, none at all. However, there might
be other reasons for installing a battery. If you must have a
battery and are on the conservative side, go for the LiFePO4
option from a reputable source, but be aware that the power
requirement may be the governing factor.
If you are more of a betting person, look very seriously
at the ‘super capacitor’ option with its ability to deliver
high power with a relatively low capacity. There is also
the hope the SC technology will live up to its promise of
a superior lifetime. And overall, keep the information in
Figs.6 & 7 in mind; big batteries are definitely not worth it
unless you are going off-grid.
SC
Australia's electronics magazine
January 2022 45
Protects up to six amplifier modules (six
single-ended or three bridged outputs)
Very simple, small in size and low in cost
Can operate from the same power supply as the
amplifiers (up to ±40V DC)
Disconnects the speaker(s) in 100ms for full
rail DC fault <at> 30V
Provides a 1-2 second turn-on delay,
allowing amplifier outputs to settle
Insensitive to low-frequency AC
signals
Uses DPDT relays with contacts rated to
break 10A <at> 28V DC (repetitive)
Multi-Channel
Speaker Protector
If you’re driving a lot of speakers, you will need a matching compact speaker
protector to prevent driver destruction, should something go wrong! Our
Speaker Protector, when combined with our Hummingbird Amplifier module
(published last month), is excellent when driving stereo loudspeakers with
an active crossover or for surround sound systems where you have many
speakers to drive.
A
re your expensive speaker drivers
protected if the worst happens,
and an amplifier module failure results
in them having direct current applied?
This very simple and effective board
matches our Hummingbird amplifier
modules, protecting between one and
six channels with a switch-on delay in
a PCB measuring just 67 x 120mm for
up to six channels, or 67 x 91mm for
the four-channel version.
Over a few years of building hifi
and PA equipment, it would be fair to
say that this author has not destroyed
that many speaker drivers. But when
I have, it has always been expensive,
painful and inconvenient.
The experience of watching a 60W
amplifier deliver 40V DC to the voice
coil of a very expensive driver that represented months of savings is burnt in
my memory. This was a 250W driver
but it was no match for 40V DC! In a
matter of seconds, the voice coil turned
into smoke, much faster than a human
being could turn the power off—all for
the sake of a $1 insulator.
46
Silicon Chip
There have been two main destructors of my drivers:
1. Over-excursion of drivers, particularly in vented enclosures
below resonance without appropriate subsonic filtering. This is
a surefire way of killing a bass
driver. That was addressed by the
Active Crossover presented in the
October & November 2021 issues
(siliconchip.com.au/Series/371),
which includes a subsonic filter.
2. By DC from the output of an
amplifier, either due to a failure
in the amplifier or finger trouble
by the builder. (Have you ever left
a fuse out or forgotten to connect
a wire?)
This project solves #2.
You might ask: what about over-
powering a speaker? Won’t it blow up
that way too? In my experience, that
takes a heroic effort if your crossover
is set up correctly, so we leave the volume control to your discretion.
By Phil Prosser
Australia's electronics magazine
The impetus
Building an Active Crossover combined with six Hummingbird amplifier modules, I found myself running
out of room. To fit this lot with power
supplies into a 330mm-deep 2RU case,
I had to move from beer mat sketches
to CAD and ‘the computer said’ that I
needed to make the speaker protector
small. So I did.
This device will protect your
speaker from most amplifier failures.
The modest investment will pay itself
off the first time it activates, but we all
hope this is one project that you never
see ‘work’.
There are many ways of approaching
a speaker protector. This design aims
to keep it simple and small by keeping
the parts list to a minimum.
Circuit details
The circuit used is straightforward,
as shown in Fig.1, with three duplicated stereo sections providing the six
protection channels.
The main part of the Protector
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Fig.1: the Speaker Protector has three
identical sub-circuits handling two
channels each. Each input signal
passes through a simple RC lowpass filter and is applied to three
transistors. If a large DC voltage is
detected, those transistors switch
off the associated DPDT relay,
disconnecting the speaker from the
amplifier. A basic linear power supply
provides around 24V to drive the
relay coils and incorporates a switchon delay of around one second, to
avoid thumps.
circuit is elegant, but it might not be
obvious how it works at first glance.
Its first job is to detect the presence
of DC at an amplifier output, connected
to one of the AMP x OUT terminals
at right. This is done by the 100kW
input resistor and 47μF bipolar capacitor, which form an RC low-pass filter
with a -3dB point (corner frequency) of
0.25Hz. The output of this filter feeds
a DC detector that triggers at the Vbe
voltage of a transistor, around 0.6V.
So for regular operation, the amplifier must generate less than 0.6V at the
output of this filter. Choosing 10Hz as
a ‘safe’ low frequency limit and assuming an amplifier that can deliver 100W
into 4W, we can calculate that only
135mV would appear on the output
of the filter. So it won’t trigger during
regular amplifier use.
But say an amplifier goes faulty and
delivers its rail voltage of 40V DC (of
either polarity) to the output instead
of an AC waveform. In that case, after
100ms (0.1s), the low-pass filter output will reach 0.84V, which will definitely trigger the DC detection circuit
that follows. This filter operates identically for both positive and negative
voltages.
With 40V across 8W for 100ms,
20J of energy will be delivered to the
voice coil (the impedance will drop
over time, approaching its DC resistance value, but this is a good enough
siliconchip.com.au
Australia's electronics magazine
January 2022 47
Parts List – Multi-Channel Speaker Protector
1 double-sided plated-through PCB coded 01101221, 67 x 121.5mm
3 (2) 30V DC 10A contact, 24V DC coil DPDT PCB-mount/cradle relays
(RLY1-RLY3) [Altronics S4313, Jaycar SY4007]
8 (6) 2-way 5.08mm pitch mini terminal blocks (CON1-CON8)
1 44mm-tall, 16.5 x 10mm PCB-mount finned heatsink (HS1; for Q16)
[Altronics H0645]
1 TO-126 or TO-220 silicone insulating washer and insulating bush
[Altronics H7230, Jaycar HP1176]
1 M3 x 10mm panhead machine screw
1 M3 shakeproof washer
1 M3 hex nut
4 tapped spacers & 8 machine screws (to suit installation)
Semiconductors
16 (11) BC547B/C 50V 100mA NPN transistors, TO-92
(Q1-Q3, Q5, Q6, Q8-Q10, Q12, Q13, Q15, Q17-Q19, Q21, Q22)
6 (4) BC557B/C 50V 100mA PNP transistors, TO-92 [BC558-9B/C will also
work] (Q4, Q7, Q11, Q14, Q20, Q23)
1 BD139 80V 1.5A NPN transistor, TO-126 (Q16)
1 27V 1W zener diode (ZD1) [1N4750]
3 (2) 1N4004 400V 1A diodes (D1-D3)
Capacitors
6 (4) 47μF bipolar/non-polarised electrolytic [Jaycar RY6820]
3 47μF 50V electrolytic [Altronics R4807 or Jaycar RE6344]
Resistors (all 1/4W 1% metal film axial)
6 (4) 33k-100kW (see text; if unsure, use 100kW)
1 47kW
3 (2) 4.7kW
(n) for the four-channel version (PCB code 01101222, 67 x 91mm), the
quantities required are listed in red.
approximation). This will make a solid
thump and probably make you jump,
but it won’t cause anything to catch
on fire. Even better, if the fault exists
from switch-on, the speaker will simply never be connected.
The DC Detector comprises a total
of three transistors. For the top-most
section in Fig.1, these are Q2, Q3 and
Q4. Positive DC detection is handled
by Q2, which has its collector tied
directly to the 4.7kW load resistor. A
positive voltage from the filter of more
than about 0.6V will switch this transistor on and consequently pull the
base of Q1, an emitter follower, low
and thus turn off the relay.
Q3 and Q4 detect negative voltages. NPN transistor Q3 is connected
in a common-base configuration; its
base is tied to ground, and its emitter
is the input. A negative input voltage will pull current from 0V via the
base-emitter junction, causing its collector to sink current. Because the current it sinks at the collector goes to the
emitter, this current must be kept low.
Hence, this tiny current is buffered
by Q4, a PNP device connected as an
48
Silicon Chip
emitter-follower. The emitter of Q4
connects to the same resistor as the
collector of Q1. So a negative DC voltage from the filter similarly pulls the
base of Q1 low, switching the relay off.
There is a balance in this circuit
between setting a low cut-off frequency and the minimum DC voltage
at which the circuit will switch the
relay off. 47μF is a reasonable maximum for the filter capacitor, so any
tweaking is best done by varying the
value of the input resistor(s).
We chose the 100kW value to guarantee no problems with false triggering for very high power, very low frequency applications. But if you are
not protecting a subwoofer, any value
greater than 33kW should be fine and,
as a bonus, lower values will provide
faster turn-off for fault conditions.
The 100kW resistors also affect the
lowest DC voltage that will cause the
detector to trigger. A fault in the amplifier front-end could cause a few volts
DC to be present at the output, and if
applied to a driver for long enough,
it could overheat and be damaged.
So ideally, we want to detect that
Australia's electronics magazine
condition too, not just a fault where
it immediately pegs to one of the supply rails.
Assuming a minimum transistor
hFE of 120, and that the relay will
switch off with 20V across the 4.7kW
resistor (leaving just a few volts across
the relay coil), the transistor base current must be at least 20V ÷ 4.7kW ÷ 120
= 35μA (or thereabouts) to switch the
relay off. This means the DC from the
amplifier must be at least 3.5V (35μA
x 100kW) to trip the relay off.
But this is with a worst-case hFE
value. We recommend using BC547B
or BC547C transistors, which have
higher guaranteed hFE figures and
will switch the relay off with about
1.5V DC on the input. Lowering the
input resistors would reduce that trip
voltage further.
The DC Speaker Protector disconnects the speaker any time that DC is
detected. The relays used are robust
and should be able to interrupt the
fault current that can be expected from
a Hummingbird amplifier module or
similar. However, there is the possibility that upon disconnection, the voltage and current will be high enough to
form an arc between the relay contacts.
The normally closed contact of the
relay is used to shunt this current to
ground when the speaker is disconnected. So if an arc forms and current
continues to flow, the amplifier’s DC
fuse for that rail will blow, and the
arc will extinguish. You likely have a
failed output transistor already, so a
blown fuse won’t exactly be high on
your list of concerns.
We have put three sets of this circuitry on one board, allowing six standard amplifier channels to be monitored and protected. The relay selected
has a standard pinout and is available
from many suppliers. Make sure that
you get the correct version, though; we
are specifying 24V DC coils, though
you could use 12V provided you adjust
the DC regulator, and the BD139 can
handle its heat load (see below).
The circuit uses the power ground
pin as the ground reference. This connects to the Earth of the power amplifiers being protected. Since the inputs
are already paired up, this Protector
would work well for DC protection in
a bridged amplifier.
The power supply
The power supply is a basic seriespass regulator generating about 25V
siliconchip.com.au
DC. The relays need 24V on their coils,
and this suits amplifiers with various
rail voltages. It can be adapted for
supplies below ±25V or above ±40V
(see below).
The power supply provides a
turn-on delay of about one second.
This is because the 47kW resistor
delays the charging of the 47μF capacitor at the base of Q18. This applies to
all channels protected by the board.
As you increase the supply voltage,
the turn-on delay decreases slightly
because the capacitor will charge
faster. You could compensate for that
by increasing the resistor value if
needed.
If you have an amplifier with rails
below ±25V, you have the option of
swapping the relays for 12V DC coil
versions and make necessary adjustments in the regulator (we expect a
15V zener would work well for ZD4).
Similarly, if you have higher rail voltages, this should be fine; just watch the
sizing of the heatsink. The specified
Altronics H0655 heatsink should be
fine for any normal rail voltage.
Construction
Construction is straightforward.
There are two PCBs available; a
six-channel version (coded 01101221,
67 x 120mm) and a four-channel version (coded 01101222, 67 x 91mm).
We have described the six-channel
version here; the four-channel version
is identical except that one relay and
its associated components are omitted, so the PCB is smaller. Refer to the
appropriate overlay diagram, Fig.2 or
Fig.3, during assembly.
Start with the resistors and diodes.
Make sure you get the diodes in the
right way around. Then mount the
two-way terminals for power, each
input/output pair and the Earth terminal to prevent arcing in the relays
(CON8).
Now is time to solder in the BC5XX
transistors. Try to mount them at the
same height so it looks neat.
Next come the capacitors. The three
47μF polarised capacitors need to be
rated at 50V DC, and all go in the same
way, with the longer positive leads to
the pads marked +. The six 47μF bipolar/non-polarised electrolytic capacitors do not need a high voltage rating
as they will never see more than 0.6V
– they mount to the PCB in any orientation.
Now fit the BD139 to the heatsink
siliconchip.com.au
Figs.2 & 3: build
the smaller board
to protect up to
four channels, or
the slightly larger
board for five
or six channels.
Assembly is
straightforward;
all components are
through-hole types
and can be fitted in
order from shortest
to tallest (the latter
being the relays
and heatsink for
Q16).
The finished Speaker Protector board will look something like this. Note the
holes drilled into the board under the heatsink to allow convection to pull fresh
air up from underneath. The CON8 (GROUND) terminal block is missing on this
prototype version; you could leave it off, but it provides better protection for the
speakers if you wire it up to the amplifier Earth.
Australia's electronics magazine
January 2022 49
The Multi-Channel
Speaker Protector comes
in a six-channel (pictured) and
smaller four-channel version. The
four-channel version would be suited
to a two-way stereo speaker system
with an active crossover or a bridged
stereo amplifier.
using an insulating washer, 10mm M3
machine screw, locking washer and
nut. Solder the heatsink to the PCB, but
remember it can be hard to get enough
heat into it to solder those big pins.
Finally, mount the relays. The PCB
has 1.5mm holes which are the minimum that this family of relay recommends – the devices from Altronics
and Jaycar leave a fair bit of room in
the holes. Solder them in well.
Testing
Now that you have all the parts
mounted, it is time to test it out. During
the initial tests, leave the amplifier terminals (CON1-CON6) disconnected.
First apply power and check for the
25V output of the regulator The end
of the closest 4.7kW resistor right near
Q11 is a convenient place to probe;
you can use the anode of any of diodes
D1-D3 as a ground reference. The reading should be between 24V and 26V
for an input above 32V DC.
If this is not present or correct, check
that ZD4 has about 27V across it; if not,
look to the 47kW resistor and transistors Q16 & Q18. Check that these two
transistors are the right types and soldered in correctly. Also check for short
circuits – is the BD139 getting hot?
After a second or two, the relays
ought to click in. If this does not happen, check the voltage on the bases of
Q1, Q8 and Q15 (the driver transistors
for the relays). Are these within a volt
50
Silicon Chip
or two of the 25V rail? If not, check
that they are the proper devices and
soldered in correctly.
Check the voltage at the output
of the RC filters. The voltage at both
ends of the 100kW resistors (or other
value you might have changed them
to) should be close to 0V. If not, check
that the BC547 and BC557 parts are
in the right places and orientated
correctly.
Assuming the relays do switch on,
let’s check that they will trip off correctly.
The easiest way to test it is to take
a 9V battery and connect the negative
end of the battery to the ground terminal on the DC protector. Then touch a
wire from the positive pin of the battery to the “AMP” terminal of each
installed channel of the DC protector.
The associated relay should switch out
almost instantly.
Repeat this for all channels, checking that the relays switch quickly.
Then repeat the test with the battery
the other way around (ie, positive terminal to GND and negative to the AMP
terminals).
If a channel does not switch as
expected, measure the voltage at both
ends of the 100kW resistor. One should
be ±9V, the other ±0.6V.
If the ±9V end is not correct, there is
a short or open circuit somewhere in
that area. If the other end is not close
to +0.6V, check the two NPN transistors on the DC detector (eg, Q9 and
Q10), especially their orientations.
Check the associated PNP transistor
(eg, Q11) for a fault where you aren’t
registering -0.6V.
We don’t suggest you do this, but to
verify that the Protector does indeed
protect the driver, we connected a 4W
subwoofer to the DC Speaker protector
along with a 6A limited, -34V power
supply to the “AMP” input of the Protector. There was a solid thump and
click as the relay saved the sub from
Scope 1: the blue trace is the voltage across a 4W loudspeaker driver (zero volts
at top), while the yellow trace is -34V applied to the DC Speaker Protector from
a bench supply. The speaker is disconnected in less than 80ms. The AC voltage
generated by the cone movement due to back-EMF after the relay disconnected
the driver will not occur in this final version as long as CON8 is connected to
Earth, as that will brake the cone movement.
Australia's electronics magazine
siliconchip.com.au
Silicon Chip
Binders
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$19.50
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Remember to fit an insulating washer to the BD139 transistor (visible above) to
prevent it from shorting out on the heatsink. Also note the use of shakeproof
washers on all screws so they won’t loosen due to vibration or movement.
inevitable destruction. We monitored
this with an oscilloscope, and the
result is shown in Scope 1.
We noted a flash of arcing as the
speaker was disconnected, which is
no surprise when breaking the very
high direct current flow. Please don’t
try this at home, as a speaker protector
does not make this sort of thing safe
for your speaker.
Application
The DC Protector needs to be connected to the power amplifier ground/
Earth via the provided terminal
(CON8) and supplied with 30-40V
DC to the power connection (CON7).
If your amplifier has a higher positive
rail voltage than this, you can use a 5W
wirewound resistor to drop the supply voltage to the Protector. The six-
channel Protector draws about 100mA,
so a 100W 5W resistor will drop 10V
and dissipate about a watt.
Connect the terminals marked AMP
to the amplifier and the corresponding
SPKR terminal to your speaker outputs. It’s OK to leave some channels
unused; for example, if you have a 3or 5-channel amplifier. Once installed
in your amplifier, let’s hope that you
never hear those relays click unexpectedly. But if you do, you will be glad
SC
they are there!
Are your copies of SILICON
CHIP getting damaged
or dog-eared just lying
around in a cupboard or on
a shelf? Can you quickly
find a particular issue that
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Silicon Chip Publications
PO Box 139
Collaroy Beach 2097
Scope 2: this scope grab shows the response time of the Protector to a 20V
DC fault. The input voltage step is at t=0 and the output starts to drop before
t=60ms. It reaches 0V before t=80ms. The 80ms delay is due to the RC time
constant of the filter reaching 0.6V.
siliconchip.com.au
Australia's electronics magazine
Order online from www.
siliconchip.com.au/Shop/4
or call (02) 9939 3295
and quote your credit card
number. *See website for
delivery prices.
January 2022 51
PRODUCT SHOWCASE
Global power supply repair
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Since 1984, Switchmode has serviced over 6000 models of equipment from more than 1400 different
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Espressif ESP32-S2 MINI WiFi modules from Mouser
Mouser Electronics is now stocking the ESP32-S2 MINI modules from
Espressif Systems. These generic
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To learn more about the ESP32-S2
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Mouser Electronics Inc.
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Low input bias operational amplifiers from Microchip
Microchip's new MCP6006/7/9 and
MCP6476/7/9 series of operational
amplifiers have low input bias currents
and rail-to-rail input and output operation. This family is unity-gain stable and has a typical gain-bandwidth
product of 1MHz or 3MHz.
The benefits of these low-cost devices
include:
• Operation from a single supply
as low as 1.8V
• A low maximum offset voltage of
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excellent measurement accuracy without breaking the budget
52
Silicon Chip
• Both the MCP6006/7/9 and
MCP6476/7/9 series of amplifiers
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• Integrated EMI filters provide
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• They are specified over the
Australia's electronics magazine
extended temperature range from
-40°C to +125°C.
The MCP6006/6R/6U, MCP6007,
MCP6009 are single, dual and quad
1MHz op amps - see siliconchip.com.
au/link/abbc
The MCP6476/6R/6U, MCP6477,
MCP6479 are single, dual and quad
3MHz op amps - see siliconchip.com.
au/link/abbd
Microchip Technology
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siliconchip.com.au
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SZ1925
SZ1924
Rated at 20A for a 12V system (10A for 24V) up to a
maximum 45A per panel. Easy installation.
2, 4 & 6 way available. SZ1923-SZ1925
HIGH QUALITY
Looking for more product information?
Visit your local store or our website jaycar.com.au
NOW
3495
NOW FROM
$
$
SAVE $5
SAVE 20%
2495
Fuse Blocks with Bus Bar
Accepts up to 30A per output with handy
fuse-blown indication. Negative bus bar.
6 Way
SZ2031 NOW $24.95
12 Way
SZ2032 NOW $34.95
SZ2032
EA
Panel Mount Circuit Breakers
High quality units with multi-wire
gauge inputs/outputs. 60A, 120A &
200A available. SZ2081-SZ2085
We reward our industry professionals
CCTV Kits Sale
Selected range of Concord and Swann models available:
• 4 channel & 8 channel
• 4, 6, & 8 cameras
WHILE STOCKS LAST!
• 1080p & 4K
DVR Kits
Scan to view range
Order online, collect in store
Selected discontinued CCTV kits we can no longer afford to hold stock.
See website or contact your local store to check stock.
STOCK IS LIMITED. ACT NOW TO AVOID DISAPPOINTMENT.
Sorry NO RAINCHECKS.
NVR Kits
QV5600
QV5000
NOW FROM
NOW FROM
399
849
$
$
SAVE<at>$130
SAVE<at>$200
A DVR (Digital Video Recorder) uses coax cables to run video from the camera
to the DVR. Each camera needs its own power source using a secondary cable
between the power supply and cameras via a splitter.
Limited stock. In-store only.
An NVR (Network Video Recorder) records using IP cameras and Cat5/Cat6
Ethernet cables, which allows for an easy setup. Ideal for home/office or
commercial environments.
Limited stock. In-store only.
All kit contents include: Digital video recorder (or Network video recorder), cameras, power and video cables, adaptor
and splitter, USB mouse, HDMI cable and Network cable.
MP5205
NOW FROM
129
SMART POWER
BACKUP
$
STAY CONNECTED
DURING POWER FAILURE
HIGH CAPACITY
NOW FROM
2995
SAVE<at>$50
$
SAVE $5
Line Interactive UPS
Alarm & NBN Back-up Batteries
MP5224
High quality batteries for standby,
emergency and back-up power applications.
7.2Ah SB2486 NOW $29.95
9.0Ah SB2487 NOW $39.95
Save on Wireless Security
1080p Smart
Wi-Fi Cameras
See and talk to visitors via your
Smartphone, even when not home.
Records to microSD card (sold
separately). 170°C viewing angle.
IR night vision. QC3886
32GB microSD card XC4992 $36.95
5995
NOW
24
$
95
SAVE $10
Wireless Driveway
& Entry PIR Alert Kit
Alerts alarm when movement is
detected. Up to 8m PIR detection
range. Mounting hardware included.
LA5178
SAVE $20
NOW FROM
99
INDOOR CAMERAS
Bullet with Infrared LEDs
QC3906 NOW $59.95
Pan Tilt
QC3900 NOW $79.95
OUTDOOR CAMERAS
IR Illumination
QC3864 NOW $99 SAVE $30
Pan Tilt Zoom
QC3859 NOW $119 SAVE $30
$
SAVE 20%
QC3859
99
1080p Smart Wi-Fi
Doorbell + Chime
NOW FROM
$
Used as standalone or
as part of a system to
keep an eye on your
property. Built-in motion
detection, app control
and 2-way audio.
NOW
SAVE $50
SB2487
QC3900
Keep your surveillance systems, PC and other
devices running longer during a power failure.
600VA/300W MP5224 NOW $139 SAVE $20
650VA/390W MP5205 NOW $129 SAVE $20
1500VA/900W MP5207 NOW $299 SAVE $50
$
SB2486
TERMS AND CONDITIONS: REWARDS / CLUB MEMBERS FREE GIFT, % SAVING DEALS, & MEMBERS OFFERS requires ACTIVE Jaycar Rewards / membership at time of purchase. Refer to website for Rewards / membership T&Cs. IN-STORE ONLY refers to company owned stores and not available to Resellers. Page 6: CCTV Kits Sale:
Selected items only. In-store only promotion and not available to Resellers. No rainchecks. Page 7: Clearance: Selected items only as listed. In-store only promotion and not available to Resellers. SUPPLY CHAIN DISRUPTION. We apologise for factors out of control which may result in some items may not being available on the
advertised on-sale date of the catalogue.
Clearance
Order online, collect in store
Listed below are a number of discontinued (but still good) items that we can no longer afford to hold stock. Please ring your local store or search our website to check stock.
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STOCK IS LIMITED. ACT NOW TO AVOID DISAPPOINTMENT. Sorry NO RAINCHECKS.
Test & Tools
SAVE
HALF PRICE QP5014 $17.95
$8.95
$9
2 Channel IR Extender Kit
AR1812
$79.95 $44.95
$35
10W Hot Glue Gun
TH2050 $12.95
$7.95
$5
2 Core Speakon Audio Cable 10m
WA7102
$54.95 $39.95
$15
3.5 Digit Jumbo LED Panel Meter
QP5585 $34.95 $19.95
$15
AC1757
$49.95 $24.95
$25
HALF PRICE QP5570 $27.95 $13.95
$14
23"-55" Slimline LCD TV Wall Bracket
CW2864
$20
3000A True RMS AC High Current Clamp Meter
QM1568 $49.95 $34.95
$15
ORRP
$44.95 $24.95
50m 1080p HDMI Cat5e/Cat6 Extender with Infrared
AC1783
$99.95 $69.95
$30
4P/6P/8P/10P Modular Crimp Tool
TH1936 $54.95 $39.95
$15
Boom Box Amplifier with Bluetooth®
QM3410
$49.95 $39.95
$10
6" Insulated Side Cutters
TH1985 $24.95 $17.95
$7
Ceiling / Wall Speaker Bracket
CW2841
$19.95 $12.95
6.5" Long Nose Pliers
TH1986 $24.95 $17.95
$7
Composite AV to USB Video Recorder
AC1790
$109
AC5010
AC5012
3.5 Digit LCD Panel Meter
WAS
Sight & Sound
NOW
0 - 5A MU45 Panel Meter - Moving Coil Type
Cat. No
600A True RMS AC Clamp Meter
QM1630 $59.95 $44.95
$15
7" Bull Nose Pliers
TH1984 $24.95 $17.95
$7
75mm 3" Sheet Metal Bending Pliers
TH2336
Adjustable Compression Crimping Tool
TH1800 $24.95 $17.95
Budget SMD Vacuum Pick-up Tool
$29.95 $19.95
HALF PRICE
Concord 4-Way 4K HDMI Switcher
Concord 4x2 4K HDMI Matrix Switcher Splitter
HOT PRICE
WAS
NOW
SAVE
$7
$79
$30
$129
$89
$40
$249
$199
$50
Digital Audio Converter & Repeater
AC1592
$49.95 $29.95
$20
$7
Digital to Analog Audio Decoder
AC1658
$99.95 $79.95
$20
$9
Economy UHF/VHF Masthead Amplifier
LT3276
$49.95 $24.95
$25
$12
Gooseneck Microphone for DJ / Mixing Desks
AM4012
$17
$99
$30
ORRP
$39.95 $22.95
Grey Beanie with Bluetooth® Speakers
ST3216
$29.95 $19.95
$10
HALF PRICE TH1816 $13.95
$6.95
$7
MHL™ to HDMI Lead with 11 Pin Samsung Adaptor
TH1887 $14.95
$8.95
$6
PC Monitor Hanging Cubicle Bracket
HALF PRICE TH1978 $17.95
$8.95
Heavy Duty Coax Crimping Tool
TH1832 $34.95 $22.95
IP67 True RMS Autoranging Cat IV DMM with
Wireless USB Interface
QM1571
PLCC Extractor
$10
2 Way DisplayPort Switcher
Cat. No
Precision 6 Long Nose Pliers
$129
WQ7428
$19.95
$9.95
$10
HALF PRICE CW2834
$39.95 $19.95
$20
HALF PRICE TH1831 $39.95 $19.95
$20
Speaker Polarity Tester with Tone Generator
AA0414
$34.95 $24.95
$10
Spiral Drive Drill/Driver
TD2089 $25.95 $14.95
$11
TOSLINK & Coax Audio Cat5e/6 Extender with Infrared
AC1733
$69.95 $49.95
$20
Thermocouple Thermometer - 2 Input
QM1601 $79.95 $64.95
$15
USB Type-C Lapel Microphone
HALF PRICE AM4015
$29.95 $14.95
$15
Ratchet Crimping Tool for F-Type Connectors
Power
Cat. No
WAS
NOW
MB3816 $49.95 $29.95
10,000mAh Power Bank with USB and Qi Charger
SAVE
Security
Cat. No
WAS
NOW
SAVE
$20
1080p Wi-Fi IP Camera with Security Alarm
QC3870
$129
$89
$40
WQ7278
2 Outlet Power Garden Stake
HALF PRICE MS4097 $19.95
$9.95
$10
20m CCD Camera Extension Cable
24-Hr Mechanical Mains Timer
HALF PRICE MS6109 $19.95
$9.95
$10
4 Door RFID Access Controller
HOT PRICE
LA5359
$199
$149
$50
HOT PRICE
QC8047
$229
$179
$50
QC3667
$16.95
$9.95
$7
$64.95 $44.95
$20
24VDC 2.5A 65W Switchmode Mains Adaptor with 7 Plugs
MP3562 $49.95 $29.95
$20
720p Motion Wi-Fi Camera with Flood Lights
24VDC to 12VDC 6A Converter
MP3064 $74.95 $59.95
$15
BNC to Cat5e/6 UTP AHD Video Balun Kit
40W 24V 1.67A Dimmable LED Power Supply
MP3375 $79.95 $54.95
$25
Car Alarm Electronic Siren
HALF PRICE
LA8908
$19.95
$9.95
$10
60W 48V 1.25A Desktop Power Supply
MP3256 $49.95 $29.95
$20
CCTV Camera External Mounting Bracket
HALF PRICE
QC3337
$14.95
$7.45
$7.50
75W 24V 3.15A Dimmable LED Power Supply
MP3379 $99.95 $69.95
$30
Concord 5MP PIR Bullet IP Camera
QC5620
$149
$109
$40
AC Power Meter with LCD
QP2325 $29.95 $24.95
$5
Multifunction 5.5” GPS Head-Up Display
LA9034
$99.95 $79.95
$20
Dual USB 4.8A Car Charger with LCD Voltage Display
MP3692 $14.95
$5
Smart Lock Deadbolt Kit with Bluetooth®
LA5095
$99.95 $79.95
$20
Dual USB Mains Power Adaptor
MP3459 $26.95 $16.95
Swann 4MP IP Outdoor Camera
QV9014
$149
$109
$40
Dual USB Wall Charger with LED Night Light
MP3429 $14.95
HALF PRICE
LA5206
$12.95
$6.45
$6.50
Fast Two Hour Ni-MH Battery Charger
MB3549 $32.95 $22.95
$10
Wireless Panic Button Suit Wi-Fi Camera System HALF PRICE
QC3872
$19.95
$9.95
$10
Lithium-Ion CR123A Battery Charger
MB3581 $44.95 $29.95
$15
Wireless PIR Suit Wi-Fi Camera System
QC3876
$29.95 $14.95
IT
$9.95
$8.95
$10
$6
Cat. No
WAS
NOW
SAVE
HOT PRICE MP3471
$129
$89
$40
2 Bay USB 3.0 SATA HDD RAID Enclosure
XC4688
$99
$79
$20
2GB Digital Voice Recorder
XC0387 $79.95 $59.95
$20
3.5" USB2.0 External HDD Case
XC4669 $29.95 $24.95
$5
3.5" USB3.0 SATA HDD Enclosure
XC4667 $39.95 $29.95
$10
Miniature 1080p DV Camera with Wi-Fi
QC8102 $69.95 $49.95
$20
Monitor Stand with USB Hub and Card Reader
XC4312 $29.95 $24.95
$5
Mouse Pad with Wireless QI Charger
XM5098 $29.95 $19.95
$10
144W 12-24VDC Laptop Power Supply
OTG Type-C USB Card Reader
Thunderbolt™3 Dock with 4K HDMI, USB 3.0 Port
& Card Reader
USB to Parallel Bi-Directional Cable
HALF PRICE XC5621 $14.95
HOT PRICE
$7.45
XC4938 $99.95 $59.95
HALF PRICE XC4847
$39.95 $19.95
Window & Door Entry Alarm - 2Pk
Kits, Science & Learning
Cat. No
WAS
NOW
$15
SAVE
3MP USB Portable Digital Microscope
QC3191
$59.95 $49.95
$10
5MP Camera for Raspberry Pi
XC9020
$24.95 $14.95
$10
5MP Camera for Raspberry Pi with IR LED
XC9021
$49.95 $34.95
$15
All Terrain Multifunction Tracked Robot
KJ8918
$69.95 $49.95
$20
KJ9029
$19.95
Hydraulic Robot Arm Kit
KJ8997
$59.95 $44.95
Long Range LoRa IP Gateway
XC4394
MeetEdison Robot Kit
KR9210
R/C Motorised Robot Arm Kit
KJ8995
$40
Salt Water Fuel Cell Engine Car Kit
KJ8960
$28.95 $19.95
$9
$20
Squishy Circuits Standard Kit
KJ9350
$39.95 $29.95
$10
$7.50
Dual Motor Gearbox Kit
HALF PRICE
$99
$9.95
$69
$99.95 $79.95
$99
$89
$10
$15
$30
$20
$10
SAVE<at> 500
$
Desktop
3D Scanner
3X FILAMENT
COLOUR MIXING
TECHNOLOGY
Watch real life objects become
digitized before your eyes.
Scans up to 250Hx180Dmm.
Folds for easy storage.
Supplied with MFStudio
software with +Quickscan.
TL4420 In-store only.
999
$
SAVE $500
CLEARANCE
699
109
$
DOBOT
MOOZ-3Z
Triple Filament 3D Printer
SAVE<at>$150
19" Rack Mount Cabinets
6U to 12U in Swing or Fixed frame. Ideal for IT or phone system installations, PA
systems, etc. Solid steel powder coated to provide high strength and rigidity.
6U Swing Frame
6U Flat Packed
HB5180 NOW $164 SAVE $115
HB5170 NOW $109 SAVE $80
6U Assembled
12U Swing Frame
HB5171 NOW $129 SAVE $90
HB5182 NOW $199 SAVE $150
12U Flat Packed
HB5174 NOW $149 SAVE $100
Equipped with a three-color print head for colour mix print. Easy-to-use
controller and mobile app. Featured with 3.5" LCD touch pad, Wi-Fi or USB
connectivity, magnetic heat bed and more.
Prints up to 100Hx100(Dia.)mm.
TL4412 Limited stock. In-store only.
SAVE
7"
NOW
249
$
50
$
2.4GHZ
EXPANDS
UP TO 4 CAMERAS
SAVE $50
4 Channel
720p Wireless DVR & Camera Kit
Allows you to connect via Ethernet to your
modem/router to view the camera while
outside the home or office. Records to SD
card (sold separately). Infrared camera
for day/night recording. QC3764
Spare 720p Camera QC3765
NOW $119 SAVE $30
32GB microSD card XC4992 $36.95
Professional Sound
Level Meter
Wide dynamic range
from 30dB to 130dB. Fast
(125ms) or Slow (1s)
response. USB connectivity.
QM1598
SAVE $50
5MP USB
Digital Microscope
10x to 300x magnification
for extra detail. LED
illumination. Adjustable
focus dial. QC3199
NOW
249
$
SAVE $50
FAST WI-FI TO EVERY
CORNER OF THE HOUSE
NOW
199
$
NOW
149
$
CAPTURES GEOMETRY
IN AS FAST AS 1 MINUTE!
NOW FROM
$
LCD
NOW
SAVE $50
AC1200 Wi-Fi
Mesh Network &
Satellite Kit
Speeds up to 1200Mbps (5GHz 867Mbps
+ 2.4GHz 300Mbps). Expandable with
additional satellite modules. YN8564
Extra Satellite Module
YN8566 NOW $99 SAVE $30
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CIRCUIT NOTEBOOK
Interesting circuit ideas which we have checked but not built and tested. Contributions will be paid for at
standard rates. All submissions should include full name, address & phone number.
Conway’s Game of Life on the Micromite
In 1970, mathematician John Horton Conway devised The Game of Life.
It illustrates how complex patterns
can be created by very simple rules.
This has many parallels in the natural world. The Game is based on an
infinite 2D grid of square cells. Thus,
each cell has eight neighbours.
Four simple rules are then applied:
1. If a live cell has one or no neighbours, it dies through loneliness
or under-population.
2. If a live cell has two or three
neighbours, it lives on to the next
generation.
3. If a live cell has four or more
neighbours, it dies through
over-population or overcrowding.
4. If a dead cell has exactly three
neighbours, it is born by reproduction.
An initial pattern of live cells is
entered into the grid, and the Game is
started. The Game then steps through
siliconchip.com.au
each generation. Some patterns die
out quickly, some become stable, and
others multiply indefinitely. For more
information, see https://w.wiki/3TKJ
I have developed two versions of
the Game of Life. The first runs on the
Micromite LCD BackPack with the
2.8in ILI9341-based touchscreen and
does not require any additional hardware. In addition to several pre-defined
starting patterns, the user can create
their own.
The second is designed as a standalone PCB (using the circuit shown
here) with a small 0.96in IPS display, and it can be used as an interactive display with the addition of
two pushbuttons or an infrared (IR)
remote control.
Alternatively, it can operate in fully
automatic mode, taking about 55 minutes to complete an entire cycle of all
the preset starting patterns. This can
be incorporated as wearable jewellery
Australia's electronics magazine
such as a brooch, or in other novelty
applications.
The software driver for the IPS display was written by Peter Mather and
edited by Peter Carnegie – see www.
thebackshed.com/forum/ViewTopic.
php?TID=7137
While the original Game was
designed for an infinite 2D grid of
cells, in the Micromite version, the
grid is limited to 32 x 24 cells for the
BackPack version or 32 x 20 cells for
the smaller IPS display. There is the
option for cells to drop off the edge
of the display, or wrap around from
one side to the other. The best choice
depends on how the initial pattern
develops.
For the circuit of the BackPack-based
version, see one of the BackPack
articles. The standalone version
shown here uses the same PIC32MX170F256B-50I/SP microcontroller programmed with the Micromite software,
plus a simple power supply and the
0.96in ST7735S-based 80 x 160 pixel
January 2022 61
The circuit built on a home-etched PCB at upper left, with two close-up shots
of the display in action. The software and PCB gerber files can be downloaded
from siliconchip.com.au/Shop/6/6085
IPS display. The display is controlled
using the SPI protocol via eight connections:
• GND and Vcc supply 3.3V.
• SCL (SCK in SPI mode) and SDA
(SDI in SPI mode) are the two SPI
protocol pins that connect to pin
25 (SPI Clock) and pin 3 (SPI out)
on the PIC chip, respectively.
• RES, DC and CS are control signals connected to pins 23, 22 and
21 on the PIC.
• BLK is the backlight control pin.
It is not used in this application.
The power supply is a simple 3.3V
linear regulator. An infrared (IR)
receiver or two push buttons (or both)
can optionally be connected to control
the display.
The IR receiver connects to pin 16
on the micro. If installed, you can
access the menu of preset demonstration patterns. The optional pushbuttons connect to pins 9 and 10. They
provide forward and backward scrolling through the menu of preset demonstration patterns.
Alternatively, pin 9 or 10 (or both)
can be permanently connected to
ground by fitting a wire link in place
of the switch. In this case, the display
runs in automatic mode, scrolling
through each of the pre-defined starting
patterns in turn as soon as the power
is applied. Pins 9 and 10 have weak
internal pull-up currents and thus do
62
Silicon Chip
not require external pull-up resistors.
In operation
Both versions start automatically
when power is applied. With the
BackPack version, you can select the
various pre-defined starting patterns
by using the up and down arrows on
the touchscreen. Touching the screen
whilst the Game is running returns to
the menu.
There is also the option of defining
your own starting pattern by touching
individual cells on the screen. Each
touch toggles a cell on or off. In this
case, a small red square at the bottom
right-hand corner acts as an Enter and
Start key. As mentioned above, the
standalone version uses the IR receiver
or pushbuttons to move through the
starting patterns menu.
Pressing the ‘next’ and ‘previous’
remote control buttons scroll through
the menu of preset demonstration
patterns. Pressing any other button
on the remote selects the menu item.
Pressing the ‘next’ or ‘previous’ button whilst the Game is running returns
to the menu.
You can set up your remote control
codes without amending the program
by pressing any key on your remote
control while the initial screen is displayed. You will then be asked to press
the key you want to assign to ‘next’
and then the one you want to assign
to ‘previous’.
These are then stored in non-volatile
memory so that they will be preserved
when the power is removed.
Alternatively, set the constants IR_
device, IR_next and IR_previous in the
Micromite program to match the codes
produced by your remote control.
With the pushbutton version, holding the pushbutton scrolls through the
menu items and releasing the pushbutton selects the menu item. Pressing
a button while the Game is running
returns to the menu.
Kenneth Horton,
Woolston, UK. ($150)
Circuit Ideas Wanted
Got an interesting original circuit that you have cleverly devised? We will pay
good money to feature it in Circuit Notebook. We can pay you by electronic
funds transfer, cheque or direct to your PayPal account. Or you can use the
funds to purchase anything from the SILICON CHIP Online Store, including PCBs
and components, back issues, subscriptions or whatever. Email your circuit
and descriptive text to editor<at>siliconchip.com.au
Australia's electronics magazine
siliconchip.com.au
Alternative PCB joiner for Linear MIDI Keyboard
Since designing the Linear MIDI
Keyboard (August 2021; siliconchip.
com.au/Article/14997), we realised
there is another way to join the PCBs.
The cut-down pin headers described
in that article are inexact and tricky
to fit, so we designed a small PCB to
make it easier.
We wrote that the pin headers should
be fitted before the switches, but the
Joiners are much easier to work with,
allowing fully assembled Keyboard
PCBs to be joined.
Two of these Joiner PCBs are needed
to join a pair of Keyboard PCBs; this
means a total of 14 Joiner PCBs for a
full 64-note Keyboard.
The Joiner PCBs have a tight solder
mask on one side to stop the solder
spreading and bridging the pads, so
this side should be against the Keyboard PCBs. The side with large solder pads goes on the outside.
Place the Joiner PCB onto the Keyboard PCB. It should line up with
the edges of the silkscreen printing
on the Keyboard PCB. Like any surface mounted part, tack one pad to
correctly locate the Joiner and adjust
as needed.
Unlike the pin header, you can
apply the iron from directly above.
Feed a generous amount of solder into
each pad hole. Surface tension should
pull the solder into the hole and onto
the pad, as long as all surfaces are
parallel and flush against each other.
Gently flip the Keyboard PCBs over
and repeat for the other side using a
second Joiner.
Now test for continuity between
adjacent PCBs. The pads on CON1,
CON3 and CON5 should bell out in
sequence, while those on CON2 and
CON4 will match and also should
connect to different pads on CON6.
If you are unsure, you can also check
the troubleshooting tips at the end of
the MIDI Keyboard article.
Tim Blythman,
Silicon Chip.
Compact reed relay module
Most of the relay modules available
on the internet, although quite inexpensive, are very large due to uncertain
voltage and current requirements. I
needed something smaller, suitable for
use on a breadboard. As many relays
have very short pins, the only option
was to design my own module.
Reed relays are my best option, not
only because of their small size, but also
for their characteristics. Reed relays
have hermetically-sealed contacts, protected against possible oxidation.
They also provide more consistent
switching at low signal levels, requiring less power to operate and with a
better on-resistance.
This is because reed relays use the
magnetic field from the coil to pull sets
of ferromagnetic reed switch contacts
together, which are already in very
close proximity. Thus they do not need
a larger and more complicated armature arrangement.
The relay module has four reed
relays in 4-pin SIL packages along
with SMD driver transistors, hidden
on the underside, plus a set of telltale LED indicators. The driver base
resistors and LED current-limiting
resistors are also SMD parts, keeping
siliconchip.com.au
the module very compact.
The two sets of relay contacts and
the driving connections are each broken out to 4-pin headers, while power
is supplied to the module via a 2-pin
Australia's electronics magazine
header. EAGLE and Gerber files for the
PCB are available from siliconchip.
com.au/Shop/6/6084
Gianni Pallotti,
North Rocks, NSW. ($75)
January 2022 63
The Pic Mite
A BASIC compatible interpreter
running on the Raspberry Pi Pico
Words and MMBasic by Geoff Graham, Firmware by Peter Mather
The PicoMite is a BASIC interpreter running on a Pi Pico which
supports over a dozen display panels, including OLED and e-Ink panels.
Connecting one is easy, as shown here. The PicoMite has extensive
support for displaying graphs, images and graphical objects, plus more.
T
he Raspberry Pi Pico is a microcontroller module with plenty of
memory, I/O and a USB connection.
Even better, it is cheap as chips and
readily available. The only problem is
that you need to be an expert programmer to get it to do anything.
That changes with the PicoMite, a
version of our popular MMBasic interpreter running on the Raspberry Pi
Pico. This lets you program it in the
easy-to-learn BASIC language with full
access to all of the Pico’s advanced
features. And this costs nothing; the
PicoMite firmware is entirely free for
you to download and use.
We have previously described the
Raspberry Pi Pico (December 2021;
siliconchip.com.au/Article/15125),
covering the hardware and programming requirements for the Pico using
the C or Micropython programming
languages. However, programming in
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Silicon Chip
C is beyond most casual experimenters. Micropython is easier, but it is still
a new language for most people and
takes time to learn.
MMBasic should be familiar to most
regular readers of Silicon Chip. It is
an implementation of the BASIC programming language, which is largely
compatible with Microsoft BASIC. It
has been used for over a decade (!)
on our Maximite series of computers
(since March 2011) and Micromite
controllers (since May 2014).
The BASIC language was initially
designed to teach programming and
therefore is easy to learn and use. You
can get it to do something with just
one line, and the programming environment is particularly easy.
A single keypress will set your program running and, if it fails with an
error, you will get a plain text error
message. A second keypress lets you
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jump back into the editor with the cursor positioned on the line that caused
the error.
MMBasic also makes it easy to use
the hardware features of the Raspberry Pi Pico. They are accessed using
straightforward high-level commands
that avoid the complexities of dealing
with the RP2040 chip and its hundreds of programming registers (the
data sheet for the RP2040 alone runs
to over 600 pages).
For example, this is all that you
need to send the word “hello” out of
a serial port:
SETPIN GP13, GP16, COM1
OPEN “COM1:” AS #1
PRINT #1, “hello”
The first line allocates the I/O pins
as the serial port, the second initialises the port and the third sends the
text. Easy.
siliconchip.com.au
MMBasic features
A major feature of the PicoMite is
that it uses a full implementation of the
BASIC language, not some cut-down
version. You have three data types
(double precision floating point, 64-bit
integers and strings), long variable
names, arrays with multiple dimensions and user-defined subroutines
and functions. The list opposite gives
an idea of its other features.
MMBasic is largely compatible with
Microsoft BASIC, so many programs
downloaded from the Internet will run
with little change.
MMBasic also includes a built-in
full-screen editor which lets you edit
large programs directly on the Pico
Mite. The edit/run/edit cycle is very
fast, with a single keypress to jump
between editing and running the program, then another to go back to editing again.
MMBasic supports the full Raspberry Pi Pico set of hardware features,
many of which are mentioned in the
features list. MMBasic also adds features not native to the Raspberry Pi
Pico, including support for SD cards
and over a dozen LCD panel types,
including touch input and advanced
graphics.
These capabilities are all covered
in detail in the PicoMite User Manual, downloadable from the Silicon
Chip website at siliconchip.com.au/
Shop/6/6060, or the author’s website (http://geoffg.net/picomite.html).
That’s an extensive document, so the
remainder of this article will cover the
highlights and most important aspects
of the PicoMite.
The firmware is structured to work
on any module using the RP2040 processor with at least 2MB of flash memory. As described in our article on the
Pico, the RP2040 processor is used on
many boards, including the Arduino
Nano RP2040 Connect, the Adafruit
Feather RP2040 and other variants
from companies like Sparkfun and
Pimoroni.
So you can load and use the Pico
Mite firmware on these just as well.
We have published several MMBasic programming tutorials, including a two-part series on Getting Started
with MMBasic in February, March,
May & June 2017 (siliconchip.com.au/
Series/311) and Advanced Programming with MMBasic in the November
& December 2016 issues (siliconchip.
com.au/Series/307).
siliconchip.com.au
Full-featured, Microsoft BASIC compatible interpreter running on
the Raspberry Pi Pico.
Will work on any RP2040-based module with at least 2MB of flash.
Runs from 1.8-5.5V at 11-43mA, depending on the CPU clock
speed.
Variables can be floating-point numbers, 64-bit integers or
strings with support for long variable names, arrays with
multiple dimensions, extensive string handling and user-defined
subroutines and functions.
A focus on ease-of-use with a beginner-friendly programming
language, informative error messages and a rapid development
cycle.
Full support for all 26 Raspberry Pi Pico input/output pins and
features. All pins can be digital inputs or outputs, along with up to
three analog inputs, two bidirectional serial ports to over 1Mbaud,
two SPI master ports to over 30MHz, two I2C master ports, 16
pulse-width modulated (PWM) outputs and 1-Wire I/O pins.
Up to ten programs can be saved on the module, each up to 80KB;
chaining allows for programs up to 800KB. RAM for variables,
arrays and buffers is configurable and can be up to 80KB.
Any program can be set to automatically run on power-up or reset.
Configurable clock speed (48 to 250MHz).
Internal temperature sensing of the processor.
Supports colour displays up to 3.5in (diagonal), allowing the BASIC
program to display text and draw lines, circles, boxes, etc in 65,535
colours. Resistive touch controllers are also supported.
SD cards up to 32GB formatted in FAT16 or FAT32 are fully
supported. This includes opening files for reading, writing or
random access and loading and saving programs. It can play audio
files (WAV format) on PWM outputs.
Built-in support for commonly used devices including infrared
remote controls, ultrasonic distance sensors, temperature sensors,
humidity sensors, text display modules, battery-backed clock,
numeric keypads and more.
Programming and control via USB with no special software
required; any computer running a VT100 terminal emulator will
work.
Programs can be easily transferred from a computer (Windows,
Mac or Linux) via SD card, by using the XModem protocol or by
streaming the program over the USB console.
The built-in full-screen editor includes advanced features such as
colour-coded syntax, search and copy, cut and paste.
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January 2022 65
up; the PicoMite will disconnect and
then reconnect as a USB flash drive
on your computer, ready for the firmware upload.
The console
The Raspberry Pi Pico is a popular,
low-cost microcontroller module with
plenty of memory, speed and I/Os. With our PicoMite
firmware, you can program it in the easy-to-learn BASIC
language with full access to all of the Raspberry Pi Pico’s advanced features.
Micromite compatibility
For readers familiar with our Micromite series of microcontrollers, the
PicoMite is fully compatible with just
a few differences to accommodate the
unique hardware aspects of the Raspberry Pi Pico.
This compatibility is so complete
that you can take a BASIC program
such as that used on our Micromite
Air Quality Monitor (February 2020;
siliconchip.com.au/Article/12337)
and run it on the Raspberry Pi Pico
with few or no changes (see screen
grab overleaf).
The PicoMite essentially implements all the features of the Micromite Plus except for display panels
with a parallel interface, the library
function and attached keyboards. Features inherited from the Micromite
Plus include embedded C code, support for serial LCD panels, embedded
fonts, advanced graphical (GUI) controls and an SD card interface with full
FAT32 filesystem support.
The PicoMite has fewer I/O pins
than the Micromite Plus but it runs
faster (up to 250MHz) and can accommodate larger programs. Probably its
best feature is that it is a complete
module with a USB connector, power
supply and breadboard-friendly interface pins—all for a ridiculously low
price (as little as $6!).
Loading the firmware
The RP2040 processor has a small
amount of fixed read-only memory
reserved for loading the firmware
(called the bootloader), making it easy
to load and test new firmware without
special software.
The following process will work
with any modern computer (Windows,
macOS or Linux).
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First, download the PicoMite firmware from one of the sites linked
above. This is a zipped archive and
the firmware file inside it has an extension of “.uf2”.
Hold down the white button marked
BOOTSEL on the top of the Pico and
plug its USB interface into your computer while still holding down the
button. Your computer should make
a sound indicating a new USB device
has been discovered, and the Pico will
appear as a USB flash drive on your
computer.
Finally, drag and drop the firmware
file onto the ‘drive’ created by the Pico,
and your computer will upload it to
the Pico. When the copy is complete,
the Pico will automatically restart running MMBasic and reconnect to your
computer, this time as a virtual serial
port over USB. The green LED on the
top of the Pico board will start slowly
flashing to indicate that the PicoMite
firmware is now running.
The only purpose of the drive created by the Pico is to load firmware;
any other type of file copied to it will
be ignored. The firmware file will
vanish when the copy completes, so
this drive cannot be used as a memory stick.
The handy thing about this process
is that you can use it to install whatever firmware you like – you can easily
upgrade (or downgrade) the PicoMite
firmware or install something completely different (like Micropython)
then later revert to the PicoMite firmware if you so wish.
To make it easier to upgrade the
PicoMite firmware, you can issue
the command UPDATE FIRMWARE
at the MMBasic command prompt.
This will be as if you had pressed the
BOOTSEL button while powering
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When the Raspberry Pi Pico reconnects to your computer following the
firmware installation, it will act as an
asynchronous serial port over USB.
This is the MMBasic console; using
this, you can configure MMBasic,
load/run/edit programs etc. This will
be familiar to anyone who has worked
with the Micromite and it works the
same.
The serial port uses the CDC protocol and the drivers for this are standard
in Windows 10 and will load automatically. For Windows 7 or 8.1, you will
need a tool like Zadig (https://zadig.
akeo.ie/) to install a generic driver
for a “usbser” device. For macOS and
Linux, see the notes in the PicoMite
User Manual (but generally, it will
‘just work’ with a recent version of
either OS).
To use the console, you need to
install a terminal emulator which will
send your keystrokes to the PicoMite
and display anything sent back by it.
The recommended emulator for Windows is Tera Term (http://tera-term.
en.lo4d.com/) which is free to download and use.
The terminal emulator will need to
know the number of the virtual serial
port generated when the PicoMite is
connected to your computer. With
Windows, you can find that using
Device Manager. This port number
is entered in Tera Term by going to
Setup → Serial Port... The other settings, including the baud rate, can be
left at their defaults.
Note that setting the baud rate to
1200 is another way of forcing the
Pico into its update firmware mode,
so avoid using that rate.
With everything set up, pressing the
Enter key in your terminal emulator
should cause the PicoMite to echo back
the greater than symbol (>), which is
the MMBasic command prompt. To
verify that you are indeed connected
to a miniature BASIC computer, you
can try a few commands:
PRINT MM.VER
Displays the version number of the
firmware.
MEMORY
Displays the amount of free memory.
siliconchip.com.au
PRINT PI
Displays an approximation of pi (π).
Test program
The standard test that people use
when experimenting with a new
microcontroller is to get it to flash one
LED on and off.
For this, we can use the green LED
on the top of the Pico’s PCB. When
MMBasic is running, this will slowly
flash on/off, but for our test program
we will take control of it and cause it
to flash much more rapidly.
The easiest way to enter a short
BASIC program to do that is with the
PicoMite’s built-in editor.
This works the same as most of the
editors that you will have used in the
past. For example, any text typed in
will be inserted at the cursor’s location,
the arrow keys will move the cursor
around, the delete key will delete the
character at the cursor and the backspace key will delete the character
before the cursor.
The MMBasic editor has many
other functions (search, replace, copy,
paste etc) and these are detailed in the
PicoMite User Manual.
Type in the command EDIT at the
command prompt to start the editor,
then type in the following program:
SETPIN GP25, DOUT
DO
PIN(GP25) = 1
PAUSE 100
PIN(GP25) = 0
PAUSE 300
LOOP
When you have finished, press the
F2 key on your keyboard (or CTRL+W).
This will save your program, exit the
editor and start the program running.
You should be rewarded with the LED
on the Pico rapidly flashing.
If something goes wrong, you will
get an error message. In that case,
rerun the editor with the EDIT command and it will place the cursor on
the line that caused the error, ready
for you to correct it.
The program starts by defining the
I/O pin driving the LED (GP25) as an
output, which places it under our program’s control.
Then the program enters a loop
where the pin is set high (which illuminates the LED) followed by a short
pause of 100ms, then low followed
by a 300ms pause. This repeats continuously.
siliconchip.com.au
You can break out of this program by
pressing CTRL+C, which will return
you to the command prompt where
you can (if you wish) restart the editor
and modify the program—for example, altering the delays to change the
flash rate.
Saving the program
On the PicoMite, the BASIC program
is held in RAM. This is necessary for
good performance; flash memory is
on a separate chip to the RP2040 processor and is accessed via a relatively
slow serial interface, while the RAM
is inside the RP2040 and therefore
quick to access.
The PicoMite firmware also loads
critical sections of the MMBasic
interpreter into RAM. This way, even
though most of the PicoMite firmware
is held in flash memory, BASIC programs run just as fast on the PicoMite
as on other microcontrollers with
internal flash memory.
RAM is volatile, and its contents
are lost if the power is interrupted.
So the PicoMite will automatically
save a copy in a reserved area of
flash memory and restore that on
power-up – or when the processor
is restarted. The result is that you
are not aware of the volatile nature
of RAM.
You can save multiple programs in
the PicoMite’s flash memory using the
command “FLASH SAVE n”, where n
is a number between 1 and 10 which
indicates the saved program’s location
in flash memory. This means that you
can save up to 10 independent programs to flash.
For example, to save your program
in location 1, you would use this command:
FLASH SAVE 1
And you can run it anytime using
this command:
FLASH RUN 1
If you want this program to start running automatically every time power
is applied, issue the command:
OPTION AUTORUN 1
Similar commands allow you to list
the flash locations, erase locations,
overwrite locations etc. If you have
attached an SD card to the PicoMite
(details below), you can also save,
load and run programs from the SD
card.
Be aware that any programs saved
to the flash memory can be corrupted
when upgrading the firmware, so they
should be backed up before upgrading. This is because programs saved
to flash have had keywords converted
to tokens, and the upgraded firmware
may use different tokens.
If you forget and find your saved programs corrupted, you can downgrade
to the previous version, back up your
programs and then upgrade again.
PicoMite inputs & outputs
The I/O pin layout of the PicoMite
is shown in Fig.1. There are 26 usable
I/O pins. All can act as digital inputs
or outputs, while three can be used
as analog inputs (to measure voltage).
There are also seven ground pins,
one 3.3V output for external circuitry
Fig.1: the I/O pins on the Raspberry Pi Pico and their capabilities under
MMBasic. The full details are in the PicoMite User Manual, but here are some
notes. VBUS is the 5V supply from the USB port, VSYS is the 5V input to the
SMPS, 3V3EN enables the 3.3V regulator (low = off), RUN is the active-low reset
pin, ADC VREF is the reference for voltage measurement and AGND is analog
ground.
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January 2022 67
and some other pins, which we will
cover later.
The pins can be referenced by their
pin number on the Pico board (4, 5,
6 etc) or their logical reference (GP2,
GP3 etc). These are shown in green in
Fig.1. For example, within MMBasic,
PIN(17) and PIN(GP13) refer to the
same I/O pin.
To define how a pin works, you use
the command “SETPIN pin, function”.
Here, ‘pin’ is the I/O pin reference
(eg, GP13) and ‘function’ is how you
wish the pin to act. Common functions are DIN (digital input), DOUT
(digital output), AIN (analog input),
FIN (measure frequency) and so on.
The PicoMite User Manual describes
these in detail.
As an example, the following will
configure GP7 to measure frequency:
SETPIN GP7, FIN
As the PicoMite firmware has been
designed to run on other boards that
also use the RP2040 processor, the four
I/O pins that are hidden on the Raspberry Pi Pico (GP23, GP24, GP25 and
GP29) are usable in MMBasic as they
may be exposed on other modules.
The pin allocations for functions
such as SPI, I2C and serial are somewhat configurable. For example, the
receive pin for the second serial port
(COM2:) can be GP5, GP9 or GP21 and
the transmit pin can be GP4, GP8 or
GP20. These pins are marked in cyan
in Fig.1, as COM2 RX and COM2 TX.
These pin allocations work equally
well but must be configured via the
SETPIN command before opening the
serial port.
The Pico has two serial ports,
two SPI ports, two I2C ports and 16
PWM-capable outputs. Within MMBasic, they are all accessed in the
same way; first, allocate the I/O pins
using Fig.1 as your guide, then open
the channel or device, then use the
function.
Powering the PicoMite
The Raspberry Pi Pico has a particularly flexible power system which
gives the user several options for powering the module. The power supply
is shown in Fig.2 and consists of the
main USB input, where the 5V power
from this source is fed via a schottky
diode to a switch-mode power supply (SMPS) that is capable of both
buck (step-down) and boost (step-up)
operation.
Its 3.3V output is used to power the
rest of the board and is made available
on an edge pin (3V3) for powering
external circuitry.
The SMPS has an input range from
1.8V to 5.5V, which lends a great deal
of flexibility to the Pico. It means that
it can be powered via USB or a USB
charger, a single Li-ion cell or a couple of AA cells, to name a few options.
In general, there are three ways to
supply power. The first is simply a
USB source such as a laptop plugged
into the USB socket. An alternative
power source might be required for
embedded applications, and this can
be supplied via a schottky diode to the
pin marked VSYS (pin 39).
The schottky diode means that
either or both the USB and external
power source can be present without
interfering with each other. This is
handy if you want to plug a laptop into
the Pico’s USB socket to debug your
code while the module is in-circuit.
The third method is to short the
3VEN pin (pin 37) to ground and
supply an external source of 3.3V to
the module via the 3V3 pin (pin 36).
Grounding 3VEN will shut down the
SMPS regulator and disconnect its output so that the 3V3 pin can be used as
a 3.3V power input.
The switching regulator generates a
lot of electrical noise, so using a linear
regulator to supply 3.3V to the board
will make it much easier to use the
analog inputs and produce noise-free
audio signals using PWM.
The power consumption of the
PicoMite is modest. At its default
125MHz CPU clock, it draws about
21mA. This does not include any
power drawn from the I/O pins or the
3V3 pin.
The RP2040 processor’s clock can
be varied from 48MHz to 250MHz
under control of MMBasic (using the
“OPTION CPUSPEED” command),
and the power drawn varies accordingly, from 11mA to 43mA.
Three AA alkaline cells can power
the PicoMite running at 48MHz for
weeks of continuous operation.
Note that the specified top clock
speed for the Raspberry Pi Pico is
133MHz; anything above that is
regarded as overclocking. We tested
several modules and most worked at
250MHz, so that can be considered a
viable option.
Special device support
The PicoMite inherits support for
several special devices from the Micromite. This includes an infrared remote
control decoder supporting Sony and
NEC remote controls, allowing BASIC
programs to act on signals from universal remotes.
Other natively supported devices
include temperature sensors, humidity sensors, ultrasonic distance sensors,
numeric keypads, and two-line LCD
modules. All of these are easy to use.
For example, the DISTANCE() function will trigger an ultrasonic distance
sensor, wait for the echo and return
the distance to the target in centimetres for your BASIC program to act on.
As another example, if you want
to measure temperature, just attach a
DS18B20 sensor and use the TEMPR
function to get the temperature in °C
with a resolution of 0.1°C. You do not
need to load libraries or write many
lines of code; these functions are built
in, and they just work.
SD card support
The PicoMite has built-in support
for SD cards up to 32GB, formatted as
FAT16 or FAT32. This includes full
read/write for both programs and data
files, navigating through subdirectories and support for long filenames.
The files created by the PicoMite can
be read and written on computers running Windows, Linux or macOS.
Fig.2: the Raspberry Pi Pico has a flexible power system. The input
voltage from either the USB or VBUS inputs is connected through a
schottky diode to the buck-boost switch mode power supply, which
produces 3.3V. This accommodates input voltages from 1.8V to 5.5V,
allowing the PicoMite to run from a wide range of power sources,
including single Li-ion cells and 2-3 alkaline cells.
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siliconchip.com.au
Fig.3: the PicoMite
has full support for
(micro)SD cards.
This diagram
shows one way of
connecting an SD
card to the PicoMite
and matches the
example configuration
commands listed in
the text. MMBasic can
open files for reading,
writing or random
access and load or
save programs with
cards up to 32GB
formatted with FAT16
or FAT32.
Communication with SD cards is via
the SPI protocol, also used by many
LCD panels and touch controllers.
These all use what is called the System SPI port on the PicoMite, and the
I/O pins used by this port need to be
specified before any of these devices
can be used. This is done using the
following command:
OPTION SYSTEM SPI CLK, TX,
RX
Here, CLK, TX and RX are the pins to
use for these functions (as determined
from Fig.1). For example, the following
will dedicate the second SPI channel
(called SPI2) to the System SPI function and define the I/O pins to use:
OPTION SYSTEM SPI GP10,
GP11, GP12
This option will be saved in flash
memory and will be automatically
reapplied on power-up, so it only
needs to be entered once. Additionally, other SPI devices such as display panels will also use this port,
so it does not need to be redefined
for them. When allocated to the System SPI function, that port will not be
available to the BASIC program (ie,
it will be dedicated to the firmware).
One thing to watch out for is that this
command and other similar OPTION
commands will cause the PicoMite to
restart and that will disconnect your
USB console connection, so you will
need to re-establish it after entering
the OPTION command.
With the System SPI port defined,
you can tell MMBasic that an SD card
is connected and what pin to use for
the Chip Select signal (CS). For example, if you used GP22 for Chip Select,
the command would be:
OPTION SDCARD GP22
As before, this option will be saved
and automatically reapplied on powerup. It will also cause the PicoMite to
restart.
Fig.3 shows how the SD card socket
should be wired up. With that done
and the SD card interface configured
in MMBasic, you can pop a card into
the socket and try the “FILES” command, which should list the files and
directories on the card.
PWM and audio output
With 16 PWM outputs, the Pico
Mite has so many that you could (for
example) dedicate some to controlling
indicator LEDs. Your program can then
create some cool effects by ramping
the brightness up and down rather
than simply switching the LEDs off
and on. An RGB LED driven by three
Connecting an SD card is simple and MMBasic provides full access to the files and directories on the card. BASIC
programs can open or create files for reading, writing or random access, navigate the directory structure and create or
delete directories. The files created by MMBasic can be accessed by computers running Windows, Linux or macOS. This
does not match Fig.3 exactly, but only because a different GND pin has been used.
siliconchip.com.au
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January 2022 69
PWM outputs would let you create
almost any colour.
One important use for PWM outputs is to generate program-controlled
voltages, which can control analog
devices such as motor speed controllers. For this, you just need to add a
simple low-pass filter (details in the
user manual) on the output to remove
the carrier frequency.
Another use is to play stereo WAV
audio files from an SD card via a lowpass filter. These sound effects can
be almost anything: chimes, voice
instructions, a warning siren or simply background music.
Playing the audio does not interrupt
the BASIC program as MMBasic will
play it in the background, so your program can continue doing its job (eg,
controlling some process) regardless
of the duration of the audio output.
The audio output can also generate
precise sinewaves for a simple “beep”
or, because the frequency is very accurate, test the response of loudspeakers
and other audio components.
Display panels
The PicoMite includes support for
many display panels using various
controller chips. These are mostly
LCDs, but it also supports OLED and
e-Ink based panels, ranging from a
tiny 84 x 48 pixels to a more substantial 480 x 320 pixels. All of these use
either the SPI or I2C interfaces.
Panels using a parallel interface
(as on the Micromite Plus) are not
supported as there are not enough
I/O pins on the Raspberry Pi Pico to
practically implement that type of
interface.
Two popular series of LCD screens
are based on the ILI9341 and ILI9488
controllers. The ILI9341 version
comes in various sizes from 2.2in to
2.8in diagonal with 320 x 240 pixels.
The ILI9488-based panels are generally 3.5in diagonally and have 480 x
320 pixels. Both use the System SPI
bus, which needs to be configured as
described above.
Both LCD panels are set up similarly:
OPTION LCDPANEL CTRL, OR,
DC, RST, CS
Where CTRL is the name of the controller chip, OR is the orientation (portrait, landscape etc), DC is the pin to
use for the data/control signal, RST is
the pin used for the reset signal and
CS is the chip select pin.
For example, to set up a panel with
the ILI9341 controller in landscape orientation, wired as in Fig.4, the command would be:
OPTION LCDPANEL ILI9341,
L, GP26, GP27, GP28
That’s assuming you already have
System SPI on GP18, GP19 & GP20 to
suit the wiring shown in Fig.4.
With the display panel configured,
you can test it by running the command GUI TEST LCDPANEL and you
should be greeted with multiple overlapping circles popping up all over
the LCD screen (as shown in the lead
photo). To terminate the test, press
any key.
Two of the supported displays use
an I2C interface. To connect these, the
System I2C interface must be configured similarly to the System SPI interface. The command is:
Fig.4: here’s one way to wire up a touchscreen to the PicoMite. If you connect
an SD card at the same time, you need to use the same SPI RX, TX and CLK
connections for both. While this shows an ILI9341-based 320x240 display, the
connections required for the ILI9488-based 480x320 touchscreens are virtually
identical.
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Silicon Chip
Australia's electronics magazine
OPTION SYSTEM I2C SDA, SCL
Currently, the only other device that
uses the System I2C interface is the
real-time clock.
Many LCD panels incorporate a
resistive touch interface. This controller also uses the SPI protocol and
should be connected as per the System SPI interface (like in Fig.4). Configuring the touch interface is straightforward, but it needs to be done after
configuring the display panel. The
command is:
OPTION TOUCH CS, IRQ
CS is the Chip Select output pin and
IRQ is the interrupt input pin. For the
circuit shown in Fig.4, this would be:
OPTION TOUCH GP22, GP21
After the PicoMite has restarted, you
need to calibrate the touch system with
the GUI CALIBRATE command. This
will progressively draw a target on all
four corners of the screen for you to
touch and the firmware will use that
to accurately identify the pixel coordinates of any touch.
Graphics support
Connecting an LCD screen is quite
common in the microcontroller world.
What sets MMBasic apart is its extensive support for displaying graphs,
images and graphical objects on the
screen. This, along with the touch
input, means that a user of your program can control your gadget using a
colourful LCD screen with intuitive
on-screen objects such as switches,
keypads, dials and lights.
The basic drawing commands allow
you to set any pixel to any colour,
draw lines, circles and boxes and
draw text anywhere on the screen in
any colour. The PicoMite includes
seven differently-sized fonts, and you
can embed more fonts in the BASIC
program to provide precisely the look
you want.
If an SD card is fitted, the program
can load images from the card and display these on the LCD panel. You can
use this to show a logo or load a textured graphical background.
The PicoMite has also inherited
the advanced GUI controls from the
Maximite Plus. These include radio
buttons, checkboxes, on-screen dials,
numeric input fields and much more.
All of these require just one command
in the BASIC program to define their
siliconchip.com.au
One feature (of
many) that sets the
PicoMite apart is its
extensive support
for graphs, images
and graphical
objects. Along with
the touch input,
this means that
users can control
your gadget using
a colourful LCD
screen with intuitive
on-screen objects
such as switches,
keypads, dials and
lights.
position and characteristics (colour,
size etc).
From then on, MMBasic will
manage the control for you. That
includes making a button look like it
is depressed when touched, checking
a check box, drawing a graph etc. All
that the BASIC program needs to do
is check the status of a control (ticked,
depressed etc) and take the appropriate action.
The most advanced GUI control is
the Text Input Box. When touched by
the user, MMBasic will pop up a full
on-screen QWERTY keyboard for text
input. This allows the user to enter any
text required by the program. While
a full keyboard sounds as if it would
be impracticable on a small display
panel, it is actually quite useable, even
on the 2.8in LCD screens.
More information
The PicoMite is fully
compatible with our
Micromite series of
microcontrollers,
with just a few
differences to
accommodate the
unique features
of the Raspberry
Pi Pico. This
screenshot shows
the PicoMite
running our
Micromite Air
Quality Monitor
from February 2020,
originally designed
for the Micromite
LCD BackPack.
The PicoMite is supported by the
PicoMite User Manual, which can
be downloaded from the S ilicon
Chip website at siliconchip.com.au/
Shop/6/6060, or the author’s website
(http://geoffg.net/picomite.html). This
manual runs to over 160 pages and
covers the details of using the Pico
Mite and writing programs, including a tutorial on programming in the
BASIC language.
There is also an active user community on The Back Shed Forum
(thebackshed.com/forum/ViewForum.
php?FID=16), where many PicoMite
users and experts in BASIC programming hang out. They are a friendly
bunch and will be happy to help out
if you are stuck on a complicated
problem.
The PicoMite firmware is completely free, and you can get the Raspberry Pi Pico for as little as $6, so the
cost of playing with this powerful little fellow is tiny. Why not give it a go?
You might just want to have fun making a LED flash, but it could evolve
into your next burglar alarm or reticSC
ulation controller.
While it has
fewer I/O pins,
you can also turn
other RP2040based boards like
this Tiny2040
into a PicoMite
with the same
firmware.
siliconchip.com.au
When the user touches a text box on the screen, a keyboard like this pops up,
allowing them to enter a name or other text string.
Australia's electronics magazine
January 2022 71
Using Cheap Asian Electronic Modules
By Jim Rowe
Geekcreit’s LTDZ V5.0
Spectrum Analyser
This compact unit is low in cost but can perform spectral analysis from
35MHz to 4.4GHz. It also includes a tracking generator for frequencydomain analysis of filters, RF amplifiers and similar items. It needs to
be controlled from a PC via a USB cable (which also provides its 5V DC
power supply), using a very impressive free application.
A
bout a year ago, I bought an earlier version of the Geekcreit LTDZ
spectrum analyser, which came as a
‘naked PCB’ module. The idea was to
check it out and write a review for Silicon Chip, but I wasn’t too impressed
when I tried it out.
The software needed to control it
was both difficult to find and rather
flaky, and the unit itself had poor sensitivity combined with a relatively
high noise floor. There wasn’t much
I could say about it that was positive,
so I decided to give it a pass.
But earlier this year, I found that an
improved version of the analyser had
become available (the LTDZ V5.0),
coming inside an extruded aluminium case and not costing all that much
more than the original ‘naked’ version.
I also discovered that although
Geekcreit was still recommending
the same control software that I had
found so problematic, a much better
program had appeared – one that you
can download for free.
It’s called VMA Simple Spectrum
Analyser (VMA SSA), written by Vitor
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Silicon Chip
Martins Augusto, who lives in Portugal, and it can be downloaded from
his site: siliconchip.com.au/link/ab87
So I went ahead and ordered an
LTDZ V5.0 from the Banggood website (siliconchip.com.au/link/ab88),
paying US$46 plus US$4.87 for shipping, which came to a total of $75. I
also downloaded Mr Augusto’s VMA
SSA software.
As you can see from the photos, the
LTDZ V5.0 is quite compact at 62 x 55
x 19mm, not counting the two SMA
connectors extending from the input/
output end.
It also weighs only 83 grams. It
comes complete with a 950mm-long
USB2.0 cable, with a Type-A plug at
one end and a micro Type-B connector
at the other end, to connect it to a PC.
The LTDZ V5.0 is quite well made,
although the panels at each end of the
case in the unit I received had holes
for the countersink-head mounting
screws which were not countersunk.
This made it look unfinished until I
removed the panels and countersunk
their holes to complete the job.
Australia's electronics magazine
This also gave me the opportunity
to examine the PCB inside and take
its photo. All of the components in
the LTDZ V5.0 are mounted directly
on this PCB.
Like the Geekcreit VHF-UHF signal
generator module I reviewed recently
(December 2021; siliconchip.com.au/
Article/15139), the LTDZ V5.0 uses
the Analog Devices ADF4351 digital
PLL synthesiser chip. In fact, it uses
two of them: one in the analyser section, and one in the tracking generator
(TG) section.
The ADF4351 is quite a complex
device, but we had a pretty detailed
description of how it works in the May
2018 issue, specifically my review of
the Digitally Controlled Oscillator
module (May 2018; siliconchip.com.
au/Article/11073).
So please read that article if you
want to know more about how this
chip works. You can also find the
data sheet for it at: siliconchip.com.
au/link/aajc
By the way, the LTDZ draws about
100mA from the PC in standby mode,
siliconchip.com.au
Fig.1: block diagram of the LTDZ 5.0
module. The most important sections are
the two ADF4351 synthesisers and the
STM32 ARM microcontroller.
rising to about 350mA when it’s scanning with the tracking generator also
running.
How the analyser works
I have prepared a block diagram
(Fig.1) that shows how the LTDZ 5.0
works. The ADF4351 chip at the bottom of this diagram forms the heart of
the analyser section, while the one at
upper right provides the tracking generator function.
The STM32F103 MCU (microcontroller) handles the operation of both
sections, directed by the software
running in the PC. The two USB signal lines (D- & D+) from the LTDZ’s
micro-USB connector at upper left
pass through a CH340G USART chip
before reaching the MCU. The micro
has an 8MHz clock crystal, while the
CH340G has a 12MHz crystal.
Both ADF4351 synthesiser chips are
supplied with their master reference
clock from the 25MHz crystal oscillator at centre right. But they are controlled by the MCU via two separate
SPI (serial program interface) ports.
The analyser ADF4351 is controlled
via the MCU’s SPI1 port (SPI_SCK,
SPI_MOSI and SPI_NSS), while the
tracking generator ADF4351 is controlled via the SPI2 port.
The spectrum analyser section of
the LTDZ involves the devices and signal paths shown at lower left in Fig.1.
This spectrum analyser operates
similarly to a ‘superheterodyne’ radio
receiver, where incoming signals at a
relatively high frequency are shifted
down to a much lower fixed IF (intermediate frequency) before being
detected.
In this case, the ADF4351 at lower
centre corresponds to the local oscillator (LO). Its output is fed to one input
of the IAM-81008 double-balanced
mixer while the Analyser’s input signal goes to the other input. So its output will be the heterodyne products
of the two signals.
The mixer’s output signal then goes
through a low-pass filter to remove any
‘sum’ heterodyne components, leaving only the difference, which is the
IF signal we want.
This is then fed to an AD8307 logarithmic amplifier and detector, which
generates a DC output voltage proportional to the IF signal level. This, in
The internals of the
Geekcreit LTDZ spectrum
analyser.
siliconchip.com.au
Australia's electronics magazine
January 2022 73
Screen 1: the VMA SSA software output when the LTDZ input is terminated
with a 50W resistor over its frequency range of 35-4400MHz.
Screen 2: the LTDZ input was now connected to an external VHF/UHF discone
antenna with a plot over 200-208MHz. The average signal level was -49dBm
over that range.
turn, goes to an analog-to-digital input
(ADC123) of the MCU.
As a result of all this, the MCU can
measure the input signal level corresponding to the current frequency of
the ADF4351’ local oscillator’.
As the MCU changes the LO frequency over the selected range, it can
send measurements of the input signal level at each point back to the software running in the PC. The software
can then take these measurements
and present them as a graph, plotted
against frequency. That’s how this type
of spectrum analyser works.
This is the same basic system used
in many spectrum analysers (while
some instead use very fast sampling
and a digital Fourier transform). But
in place of the simple low-pass filter between the mixer and the log
detector, high-end models have several selectable bandpass filters which
offer a choice of resolution bandwidth
(RBW) settings.
Most higher-end units also have a
wideband amplifier between the RF
input connector and the mixer’s input,
increasing the analyser’s input sensitivity. This is so that they can analyse
lower level signals, like those from
many antennas.
The tracking generator is really just
the second ADF4351 chip, which the
MCU can program to provide an output signal of the same frequency that
is currently being sensed by the analyser section, at a relatively constant
level of approximately 0dBm (224mV).
The tracking generator can be
switched on or off using pushbutton
switch S1, so it can be turned on only
when needed.
There are also four indicator LEDs
shown in Fig.1. LED1 indicates when
the tracking generator is enabled,
LED3 when the LTDZ has power
applied, LED4 when the analyser section is working, and LED2 when both
ADF4351s are locked to the designated
frequency.
The VMA SSA application
Screen 3: a Gratten GA1484B VHF-UHF signal generator was used to provide
the LTDZ with an unmodulated 2.5GHz output at 0dBm. The software was then
set to scan over 2.4-2.6GHz.
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Silicon Chip
Australia's electronics magazine
As mentioned earlier, Mr Augusto’s VMA SSA software can be downloaded for free (siliconchip.com.au/
link/ab87). You can also download
a 54-page PDF User Guide from the
same page.
However, after downloading and
installing the app, you have to contact him by email to obtain an activation code before you can run it. This
siliconchip.com.au
activation code will only function for
up to three months, after which you
will have to request another code. Or, if
you wish, you can make a small donation via PayPal of around US$10, after
which you will be sent a ‘permanent’
activation code.
After using VMA SSA for a short
time, I was so impressed that I sent
Mr Augusto a donation of $25 and
received a permanent activation code.
There is no doubt in my mind that it’s
massively better and much easier to
use than the NWT4.11.09 software that
Geekcreit still recommends.
Incidentally, the file you download
from Mr Augusto’s site is zipped, but
when you unzip it, you will get the
main EXE file plus several auxiliary
files.
All you have to do is copy it to a
suitable folder and then launch the
executable. But don’t install it to “C:\
Program Files” or “C:\Program Files
(X86)” because Windows 10 limits
access to files in those folders, which
can cause problems.
The ‘front’ of the LTDZ module houses the SMA sockets for the RF input
and output connections. There are two status LEDs which show the current
operating mode.
Trying it out
All I had to do initially was plug
the LTDZ into my computer using the
supplied cable and launch the VMA
SSA software. Next, I clicked on its
Setup menu, to tell it the virtual COM
port number which the LTDZ has been
assigned (in my case, COM3) and the
particular Analyser model.
The VMA SSA application can
work with five different units, with
the LTDZ V5.0 listed as “SMA Simple Spectrum Analyser Version 2 –
35MHz-4.4GHz – ADF4351”.
You then need to select the “Spectrum” option at the top left of the
screen. This gives you the main screen
for spectrum analysis, as shown in the
screen grabs.
Most of the screen is occupied by
the centre plotting graticule, with a
narrower graticule below it that can
show a ‘waterfall’ display (although
the two can be swapped, if you wish).
On the right are most of the control
setting controls, with a large START/
STOP button at the top.
Click on any of the small Frequency
setting boxes on the right opens a ‘keyboard’ dialog box that makes it easy
to enter a new frequency. This also
applies if you click on any of the other
small boxes, for example, the “Samples” box, the “Wait (us)” box or the
“Marker1” or “Marker2” boxes.
siliconchip.com.au
The ‘rear’ of the module houses a micro Type-B USB socket for connecting to a
computer, plus two more status LEDs to indicate STM32 operation and power,
and a pushbutton labelled “KEY” which controls the tracking generator.
Screen 1 shows what was displayed
when I fitted a 50W termination to the
LTDZ input, set VMA SSA for the full
span of 35-4400MHz and clicked the
START button. This is the ‘noise floor’
of the LTDZ, which is almost constant
at -76.9dBm over the whole frequency
range.
Screen 2 shows what was displayed
when I connected the input of the
LTDZ to an external VHF/UHF discone
antenna, and set the VMA SSA software to scan from 200MHz to 208MHz
(the frequency range used by Sydney’s
DAB+ transponders). The full range of
transponder signals is shown, with an
average level of about -49dBm. Note
Australia's electronics magazine
those five sharp ‘notches’ though; more
about this shortly.
The next step was to power up
my Gratten GA1484B VHF-UHF signal generator and set it to produce
an unmodulated output of 2500MHz
(2.5GHz) at 0dBm. I then connected its
output to the LTDZ input via a 2m-long
SMA-SMA cable, and set the VMA
SSA software to scan from 2400MHz
to 2600MHz (a span of 200MHz).
This resulted in the display shown
in Screen 3, where you can see the
main signal spike at 2500.00MHz
accompanied by a pair of smaller
spikes (about -66dBm) about 25MHz
on either side. There are also a couple
January 2022 75
Screen 4: a ‘close-up’ of the output from Screen 3, this time with a range of
2495-2505MHz, which shows the singular peak from before was actually a pair.
Screen 5: the bandpass curve over 800-1300MHz of a FlightAware ADSB filter.
Note the flat response between 1000-1150MHz that falls away at both ends.
Screen 6: the plot of a Mini-Circuits -30dB attenuator over the full 35-4400MHz
range is fairly smooth until it starts dipping past 3.7GHz.
76
Silicon Chip
Australia's electronics magazine
of much smaller spikes of -73/-74dBm,
about 75MHz on either side.
I’m sure those extra spikes are not
coming from my signal generator,
because they don’t show up when
I check it with my Signal Hound
USB-SA44 spectrum analyser.
They are probably the result of the
LTDZ’s fixed and relatively wideband
RBW. The other thing to note about
this display is that the amplitude of
the main signal in the centre is about
-13dBm, quite a bit lower than the generator’s 0dBm output.
This is considerably lower than
you’d expect, even allowing for losses
in the 2m long SMA-SMA cable (about
2.5-3.0dB).
Notch artefact
The next step was to leave the signal generator set to 2500MHz with
0dBm output and connected to the
LTDZ input, but to change the VMA
SSA app’s frequency settings to
give a much smaller spectrum span
of 10MHz (ie, 5MHz either side of
2.5GHz). This gave the display shown
in Screen 4.
The spike at 2500MHz has now
expanded into a pair of ‘twin peaks’,
with a fairly deep notch between them.
The twin peaks reach an amplitude of
about -2.5dBm, much closer to the correct value. But the notch in the centre
reaches down to about -31dBm, which
is a bit disconcerting.
It turns out that this kind of notch is
basically due to the fixed and relatively
wide RBW of the LTDZ and similar
low-cost analysers. As Vitor Augusto
explains in his blog post dated 13th
October 2017 (siliconchip.com.au/
link/ab8a), the fixed and wide RBW
causes them to have a ‘blind spot’ in
the centre of their ‘scanning slot’ as
the Analyser moves the input signals
past it.
It’s this blind spot that causes a
notch in the centre of signals with a
narrow bandwidth. That’s why professional (and much higher-cost) spectrum analysers give you a choice of
RBW settings, as low as 10kHz
Mr Augusto has included a notch
function into his VMA SSA app,
which, when selected, can fill in this
kind of notch by replacing it with a
straight line between the twin peaks.
But this is just a cosmetic workaround,
as he admits; crunching the scanning
data to truly remove the notching
would be pretty complicated.
siliconchip.com.au
In another post dated 4th February
this year (siliconchip.com.au/link/
ab89), Mr Augusto announced that
a colleague of his named Domenico
had put much work into improving
the performance of LTDZ analysers.
This is both in terms of improving the
hardware (presumably concentrated
around the low-pass filter) and revising the firmware in the STM32F108
MCU.
In his February post, Mr Augusto
provided a link to a beta version of
Dominico’s revised firmware. However, he didn’t give any details of
Dominico’s changes to the LTDZ’s
hardware.
More details on the
current product
Getting back to my review of the
product as it stands today, I decided
to try using the LTDZ’s tracking generator to perform a couple of spectrum
scans of circuitry connected between
the tracking generator output and the
Spectrum Analyser input.
The first item I scanned was a FlightAware ADSB bandpass filter. This was
connected via a 150mm-long SMASMA cable. Then after pressing the
“Key” button (S1) on the rear of the
LTDZ’s case to turn on the tracking
generator, it was simply a matter of
setting VMA SSA to scan between
800MHz and 1300MHz, and clicking
on the START button.
The filter’s bandpass curve was
then displayed, as shown in Screen
5. The filter has a flat response from
1000MHz to 1150MHz, with an insertion loss of about 4dB, falling away
quite steeply at either end. Just the
shot for receiving ADSB signals centred on 1090MHz!
Finally, I ran a series of tests using
SMA-SMA fixed attenuators, again
connected between the TG output
and the analyser’s RF input using a
150mm-long SMA-SMA cable. For
these tests, the VMA SSA app was
set for a full scan from 35MHz to
4400MHz, to show how the attenuators behaved over the entire range.
I also checked the span with the
150mm long cable by itself, for reference.
Screen 6 shows the result for a
Mini-Circuits -30dB attenuator. As
you can see, it’s reasonably smooth
over the full range, apart from a small
bump in the centre and a couple of
dips at about 3700MHz and 4100MHz.
Overall, it just curves slowly upward
from -30dBm at 35MHz to -25dBm
at 2400MHz, then slowly downward
to -30dBm at about 3400MHz and
further down to about -40dBm at
4400MHz.
The result when checking the
150mm cable by itself was somewhat
flatter, varying from about -5dBm at
35MHz to -3dBm at 470MHz and then
curving down and up by less than
2dB right up to 4400MHz. But it also
had dips at 3700MHz and 4100MHz,
which might be due to reflections in
the cable.
My verdict
The Geekcreit LTDZ V5.0 spectrum
analyser is a low-cost unit that must
be used in conjunction with a PC, and
operates over a wide frequency range,
from 35MHz to 4400MHz. It also boasts
a tracking generator covering the same
frequency range, with an output level
of around 0dBm.
Used together with Mr Augusto’s
VMA SSA application, it’s capable
of performing a surprising number of
spectrum analysis jobs.
But it does have a few shortcomings, of which the most irritating is
probably those ‘notches’ which appear
in the centre of narrow-band signal
peaks. These are caused by the fixed
and wide bandwidth of the low-pass
filter between the IAM-81008 double-balanced mixer and the AD8307
log amplifier/detector.
The LTDZ does have another shortcoming: its relatively low sensitivity.
Its noise floor is about -76dBm, which
corresponds to 35μV. That means it
will be effectively ‘blind’ for signals
below 50μV or so.
Presumably, this low sensitivity is
because there is no amplifier between
the LTDZ’s RF input connector and
the input of the IAM-81008 mixer.
So it might be possible to improve
the sensitivity by connecting a lownoise wideband amplifier ahead of
its RF input.
There are a few of these currently
available, some even having the
amplifier circuitry inside a shield –
either on the PCB, or by fitting the
complete amplifier inside a small
metal case.
I have ordered a couple of these
amplifier modules to try them out with
the LTDZ, and if the results are satisfactory, I will cover them in a future
SC
article.
SMD Test
Build it yourself Tweezers
● Resistance measurement:
10W to 1MW
● Capacitance measurements:
1nF to 10μF
● Diode measurements:
polarity & forward voltage, up to about 3V
● Compact OLED display readout
● Runs from a single lithium coin cell, ~five years of standby life
● Can measure components in-circuit under some circumstances
Complete Kit for $35
Includes everything pictured, except the
lithium button cell and brass tips.
October 2021 issue
siliconchip.com.au/Article/15057
SC5934: $35 + postage
siliconchip.com.au/Shop/20/5934
Vintage Radio
The Mysterious Mickey OZ by Astor
By Ian Batty
This is an iconic,
well-performing radio
from the early 1930s;
it was built into a
Queensland Maple
case, and is a ‘must
have’ for any serious
collector of Australian
electronic technology.
However, it’s a
nightmare to work on.
T
his radio was previously described
by Rodney Champness in the
March 2004 issue (siliconchip.com.
au/Article/3438), but as it’s an important early Australian set, I decided to
revisit it in a more in-depth manner.
That earlier article went into very little detail on how the circuit operates,
and the radio was not actually restored
nor tested. Some aspects of the circuit
are unusual and interesting, as I shall
describe later.
The Astor Mickey began as a transformerless AC/DC set adapted from an
American 110V design. All valve heaters were in series, with the US design
modified for the Australian release as
serial numbers 1 to 460. The 110V set’s
heater dropping resistor was increased
to 580W to permit operation on our
nominal 230V mains and maintain the
heater string voltage of around 69V.
This resistor dissipated some 51W of
the total 80-odd watts.
This heating was managed by ventilation slots in the sides and bottom
of the compact timber cabinet, and
by inserting a sheet of asbestos inside
the upper right (viewed from behind).
The asbestos heat shield continued well in to the 7000 series. From
around 1935, some early models that
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Silicon Chip
had been returned to the factory were
re-released with a repaired chassis and
new cases. The sets are distinguished
by the curved ‘ogee’ depression in the
case’s front edge, but low serial numbers. Also, some sets had an asbestos
sheet fitted between the output valve
and the mains transformer.
Asbestos is a known carcinogen.
The complete serial numbers of these
sets are not known. At some point, the
asbestos sheet was replaced by a thin
sheet of timber. Readers are advised
to examine their sets to determine
whether the asbestos is in place. For
advice on how to handle asbestos, see
siliconchip.com.au/link/ab9k
Notable aspects
Donald Haines lodged his
US2148266 pentagrid patent in 1933
(the design used in the 2A7/6A7/6A8
and descendants), and Astor released
the AC/DC Mickey in that same year.
So it’s a standout example of a very
early superhet.
Other notable aspects of this set are
the use of back bias for the 6B7 and the
use of regeneration in the converter,
a most unusual circuit strategy used
Article sources
This article draws on Philip Leahy’s Circuits 1934-1940 Book 11, Astor/Breville Circuits and its Supplement, published by the Historical Radio Society of
Australia (HRSA). Philip, assisted by Jim Easson, has collected comprehensive circuits and technical notes for very many radios made and sold in Australia, and the Astor/Breville book has proven invaluable in writing this article.
Refer to Philip’s book for complete descriptions, circuit diagrams, circuit
voltages and sensitivity/performance figures.
Consider also getting Philip’s entire series – it contains many Australian
radios not listed in the famous Australian Official Radio Service Manuals that
were either not included, released before the AORSMs began publication in
1938, or manufactured after the AORSMs ceased publication in 1956.
See the HRSA website (www.hrsa1.com) for Leahy’s ten-volume series’ contents, but note that book ten is still in preparation at the time of writing this.
Australia's electronics magazine
siliconchip.com.au
It’s important to note that most
models of the Astor Mickey
OZ used asbestos in the
timber cabinet, so the utmost
care should be taken when
handling this – siliconchip.
com.au/link/ab9k
The cabinet itself is small
for its time at 305mm wide,
180mm high and 140mm deep.
only by a very few designers, and one
that had disappeared by the late 1930s.
Returning to the power supply, serials 461 onward used a mains transformer with full-wave rectification.
The change to AC-only operation
resulted in the OZ circuit of 1933
(Leahy, p11; see adjcaent panel). This
design underwent frequent change;
consult Leahy for the most complete
collection of circuits. He lists six variants.
The basic circuit was also used
for other Mickey sets (the Bakelite
EC and the stunning Mickey Grand
among them) and for other, later sets
from Astor.
The set I’m describing, serial number 7490 (OZ7490), appears in the
Leahy Supplement on p11. The principal difference from the more common issues is the use of back-bias for
the demodulator/AGC/audio valve, a
duo-diode pentode 6B7.
There were many changes to the OZ
circuit, the cabinet and even the dial
cloth and cabinet ventilation/geometry over the production run. Philip
Leahy and Jim Easson have compiled
the most complete list of these changes
(see the adjacent panel).
nightmare to work on is that it looks
as though one team bolted the power
transformer, IF cans and gang on to
the top of the chassis, the next team
turned it upside down and threw in a
handful of parts before the final team
just soldered everything to everything else.
Using the military criteria of Reliability, Maintainability and Availability, I give it scores of 8, 0, 10, getting
zero for maintainability only because
you can’t give a negative score.
All wiring is point-to-point without
tagstrips; my set had several instances
of connected components just having
their pigtails twisted together in midair and soldered.
You can pick repairs and modifications pretty easily. Resistors are mostly
the old ‘cartridge-cap’ body-end-band
coded or cylindrical ‘dogbone’ bodyend-dot coded types. All original
non-electrolytic capacitors were from
Aerovox or TCC.
The picture overleaf of an original
Mickey, supplied by Andrew Wakeman, shows four ‘dogbone’ resistors
(three green and one red), and one
cartridge-cap resistor (purple body).
There is also a large paper capacitor
(C27, sitting vertically) with a band of
black friction tape insulating some of
the back-bias circuit’s solder connections. The undisturbed friction tape is
factory-original.
Reality check
The reason I described this set as a
The overall layout of the chassis was
very compact, with metal sheeting
needed to help with airflow. This set
was serial number 7490.
siliconchip.com.au
Australia's electronics magazine
January 2022 79
A simple notch filter (rather than the
bandpass filter used) would have given
immunity to IF breakthrough without
compromising the performance.
Converter
The top view of the chassis gives a better look at the ‘messy’ arrangement near
the tuning gang which is for the antenna circuitry.
Circuit description
The circuit is shown in Fig.1. There
is a filter circuit (L1/C1) between the
antenna connection and the antenna
coil primary (L2).
Some references describe this as
necessary to suppress interference/IF
breakthough from marine/spark transmitters in the lower end of the HF
band, and to suppress image responses
in the 986~2111kHz range.
By 1932, 500kHz had been declared
as the International Distress Frequency, but would have presented
little interference due to infrequent traffic. ‘Everyday’ maritime
communications were relocated to
frequencies of 425, 454, 468, 480 and
512kHz, so the potential for IF breakthrough (especially from the 454kHz
allocation) would have been a reality.
The filter certainly does have significant attenuation towards the bottom
end as the sensitivity graph (Fig.4) and
the IF injection voltages on the circuit diagram show. It would also (as
the manufacturer’s description states)
improve image suppression as the set
is tuned past about 1000kHz. Unfortunately, it does this by cutting receiver
sensitivity, by a factor exceeding two
times at the top end.
The 6A7 converter uses grid 1 for the
oscillator grid and grid 2 as the oscillator anode in the conventional pentagrid circuit. It uses ‘padder’ feedback,
where the primary winding couples
via 1nF capacitor C14 to the secondary, in addition to the mutual inductance between primary and secondary.
That RF connection goes to ground via
padder C12, a fixed 300pF shunted by
a variable 30~60pF.
Padder feedback is used to improve
oscillator activity (and thus conversion
gain) in converters with known weak
oscillator performance. Although the
6A7 is specified for anode voltages as
low as 100V and should work reliably
with the conventional circuit, OZ7490
showed considerable variation in
oscillator output over the tuning band.
The use of padder feedback suggests
that the conventional transformercoupled “Armstrong oscillator” design
was found inadequate with the set’s
low HT.
The tuning dial, with reduction
drive, is uncalibrated. It is marked
(confusingly) as “100” at the low end
of the band to “0” at the high end –
see Fig.2.
Fig.1: a redrawn version of the Astor
Mickey OZ (serial 7490) circuit with
suggested test points. The original
circuit is available but the labels are
hard to make out.
80
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
An original Mickey showing four
‘dogbone’ resistors and one large
paper capacitor.
IF circuitry
The IF transformers have tuned primaries and secondaries. Despite their
somewhat ‘agricultural’ construction,
OZ7490 returned a -3dB bandwidth
of ±2kHz, and a -60dB bandwidth
of ±35kHz, an acceptable selectivity
even today.
The first IF’s primary tuning capacitor (C9) is a bit of a head-scratcher,
as its ‘cold’ end is returned not to the
HT side of the primary (as is nearuniversal), but to the converter cathode.
This gives a feedback path from
The vacant space in my set and the chassis hole to the right would have been
occupied by the internal/external speaker switch on earlier releases. No original
electrolytic capacitors remain in my set.
the converter’s anode to its cathode
via the first IF primary tuning capacitor, C9. As there is no signal inversion between cathode and anode (the
‘grounded grid’ principle), C9 forms a
capacitive voltage divider with cathode bypass capacitor (C8) to give positive feedback and a moderate boost
in gain. This explains the ‘low’ value
used for C8.
OZ7490 used 10nF, while Leahy
(Supplement, p11) shows 6nF. You
would expect it to be the same as the
IF amplifier’s C16 bypass value, 50nF.
This is a reminder of just how clever
some early designs were. In practice,
the feedback circuit in OZ7490 gives
a gain of some +4dB, about 1.5 times;
the lower value of 6nF would give
more boost.
For a full description of this part of
the circuit, including a warning about
oscillation, see Leahy, p108. That
reference describes the design’s use
in the similar model AC.
Loudspeaker driving
The OZ model uses an electrodynamic speaker on a plug-in frame that
mates to a chassis-mounted four-pin
socket, held in by two side catches.
This allows the entire speaker assembly to be removed easily.
The initial release used a 1.9kW field
coil, which was reduced to 1.35kW,
then 1.2kW. The Type 43 output valve
is specified for a 4kW load, implying
that that the speaker transformer has
a 4kW primary.
As the field coil is used as the filter
choke in a back-bias circuit in most
versions, back-bias voltages change
with field coil resistance. The power
transformer’s HT secondary voltage
must be suited to the field coil resistance, thus restorers need to know
Fig.2: this is how the dial markings correspond to the actual tuned frequencies.
Not only is the tuning dial unusual because it is marked 0-100 without any
frequencies, but also because setting it to 0 tunes it to the highest frequency, and
100 the lowest.
siliconchip.com.au
Australia's electronics magazine
January 2022 81
which field coil they have if they
intend to replace the power transformer. Be aware that there were at
least three different mains transformers over the life of the model.
OZ7490’s speaker was marked as
1.35kW but it measured as 1.195kW.
If the speaker is replaced with one
having a different field coil resistance,
that will alter the back-bias supply,
so unless you also change the power
transformer secondary voltage, the
resistive divider may need modification to preserve the output valve’s bias
supply of around -19.5V (measured as
-18.5V at the grid using a 10MW input
impedance voltmeter).
Some sets also use back-bias for
the 6B7 demodulator/AGC/first audio
stage. Matching the divider to the field
coil’s voltage drop is vital for correct
operation.
You might see sets with a 550W
resistor in series with the field. This
allowed the lower-resistance 1.35kW
(later 1.2kW) speaker to be substituted
for the original while demanding no
modification to the back-bias circuit.
The “Minnie” (ad shown in Fig.3)
also used an electrodynamic speaker
with transformer attached. Contained
in a case approaching the size of a
console radio, it gave much-improved
bass response. Connecting via a fourpin socket on the back of the chassis, output was switched from the
internal speaker to the Minnie via a
side-mounted switch.
The switch was no longer fitted by
OZ9490, with the hole in the cabinet
side remaining, and the socket hole
in the chassis rear blanked by a Bakelite sheet.
Power supply
The AC/DC set used the 25Z5’s two
diodes in parallel to form a half-wave
rectifier. This would have given an HT
of only about 140V, common in early
US mains-powered sets.
From 461 onwards, a conventional
mains transformer with a centretapped secondary and the 25Z5 were
used in a full-wave circuit. While it
would have been possible to wind
the mains transformer to give a more
common (higher) HT voltage, Astor’s
designers chose to keep the original RF/IF/Audio design, keeping the
low HT.
The basic Mickey design was used
for other models for several years,
so low HT voltages were a feature of
Astor designs for some years following the OZ.
The 25Z5, with two independent,
indirectly-heated diodes, was also
used as a voltage doubler in 110V AC
sets, for an HT closer to the more common 200~250V.
Readers may hesitate over the
speaker field being in the negative
Fig.3: an ad for the Astor Minnie Mouse “console-size” extension speaker.
Despite a similar style to the OZ cabinet, it gave better bass response.
82
Silicon Chip
Australia's electronics magazine
supply lead. This arrangement works
just as well as the more common
positive-lead connection, with the
same total voltage loss, and with two
advantages. Firstly, the voltage drop
across the field can be used to provide ‘free’ back bias; the voltage drop
is there anyway, so why not use it
rather than adding an extra resistor
with more HT loss?
Secondly, since the entire field is
no longer at HT potential, failures
due to electrolytic corrosion are much
less likely.
The two HT filter capacitors were
originally contained in a single tinplate case, but these were absent
from OZ7490. The capacitors were
described as ‘dry’ electrolytics, distinguishing them from the liquid-filled
vertical cylindrical types common at
the time. The original filter caps were
replaced by a Ducon ‘pigtail’ tubular
type (more on that later).
The paper types in the set were
Chanex, Ducon and Aerovox brand
while the mica types were TCC.
Valve biasing
Valve biasing varies from one
model to another. The AC/DC set used
back-biasing on the output valve but
individual cathode biasing on the
other three.
Converter biasing, initially using
fixed-cathode bias, was changed to
preset variable from around serial
number 7100 on, as found in OZ7490.
The converter’s local oscillator
anode is supplied from the main HT
via a 10kW resistor in all circuits, but
the converter screen supply comes
from the R13-14-15 voltage divider
strung between HT and ground.
The original cathode bias on the
6B7 circuit deserves comment. From
the initial issue to about serial 7100, it
was supplied by a 7kW cathode resistor and bypassed using a 5μF capacitor, raising the cathode above ground
and providing negative bias for the
pentode section.
But this also put a negative bias
on the demodulator/AGC diode pair,
so that the demodulator would not
respond to weaker signals at all. To
prevent this, the volume control, acting as the diode load, is returned to
the 6B7 cathode.
The demodulator works as usual,
and the AGC operates with no delay
bias. The only odd effect is to put the
entire AGC line a volt or two above
siliconchip.com.au
ground. This means that the converter
and IF amplifier grids are also above
ground. This unusual biasing is compensated by the cathode voltages being
a little higher than usual.
The 6B7 uses very low screen and
anode voltages (19V and 36V respectively), derived from the R13-R14-R15
HT divider.
However, this ‘starved’ design gives
a stage gain close to 50 times, adequate
for the application. Against this, the
Type 75 triode used in the later model
EC can achieve a similar gain with a
simpler circuit.
From about serial 7100 onward
(including OZ7490), the 6B7 cathode
is connected to ground, with backbias for the pentode section. This corrected the problem of a positive AGC
line, so the AGC circuit works just as
you’d expect it: 0V for no signal and
increasingly negative as the signal
strength increases.
No manufacturer drawing exists, but
Leahy’s Supplement has the correct
circuit. The later EC model also uses
back-bias on its Type 75 duo-diode triode’s audio section.
OZ7490’s output valve has around
-19.5V applied from the back-bias
divider, with its control grid returned
to ground. Serial numbers from about
1300 to 5300 see the control grid
returned to ground with an 810W cathode bias resistor and 5μF electrolytic
bypass capacitor.
A final note on terminology: original
texts refer to semi-variable capacitors
as ‘padders’, regardless of their function. Thus the semi-variable capacitor C9 (tuning the first IF primary) is
described as a ‘padder’, as is C12, the
LO tracking circuit. Modern terminology describes C7 (and C9, 11, 13, C16
and 18) as trimmers, reserving ‘padder’ for capacitors such as C12 alone.
Repairs
I bought this set at an HRSA auction
some years ago and it was on display
until just recently. On inspection, it
showed some activity, mostly hum.
Some capacitors had been replaced,
along with the 6B7 load resistor (R11).
Bias divider R16-R17-R18 had been
modified to add a resistor in parallel
with R18, and an extra bypass capacitor had been added across R18.
The mains lead was figure-8 flex
and was not secured against twisting
or pulling. I replaced it with a clothcovered three-core lead that is held to
siliconchip.com.au
the chassis with a cord anchor. While
the anchor is a modern device, it gives
complete security and will not split or
perish as rubber grommets can.
The bias voltage on V4 (the output
valve) was low, as was the HT voltage. The first HT filter capacitor (C23)
was missing.
Valve testing showed converter V1
to be weak, so I replaced it. All the
others tested OK. This was a relief, as
the Type 43 and 25Z5/25Z6 (with 25V
heaters) are not so readily available as
the 6V heater types.
I attacked the bias divider first. The
added electrolytic capacitor (across
R18) had enough leakage to leave the
6B7 with virtually no bias. As the
capacitor was disrupting the circuit
and was not needed, I removed it. The
leakage would have been acceptable in
a cathode bias circuit but was a disaster
in a high-resistance bias circuit passing only microamps.
C27 was also leaky, so I replaced
it with a fawn-coloured Philips type.
I reworked the set with new resistor
values to give the correct voltage for
the output valve, setting the bias for
the 6B7 audio driver on a trial-anderror basis for maximum gain, winding
up with 13kW for resistor R18.
But the HT was still low. I had
assumed that since V4 draws the most
HT current, its low bias would have
caused excessive current drain, pulling down the HT.
OZ7490 has an octal 25Z6 rectifier
fitted as a replacement of the original
6-pin 25Z5. Sets later than OZ7490
still have the 6-pin 25Z5 in place,
and all circuits show this valve
rather than the 25Z6. This is a
reminder of just how hard it can
be to find a Mickey in original
condition.
Circuit modifications – and the
absence of the correct schematic for this set – meant
that the missing first HT filter had been
overlooked. Putting in a replacement
brought the HT up to around 130V, so
the faulty bias circuit probably had less
effect than I first thought.
The audio stage now worked but
there was a background hum at 50Hz.
This was not a filtering problem;
the unshielded lead from the 6B7’s
demodulator circuit up to the volume
control ran past the mains-supplied
heater wiring.
The fix was to strip off the braid
from an old piece of shielded wire,
sleeve it over the existing audio lead
and solder it to ground, then slide a
piece of old-fashioned waxed cambric
‘spaghetti’ over the braid. This addition blends with other insulation in the
set. Tip: warming up cambric with a
heat gun or hair dryer makes it much
more flexible.
Next, I checked the function of the
RF/IF end. The IF channel lined up
pretty well, and feeding in about 20μV
to the converter grid gave good output.
The IF seemed ‘happy’ at 466kHz, so I
didn’t attempt to force it down to the
specified 456kHz.
This might upset the purists, but it’s
only about 2% off and the set works
just fine. I was concerned about possibly causing hard-to-fix damage if I
tried to adjust it any further.
That said, it was very deaf from the
antenna terminal. As described earlier, the L1-C1 combination is aimed
The side view of the Astor
Mickey OZ clearly shows
the filter circuitry for the
antenna.
Australia's electronics magazine
January 2022 83
at attenuating signals below the broadcast band to prevent breakthrough.
Disconnecting L1-C1 and injecting a
signal to C3 gave a better result, but
still not what I expected.
Resistance checks confirmed that
inductor L1 was continuous and that
capacitor C1 was not shorted. Then I
noticed twisted wires in the antenna
circuit assembly, taped with black
friction tape.
I realised that this is C4, a ‘gimmick’ capacitor to improve top-end
sensitivity. Undoing the tape, I discovered that the wire ends had been
twisted together. This was clearly a
factory error.
After rectifying this, the sensitivity
was better (see Fig.4) but still low. This
turned out to be caused by the L1-C1
filter. Bypassing that, I got 50mW output for just 7μV input at 600kHz (this
is without the L1/C1 filter – red line
in Fig.4). That’s up there with the better sets. So if you have a Mickey with
that L1-C1 filter circuit and want the
best performance, disconnect it and
connect your antenna to C3!
Performance
This set gives surprisingly good performance; the figures quoted below
are with the L1-C1 bandpass filter in
circuit and using a standard dummy
antenna between the signal generator
and radio. See the sensitivity chart
(Fig.4) for the intrinsic performance
without the filter.
For 50mW output the sensitivity is
7μV at 600kHz and 28μV at 1400kHz.
It’s noisy, though, with a signal plus
noise to noise ratio of about 14dB in
both cases. To get 20dB, the tested
set needed around 145μV and 60μV
respectively. The RF bandwidth is
±2kHz at –3dB and ±35kHz at –60dB.
The AGC circuit gives an output
change of 6dB for a 40dB input range.
It would not overload even with 1V at
the input!
The maximum audio output is 0.5W
at 10% THD. At 50mW, THD is 1.5%,
and at 10mW it’s 2%.
The response from antenna to
speaker is 155Hz to 1.9kHz; from the
volume control it’s 150Hz to over
3.2kHz.
Marcus and Levy (p47) quote the
input level for an equivalent all-octal
set of 5~12μV.
So this set’s best figure of 7μV without that bandpass filter is remarkably
good. Leahy (p119) quotes figures for
the very similar BC set that confirms
my test results, and agree with Marcus
and Levy’s figures.
Conclusion & thanks
Restored to original cosmetic condition, this is a set that will have visitors dwelling on it and admiring its
design and finish.
Restored to proper working condition, it’s a solid performer that ranks
among the better sets of any era.
And it’s a midget. We’re probably
used to compact mantel sets from the
1950s and 1960s, but this was serious
miniaturisation for 1933. Read radio
magazines and journals of the day and
you won’t see too many sets that rival
the Mickey for compactness.
These come up for sale from time to
time, and I think the Mickey OZ is a
‘must have’ for any Australian collector.
I’d like to thank Jim Easson and
Philip Leahy of the HRSA for background information on the entire
Mickey product line. You’ll find
HRSA founder Ray Kelly’s history
of the Mickey, including the controversy with Disney Studios over naming rights, in Philip’s book.
Thanks also to Alby Thomas and
Andrew Wakeman of the HRSA for
their generous provision of the original filter capacitor block and underside photos, and to the HRSA’s Mickey
Special Interest Group (MSIG) for their
advice.
Not an HRSA member? Visit www.
hrsa1.com and find out how we can
help you explore the wonderful (and
weird) world of radio. And don’t forget our Mickey Special Interest Group.
References
Fig.4: sensitivity measurements were made across the broadcast three different
ways: feeding the test signal directly into the antenna terminal (blue line),
directly into L2, bypassing the input filter (red line, giving the best sensitivity
figures) and with the factory error that caused C4 to be shorted out (green line).
As you can see, this simple mistake had a significant impact on sensitivity.
84
Silicon Chip
Australia's electronics magazine
• Leahy, P. N., Circuits 1934-1940,
Book 11, 2019, Historical Radio Society of Australia (www.hrsa1.com)
• Leahy, P. N., Astor ‘Mickey’ OZ
Supplementary Information to HRSA
Circuit Book 11, (siliconchip.com.au/
link/abav)
• Johnson, R., The Astor “Mickey
Mouse” and its descendants, Electronics Australia, July 1996.
• Marcus, W., & Levy, A, Elements
of Radio Servicing (PDF: siliconchip.
com.au/link/ab9l)
SC
siliconchip.com.au
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219
$
T 1539
SAVE 20%
Ideal
for DIY DC
power
wiring
The Ultimate
Battery Fuel Gauge.
Accurately measures battery voltage, current,
power, real capacity and remaining run time of your
connected battery (suitable for any type of chemistry
and voltages between 8V to 120V). Includes
50A shunt with 2m cable. 1% accuracy. Cut out
dimensions: 53.5 x 37.5mm.
40
Weather
resistant!
$
N 2099A
Easy DIY
install! Great
for 4WDs
Ratchet Lug Crimper
Quick and easy crimping for Anderson SB50
connectors and other uninsulated lugs
between 20AWG & 8AWG.
30
$
Monitor your car
battery from your phone!
X 0225A
The ultimate camping,
fishing, anything light!
Ensure your battery doesn’t go flat
with this handy Bluetooth® battery
monitor. Provides live feedback on
your vehicle or auxiliary battery, plus
handy long term stats.
Provides 5 hours use from a high spec lithium
battery - or use it as a USB battery bank
to charge your phone. Folds flat for easy
storage. 10W, 1000 lumens.
L 2003
Includes 10m
cable & mounting
hardware
89
Premium Deep Cycle SLA Batteries
$
Caravan/Boat Television Antenna
Get crystal clear TV reception wherever you
travel! Omnidirectional 360° design requires no
adjustment when you park up. Easy DIY install.
Anderson
Style Panel
Socket
Easy connection for
solar panels and
auxiliary batteries.
Mounting hole:
40x21mm.
SAVE 38%
M 8521A
SAVE 16%
30
$
6/12V Plug In Battery
Charger & Maintainer
P 7810
14.95
$
Offers hassle free maintenance charging for 6
& 12V lead acid batteries. Ideal for protecting
seldom used vehicles from battery discharge.
Croc clip or ring terminals. 600mA output.
Ideal for every day discharge in equipment such as golf buggies,
wheelchairs, forklifts etc. Easily user replaceable.
Model
Capacity
RRP
NOW
SG4554
26Ah
$129
SG4560
33Ah
$159
SG4563
40Ah
$199
SG4567
60Ah
$259
SG4571
80Ah
$342
SG4573
90Ah
$359
SG4577
110Ah
$435
$99
$129
$159
$209
$275
$319
$345
Order online at altronics.com.au | Sale pricing ends January 31st
Commercial grade cells
for high performance
Top workbench savings!
SAVE $370
SAVE $44
K 8604
145
$
Super hot 1350°C
flame with high output
nozzle. Handheld or self
standing design for tasks
such as heatshrinking,
the gas!
Don’t forget r can.
model making, silver
pe
.35
$9
T 2451
soldering! Easy to refill.
SAVE 22%
999
$
High Output
Blow Torch
M 8305 5A
SAVE $40
Everything a
maker space
needs in one
compact unit!
119
$
M 8303 3A
T 2496
Compact 30V Lab Power Supply
62
$
Great for servicing, repair and design of electronics.
Low noise switchmode design. Fine & coarse voltage
and current controls. 3A or 5A max models. Size:
85Wx160Hx205Dmm.
SAVE $22
88
$
Charges
a laptop, a
phone & tablet
at the same
time!
SAVE $34
85
$
or 2 for $120
D 2323
T 2098
Bench Mount USB PD Charger
A 96W USB type C power delivery charger, plus dual
QC 3.0 USB charging in the one compact near flush
mount unit. Requires 60mmØ hole.
Includes power supply.
300W Adjustable Solder Pot
Tin multiple stranded hookup wires or remove multi-pin
connectors from boards quickly and easily. Takes up
to 1350g of solder. Stable temperature control: 200480°C. Suitable for lead free and leaded work. 1kg
leaded solder bar $64.95 (T 1140A). 300W.
Creality® CP-01
3D Printer / CNC Router / Laser Engraver
The ultimate do-it-all maker machine for the workbench. Create amazing
prototypes and one off designs with this all in one mini home factory.
Includes three interchangeable machine heads for cutting, etching and printing
each with excellent accuracy. Easily assembled from flat-pack in just a few
minutes. Router & engraver suitable for plastics, wood, PCBs, laminates etc.
SAVE 27%
29
$
T 2186A
T 4015A
SAVE 15%
29
$
101 Pc Ratchet Driver Kit
Never lose a tiny screw again!
Features 95 security, philips, pozi and slotted bits
made from tough S2 alloy. Includes ratchet handle
with comfy rubber grip. See web for full contents list.
A 35x26cm heat resistant silicon work mat, plus a
25x20cm magnetic mat to keep screws and materials
organised while you work.
INCLUDES:
• Conical tip • Hot air blower
• Hot knife/plastic finishing tip
• USB cable • 1m solder
• Tip sponge.
SAVE $40
T 2694A
30W Lithium ‘Go Anywhere’ Soldering Iron
45 minute run time. 600°C max. Ideal for occasional soldering jobs or light duty
repairs and field servicing. Recharge by USB power adaptor in your car or at home
- or USB battery bank. Includes replaceable 18650 battery.
Cut, Polish, Grind,
Sand & Carve.
TOP
VALUE!
T 2802
T 2748A
22
$
.95
27
$
.95
X 0433
16.95
$
5” Premium Cutters
Chewed out a screw?
Get a crisp close up view!
Tough chrome vanadium blades
stay sharp for longer. Ideal for
PCB assembly, cutting solid core
wiring etc.
No problem! This unique set of
pliers features serrated jaws, plus
serrated opening on the front for
extracting screws up to 13mmØ.
A handy accessory for any workbench, this 130mm 6x magnifier
uses premium quality glass and
LED lighting for a clear view.
165
$
Great for finishing and
smoothing your 3D prints and plenty of other odd jobs
and hobbies! Powerful 130W
motor with variable speed
between 8000 and 33000
RPM. Included is a 172pc
SAVE 18%
accessory kit of grinding
wheels, drills, cutters,
sanding discs & polishing
pads. T 2120
69
$
Order online at altronics.com.au | Sale pricing ends January 31st
Expand your AV system.
Opus One® 140W
Soundbar Wireless Subwoofer
SAVE $40
Demo in
store!
199
$
Our new premium finish soundbar offers rich, clear sound from
it’s 6 high performance speaker drivers, plus a 8” subwoofer
which can be placed anywhere in your lounge room thanks to
wireless connectivity. Offers bluetooth audio streaming from
your favourite devices, plus S/PDIF digital audio input for
connection to your TV (cable included).
C 5064
$90
299 SAVE
$
Opus One® Bluetooth Bookshelf System
Soundbar: 97 x 8 x 7.5cm,
Subwoofer: 30 x 25 x 30cm
C 5059
Similar spec to $600 systems with sound quality that’s just as good!
Want top notch sound for your games, hi-fi listening or home theatre?
These new active bookshelf speakers need no amplifier, just plug them
in and connect via Bluetooth, digital S/PDIF or stereo RCA. Amazing
sound for their price with a sleek oak grain finish - looks great with grilles
on or off! Size: 146 x 164 x 240mm.
SAVE $50
SAVE $40
189
119
A 4201
A 1116
SAVE $30
LED base
light shows
when your
mic is on
$
$
109
$
D 0981
SAVE $19
50
$
Add Bluetooth® audio to your
favourite speakers!
Why buy new bluetooth speakers when you can
add this module to existing speakers? Streams
music direct from your phone! 2 x 25W RMS
output. Bluetooth 4.1. Includes power supply.
SAVE 33%
59
Bluetooth® 2x50W Amplifier
Stream audio directly from your device to your speakers
in the study or entertaining area. 3.5mm and RCA inputs.
Class D design. Internal headphone amplifier. Includes
power supply, banana speaker plugs & 3.5mm to RCA
cable.
4 Channel USB Mixer
With Equaliser & FX
USB Gooseneck Mic
A 2548
Want to get into recording podcasts, voice
overs or making your own audio samples?
This mini USB mixer connects directly to
your PC or Mac and is powered directly from
USB. Includes 3 band EQ and effects.
Great for gaming, YouTube and
livestreaming. Quality omnidirectional
mic insert. Mic gain and mute control
knob with LED lighting.
Indoor Pan
& Tilt Wi-Fi
Camera
A 0920
$
AE1101
Adds up to 200m range to
your IR remote controls!
Wireless Infra-Red Repeater
Use your remote control up to 200m away (line of sight) from
your equipment. Perfect for controlling your AV system from
the patio or entertaining area. Includes plugpacks, IR emitter &
receiver.
SAVE $20
SAVE 24%
Bluetooth®
3.5mm Jack
15
$
Instantly add wireless audio to any
3.5mm input - like your car, headphones or home amp. USB rechargeable battery provides 4 hrs listening.
S 9846
1080p Wi-Fi Cube Camera
• Internal battery - set it up anywhere!
• Day/night with IR • USB rechargeable • Includes stand • Simple
motion activated recording.
Western Australia
Build It Yourself Electronics Centres
Sale Ends January 31st 2022
Phone: 1300 797 007 Fax: 1300 789 777
Mail Orders: mailorder<at>altronics.com.au
69
$
» Perth: 174 Roe St
» Joondalup: 2/182 Winton Rd
» Balcatta: 7/58 Erindale Rd
» Cannington: 5/1326 Albany Hwy
» Midland: 1/212 Gt Eastern Hwy
» Myaree: 5A/116 N Lake Rd
Makes a great baby or
pet monitor, this camera
features intelligent tracking of moving objects
within the frame. 2-way
audio with mic and
speaker. 5m IR night
time coverage. Requires
5V 1A USB power
supply.
SAVE $10
S 9017A
69
$
Victoria
08 9428 2188
08 9428 2166
08 9428 2167
08 9428 2168
08 9428 2169
08 9428 2170
» Springvale: 891 Princes Hwy
» Airport West: 5 Dromana Ave
03 9549 2188
03 9549 2121
New South Wales
» Auburn: 15 Short St
02 8748 5388
Queensland
» Virginia: 1870 Sandgate Rd
07 3441 2810
South Australia
» Prospect: 316 Main Nth Rd
08 8164 3466
Please Note: Resellers have to pay the cost of freight & insurance. Therefore the range of stocked products & prices charged by individual resellers may vary from our catalogue.
© Altronics 2021. E&OE. Prices stated herein are only valid until date shown or until stocks run out. Prices include GST and exclude freight and insurance. See latest catalogue for freight rates.
*All smartphone devices pictured in this catalogue are for illustration purposes only. Not included with product.
B 0091
Find a local reseller at: altronics.com.au/storelocations/dealers/
SERVICEMAN’S LOG
Designing for unrepairability
Dave Thompson
A lot of equipment these days is designed to be compact and easy to
assemble, but little attention is given to repairability. That’s why so many
devices are essentially disposable. There’s no information like circuit
diagrams or repair manuals available, so once something goes wrong, in
the bin it goes. It’s sad.
I
’ve mentioned before that I get a lot
of random devices into the workshop for repair. Once people hear I
can do this sort of thing, they all seem
to pour out of the woodwork with
all manner of strange and wonderful
things for me to fix.
One of the problems I have with
this is that many of these devices are
no longer supported, built to fail and
designed not to be repaired, or simply not worth the considerable time
it would take to fix them.
The other day, a guy brought in
a hand-held Garmin Rino 650 GPS
siliconchip.com.au
transceiver. This is a very handy unit
because not only is it a fully-featured
satnav system, it is also a two-way
radio, so hunters who have other
compatible transceivers can talk to
each other over quite long distances
in the bush.
These devices have a touchscreen
menu system and a PTT (push-to-talk)
button on the side of the rubberised
case, so they work much like the typical ‘walkie-talkie’ type devices we all
know and love.
The problem with this one was that
there was no sound output, so while
it can still be used as a standard navigation system, there were no audio
Australia's electronics magazine
prompts and obviously no radio transceiver function.
These devices are designed to be
rugged. They use heavy rubberised
plastics and lots of rubber bungs and
stoppers to provide basic weatherproofing. Pulling them apart isn’t too
onerous, with the usual long Torx-type
screws (which require the exact driver
bit or they aren’t going anywhere) and
the increasingly typical hidden screws
buried beneath barely-removable case
flashings.
If one isn’t thorough, trying to pry
apart a case that still has screws holding it together can end up a real mess,
especially if one isn’t having a good
January 2022 89
day and the red mist comes down in frustration!
With all the screws removed, the two halves of the case
separate relatively easily, but then the space is so tight that
you have to hold your tongue one way while the planets
align before the board assembly can be eased out. There
is literally only one way it can come out, and finding just
where that sweet spot is can be maddening.
Once I got the board out, it was pretty obvious I was not
going to be able to do much with that part of it unless the
problem was caused by something simple like a blown or
faulty speaker. The speaker was one of those super-thin
permanent-magnet types, about 25mm in diameter and
plastic-welded into the front of the case.
There was no physical wiring connecting the speaker;
the board simply pressed against it, and a couple of tiny
gold spring contacts on the PCB rested against the speaker’s terminals.
I guess with everything crammed in so tightly, this system does work well, but I’d imagine any moisture that
gets inside might interrupt this type of connection, so I
resolved to take that into account as well.
I decided to check the speaker first. My trusty multimeter could handle this with a quick touch to the speaker
terminals with the meter set to x1 on the ohms scale. A
click from the speaker told me it was working, which, to
be honest, made my heart sink a little because I was hoping it would be one of those silly fixes that resolves everything with a minimum of fuss and expense.
But no. There was obviously something further up the
audio chain that was stopping this from making noise. As
is usual in these situations, I hit Google to see if I could
locate any circuit diagrams or schematics that may help.
I found nothing but a wealth of misinformation. However, one theme kept cropping up: that on this model, it
is easy to mute the output by accident whilst perusing the
menu system, so many people had resolved the no-sound
issue by simply un-muting the audio.
I reassembled the GPS to the point that I could fire it
up and go through the menu options on the touchscreen.
The sound was not muted, which was disappointing, but
there was also an option to set the handset to vibrate. I
had seen the tiny vibrator motor mounted on the circuit
board, so I knew it had that feature available.
90
Silicon Chip
I set that to on, so at least there was some haptic feedback when something happened, though that wasn’t going
to help get the two-way radio working...
Breaking it down the second time wasn’t as finicky a
job as the first time, so that was something. But trying
to track anything back from the speaker side was a nonstarter. The multi-layer PCB was stacked with the smallest
SMD components I’ve seen for a while, and though some
did have numbers printed on them, I could find nothing
about what they were.
Even if I could find a replacement, removing them
would require specialised tools that I don’t have, and if I
tried to do it, I’d likely have just damaged the board further. So, this was one that I couldn’t help with.
Garmin no longer runs a swap-out refurbishment program for this model, so they were no help. While I did
check the usual auction sites for spares and replacement
units, I could only find models being sold for spare parts,
and they could very well have the same problem as this
one – the vendors couldn’t tell me what had gone wrong
with them.
At almost half the price of a new unit, buying dead
handsets in the hope that something might work was just
not feasible (or sensible). The owner was philosophical
about it; at least we’d had a look and determined it wasn’t
worth pursuing. He’d still use it as a GPS but would have
to do without the radio/audio side of it.
Next!
Another client brought in an old ’70s clock radio. It had
been in the family for years, and though it worked, one
of the red seven-segment LED displays had faded enough
that it was difficult to read the time.
This is a classic example of whether to repair or not,
and why each case should be taken on its own merits. The
clock radio had been bought for the current client back
in the day by his dad, and so it had a lot of sentimental
value. He had used it in his workshop for many years and
wanted to see it going properly.
I advised him that I could likely fix it, but he might
be looking at way more than a replacement clock radio
from some big-box store might cost. He was OK with that
because the sentimental value was greater than that for
him. I told him I’d see what I could do.
Working on these older devices is so much nicer than a
lot of today’s stuff: plain screws, simple engineering holding it all together and basic analog components with designations printed on them. Almost anything inside it could
be repaired, or even fabricated to fit if that’s what it takes.
This clock just had a single dim display from the four
onboard, and I guessed that it had simply faded with age,
as many LEDs of all types of this era do. The big question
was what type of display it is and the pin configuration,
because I literally have a parts drawer full of reclaimed
and NOS (new old stock) red seven-segment LED displays, and I felt confident one would fit in this old-timer.
I’ve said before; I’m not exactly a hoarder – at least not
to the extent I have to sleep standing up in the laundry
because all the rooms are stacked floor to ceiling – but my
workshop is quite ‘busy’, with parts drawers and shelves
groaning under the weight of stuff I’ve accumulated over the
last 40 years or so. That’s not including all the other things
I inherited from dad’s very similarly-appointed workshop.
Australia's electronics magazine
siliconchip.com.au
The new display was a little brighter, but not too bad. I
guess I could have installed a resistor in the ground line
in an effort to dull it, but I thought that once the plastic
front was in place, it would look OK.
I was right; once reassembled, the red plastic cover the
LEDs shone through, which was a bit faded and scratched
itself, tempered any bright spots on the new display, and
it looked just as good as the others.
The customer was pleased, and I’m trimming down my
component stocks the right way, one at a time.
On the slow boat from China
The rationale is that if I come across a new-old-stock
seven-segment display, I’m not about to throw it out just
because I’m running out of room, so it gets squeezed into
the drawer with the others.
While there isn’t a huge call for components like this
anymore, I could almost guarantee that if I did have a
colossal clean-out and biffed a lot of this stuff away, the
very next day, a job would come in that requires something I have just binned.
This clock-radio job has proven that it would have been
folly for me to throw these displays away because, as luck
would have it, I had several that could do the job. My main
concern was that if I fitted it successfully, this ‘new’ one
would be much brighter than the remaining original displays. As I didn’t have four the same, I couldn’t replace
them all. Still, I’d cross that bridge when I got there.
It was a bit tricky to manipulate the various PCBs into a
position that I could de-solder the dud display. The separate
boards were all linked together using that multi-stranded,
hard plastic insulated joining cable. It’s great stuff for a
strong interconnecting joint, but over time it gets brittle and
breaks easily. If I did break a link, I could always replace it,
but it’s better not to bend these old parts around too much.
The smell of the old solder brought back memories of
watching dad in his workshop when I was a little kid; it’s
strange how some odours stay with you. It’s likely seriously unhealthy, with all the fumes that come off when
heated, but it smells of home to me.
Getting the old dim display out was easy; I just wiggled it free after removing all the solder. The PCBs are
pretty hardy from those days, but like all electronics,
excess heat can do a lot of damage. So I just took care
not to overcook it.
I lined the new one up with the others and soldered
it in – it was really that simple. I flexed the boards back
into their original positions and sat it all carefully on the
bench before plugging it in and lighting it up.
siliconchip.com.au
You might recall a story a while back about an electric bike that I couldn’t finish repairing as I was waiting
on parts from China (June 2021 issue; siliconchip.com.
au/Article/14895). More specifically, I was waiting for a
new speed controller, because the old one had gone up
in a puff of smoke.
The problem was that I didn’t know if it was just the
controller that had failed, or whether the motor assembly built into the back wheel had shorted and burned
things out, or both. The controller was far cheaper to
replace than the wheel/motor assembly, so that’s the
bit I bought first.
I’d sourced one easily enough, as they appear to be
at least partially standard devices, but it took forever to
get here. When it did arrive, I installed it – thankfully,
most of the connections are also relatively standardised
– though I’d taken lots of photos before I pulled the old
one out as a precaution.
I charged the battery, which had been sitting for a while
and was discharged, and when all was ready, turned the
key and wound in a bit of throttle. In a flash, the new
controller was toast.
As I’d already previously checked the external wiring to the motor for obvious shorts between themselves
and to ground, I thought nothing was apparently wrong
with it. Still, without a compatible controller, I couldn’t
check it properly.
Therefore, the controller was intended to be a sacrificial lamb and did its job by telling us that there was no
point in carrying on and sinking even more money into
it. It was a shame, really, as it was a cute little thing and
not cheap to buy in the first place.
Last call
And finally, I had a guy bring in a PCB from a heat
pump compressor. These are pretty large, and he said no
one in town is repairing them anymore after a well-known
repairer shut up shop due to the pandemic.
Items Covered This Month
•
•
•
•
The art of unrepair
Macbook Air repairs
Repairing a double-clicking computer mouse
Replacing damaged varistors in two Panasonic
microwaves
Dave Thompson runs PC Anytime in Christchurch, NZ.
Website: www.pcanytime.co.nz
Email: dave<at>pcanytime.co.nz
Australia's electronics magazine
January 2022 91
I know next to nothing about these
things, but how hard can it be? Circuit diagrams for common models are
widely available for service guys, and
the bloke (an installer/engineer) said
he could get a circuit if I needed one.
The fault was that the compressor
motor no longer ran, and he suspected
the motor driver section of the PCB had
failed. To start with, I asked him if he’d
tested the motor itself. He hadn’t but
claimed not many fail, so it was most
likely the board.
He left it with me, and I got out the
magnifying glass to see if I could find
something obvious. I could see no
burned areas and there was no acrid
‘dead component’ smell, so I doubted
this was the problem.
There were two onboard fuses,
though, so I checked them. One was
blown. I replaced it with one of the
same specifications and called the
installer chap to say there was nothing obvious here.
He went back to the house and
pulled the motor, bringing it straight
around. It was shorted every which
way I could measure it according to
my meter, so that was likely the problem. Whether it had smoked the PCB
itself was anyone’s guess.
But again, it is way cheaper to
replace a motor than a PCB in these
units, so he took both away and
installed a new motor, wired in the
old PCB and voila! The thing fired up
and is still running well today.
It just goes to show that sometimes
the simplest things can go wrong,
but our tendency to over-complicate
things can point us off in the wrong
direction.
He cursed himself for not checking
those onboard fuses instead of wasting
time taking the board out, but he made
his assumptions on his own experiences. If he’d tested the motor, he’d
have found the fault straight away, so
I can be sure that’s what he’ll do next
time. Either way, it was a super-easy
fix for me, and everyone was happy.
Macbook Air repairs
B. P., of Dundathu, Qld previously
wrote in to describe several MacBooks
that he brought back into service. Well,
he’s up to it again, this time rescuing
some MacBook Airs from the rubbish tip...
Some time back, a friend gave me
several MacBook notebooks. I was able
to repair three using parts from those
92
Silicon Chip
and others that I already had. There
was also a MacBook Air, but I’d been
unable to test it because I only had
Magsafe 1 chargers and the MacBook
Air uses a Magsafe 2 charger.
More recently, I was given another
MacBook Air notebook, but I still
didn’t have a Magsafe 2 charger. Now
I had two of these MacBook Air notebooks and no way to test them. I’d
previously looked into the price of a
charger, but as they were around $40
or more, I didn’t want to spend that
sort of money without knowing if these
notebooks even worked.
I decided to look on eBay for a
replacement Magsafe 2 cable, and I
found one for $11.95, so I ordered
it. When it arrived, I dug out a 14.5V
charger with a Magsafe 1 cable, and
I cracked the charger apart using circlip pliers. One side of the shell came
off fairly easily, but the inside of the
charger proved challenging to get out
of the other half of the shell.
After I managed to remove it, I desoldered a wire and removed the copper
wrap. I was then able to desolder the
old cable and solder in the new one.
Then I refitted the copper wrap and
re-soldered the wire, and put the charger back together. The case clipped
back together nicely, without needing to glue it.
I grabbed one of the notebooks and
connected the charger to it. I waited
a minute and then pressed the power
button. I heard the familiar Mac boom,
so that was a good sign. The MacBook
loaded up with the previous user’s
account without needing a password,
but something wasn’t right. There was
no dock.
Then I discovered that the keyboard
and trackpad didn’t work, and I wondered if they had been disabled, so I
decided to boot from a USB installer
and check.
I had an earlier version of Catalina
on a USB, so I’d use that for now and
update it later. I pressed the Option
key and got the option of booting from
the HDD or the USB drive. The trackpad now worked, so I chose the USB
installer. I returned later, but now
the keyboard and trackpad no longer
worked; they were obviously faulty
and only worked intermittently.
I put this MacBook aside and
grabbed the other one to check it. Once
again, it started up, but I got a folder
with a question mark in it, indicating
that the eSATA SSD had either been
wiped or removed, so I booted from
the USB installer. There was still no
HDD present, so I guessed it had been
removed.
I took the back off, but I found
that the SSD was actually present. I
removed it and replaced it and tried
again, but it still didn’t show up. I
suspected it might be faulty, so I took
the back off the first MacBook Air,
removed the SSD and installed it in
the second MacBook. But it still didn’t
show up; I knew it was good, which
meant there was a fault with the motherboard.
I decided that the best option was
to swap the good motherboard from
the first MacBook Air into the second
MacBook Air. But this second MacBook had been dropped and there was
a significant dent in the front righthand side of the base and the lid, as
well as the base being bent where the
left USB port is, and the lid would not
close properly.
The other shell was in much better
shape, but I didn’t want to swap over
the keyboard, which is a massive job.
From what I’ve seen on YouTube videos with MacBook repairs, the keyboards are held in with a million tiny
screws, so I would have to repair the
damaged case.
I managed to tap the front corner
of the top case back into shape and
straighten the bent area at the USB
port, but I didn’t want to try to fix
the lid, as I could risk breaking the
screen. Instead, I would swap over
the good lid.
I started by dismantling the first
MacBook with the working motherboard. I removed the battery, then the
motherboard. I put the battery, motherboard and back of the shell aside to
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Left: the left-most charger is a
Magsafe 1, while the one on the right
is Magsafe 2. The Magsafe 2 charger
uses the same pins, but has a slightly
longer connector,
fit to the repaired case. The reason for
using this back is that it has the correct
serial number of the motherboard on
it. I’d use this battery, as it was already
fully charged, and I knew it was good.
I disassembled the second MacBook
similarly, then swapped in the good lid
and fitted the good parts. Now the lid
closed properly after the shell repair.
I also put fresh thermal compound on
the heatsink and cleaned the fan at the
same time. For the moment, I just sat
the back on, in case I had to do anything else inside, and I turned it over
and connected the charger.
The MacBook started up, and this
time, all was well with the keyboard
and trackpad and I finished the installation. I decided to check for updates
and was offered the latest version of
macOS as an upgrade.
The download finally finished, so
I copied the installer to an external
hard drive, and I also copied it to a
folder on the desktop before running it.
After some time, it was installed and I
was greeted with a terrible wallpaper,
which I quickly changed to the Big Sur
photo after I logged on.
Further testing indicated that this
MacBook Air notebook was working
correctly, so the $11.95 investment for
a replacement Magsafe 2 cable was a
good move. I screwed the back on permanently, gave it a quick clean and it
was complete.
This was a successful exercise in
taking two unusable notebooks and
making one good one. I don’t yet
know if the leftover parts will be of
any use, but I have kept them in case
I get another broken MacBook Air in
the future.
When I’d had the other MacBook
Air apart, I could see some corrosion
around the connection for the trackpad, so that explained why it didn’t
work reliably. It looks like someone
had spilled liquid on the trackpad,
which had seeped through and got
into the connector. I haven’t looked
into it any further to see whether that
damage is fixable. It might be.
Apparently, the small chip in the
trackpad cable also controls the keyboard, explaining why both had
stopped working.
Working on Mac computers and
MacBook notebooks is vastly different
to working on PCs and Windows laptops. Mac computers and Macbooks
need a lot more different tools, and
they are a lot more compact.
siliconchip.com.au
Below: the Macbook Air opened up,
so that the motherboard could be
swapped.
Australia's electronics magazine
January 2022 93
Repairing a computer mouse that double-clicks
D. S., of Maryborough, Qld made a similar repair to our
own serviceman, who described fixing a computer mouse
in the May 2021 issue...
Dave’s mouse repair story made me chuckle. A couple
of weeks ago, I was in a similar situation. A young fella
had a problem with his mouse; apparently, it was double-clicking on the right mouse button whenever it was
pressed. This, I was told, was “not a good thing when facing off with opponents in various online games”.
I asked if he had played with any of the settings in the
PC or the mouse’s installed software. He said he hadn’t,
and without the PC, I had to take his word for it. I did ask
if it was worth repairing, given that the repair might cost
more than a new mouse. I was told in no uncertain terms
that this was his “gaming mouse”, and he simply could
not replace it, as it had cost over $100 new.
I plugged it into my PC and ran it through its paces.
It certainly had many buttons, and they all worked as
expected, except the right button. It did indeed double-click with every single press.
The screws holding it all together were hidden under
more of those Teflon coated cushions, which I managed
to save.
Internally, the mouse looked like it was a nesting home
for a cat or other small pet. The internal optics for the
scroll wheel were buried under a soft blanket of pet hair,
which extended across most of the mainboard.
After I removed all that, I could test the microswitch on
the board, and sure enough, it was faulty. After removing
the small daughterboard, the mainboard came out, and I
removed the offending microswitch.
It was a fairly common part, even though it did have the
Logitech logo on the side, so I quickly found a replacement. It all worked fine once reassembled, and the young
gentleman was very happy.
I did mention the pet hair inside the mouse (shouldn’t
that be the other way around, mouse hair inside the cat!),
and he smiled and said the family cat often slept on his
desk, so that answered that question.
I have also repaired his monitor twice, once for a bad
tactile on/off switch and again when the mainboard
stopped working. Both were easy fixes, although I had to
buy 250 tactile switches in a nice neat little case; I will
soon be ordering more, as I replace more and more of
these switches.
Like Dave Thompson, my eyes are not so good nowadays, so soldering the 2.1 x 2.8mm switches required the
use of a desktop magnifier.
I also have a repair story involving Coca Cola and a JVC
65cm LED TV. I won’t bore you with the details; suffice
to say, it no longer worked.
The photo below shows what I found after checking the
power supply board and the T Con board. Coke always
makes a mess of electronics.
When these accidents happen, turn it off and get it to
a service person ASAP. Don’t ignore it just because the
TV (or whatever it is) still works. That’s what this teenage
customer did, and check out the resulting damage. After
I explained the fault and the time it may take to repair, I
got the feeling that this young fellow would be mowing
the lawn to pay Dad back for the cost of the repair.
It took a couple of hours to clean it up and get it working again. Rest assured that the offending teenager learned
a lesson and got Dad out of mowing for a while...
Damaged varistors in two microwave ovens
R. S., of Fig Tree Pocket, Qld has been busy fixing many
appliances, including two microwaves. Despite being
different models (both by Panasonic), they failed for the
same reason...
Both microwave ovens had intact mains fuses, but the
protective varistor across the mains on both microwave
ovens’ control/display boards were damaged. I think
this could be due to mains surges. This varistor is a
VDR10D511 10mm diameter, 511V varistor. There are also
protective capacitors on the mains supply input board.
The NN-SF574 oven (quite new) uses an inverter for
the control board supply with a Panasonic flyback control
IC and a high-frequency transformer. The varistor across
the mains is fed by a fine track marked PF1, which acts
as a fuse. This saved the board; replacing the track with
some fine wire and fitting a new varistor got the oven
going again.
A new control board is about $110, and a new oven
about $225. The NN-ST671 oven is an older design, with
The doubleclicking
mouse’s PCB,
shown at left,
had faulty
microswitches.
At right is a
section of the
power supply
board of a 65in
monitor. Some
corrosion can
be seen on the
connectors
from a soft
drink spillage.
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a small 50Hz transformer on the control board. Again,
the mains varistor is fed by a fine track, which I had to
replace along with the varistor. In this case, the varistor
was sleeved with a high-temperature fabric. Perhaps varistors have caught fire or exploded in the past.
I also repaired a Dome 24 wine cooler, Item No 900096.
Taking the back cover off showed it was a Peltier Effect
cooler with a large heatsink. There were two fans on the
outside to remove the outside heat, plus one on the inside
to distribute the cold air.
The constant current switching power supply for the
Peltier device had a blown fuse on the mains side. The supply uses a TL494 switching regulator driving two 13005
400V transistors connected in a totem-pole arrangement,
probably to increase the voltage rating.
Both 13005 transistors measured short circuit, as did
the STPS2045 dual schottky output rectifier (2 x 10A
45V). After replacing these, I put a light bulb across the
blown fuse and connected the mains. The bulb stayed on,
so there was still a problem.
I was surprised to find that two of the 1N4007 rectifiers
in the full-wave bridge were also shorted on the mains
input side. I am used to the large, sturdy rectifier bridges
used in microwave oven inverters which never fail; the
switching IGBT goes first.
Replacing the 1N4007s and the fuse got the cooler working again, with about 1.5V across the Peltier Effect device.
I did not measure the current. The big test will be when
summer comes, to see if the wine stays cool.
I also fixed a Kambrook K1780 steam iron. The series
capacitor in its power supply was a 560nF 250V DC
rated type that was down to about 430nF, so there was
not enough voltage to operate the 24V relay that connects the mains to the iron heating element. So the iron
would not heat.
I notice that the capacitor manufacturers derate the
voltage rating for AC, to about 60% of the DC voltage rating. For example, a 400V DC capacitor has an AC rating
of about 240V.
On that basis, the original 250V DC rated capacitor was
not adequate for the task. It seemed to have been chosen
for its small size, to fit in the space, rather than for a suitSC
able voltage rating.
The damaged VDR10D511 511V varistors taken from the
Panasonic microwave ovens.
siliconchip.com.au
Australia's electronics magazine
January 2022 95
REMOTE CONTROL
RANGE
EXTENDER
Most remote controls use pulses of infrared light to control equipment. This
usually only works reliably up to a few metres and is easily blocked by furniture,
people, plants... just about anything. Convert an IR remote to use UHF instead,
and it will work at much longer ranges. It will even work when something is
between the remote and the device, regardless of where the remote is pointed!
M
ost of the time, infrared remote
controls work very well. But
there are times where they
are woefully inadequate. This could
be because there is an obstruction
between the remote control and appliance to be controlled. Or the receiver
on the device may be awkwardly
placed, making it difficult to direct
the infrared beam to it.
Sometimes you might even want to
use the remote control in a different
room from the appliance to be controlled.
Or you might need to position the
appliance so that the receiver is not
facing where you will usually be
located, such as a projector, where it
will typically be behind you. Sometimes you can reflect the IR signals
using the projector screen, but that
doesn’t always work reliably.
Regardless of why the IR signal
doesn’t work well, this device is a great
solution. It allows you to convert the
infrared remote to transmit using UHF
radio signals rather than infrared light.
Another small box positioned in front
of the infrared receiver on the appliance picks up these radio signals and
transmits IR directly into the device’s
receiver.
Note that if you have more than one
appliance to be controlled, you could
convert all their remotes to transmit on
UHF and use a single UHF-to-IR converter to relay the signals to all those
devices. That’s provided the appliances are in the same vicinity, so that
the light from a single transmitter can
reach all their receivers.
Concept
Fig.1 shows the general arrangement
for the Range Extender. Fig.1(a) shows
how the IR-to-UHF Converter works,
while Fig.1(b) shows the UHF-to-IR
Converter.
Fig.1(a): the Remote Control Range Extender has two parts. The first is the IR-to-UHF Converter which runs from the
remote’s battery and converts its IR LED drive signal to a UHF transmission. The second is the UHF-to-IR Converter which
picks up those UHF signals and drives an infrared LED with appropriate modulation to control the appliance(s).
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IR-to-UHF Converter
❚Transmission range: 25m through one Hardiplank and Gyprock wall
❚Signal delay: 56μs
❚UHF transmitter power-down period: 600ms after the last signal
❚Standby current: 80nA typical at 3V supply (90nA measured)
❚Operating current: 8mA average during transmission
UHF-to-IR Converter
❚Valid transmission detection: requires 3ms minimum quieting period
❚Acknowledge LED lighting: 654ms time-out after a valid signal
❚Modulation frequency: 32.4kHz to 41.4kHz in 32 steps
❚Modulation duty cycle: 33.3%
❚Current consumption: close to 50mA during signal reception
❚IR transmission range: typically 2m to appliance receiver
By John Clarke
The IR-to-UHF Converter monitors
the signal that would normally be fed
to the IR LED. When a button on the
remote control is pressed, it produces
a ~36kHz modulated signal to drive
that LED. IC1 instead demodulates
that signal, and its output (waveform
B) is shown in scope grabs Scope 1 &
Scope 2 (which can be seen overleaf,
with the other scope grabs).
‘Demodulation’ converts the series
of brief 36kHz pulses to a signal that’s
high when the pulses are present and
low otherwise.
When IC1 detects it is receiving a
signal, it powers the UHF transmitter (IC2) and sends the demodulated
signal to the UHF transmitter’s input.
The result is that the UHF transmitter
produces a 433.92MHz modulated signal to the transmitting antenna. This
is waveform C.
So overall, the original 36kHz
modulated signal is converted to a
433.92MHz modulated signal for wireless transmission.
The corresponding UHF-to-IR Converter has a UHF receiver (RX1) that
provides the demodulated waveform,
shown as waveform D. This matches
the B waveform – see Scope 3. Processor IC1 on the second board then
uses a new 36kHz carrier to produce
a modulated waveform, waveform E,
that matches the original waveform A,
as shown in Scopes 4 & 5.
This modulated signal then drives
an infrared LED that sends the signal
onto the appliance(s) via their onboard
IR receivers.
Note that 36kHz is a typical modulation frequency used in infrared remote
controls. You can adjust the modulation frequency of the final infrared output to match that of the original remote
control, since the remote control could
use another frequency between about
32kHz and 41kHz.
Overall, the original handheld
remote signal is duplicated at the
output of the UHF-to-IR Converter.
The appliance receiving the signal is
none the wiser that any processing
has occurred.
Previously
Note that we published a similar
project named “Add a UHF link to a
universal remote control” (July 2013;
siliconchip.com.au/Article/3846).
While that project is still valid, this
one has a much smaller transmitter
circuit that can be fitted into small
infrared remote controls, unlike the
one from 2013.
This became apparent when we
tried to install our earlier design inside
a small remote control for an LCD projector. There just wasn’t any room for
it. Subsequently, the entire IR-to-UHF
circuit has been redesigned using surface mount components.
Fig.1(b): the waveforms at right, both here and in Fig.1(a) opposite, show how the original IR LED drive signal is
demodulated, then remodulated to 433.92MHz, then demodulated, then finally remodulated to around 36kHz to drive the
IR LED.
siliconchip.com.au
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January 2022 97
A real soldering challenge!
One of the main goals of this design
was for the UHF transmitter to be
tiny enough to fit inside just about
any remote control case. That rules
out using a pre-built UHF transmitter
module, and due to the relatively high
frequencies involved, the components
need to be small. Very small.
This project uses by far the smallest components we’ve ever specified
in a design.
The 68nH inductor comes in a metric 0603 SMD package (imperial 0201)
Instead of using a large pre-built
UHF transmitter module, we use a
very small UHF transmitter IC with a
few discrete components.
Remote’s battery life
One question that arises is what happens to the battery life of the modified
remote. Will the battery be flattened in
a short time when the UHF transmitter
circuitry is added?
We have made sure that there will
be a negligible effect on battery life by
having the circuitry in a sleep mode
when you are not using the remote. A
typical infrared remote control draws
about 1-2μA from the battery continuously and around 10-20mA during
infrared transmission. The UHF transmitter’s added power draw has almost
no effect on these figures.
With the IR-to-UHF Converter
installed, we measured the standby
current increasing by a mere 90nA
– that’s 0.6 x 0.3mm! Unless you have
excellent vision, it will just look like
a dot to you (if you can see it at all).
And the metric 1206 SMD inductors
(imperial 0402) aren’t all that much
bigger at 1.2 x 0.6mm.
Soldering these devices is a challenge, to put it mildly. If you decide
to go ahead, we suggest you purchase at least 10 of each (hey, they’re
cheap!). That way, if you mangle or
lose them, you can grab another one
and try again.
(0.09μA)! The current drain when a
button is pressed is essentially unaltered and possibly even a little less
than before, as the remote’s IR LED is
not used and replaced by UHF transmission, which is on average 8mA
when active.
By the way, we measured the 90nA
figure by connecting a 100kW resistor
in series with the device’s supply and
shorting it out until it went into sleep
mode. We then measured 9mV across
this resistor, which equates to 90nA
(9mV ÷ 100kW).
Receiver
The companion UHF-to-IR Converter is housed in a small plastic case.
One end of the case has a red acknowledge LED and an IR LED to re-transmit
the received UHF signal as an IR signal. There is also a 3.5mm jack socket
to allow the connection of an external
IR LED via a cable.
Even the larger (by comparison)
devices on this board are a little tricky
to solder because it’s so packed with
components – again, to keep it small
and also so it can transmit 434MHz
signals efficiently.
Besides being a useful little device
to build, if you have reasonable SMD
soldering skills and want to push yourself to achieve the next level of skill,
assembling the transmitter module
described here would be a great way
to do that.
This device either runs from a 9-12V
DC plugpack or USB 5V. The circuit
draws a maximum of 50mA when
transmitting, so any 9-12V DC plugpack or USB power source should be
suitable.
Circuit details
Fig.2 shows the circuit of the IR-toUHF Converter that’s designed to be
built into the remote control. It comprises a PIC10LF322 microcontroller
(IC1), a MICRF113 UHF transmitter
(IC2) and associated components.
IC1 monitors the infrared LED drive
signal originally used to drive the
infrared LED. The handheld remote
output will drive either low or high
to power the LED.
An open-collector driver transistor or Mosfet within the remote control IC is normally used. This output
requires a pull-up resistance to turn it
into a digital signal for sensing, which
Fig.2: the IR-to-UHF Converter section circuit deliberately uses few components to make the PCB as small as possible.
It’s powered by the typically 3V supply of the remote control (from two 1.5V cells). IC1 demodulates the drive signal that
would normally go to an infrared LED. When it detects a button press, it powers up UHF transmitter IC2 and feeds it the
demodulated signal that is then radiated by the antenna at 434MHz.
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Scope 1: the top yellow trace is the
infrared LED drive signal from the
remote control, applied to pin 1 of
IC1. This is a series of 36kHz pulses.
The lower blue trace shows the
output of IC1 at pin 4 that drives the
ASK input (pin 6) of the MICRF113
434MHz transmitter (IC2). This signal
is high whenever there is a 36kHz
signal at the input and low otherwise.
is supplied by a Mosfet we enable
inside IC1.
A 1kW pull-down resistor is shown
on the circuit, but this is only required
if the remote control has an open-collector (or open-drain) output that
drives high to power the LED. We will
describe how to check for this later.
IC1 converts the LED drive modulation (typically 36kHz) into a demodulated output at pin 4. That pin goes high
when a modulated signal is present and
low when the modulation is absent.
IC2 is a UHF transmitter that sends
digital data using two different carrier wave amplitudes. This is known
as Amplitude Shift Keying (or ASK).
For our purposes, there is no UHF
transmission when the digital signal is
low (near 0V) and a 433.92MHz carrier
transmission when the digital signal
is high (near 3V).
IC1’s demodulated signal at pin 4
is suitable for driving IC2 at its ASK
input (pin 6). Note that the pin 3 output of IC1 drives the supply input for
IC2, at its pin 3. This way, IC2 can be
shut down when not needed, drawing
no power at idle.
The transmission frequency is set
using a crystal oscillator that is multiplied by 32 within IC2 to produce the
UHF carrier. So the 13.56MHz crystal gives a carrier at 433.92MHz. This
matches the carrier frequency used in
most UHF ASK transmitter/receiver
modules that are available for lowpower UHF data transmission.
The MICRF113 and its associated
components are tiny, fitting in a much
tighter space than most pre-built UHF
transmitter modules that are available.
The supply current for IC2’s RF
output stage is via two series-connected 220nH inductors, also acting
as a 440nH driver load. The following
12pF series capacitor and 68nH inductor plus the 5pF capacitor to ground
act as a filter that removes second and
third harmonics from the UHF signal
before it passes to the antenna.
We mainly use two 220nH inductors
instead of one 470nH inductor because
we found suitable 220nH inductors
easier to source. Any inductor used in
the circuit must have a self-resonance
(SR) frequency above 433.92MHz; otherwise, it will not function as an inductor at that frequency.
Scope 2: this is the same capture as
Scope 1 except with a faster timebase,
so the 36kHz modulation is visible.
Note the delay of about 56μs between
IC1 receiving the 36kHz pulses and
producing the demodulated pulses at
its output. This does not distort the
signal because it is symmetrical.
Scope 3: the top yellow trace shows
the IR drive signal from the handheld
remote as in Scope 1, but the lower
trace is the output from the UHF
receiver in the UHF-to-IR Converter,
ie, after it has passed over the
wireless link.
Scope 4: the top yellow trace is the
infrared LED drive signal from the
original infrared remote, while the
lower blue trace is the IR LED drive
signal in the UHF-to-IR Converter.
The two waveforms are essentially the
same except for the slight delay in the
second trace, and the different voltage
levels due to the UHF-to-IR circuit
powered from 5V instead of 3V. The
signal inversion is of no consequence.
Scope5: a zoomed-in version of Scope
4 showing the modulation on both
signals. The rise time of the original
waveform at the top is slow due to the
low pull-up current from pin 1 of the
PIC10LF322. The lower blue trace is
the IR LED drive from the UHF-to-IR
Converter. The frequency has been set
to about 36kHz to match the handheld
remote. The top trace is inverted
compared to the lower trace, as the
original LED in the handheld remote
was on when the output was low,
whereas the IR LED in the UHF-to-IR
Converter LED drive is active-high.
Power for IC2
IC2’s power rail at pin 3 is bypassed
with a 1μF ceramic capacitor, while a
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January 2022 99
100nF capacitor bypasses the output
stage supply. These two capacitors
are essentially in parallel but are at
different locations on the PCB so that
the supply for each part is bypassed
directly at its supply connection.
We include schottky diode D2
between the ASK signal and the IC2
supply to boost the supply whenever
the IC is transmitting. The pin 3 output drops in voltage when supplying
current; current flowing from pin 4 of
IC1 via diode D2 assists in maintaining
a stable supply voltage for IC2.
While IC2 can operate down to 1.8V,
it’s best to keep its supply voltage as
close as possible to the 3V from the
remote battery for the best efficiency.
IC1’s supply is bypassed by another
100nF ceramic capacitor. Diode D1
is included in case the cells in the
remote are inserted the wrong way
around, causing a reverse polarity to be
applied. In this case, D1 will conduct
and reduce the reverse voltage applied
to IC1, preventing it from being damaged (at least in the short term).
UHF-to-IR Converter
The UHF signal needs to be detected
and converted back to a stream of
infrared pulses to control the appliance being operated. The UHF-to-IR
Converter circuit is shown in Fig.3,
and comprises UHF receiver RX1, a
PIC12F617 microcontroller (IC1) and
an infrared LED (LED1).
The circuit is powered via either DC
socket CON1 or micro-B USB socket
CON2. The UHF receiver is powered
continuously, ready to receive a transmission from the IR-to-UHF Converter
in the handheld remote.
With no signal present, the data output from the UHF receiver is just random noise with an amplitude of 5V. In
this state, the receiver operates at maximum gain due to its automatic gain
control (AGC). When a UHF signal is
received, the AGC reduces the receiver’s sensitivity so that the detected
signal is essentially noise-free. This
is fed to the GP5 input (pin 2) of PIC
micro IC1.
To determine if a signal is valid,
IC1 checks for periods where the data
line from the UHF receiver is at 0V for
at least 3ms. This indicates that the
AGC has reduced the sensitivity of
the receiver and that a transmission
is occurring.
The data output from the UHF
receiver matches that data applied to
the UHF transmitter. This data signal,
in part, becomes the Acknowledge
waveform that drives LED2 via digital
output GP0. The 1kW resistor limits the
LED current to around 3mA.
IC1 drives the IR LED (LED1) from
its GP1 and GP2 outputs in parallel to
provide sufficient current. The 220W
resistor limits this current to around
18mA.
The infrared LED drive signal needs
to include the same or similar modulation as that used by the original remote.
So when the data output from the UHF
receiver goes high, the GP1 and GP2
outputs are driven with pulse-width
modulated signals. The duty cycle is
33.3%, so they are high 1/3 of the time
and low 2/3 of the time.
The GP4 input of IC1 monitors the
voltage set by trimpot VR1, connected
across the 5V supply rail. Its wiper
voltage is converted to a digital value
within IC1, allowing the IR carrier
frequency to be adjusted to match the
original transmitter. The adjustment
range is from 32.4kHz to 41.4kHz in
32 steps. Setting VR1 to its mid-position gives 37kHz.
Usually, somewhere near the middle setting is satisfactory, but some
devices might require a different carrier frequency to operate reliably.
A second output is provided via
3.5mm jack socket CON3 for an external IR LED (if necessary). This LED can
be mounted near the IR receiver of the
appliance(s) being operated.
Power from a 9-12V DC plugpack
is fed in via diode D1, providing
reverse polarity protection. A 78L05
3-terminal regulator then provides a
5V supply for RX1 and IC1. Power
via the USB connector is applied to
the 5V supply rail via a 4.7W resistor.
Fig.3: the UHF-to-IR Converter PCB uses a pre-built UHF receiver module
(RX1) to pick up the signals from the transmitter, then microcontroller
IC1 adds modulation at a frequency adjustable by VR1, and drives
onboard infrared LED1 plus an external LED when plugged in via CON3.
It can run directly from a 5V USB source via CON2 or 9-12V DC from
barrel socket CON1, regulated to 5V by linear regulator REG1.
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This resistor prevents excess current
flow between the REG1 output and
the 5V from the USB should both be
connected.
Construction
The IR-to-UHF Converter PCB is
coded 15109212 and measures 15mm
x 12mm. It has components mounted
on both sides. Refer to the PCB overlay
diagrams, Figs.4(a) & (b), to see which
parts go where.
If IC1 hasn’t been programmed, do
that before fitting it. You can purchase
pre-programmed PIC10LF322 microcontrollers from our Online Shop if
you don’t have the equipment to do
it yourself.
Begin assembly by fitting the surface
mount parts on the top side of the PCB.
These can be soldered using a finetipped soldering iron. Good close-up
vision is necessary; you might need a
magnifying lens or glasses to see well
enough. Some fine-point tweezers can
help as well, to hold the components
in place.
It will be easier to install the two
220nH inductors first. Solder one pad
first and check alignment. Reheat the
soldered pad and move the device if
the inductor needs moving before soldering the second pad.
Then mount the two ICs. IC1 and
IC2 are positioned so that the small
pin 1 location dot aligns with that on
the PCB. When the IC is held with pin
1 at lower left, the writing on the IC
top face will be the right way up. IC1
will be marked LF followed by two
traceability code numbers. IC2 will
Before mounting the IR-to-UHF
Converter inside the remote, you
will need to check whether a pulldown resistor is needed.
have “F_113” etched on the top face.
Orientate the ICs on the PCB with
the pin 1 dot at upper left. For each
IC, solder one pad first and then check
their alignment. Readjust the component positioning by reheating the solder joint if necessary before soldering the remaining pins. Any shorts
between pins can be cleared using
solder wick to draw up the excess solder (adding flux paste first will help
this process).
Now diode D2 can be soldered in
before fitting crystal X1. Make sure
D2 is orientated as shown in Fig.4(a).
You can then install the remaining top-mounted components. Note
that many of the capacitors and
inductors in surface mount packages
are unmarked, so you will need to rely
on the packaging to show what they
are and their value. Mount one component at a time to avoid mixing them up.
We are using capacitors and a resistor in slightly smaller M2012/0805
packages compared to the M3216/1206
packages we use elsewhere. This
makes it easier to avoid accidentally
making solder bridges to adjacent components when fitting them.
It is also possible to lose components, so be careful and, if possible,
get spares (SMD resistors and capacitors are generally very cheap and sold
in sets).
We recommend that you mount the
These two photos show the top and bottom of the
IR-to-UHF PCB at approximately triple actual size.
Fig.4 (right): the IR-to-UHF converter PCB is packed so it can fit inside just about any
remote control case. Don’t worry too much about bridging the pins of IC1 & IC2 when
soldering them as that can be fixed quite easily using solder wick and flux paste, but do
be careful to orientate those ICs correctly and don’t mix them up. The 68nH inductor
is minuscule, so be careful not to lose it. After soldering it, check for a low resistance
reading between the antenna terminal and left end of the 12pF capacitor.
siliconchip.com.au
Australia's electronics magazine
January 2022 101
Parts List – Remote Control Range Extender
IR-to-UHF Converter
1 double-sided PCB coded 15109212, 15mm x 12mm
1 13.56MHz surface-mount crystal (X1) [RS Components 171-0468]
2 220nH 500MHz inductors, M1005/0402 SMD (L1) [RS 741-3797]
1 68nH 1.2GHz inductor, M0602/0201 SMD (L2) [element14 3386563]
1 170mm length of light-duty hook-up wire (for the antenna)
1 200mm-length of red hook-up wire
Kit (SC5993)
1 200mm-length of green hook-up wire
A kit is available for the IR-to1 200mm-length of blue hook-up wire
UHF Converter, see page 106.
Semiconductors
1 PIC10LF322-I/OT 8-bit microcontroller programmed with 1510921M.HEX,
SOT-23-6 (IC1) [Silicon Chip Online Shop]
1 MICFR113YM6 ASK UHF transmitter chip, SOT-23-6 (IC2) [RS 177-3314P]
1 1A SMD diode, DO-214AC (D1) [SM4004 or GS1G; Altronics Y0174,
Jaycar ZR1003]
1 BAT54S ➊ small signal schottky diode, SOT-23 (D2) [Altronics Y0075]
➊ BAT54, BAT54S, BAT54C, BAT54FILMY and BAT54SFIMLY are all suitable
Capacitors (all SMD M2012/0805 size ceramic)
1 1μF 16V X7R (preferred) or Y5V [Altronics R8650]
2 100nF 50V X7R (preferred) or Y5V [Altronics R8638]
2 18pF 50V C0G/NP0 [Altronics R8533]
1 12pF 50V C0G/NP0 [Altronics R8527]
1 4.7pF or 5pF 50V C0G/NP0 [Altronics R8512]
Resistors
1 1kW SMD M2012/0805 ⅛W (might not be required; see text) [Altronics
R1220]
1 10kW to 470kW ¼W axial leaded resistor (for testing)
UHF-to-IR Converter
1 double-sided PCB coded 15109211, 79 x 47mm
1 UB5 Jiffy box, 83 x 54 x 31mm
1 lid label, 78 x 49mm
1 433.92MHz receiver module (RX1) [Jaycar ZW3102, Altronics Z6905A]
1 PCB-mount barrel socket to suit plugpack (CON1)
1 micro-USB SMD Type-B USB socket (CON2) [Jaycar PS0922, Altronics
P1309]
1 3.5mm PCB-mount switched jack socket (CON3) [Jaycar PS0133,
Altronics P0092]
1 8-pin DIL IC socket (for IC1)
1 170mm-length of light-duty hookup wire
1 10kW miniature horizontal trimpot (VR1)
Semiconductors
1 PIC12F617-I/P 8-bit microcontroller, DIP-8, programmed with
1510921A.hex (IC1) [Silicon Chip Online Shop]
1 78L05 5V 100mA linear regulator, TO-92 (REG1)
1 3mm infrared LED (LED1)
1 3mm red LED (LED2)
1 1N4004 400V 1A diode (D1)
Capacitors
2 100μF 16V PC electrolytic
1 100nF 63V MKT polyester
Resistors (all ¼W 1% thin film axial)
2 1kW
2 220W
1 4.7W
Optional parts for extended IR transmitter lead
1 3.5mm mono jack plug
1 1m length of single-core screened cable
1 3mm infrared LED
1 100mm length of 3mm diameter heatshrink tubing
102
Silicon Chip
Australia's electronics magazine
68nH inductor after fitting the 12pF
and 5pF capacitors; otherwise, this
inductor may become accidentally
desoldered.
Now turn your attention to the
underside of the PCB. There are two
18pF capacitors, one 1kW resistor
and diode D1. Taking care to position
the diode correctly, with the cathode
stripe, as shown in Fig.4(b). Note that
the resistor might not be required, so
leave it off for the moment.
If you want to be sure that the
components have been soldered correctly, you can trace the connections
to the other sections of the PCB to
where there should be continuity.
For example, pin 3 of IC1 should provide a low resistance reading to pin 3
of IC2. Additionally, check that there
are no short circuits between component pins on the PCB that shouldn’t
be connected.
Pull-up or pull-down
As mentioned, the handheld remote
control might drive its output high or
low to turn the IR LED on. The way
the LED is driven determines whether
you need to install the 1kW pull-down
resistor. The internal pull-up within
IC1 is automatically activated if the
pull-down resistor is not fitted.
To determine this, first you will
need to open the remote control case.
Some remote cases are secured using
screws that are easy to spot, but they
also could be hidden under the cells.
Open the battery compartment and
remove the cells to check for screws.
Once these are out, open the case by
gently working around the sides with
a thin implement to separate the two
halves.
Once inside, locate the positive and
negative battery terminals. To check
whether the resistor is needed, it is
just a matter of making some measurements with a multimeter.
Firstly, check the resistance between
the battery’s positive terminal and the
anode (+) of the LED. If it is low (less
than 30W), you can expect that the pulldown resistor is not needed. That is
because the cathode of the LED would
be pulled down to power the LED.
If the resistance between the cathode
(-) of the LED and the negative battery
terminals is low (less than 30W), that
means the LED drive is active-high, so
the 1kW pull-down resistor is needed.
After the pull-down resistor is
soldered in place (if needed), the
siliconchip.com.au
The IR LED in the remote is replaced
with our IR-to-UHF PCB. This PCB
can then be covered with
heatshrink and placed
in the remote's
housing.
►
►
The UHF-toIR PCB can be
mounted inside a
UB5 case and placed near
the receiving device. You will need
to drill holes in the UB5 case for the
sockets and LEDs as shown in Fig.6.
assembled board can be mounted in
the remote’s case. The IR LED should
be removed.
Wire up the supply connections: +
to the +3V on the remote, GND to the
0V terminal and IN to the LED drive
pin on the remote’s IC (eg, to the pad
where the LED was soldered). You
might need to trace out the PCB to figure out which one to connect.
Place the PCB in a suitable spare
space within the remote, solder the
antenna wire, and route this around
the case in a position where it will
not be caught when it is reassembled.
Note that while we specify a 170mm
length of antenna wire, the transmission range does not suffer significantly if it is shortened. We found that
a 53mm length of antenna wire only
reduced the range by 5m compared to
the 170mm length.
Finally, clip the case together and
reinstall the securing screws if they
were present.
UHF-to-IR Converter assembly
The companion UHF-to-IR Converter is built on a double-sided PCB
coded 151009211 that measures 79 x
47mm. This clips neatly into an 83 x
54 x 31mm UB5 plastic utility box.
A 78 x 49mm lid panel label can be
attached to this.
If IC1 for this PCB hasn’t been programmed yet, do it now before continuing. As with the SMD chip, we can
supply a pre-programmed PIC12F617I/P if you don’t have the equipment to
do this yourself.
Fig.5 shows the parts layout for
this board. Start with the micro USB
socket, which is surface-mounted.
Align the solder pads with the leads
on the connector and solder one of the
mounting tabs to the PCB.
Re-check the alignment of the small
signal pins before soldering the signal
pins and then the remaining tabs. The
solder on the mounting tab can be
remelted, and the connector realigned
if it is not correct.
Check the signal pins for solder
bridges; if you find any, clear them
using solder wick. Make sure the pins
are still soldered to the PCB.
Now fit the resistors. The resistor
colour codes can be used as a guide
to their values but checking the resistances with a multimeter is also a
good idea.
Next, mount diode D1, ensuring it
is correctly orientated. The capacitors
can go in next; only the two 100μF
electrolytics are polarised. As well as
ensuring their longer leads go to the
pads marked with + symbols, they
must be bent over to clear the lid when
the PCB is mounted in its case.
REG1 can then be mounted, followed by the DC socket (CON1), the
3.5mm jack socket (CON2) and trimpot
Fig.5: the assembly of this board is straightforward as the components are much larger than on the other board. Watch
the orientations of the UHF receiver, IC1 and diode D1.
siliconchip.com.au
Australia's electronics magazine
January 2022 103
The front panel label
for the Remote Control
Range Extender can
be downloaded as a
1-1 scale PDF from
siliconchip.com.au
VR1 (set it mid-way now). Next, fit the
UHF receiver (RX1), making sure it
goes in the right way around.
Installing the LEDs
LED1 must be mounted at full lead
length (25mm) so that it can be later
bent over and its lens pushed through
a hole in the side of the box (above the
3.5mm socket). LED2 is mounted with
the top of its lens 20mm above the PCB
surface. Make sure the LEDs are orientated correctly, with their anode (longer) leads going to the pads marked “A”.
Now solder in an 8-pin DIL socket
for IC1, but do not plug the PIC micro
in at this stage. That step comes later
after the power supply has been tested.
Complete the PCB assembly by fitting
the 170mm-long antenna wire made
from insulated hookup wire.
Final assembly
The PCB simply clips into the
integral ribs of the UB5 case. Before
doing this, you need to drill holes in
the case ends for the USB socket, the
DC socket, the 3.5mm socket and the
two LEDs. The drilling diagrams are
shown in Fig.6.
The DC socket hole can be drilled
first. This is positioned 6.5mm down
from the top lip of the base at the lefthand end.
Start this hole using a small pilot
drill, then carefully enlarge it to
6.5mm using a tapered reamer. The
3.5mm socket hole is centred along
the horizontal axis at the other end of
the case, 10.5mm down from the lip.
Again, use a pilot drill to start it, then
enlarge it to 6.5mm.
The hole for LED1 can
then be
drilled 3.5mm down from the lip,
directly above the socket hole. Drill
this hole to 3mm, then drill a similar hole for LED2 about 12mm to the
right. The rectangular USB cut-out can
be first drilled and then filed to shape
with needle files.
Now clip the PCB into the slots
in the side ribs of the box (push the
3.5mm jack socket into its hole first).
Once it’s in place, bend the two LEDs
over and push them through their
respective holes in the adjacent end.
Secure the assembly by fitting the nut
to the jack socket.
The lid label can be downloaded
(in PDF format) from siliconchip.com.
au (go to “Shop” and then “Panel artwork”) and printed out onto a suitable label (see information on making labels at siliconchip.com.au/
Help/FrontPanels) and affixed to the
lid. The four corner holes for the case
screws can be cut out using a sharp
hobby knife.
Making an extension cable
Depending on how your gear is
arranged, you may want to make up a
cable with a 3.5mm jack plug at one
end and an external IR LED at the
other. Fig.7 shows the details. You
will need to use a suitable length of
single-core shielded cable, while the
LED leads should be insulated from
each other using heatshrink tubing.
Use a length of larger diameter
An extension cable can be made and attached to
the UHF-to-IR Converter via the 3.5mm jack socket
(CON3); Fig.7 has the details for how to design this
cable.
104
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
heatshrink tubing to cover the end of
the cable, including both LED leads
and part of the lens, as shown below.
►
Testing
First, check that IC1 has not been
installed. Apply power and check
there is 5V between pins 1 & 8 of the IC
socket. If not, verify the supply polarity and ensure that D1 and REG1 are
correctly orientated.
If you measure 5V, switch off and
install IC1 with its notched end
towards the adjacent 100nF capacitor.
Now reapply power and check that the
red acknowledge LED flashes when the
remote control buttons are pressed.
Next, test the appliance. The UHFto-IR Converter needs to have its IR
LED pointing towards the appliance at
a range of about 1m. If it doesn’t work,
adjust VR1 as you operate the remote
control until the appliance responds.
Usually, setting VR1 mid-way (corresponding to a carrier frequency of
around 37kHz) will be suitable.
Once it’s operating correctly, try
using the remote to control the appliance from another room. You should
get a free-air range of 20-25m, but the
range will be less than this inside a
house, depending on any obstacles
(walls, etc) between the remote and
the UHF-to-IR Converter.
Fig.6: here are where the holes need
to be drilled or cut in the UB5 Jiffy
box. The hole for the jack socket in
the right-hand end of the box can
be left out if you aren’t using the IR
extension lead, and similarly, you
only need to make one hole in the lefthand end, depending on whether you
will be using the USB or barrel socket
to supply power.
Fig.7: if you need to mount the IR
LED away from the receiver unit
(eg, mounting it directly in front
of the appliance’s receiver), you
can make up an extension cable as
shown here. It plugs directly into
the socket on the receiver.
►
SC
U Cable Tester
S
B
Test just about any USB cable!
USB-A (2.0/3.2) USB-B (2.0/3.2)
USB-C Mini-B Micro-B (2.0/3.2)
Reports faults with individual cable
ends, short circuits, open circuits,
voltage drops and cable resistance etc
November & December 2021 issues
siliconchip.com.au/Series/374
DIY kit for $110
SC5966 – siliconchip.com.au/Shop/20/5966
Everything included except the case and batteries. Postage is $10 within Australia, see our website for overseas & express post rates
siliconchip.com.au
Australia's electronics magazine
January 2022 105
SILICON
CHIP
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ONLINESHOP
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PRE-PROGRAMMED MICROS
For a complete list, go to siliconchip.com.au/Shop/9
$10 MICROS
24LC32A-I/SN
ATmega328P
ATmega328P-AUR
ATtiny85V-10PU
ATtiny816
PIC10F202-E/OT
PIC10LF322-I/OT
PIC12F1572-I/SN
PIC12F617-I/P
PIC12F617-I/SN
PIC12F675-I/P
PIC12F675-I/SN
PIC16F1455-I/P
PIC16F1455-I/SL
PIC16F1459-I/P
PIC16F1705-I/P
PIC16F88-I/P
$15 MICROS
Digital FX Unit (Apr21)
RF Signal Generator (Jun19), Si473x FM/AM/SW Digital Radio (Jul21)
RGB Stackable LED Christmas Star (Nov20)
Shirt Pocket Audio Oscillator (Sep20)
ATtiny816 Development/Breakout Board (Jan19)
Ultrabrite LED Driver (with free TC6502P095VCT IC, Sep19)
Range Extender IR-to-UHF (Jan22)
LED Christmas Ornaments (Nov20; specify variant)
Nano TV Pong (Aug21), SMD Test Tweezers (Oct21)
Refined Full-Wave Universal Motor Speed Controller (Apr21)
Model Railway Level Crossing (two required – $15/pair) (Jul21)
Range Extender UHF-to-IR (Jan22)
Model Railway Carriage Lights (Nov21)
Motor Speed Controller (Mar18), Heater Controller (Apr18)
Useless Box IC3 (Dec18)
Tiny LED Xmas Tree (Nov19)
Digital Interface Module (Nov18), GPS Finesaver (Jun19)
Digital Lighting Controller LED Slave (Dec20)
Ol’ Timer II (Jul20), Battery Multi Logger (Feb21)
5-Way LCD Panel Meter (Nov19), IR Remote Control Assistant (Jul20)
Ultrasonic Cleaner (Sep20), Electronic Wind Chime (Feb21)
20A DC Motor Speed Controller (Jul21)
Flexible Digital Lighting Controller Slave (Oct20)
Digital Lighting Controller Translator (Dec21)
UHF Repeater (May19), Six Input Audio Selector (Sep19)
Universal Battery Charge Controller (Dec19)
ATSAML10E16A-AUT
High-Current Battery Balancer (Mar21)
PIC16F1459-I/SO
Four-Channel DC Fan & Pump Controller (Dec18)
PIC16F18877-I/P
USB Cable Tester (Nov21)
PIC32MM0256GPM028-I/SS Super Digital Sound Effects (Aug18)
PIC32MX170F256D-501P/T 44-pin Micromite Mk2 (Aug14), 4DoF Simulation Seat (Sep19)
PIC32MX170F256B-50I/SP Micromite LCD BackPack V1-V3 (Feb16 / May17 / Aug19)
GPS-Synched Frequency Reference (Nov18), Air Quality Monitor (Feb20)
RCL Box (Jun20), Digital Lighting Controller Micromite Master (Nov20)
Advanced GPS Computer (Jun21)
Touchscreen Digital Preamp [2.8in/3.5in version] (Sep21)
PIC32MX170F256B-I/SO
Battery Multi Logger (Feb21), Battery Manager BackPack (Aug21)
PIC32MX270F256B-50I/SP ASCII Video Terminal (Jul14), USB M&K Adaptor (Feb19)
PIC32MX795F512H-80I/PT Maximite (Mar11), miniMaximite (Nov11), Colour Maximite
(Sep12), Touchscreen Audio Recorder (Jun14)
$20 MICROS
dsPIC33FJ64MC802-E/SP
dsPIC33FJ128GP306-I/PT
dsPIC33FJ128GP802-I/SP
PIC32MX470F512H-I/PT
PIC32MX470F512H-120/PT
PIC32MX470F512L-120/PT
1.5kW Induction Motor Speed Controller (Aug13)
CLASSiC DAC (Feb13)
Ultra-LD Preamp (Nov11), LED Musicolour (Oct12)
Stereo Echo/Reverb (Feb 14), Digital Effects Unit (Oct14)
Micromite Explore 64 (Aug 16), Micromite Plus (Nov16)
Micromite Explore 100 (Sep16)
$30 MICROS
PIC32MX695F512L-80I/PF Colour MaxiMite (Sep12)
PIC32MZ2048EFH064-I/PT DSP Crossover/Equaliser (May19), Low-Distortion DDS (Feb20)
DIY Reflow Oven Controller (Apr20)
KITS, SPECIALISED COMPONENTS ETC
IR-TO-UHF MODULE FOR RANGE EXTENDER (CAT SC5993)
(JAN 22)
SMD TRAINER KIT (CAT SC5260)
(DEC 21)
HUMMINGBIRD AMPLIFIER (CAT SC6021)
(DEC 21)
PCB and all SMDs (including the programmed micro) for the IR-to-UHF module
Complete kit includes the PCB and all on-board components,
except for a TQFP-64 footprint device
$20.00
Hard-to-get parts includes: two 0.22W 5W resistors; plus one each of an
MJE15034G, MJE15035G, KSC3503DS & 220pF 250V C0G ceramic capacitor
USB CABLE TESTER KIT (CAT SC5966)
(NOV 21)
MODEL RAILWAY CARRIAGE LIGHTS KIT (CAT SC6027)
(NOV 21)
SMD TEST TWEEZERS KIT (CAT SC5934)
(OCT 21)
NANO TV PONG SHORT FORM KIT (CAT SC5885)
(AUG 21)
MODEL RAILWAY LEVEL CROSSING
(JUL 21)
MINI ISOLATED SERIAL LINK COMPLETE KIT (CAT SC5750)
(MAR 21)
AM/FM/SW RADIO
(JAN 21)
MICROMITE LCD BACKPACK V3 KIT (CAT SC5082)
(AUG 19)
Short form kit with everything except case and AA cells
Includes PCB, IC1 (programmed), IC2, D1, L1, SMD capacitors and resistors.
Does not include reed switch, magnet, LEDs or through-hole parts
PCBs, micro, other onboard parts and heatshrink (no cell or brass tips)
PCB and all onboard parts only (does not include controllers)
- Pair of programmed PIC12F617-I/Ps
- ISD1820P-based audio recording and playback module
All parts required to build the project including the PCB
- PCB-mount right-angle SMA socket (SC4918)
- Pulse-type rotary encoder with integral pushbutton (SC5601)
- 16x2 LCD module (does not use I2C module) (SC4198)
$25.00
$15.00
$110.00
$25.00
$35.00
$17.50
$15.00
$5.00
$10.00
$2.50
$3.00
$7.50
Includes PCB, programmed micros, 3.5in touchscreen LCD, UB3 lid, mounting hardware,
Mosfets for PWM backlight control and all other mandatory on-board parts
$75.00
Separate/Optional Components:
- 3.5-inch TFT LCD touchscreen (Cat SC5062)
$35.00
siliconchip.com.au/Shop/
- DHT22 temp/humidity sensor (Cat SC4150)
- BMP180 (Cat SC4343) OR BMP280 (Cat SC4595) temp/pressure sensor
- BME280 temperature/pressure/humidity sensor (Cat SC4608)
- DS3231 real-time clock SOIC-16 IC (Cat SC5103)
- 23LC1024 1MB RAM (SOIC-8) (Cat SC5104)
- AT25SF041 512KB flash (SOIC-8) (Cat SC5105)
- 10µF 16V X7R through-hole capacitor (Cat SC5106)
$7.50
$5.00
$10.00
$4.00
$5.00
$1.50
$2.00
VARIOUS MODULES & PARTS
- 64x32 pixel white 0.49in OLED (SMD Test Tweezers, Oct21)
$10.00
- pair of AD8403ARZ10 (Touchscreen Digital Preamp, Sep21)
$35.00
- Si4732 radio IC (Si473x FM/AM/SW Radio, Jul21)
$15.00
- EA2-5NU relay (PIC Programming Helper, Jun21)
$3.00
- VK2828U7G5LF GPS module (Advanced GPS Computer, Jun21)
$25.00
- MCP4251-502E/P (Advanced GPS Computer, Jun21)
$3.00
- pair of Signetics NE555Ns (Arcade Pong, Jun21)
$12.50
- 2.8-inch touchscreen LCD module (Lab Supply, May21)
$25.00
- Spin FV-1 digital effects IC (Digital FX Unit, Apr21)
$40.00
- 15mW 3W SMD resistor (Battery Multi Logger / Arduino PSU, Feb21)
$2.50
- DS3231(M) real-time clock SMD IC (Battery Multi Logger, Feb21)
$3.00
- Pair of CSD18534 transistors (Electronic Wind Chimes, Feb21)
$6.00
- IPP80P03P4L04 (Dual Battery Lifesaver / Vintage Radio Supply, Dec20)
$5.00
- 16x2 LCD module (Digital RF Power Meter, Aug20)
$7.50
- WS2812 8x8 RGB LED matrix module (Ol’ Timer II, Jul20)
$15.00
- MAX038 function generator IC (H-Field Transanalyser, May20)
$25.00
- MC1496P double-balanced mixer IC (H-Field Transanalyser, May20)
$2.50
- AD8495 thermocouple interface (DIY Reflow Oven Controller, Apr20)
$12.50
- Si8751AB 2.5kV isolated Mosfet driver IC (Charge Controller, Dec19)
$5.00
- I/O expander modules (Nov19):
PCA9685 – $6.00 ¦ PCF8574 – $3.00 ¦ MCP23017 – $3.00
- SMD 1206 LEDs, packets of 10 unless stated otherwise (Xmas Ornaments, Nov20):
yellow – $0.70 ¦ amber – $0.70 ¦ blue – $0.70 ¦ cyan – $1.00 ¦ pink (1 only) – $0.20
- ISD1820-based voice recorder / playback module (Junk Mail, Aug19)
$4.00
- 23LCV1024-I/P SRAM & MCP73831T (UHF Repeater, May19)
$11.50
- MCP1700 3.3V LDO regulator (suitable for USB M&K Adapator, Feb19)
$1.50
- 1nF 1% MKP (5mm) or ceramic capacitor (LC Meter, Jun18)
$2.50
- ESP-01 WiFi Module (El Cheapo Modules, Apr18)
$5.00
- DS3231 real-time clock module with mounting hardware
$7.50
*Prices valid for month of magazine issue only. All prices in Australian dollars and include GST where applicable. # P&P prices are within Australia. Overseas? Place an order on our website for a quote.
PRINTED CIRCUIT BOARDS & CASE PIECES
PRINTED CIRCUIT BOARD TO SUIT PROJECT
DAB+/FM/AM RADIO
↳ CASE PIECES (CLEAR)
REMOTE CONTROL DIMMER MAIN PCB
↳ MOUNTING PLATE
↳ EXTENSION PCB
USB MOUSE AND KEYBOARD ADAPTOR PCB
LOW-NOISE STEREO PREAMP MAIN PCB
↳ INPUT SELECTOR PCB
↳ PUSHBUTTON PCB
DIODE CURVE PLOTTER
↳ UB3 LID (MATTE BLACK)
FLIP-DOT (SET OF ALL FOUR PCBs)
↳ COIL PCB
↳ PIXEL PCB (16 PIXELS)
↳ FRAME PCB (8 FRAMES)
↳ DRIVER PCB
iCESTICK VGA ADAPTOR
UHF DATA REPEATER
AMPLIFIER BRIDGE ADAPTOR
3.5-INCH LCD ADAPTOR FOR ARDUINO
DSP CROSSOVER (ALL PCBs – TWO DACs)
↳ ADC PCB
↳ DAC PCB
↳ CPU PCB
↳ PSU PCB
↳ CONTROL PCB
↳ LCD ADAPTOR
STEERING WHEEL CONTROL IR ADAPTOR
GPS SPEEDO/CLOCK/VOLUME CONTROL
↳ CASE PIECES (MATTE BLACK)
RF SIGNAL GENERATOR
RASPBERRY PI SPEECH SYNTHESIS/AUDIO
BATTERY ISOLATOR CONTROL PCB
↳ MOSFET PCB (2oz)
MICROMITE LCD BACKPACK V3
CAR RADIO DIMMER ADAPTOR
PSEUDO-RANDOM NUMBER GENERATOR
4DoF SIMULATION SEAT CONTROLLER PCB
↳ HIGH-CURRENT H-BRIDGE MOTOR DRIVER
MICROMITE EXPLORE-28 (4-LAYERS)
SIX INPUT AUDIO SELECTOR MAIN PCB
↳ PUSHBUTTON PCB
ULTRABRITE LED DRIVER
HIGH RESOLUTION AUDIO MILLIVOLTMETER
PRECISION AUDIO SIGNAL AMPLIFIER
SUPER-9 FM RADIO PCB SET
↳ CASE PIECES & DIAL
TINY LED XMAS TREE (GREEN/RED/WHITE)
HIGH POWER LINEAR BENCH SUPPLY
↳ HEATSINK SPACER (BLACK)
DIGITAL PANEL METER / USB DISPLAY
↳ ACRYLIC BEZEL (BLACK)
UNIVERSAL BATTERY CHARGE CONTROLLER
BOOKSHELF SPEAKER PASSIVE CROSSOVER
↳ SUBWOOFER ACTIVE CROSSOVER
ARDUINO DCC BASE STATION
NUTUBE VALVE PREAMPLIFIER
TUNEABLE HF PREAMPLIFIER
4G REMOTE MONITORING STATION
LOW-DISTORTION DDS (SET OF 5 BOARDS)
NUTUBE GUITAR DISTORTION / OVERDRIVE PEDAL
THERMAL REGULATOR INTERFACE SHIELD
↳ PELTIER DRIVER SHIELD
DIY REFLOW OVEN CONTROLLER (SET OF 3 PCBS)
7-BAND MONO EQUALISER
↳ STEREO EQUALISER
REFERENCE SIGNAL DISTRIBUTOR
H-FIELD TRANSANALYSER
CAR ALTIMETER
RCL BOX RESISTOR BOARD
↳ CAPACITOR / INDUCTOR BOARD
ROADIES’ TEST GENERATOR SMD VERSION
↳ THROUGH-HOLE VERSION
DATE
JAN19
JAN19
FEB19
FEB19
FEB19
FEB19
MAR19
MAR19
MAR19
MAR19
MAR19
APR19
APR19
APR19
APR19
APR19
APR19
MAY19
MAY19
MAY19
MAY19
MAY19
MAY19
MAY19
MAY19
MAY19
MAY19
JUN19
JUN19
JUN19
JUN19
JUL19
JUL19
JUL19
AUG19
AUG19
AUG19
SEP19
SEP19
SEP19
SEP19
SEP19
SEP19
OCT19
OCT19
NOV19
NOV19
NOV19
NOV19
NOV19
NOV19
NOV19
DEC19
JAN20
JAN20
JAN20
JAN20
JAN20
FEB20
FEB20
MAR20
MAR20
MAR20
APR20
APR20
APR20
APR20
MAY20
MAY20
JUN20
JUN20
JUN20
JUN20
PCB CODE
Price
06112181
$15.00
SC4849
$.00
10111191
$10.00
10111192
$10.00
10111193
$10.00
24311181
$5.00
01111119
$25.00
01111112
$15.00
01111113
$5.00
04112181
$7.50
SC4927
$5.00
SC4950
$17.50
19111181
$5.00
19111182
$5.00
19111183
$5.00
19111184
$5.00
02103191
$2.50
15004191
$10.00
01105191
$5.00
24111181
$5.00
SC5023
$40.00
01106191
$7.50
01106192
$7.50
01106193
$5.00
01106194
$7.50
01106195
$5.00
01106196
$2.50
05105191
$5.00
01104191
$7.50
SC4987
$10.00
04106191
$15.00
01106191
$5.00
05106191
$7.50
05106192
$10.00
07106191
$7.50
05107191
$5.00
16106191
$5.00
11109191
$7.50
11109192
$2.50
07108191
$5.00
01110191
$7.50
01110192
$5.00
16109191
$2.50
04108191
$10.00
04107191
$5.00
06109181-5 $25.00
SC5166
$25.00
16111191
$2.50
18111181
$10.00
SC5168
$5.00
18111182
$2.50
SC5167
$2.50
14107191
$10.00
01101201
$10.00
01101202
$7.50
09207181
$5.00
01112191
$10.00
06110191
$2.50
27111191
$5.00
01106192-6 $20.00
01102201
$7.50
21109181
$5.00
21109182
$5.00
01106193/5/6 $12.50
01104201
$7.50
01104202
$7.50
CSE200103 $7.50
06102201
$10.00
05105201
$5.00
04104201
$7.50
04104202
$7.50
01005201
$2.50
01005202
$5.00
For a complete list, go to siliconchip.com.au/Shop/8
PRINTED CIRCUIT BOARD TO SUIT PROJECT
COLOUR MAXIMITE 2 PCB (BLUE)
↳ FRONT & REAR PANELS (BLACK)
OL’ TIMER II PCB (RED, BLUE OR BLACK)
↳ ACRYLIC CASE PIECES / SPACER (BLACK)
IR REMOTE CONTROL ASSISTANT PCB (JAYCAR)
↳ ALTRONICS VERSION
USB SUPERCODEC
↳ BALANCED ATTENUATOR
SWITCHMODE 78XX REPLACEMENT
WIDEBAND DIGITAL RF POWER METER
ULTRASONIC CLEANER MAIN PCB
↳ FRONT PANEL
NIGHT KEEPER LIGHTHOUSE
SHIRT POCKET AUDIO OSCILLATOR
↳ 8-PIN ATtiny PROGRAMMING ADAPTOR
D1 MINI LCD WIFI BACKPACK
FLEXIBLE DIGITAL LIGHTING CONTROLLER SLAVE
↳ FRONT PANEL (BLACK)
LED XMAS ORNAMENTS
30 LED STACKABLE STAR
↳ RGB VERSION (BLACK)
DIGITAL LIGHTING MICROMITE MASTER
↳ CP2102 ADAPTOR
BATTERY VINTAGE RADIO POWER SUPPLY
DUAL BATTERY LIFESAVER
DIGITAL LIGHTING CONTROLLER LED SLAVE
BK1198 AM/FM/SW RADIO
MINIHEART HEARTBEAT SIMULATOR
I’M BUSY GO AWAY (DOOR WARNING)
BATTERY MULTI LOGGER
ELECTRONIC WIND CHIMES
ARDUINO 0-14V POWER SUPPLY SHIELD
HIGH-CURRENT BATTERY BALANCER (4-LAYERS)
MINI ISOLATED SERIAL LINK
REFINED FULL-WAVE MOTOR SPEED CONTROLLER
DIGITAL FX UNIT PCB (POTENTIOMETER-BASED)
↳ SWITCH-BASED
ARDUINO MIDI SHIELD
↳ 8X8 TACTILE PUSHBUTTON SWITCH MATRIX
HYBRID LAB POWER SUPPLY CONTROL PCB
↳ REGULATOR PCB
VARIAC MAINS VOLTAGE REGULATION
ADVANCED GPS COMPUTER
PIC PROGRAMMING HELPER 8-PIN PCB
↳ 8/14/20-PIN PCB
ARCADE MINI PONG
Si473x FM/AM/SW DIGITAL RADIO
20A DC MOTOR SPEED CONTROLLER
MODEL RAILWAY LEVEL CROSSING
COLOUR MAXIMITE 2 GEN2 (4 LAYERS)
BATTERY MANAGER SWITCH MODULE
↳ I/O EXPANDER
NANO TV PONG
LINEAR MIDI KEYBOARD (8 KEYS) + 2 JOINERS
↳ JOINER ONLY (1pc)
TOUCHSCREEN DIGITAL PREAMP
↳ RIBBON CABLE / IR ADAPTOR
2-/3-WAY ACTIVE CROSSOVER
TELE-COM INTERCOM
SMD TEST TWEEZERS (3 PCB SET)
USB CABLE TESTER MAIN PCB
↳ FRONT PANEL (GREEN)
MODEL RAILWAY CARRIAGE LIGHTS
HUMMINGBIRD AMPLIFIER
DIGITAL LIGHTING CONTROLLER TRANSLATOR
SMD TRAINER
DATE
JUL20
JUL20
JUL20
JUL20
JUL20
JUL20
AUG20
NOV20
AUG20
AUG20
SEP20
SEP20
SEP20
SEP20
SEP20
OCT20
OCT20
OCT20
NOV20
NOV20
NOV20
NOV20
NOV20
DEC20
DEC20
DEC20
JAN21
JAN21
JAN21
FEB21
FEB21
FEB21
MAR21
MAR21
APR21
APR21
APR21
APR21
APR21
MAY21
MAY21
MAY21
JUN21
JUN21
JUN21
JUN21
JUL21
JUL21
JUL21
AUG21
AUG21
AUG21
AUG21
AUG21
AUG21
SEP21
SEP21
OCT21
OCT21
OCT21
NOV21
NOV21
NOV21
DEC21
DEC21
DEC21
PCB CODE
07107201
SC5500
19104201
SC5448
15005201
15005202
01106201
01106202
18105201
04106201
04105201
04105202
08110201
01110201
01110202
24106121
16110202
16110203
16111191-9
16109201
16109202
16110201
16110204
11111201
11111202
16110205
CSE200902A
01109201
16112201
11106201
23011201
18106201
14102211
24102211
10102211
01102211
01102212
23101211
23101212
18104211
18104212
10103211
05102211
24106211
24106212
08105211
CSE210301C
11006211
09108211
07108211
11104211
11104212
08105212
23101213
23101214
01103191
01103192
01109211
12110121
04106211/2
04108211
04108212
09109211
01111211
16110206
29106211
Price
$10.00
$10.00
$5.00
$7.50
$5.00
$5.00
$12.50
$7.50
$2.50
$5.00
$7.50
$5.00
$5.00
$2.50
$1.50
$5.00
$20.00
$20.00
$3.00
$12.50
$12.50
$5.00
$2.50
$7.50
$2.50
$5.00
$10.00
$5.00
$2.50
$5.00
$10.00
$5.00
$12.50
$2.50
$7.50
$7.50
$7.50
$5.00
$10.00
$10.00
$7.50
$7.50
$7.50
$5.00
$7.50
$35.00
$7.50
$7.50
$5.00
$15.00
$5.00
$2.50
$2.50
$5.00
$1.00
$12.50
$2.50
$15.00
$30.00
$10.00
$7.50
$5.00
$2.50
$5.00
$5.00
$5.00
8-LED METRONOME
10-LED METRONOME
REMOTE CONTROL RANGE EXTENDER UHF-TO-IR
↳ IR-TO-UHF
6-CHANNEL LOUDSPEAKER PROTECTOR
↳ 4-CHANNEL
JAN22
JAN22
JAN22
JAN22
JAN22
JAN22
23111211
23111212
15109211
15109212
01101221
01101222
$5.00
$7.50
$2.50
$2.50
$7.50
$5.00
NEW PCBs
We also sell an A2 Reactance Wallchart, RTV&H DVD, Vintage Radio DVD plus various books at siliconchip.com.au/Shop/3
ASK SILICON CHIP
Got a technical problem? Can’t understand a piece of jargon or some technical principle? Drop us a line
and we’ll answer your question. Send your email to silicon<at>siliconchip.com.au
Capacitor value in USB
Cable Tester kit
I received the USB Cable Tester
kit that I ordered and I noticed that
a 100μF 16V electrolytic capacitor
had been supplied, but no 10μF 16V
capacitor per the parts list. Also, I
have received a component marked
4P03L04, which I have confirmed is
suitable for Q3. This is my first (and
perhaps only) go at soldering SMDs,
so it would help if you could point me
to a previous issue of SC that has some
tips. (R. L. C., Shelly Beach, NSW)
● While the 10μF specified in the
article is the minimum required, we
tested a 100μF capacitor in the prototype and found that it worked fine. So
we supplied 100μF capacitors in the
kit as we already had them in stock.
There is quite a bit of information
on SMD soldering in the December
issue (which you would not have seen
yet based on the date of your email).
That includes the second USB Cable
Tester (constructional) article and also
a separate feature article in that issue
(siliconchip.com.au/Article/15138).
Electrolytic capacitors
work well for coupling
I am considering building the 2/3Way Stereo Active Crossover (October & November 2021; siliconchip.
com.au/Series/371) for a PA system.
I noticed that you are using low-ESR
electrolytic capacitors for signal coupling between sections of the design. I
thought that these caps were designed
for switch-mode power supplies, not
for use as coupling.
As I will be using a split supply,
should I be using bipolar caps instead?
(P. S., Mount Pleasant, SA)
● Regular electrolytic capacitors,
including low-ESR types, work well
for coupling audio as long as their
values are high enough. They’ve been
used for decades in mixing consoles,
amplifiers and just about all types of
audio equipment. Arguably, low-ESR
capacitors should do a better job than
108
Silicon Chip
standard electros since they are closer
to ideal capacitors.
We don’t believe bipolar/non-
polarised capacitors are needed for
this design when used with a split supply. Polarised capacitors can be used
without problems when the bias across
them is close to 0V or even slightly
negative (within a few hundred milli
volts of zero).
SMD Test Tweezers
questions
I recently received your SMD
Test Tweezers kit (siliconchip.com.
au/Shop/20/5934); thank you. As
described, it didn’t come with a cell
or brass tips.
What type of cell is needed? What is
the voltage required? Also, what type
of tip is used in the image? What is the
part called and where can I get it? (M.
G., Endeavour Hills, Vic)
● The battery is listed as a CR2032 or
CR2025 lithium button cell on p68 of
the article in the October 2021 issue.
These are nominally 3V.
The tip is a small piece cut from a
length of brass strip; these can usually be found in hobby stores (eg, the
type that sells model railway gear)
and will probably be sold in a 30cm
length from which you will need to cut
smaller pieces. The exact dimensions
are not critical.
An online search for “brass strip”
or “brass bar” should give you a start.
Note that round brass rod is also available, but we don’t recommend it as the
rounded surface will not grip the components as well as a flat strip.
R80 kit is different
from the one reviewed
Following your review about the
R80 aviation radio (November 2021;
siliconchip.com.au/Article/15101), I
downloaded the circuit etc from your
website and bought a kit from AliExpress. But the kit received is version 7,
and now I have a kit without a circuit
diagram which makes it very difficult!
Australia's electronics magazine
Do you know where to find a circuit
diagram for this newer version? (M.
T., Dodges Ferry, Tas)
● Andrew Woodfield responds: I was
as surprised as anyone to find the
recently released R80 V6 receiver kit
has undergone such an early, rapid
and substantial change into the new
version 7. Some internet suppliers still
appear to offer the kit reviewed in the
November issue, but some now offer
(or may deliver) the revised kit.
One reason for the changes may be
the inherent V6 squelch design fault.
Other reasons may include difficulties with component availability and
sharply increased costs for parts like
the MC3361 and TA7640 chips.
The new V7 design, which uses
a pair of widely used TA2003 AM/
FM receiver chips, almost certainly
resolves the availability and cost problems. I have not tested the performance
of the V7 squelch circuit, so I cannot
comment on its effectiveness on AM,
but from what I understand, it does
work better than the V6 squelch.
To help readers with V7 kits, I have
prepared a new English version of the
kit instructions and it is available for
download from siliconchip.com.au/
Shop/6/5950
Thanks to Silicon Chip reader Nigel
Dudley for his help with obtaining the
original Chinese V7 instructions.
Is Ultrasonic Cleaner
software correct?
I built the High Power Ultrasonic
Cleaner from the September & October 2021 issues (siliconchip.com.
au/Series/350) and found it behaved
incorrectly. I have gone through the
included source code and I believe
I have found the problem. I want to
confirm my findings with the author.
The software runs a self-calibration
routine on startup and saves the result
into non-volatile RAM. On the second
run, it retrieves this stored value so it
can proceed without having to rerun
the calibration. Unfortunately, the
author appears to have made an error
siliconchip.com.au
and it stores the data in the wrong register. This causes erratic behaviour on
second and subsequent runs.
The power data register declared
in address H0702 is actually saved to
address H0700, which was declared
as the OSCTUNE value.
I am having trouble getting the unit
to operate on its maximum power setting. Using a scope and DVM, I ran the
diagnostic program (holding both buttons on startup) and determined that
my transducer (while mounted to my
reservoir filled with 4L of water) resonates at 37.5kHz while producing a
reading of 4.3V on TP1.
Now when I run the unit (recompiled with the above address problem corrected), the unit steps down to
about the 50–75% mark and a corresponding 3.3V before locking in. Any
attempt to step it higher results in the
unit stepping down again. (B. V. D.,
via email)
● The code to write the power to flash
memory is correct. The power value is
not written to H0700. The OSCTUNE,
PR1 and Power values are written
as a block write with the OSCTUNE
value written first at H0700. The write
address is then incremented (“incf
PMADRL,f”) to H0701 and the PR2
value is written, then the address is
incremented again to H0702 and the
power value written.
Regarding your difficulty achieving
maximum power, when in diagnostic
mode, find the frequency range where
you can get a reading of 4.6V, try setting it to the next lower frequency and
perform calibration. If that is not effective, try setting the frequency range
when in diagnostic mode to the highest
frequency within the range that gives
the peak reading.
Alternatively, the transducer resonance point may not be being found
correctly. Try running the diagnostics
and sweeping the frequencies to find
the maximum current by measuring
the voltage at TP1. If this voltage goes
over the maximum allowable reading
of 4.8V, reduce the number of secondary turns on the transformer. It is critical that current overload isn’t reached
at resonance.
Replacement op amps
for the Digital FX Pedal
I decided to build the Digital FX
(Effects) Pedal published in the April &
May 2021 issues (siliconchip.com.au/
Series/361) but I am having difficulty
sourcing the OPA1662AID op amp IC.
Can I substitute an NJM4585 or another
op amp? (R. D. Z., Matara, Sri Lanka)
● We don’t suggest you substitute the
NJM4585 for OPA1662AID. The minimum supply rail specification for the
NJM4585 is ±4V (ie, a total of 8V),
whereas the OPA1662AID specifies
±1.5V (a total of 3V). This IC runs from
9-12V DC in the Digital FX Pedal, so
with the NJM4585, its swing will be
severely limited, probably to the point
that the unit doesn’t work.
There certainly are other op amps
that are suitable for this design but
you would need to choose one with
a similar supply specification to the
OPA1662AID as well as low noise and
distortion.
The OPA1662AID is certainly available; at the time of writing this, element14, RS, Digi-Key and Mouser all
have that part in stock.
Arduino Profile changes
broke some code
I wonder if you could help with a
problem I am experiencing with the
Arduino code for the Clayton’s GPS
Time Signal Generator (April 2018;
siliconchip.com.au/Article/11039).
Radio, Television & Hobbies: the COMPLETE archive on DVD
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Australia's electronics magazine
January 2022 109
When I try to compile it, I get an
error message at this line in the code:
http.begin(ipapi); //URL
The message is:
call to ‘HTTPClient::begin’
declared with attribute
error: obsolete API, use
::begin(WiFiClient, url)
When the project first came out in
April 2018, the source code compiled
perfectly. Do you know why it’s throwing an error now? (J. H., Nathan, Qld)
● There has been a major version
change of the ESP8266 Board Profile for the Arduino IDE, starting with
V3.0.0 in May this year. The release
notes at https://github.com/esp8266/
Arduino/releases show that quite a
few breaking changes have been introduced since then.
We tested our Clayton’s GPS sketch
with V2.7.4 of the ESP8266 Board Profile, the most recent version before
V3.0.0, and it compiles and works as
expected. So one possible solution is to
use this older version. You can install
it using the Select Version drop-down
menu in the Boards Manager.
We have updated the sketch to work
with the most current (V3.0.2) version. The new version of the sketch
is available from siliconchip.com.au/
Shop/6/4593 Only two lines needed to
be changed, and these are marked by
comments in the source code.
Getting Theremin
volume plate working
I bought a kit of the Theremin MkIII
(January 2018; siliconchip.com.au/
Article/10931) to build for my sisterin-law for her birthday. I have a rough
understanding of electronics and have
become quite good at soldering from
some previous projects (plus, my
father is an electronics technician, so
I’ve picked up some tips).
Unfortunately, after building the kit,
the volume plate does not seem to be
working. Moving my hand closer or
further away from the plate does not
change the volume, no matter how the
volume thumbwheel is set.
Sometimes there is a slight pitch
change when my hand is closest to
the plate (which could be because my
hand gets close to the antenna) and the
sound cuts out completely when my
hand touches the plate.
I’ve checked that all the components
110
Silicon Chip
are soldered correctly, in the correct
orientation, etc and everything seems
fine. The board and instructions make
it very clear which component goes
where and in which orientation when
they are polarised. The test point voltage readings are as follows:
TP 9V: 9.01V
TP 9V’: 8.77V
TP 9V’1’: 8.07V
TP 9V’2’: 8.16V
TP 9V’4’: 8.52V
TP1: 1.24V TP2: 0.62V
TP3: 1.17V TP4: 0.56V
TP5: 0.79V TP6: 0.2V
TP7: 1.08V TP8: 0.63V
TP9: 2.01-8.48V ● TP10: 5.14V
TP11: 5.78V TP12: 5.53V
● The highest voltage is when the
VC2 thumbwheel is turned anti-
clockwise (to the left when facing the
component side). I’m not sure if this is
normal, but when turning it clockwise,
it will drop to the lowest voltage, climb
to the highest voltage again, and then
drop back to the lowest and sit at that
setting for the last bit of turning. The
‘zero beat’ seems to be in the middle
of the thumbwheel tuning.
If there is anything you can suggest
that I can check, it would be greatly
appreciated. (C. S., Craigieburn, Vic)
● Your voltage readings look OK. Your
problem is most likely related to VC2.
Try adjusting the trimmers within variable capacitors VC1 and VC2 so that
the plates can mesh fully. The setting
of VC2 will be correct at one position only, and it is pretty sensitive,
so adjust it carefully and slowly. VC2
is not meant to operate over the full
VC2 range.
Adding balanced input
to Ultra-LD Mk.3 Amp
I would like to add balanced input
connectors to some Ultra-LD Mk.3
amplifier modules (July & August
2011; siliconchip.com.au/Series/286).
I have a number of these in use, and
it would be helpful for me to be able
to connect them to other equipment
using this method; I wouldn’t need
adaptors to change between RCAs
and XLRs.
Referring to the circuit diagram, can
I simply replace the unbalanced RCA
connector with an XLR by connecting pin 2 of the XLR (+ve pin) to the
47μF input decoupling capacitor and
pin 3 of the XLR (-ve, inverted signal)
to the junction of the 1MW and 10W
Australia's electronics magazine
resistors, ie, the bottom of the feedback divider? Pin 1 (shield or Earth)
of the XLR would connect directly to
the amplifier chassis.
Is this a valid option? Your advice
would be appreciated. I have already
replaced the 10W resistor with a 47W,
as suggested in your performance
tweaks article. (J. M., Auckland, NZ)
● Yes, the method you describe
should work well, except when using
long cable runs, when hum pickup
may become evident. For a true balanced input, use our project from June
2008: the Balanced/Unbalanced Converter for Audio Signals (siliconchip.
com.au/Article/1857).
This appears to still be available
as a kit from Altronics (Cat K5522),
although the stock level is low.
Alternatively, use a transformer-
based balanced isolator such as the
Jensen DM2-2XX or PB-2XX or similar isolators, and connect the balanced
output as you describe. That way, there
will be a genuine balanced connection
to the isolator and an unbalanced connection to the amplifier. Locate the
isolator close to the amplifier input.
Studio 350 amplifier
troubleshooting
I recently put together a Studio 350
amplifier (January & February 2004;
siliconchip.com.au/Series/97). I really
like the double-sided PCBs. I installed
it into an existing case with an inbuilt
power supply; it only has a 40-0-40V
transformer, but I stacked the two 15V
windings onto the 40V windings to get
±61V DC on a good day.
The power supply filter is two
8000μF caps per side, but I did add
the 470nF caps and 15kW resistors as
per the article.
Setup was a breeze. I hooked up my
dummy 4W load and got a really nice
sinewave out, delivering 270W due to
the reduced rails. It ran like that for
about half an hour just fine.
Now comes the rub. I switched the
signal generator from 1kHz to 1.2kHz
and promptly destroyed all the output devices, total short circuit E-CB. Q8 and Q9 both survived and are
functional.
Now confession time, I had failed to
connect the mains Earth to the centre-
tap Earth of the power supply. The
whole amp was floating with no reference to Earth at all. I know, not good
continued on page 112
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siliconchip.com.au
Australia's electronics magazine
January 2022 111
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and a complete oversight on my part.
My question is, could this have been
the cause for all the output devices to
self-destruct? I have since connected
the Earth wire from the mains socket
to the power supply.
I think that, as the amp worked well
during my initial testing, it probably
doesn’t have any incorrectly placed
components or dry solder joints. I was
very meticulous in the soldering and
placing of components. Do you know
what might have gone wrong? (P. S.,
Mount Pleasant, SA)
● It is possible that not having the
mains Earth to the amplifier could
have caused the destruction, but it
seems a bit unlikely.
Have you checked what happens to
the output from the signal generator
when switching frequency? Does the
output initially clip on one half of the
cycle that could cause the amplifier
to have a DC offset for a short period,
which could cause an overload that
destroys the transistors? There is AC
coupling on the amplifier input, but it
may not be enough to save the amplifier if that happens.
You could check what happens
with no load on the amplifier, as that
shouldn’t cause the amplifier to blow
even if there is a significant DC pulse.
Modern car radio
antennas aren’t good
I have a 2018 Volkswagen with a
short 20cm roof-mounted aerial and
the radio is full of hash when driving
near railways and power lines. Is there
a better replacement aerial or accessory to improve reception? Would ferrite rings over the aerial make a difference? (M. P., Croydon, Vic)
● The problem is probably due to
Notes & Errata
SMD Trainer, December 2021: The parts list and kit for the SMD Trainer Board only
lists two 100nF capacitors when three are shown on the schematic and PCB. The
kit has been updated, but those who have already received kits should note that
the circuit will most likely work correctly without the 100nF capacitor below IC2.
Hummingbird Amplifier Module, December 2021: in Fig.7 on p23, the “E” & “B”
labels for Q12 have been swapped. In the body text of p23, MLJ15032/33 should
read MJE15032/33.
Pocket Weather Station, November 2021: in Fig.2 the DAT connection from the
DHT11 should connect to pin D4 of the Arduino Nano, not D5.
The February 2022 issue is due on sale in newsagents by Thursday, January
27th. Expect postal delivery of subscription copies in Australia between January
26th and February 11th.
112
Silicon Chip
Australia's electronics magazine
low-amplitude radio signals making their way to the radio’s antenna
input. This could be due to bad connections, especially if you live near
the sea. Make sure that all connections from the antenna to the radio
are clean and undamaged. This would
require removing the radio to check
the antenna connection at the rear and
also removing the antenna.
Any ferrite ring over the antenna
would likely reduce the antenna radio
reception and detune the antenna.
Alternatively, there may be a noise
source in the car itself. The ignition
can be the source of radio-frequency
(RF) noise with petrol engines,
although that is less of a problem
these days with plug-on-coil systems
that eliminate the spark plug leads.
The alternator could also cause noise
if the brushes are worn. Have those
aspects checked out if the problem
persists.
Unfortunately, most modern vehicles simply don’t have very good radio
reception because consumers don’t
want ugly, long aerials sticking out
of their cars. Many cars either have
a small ‘shark-fin’ antenna like yours
or use the rear demister element as
an antenna. Neither is all that great of
an antenna.
If you don’t care about the appearance, you could consider having a flexible whip-style antenna mounted adjacent to the bonnet or on the door frame.
Find a good installer who will route
the antenna wire neatly and take measures to prevent rusting, or you could
mount it yourself if you’re confident.
Identifying a
Silicon Chip PCB
I came across a circuit board
recently. I believe that it is a Silicon
Chip design and would be grateful if
you could tell me what it is used for.
The board has the label “SC 11410971
LIGHTS” on it. (G. H., Camden, NSW)
● You can look up PCB numbers on
our website at siliconchip.com.au/
Articles/ContentsSearch
Simply type the PCB code into
the “Kits / PCBs” field and click the
“Search” button. Searching for that
PCB number gives the following result:
October 1997: The Flickering Flame
For Stage Work (siliconchip.com.au/
Article/4790) by Ross Tester, kits:
Jaycar KC5234, PCBs: SC 11410971,
1 shop item
SC
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