This is only a preview of the November 2022 issue of Silicon Chip. You can view 43 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. Items relevant to "Christmas LED Icicle Decoration":
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Items relevant to "DC Supply Transient Filter":
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NOVEMBER 2022
ISSN 1030-2662
11
9 771030 266001
The VERY BEST DIY Projects!
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28 | Tiny LED Icicle
The perfect decoration for this Christmas
4 1 | LC Meter Mk3
An update to a crucial workbench tool
49 | Transient DC Supply Filter
Protect your devices from harm
62 | Active Monitor Speakers
A high-end sound system for your home
All About Torches
the history of the hand-held light
siliconchip.com.au
Australia's electronics magazine
November 2022 1
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Contents
Vol.35, No.11
November 2022
14 The Technology of Torches
Page 41
Illumination has always been an important technology for humans,
especially in a portable form for nighttime use. Once a stick with a fire on
the end, modern torches are increasingly smaller and more powerful.
By Dr David Maddison
Handheld lighting feature
56 Raspberry Pi Pico W
The Pico W is the newest Raspberry Pi module which now incorporates
WiFi functionality, all for only a few dollars more!
By Tim Blythman
Microcontroller module review
LC Meter Mk3
Raspberry Pi
76 WiFi-Synchronised Analog Clock Pico W
If you can’t get reliable GPS signals, you can adapt the GPS-Synchronised
Analog Clock (Sept 2022) to use a D1 Mini module to track time via WiFi.
By Geoff Graham
Timekeeping feature
78 Particulate Matter (PM) Sensors
In the last article of this series on air quality sensors, we take a closer look
at PM2.5 sensors, also called “dust” or “smoke” sensors.
By Jim Rowe
Using electronic modules
Page 56
Page 62
28 Christmas LED Icicle Decoration
This Tiny LED Icicle is simple to build with just a few components. It’s easy
to join multiple together, making for a great holiday decoration.
By Tim Blythman
Christmas decoration project
41 LC Meter Mk3
This modernised LC Meter measures a wide range of capacitances from
1pF to more than 1200pF with 0.1pF resolution, and inductances from
100nH to 2.5mH. It uses three AA cells and has a battery life of ~72 hours.
By Charles Kosina
Test & measurement project
49 Transient DC Supply Filter
This 12V DC Supply Filter helps prevent voltage spikes ruining your devices
or supply noise messing with their performance. It can handle up to 5A (or
10A with different inductors), and fits in a compact UB5 Jiffy box.
By John Clarke
Power conditioning project
62 Active Monitor Speakers, Part 1
These high-quality Active Monitor Speakers create a superlative sound
system to complement your living room. High-end Satori drivers are used
throughout the project and can be combined with an optional subwoofer.
By Phil Prosser
Audio project
90 30V 2A Bench Supply, Part 2
To finish our new Bench Supply, we cover the construction details with extra
attention to the mains wiring, testing and calibration procedures.
By John Clarke
Bench supply project
Active Monitor Speakers
with optional subwoofer
2
Editorial Viewpoint
4
Mailbag
30
Circuit Notebook
84
Vintage Radio
88
Online Shop
1. Digital preamp with tone controls
2. ESP32-Camera sentry
with object detection
Philips Minstrel radios by
Assoc. Prof. Graham Parslow
100
Serviceman’s Log
108
Ask Silicon Chip
111
Market Centre
112
Advertising Index
112
Notes & Errata
SILICON
SILIC
CHIP
www.siliconchip.com.au
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Nicholas Vinen
Technical Editor
John Clarke – B.E.(Elec.)
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Silicon Chip
Editorial Viewpoint
Close-up vision: use it or lose it
Like most people, as I am getting older, I have
noticed that it’s becoming harder to focus on tiny
objects close to my face. However, I think this has to
do with more than just age.
These days, due to my editorial duties, I spend a
lot more time editing documents on the computer,
answering e-mails and so on, and less time building
PCBs and such. That means my vision is fixed at the
same distance of around 30-50cm for much of the day.
When I recently managed to get far enough ahead in my editing duties to
work on some projects, I struggled working with parts that I had no difficulty
with just a few years ago. But I noticed that over time, as I did more soldering
and assembly work, much of my good close-up vision started to come back,
and I was suffering less from eye strain and such.
One of the reasons our vision deteriorates as we age is that the flexible
lens in our eyes becomes less elastic over time, making it harder to focus on
objects closer to our faces. But I wonder if that is accelerated if we are not
using our close-up vision enough.
I also suspect that the muscles that change the shape of the lens will weaken
if they are not used, leading at the very least to increased eye strain when
working with small objects or reading small type.
Regardless of the mechanism, I think you are more likely to keep your
close-up vision if you use it regularly. Having said that, it probably isn’t
great to use it too much, either. We need to spend some time looking into the
distance every day too, and many hours spent working with tiny details are
likely to result in eye strain and headaches at the end of the day.
Competition resulting in innovation
It looks like the CPU market is heating up again (quite literally in some
senses). After seemingly almost a decade of stagnation, AMD and Intel are
finally working hard to leapfrog each other. The just-released Ryzen 7000
series runs at impressively high frequencies, up to around 6GHz in stock
form, compared to around 5GHz for the previous generation AMD parts and
current Intel CPUs.
That frequency jump primarily comes down to the process node shrinking
from 7nm in the previous generation to 5nm in the current generation (see
our articles on IC Fabrication Technology in the June-August 2022 issues for
details: siliconchip.au/Series/382).
Along with efficiency improvements, the result is an approximately 30%
improvement in single-threaded performance. That’s similar to the previous
generation’s gain, so we’ve seen computer speeds jump nearly 70% in just
a couple of years.
Parallel processing users won’t be disappointed either, with the flagship
AMD CPU (Ryzen 7950X) beating the Intel i9-12900K by 42%.
And now, just after I wrote that, Intel announced their 13th-generation
parts (that we knew were coming). They are certainly an improvement over
the 12th-generation, increasing both the core count and maximum operating
frequencies. But it looks like AMD is still in the lead in many workloads, at
least for now, as Intel have not changed their node so radically.
We don’t want the situation we had for most of the last decade where AMD
was down (but not quite out), and Intel had no real competition. They would
bring out a new generation of CPUs now and then with modest improvements,
but it didn’t seem like they were really trying that hard. That laziness has
cost them their technology lead, and now they are scrambling to catch up.
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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 has 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”.
Silicon Chip magazine giveaway
I have about 20 years or more of Silicon Chip magazines
and I need to start clearing out my stuff, for any readers
who would find them useful.
Bruce Dunlop, Ashburton, Vic.
Comment: if you’re interested, send an e-mail to silicon<at>
siliconchip.com.au and we’ll pass it on to Bruce.
More on the topic of video displays
I found the articles on Video Display Technologies
(September & October 2022; siliconchip.au/Series/387)
interesting. I wonder if anyone remembers that in 1954
the French company Laboratoires Derveaux developed a
spiral scan television system that significantly reduced
the flyback time by simply having one long spiral line
per frame!
It was roughly equivalent to 600 linear scan lines, but of
course, the resolution was highest at the centre and progressively degraded towards the edges. The system was
described in the January 1955 issue of Wireless World.
Graham Lill, Lindisfarne, Tas.
Spectral Sound project is working well
I wrote to you a while ago asking for help getting the
Spectral Sound MIDI Synthesiser project working (June
2022; siliconchip.au/Article/15338). One of the things
that threw me off was the orientation of diode D2 being
shown incorrectly in Fig.9, but your erratum in the August
issue allowed me to fix that. After some more fiddling, I
finally got it all working.
I have had a fair amount of correspondence with Jeremy Leach (thanks for putting me in touch), and it has
taken quite a bit of effort. One of the problems was with
the way I was interfacing my keyboard to the synth. Purchasing a small MIDI controller and comparing voltages
allowed me to sort that out. There was no issue with the
optocoupler in the end, as I thought early on.
We ran a few tests on the mixer micro and verified that
it was working. Jeremy gave me a new build of the firmware (which should have been identical to the one you
supplied), and many things started working better. I also
reprogrammed the tone generator chips using firmware I
got from him (which should be identical to the one you
supplied), and it is now all working.
I am very happy with the result and will work with
Jeremy to enhance this project further, mainly focusing
on using signal processing for creating models of new
instruments from captured audio. Thanks for your help.
By the way, if anyone wants to modify the Spectral
Sound code, it’s vital to use the Microchip XC16 compiler
4
Silicon Chip
for programming the Mixer (and Tone Processors) to get
level 3 optimisations. These chips perform time-critical
tasks, so optimisation is extremely important. Trying to
use the free XC8 compiler just doesn’t work because the
compiled code won’t run fast enough.
Dan Amos, Macquarie Fields, NSW.
DIY TV sets from the 1950s
David Maddison’s articles on
Display Technology brought to
mind some of my distant past
(siliconchip.au/Series/387).
In the late 1950s, I built a TV
set described in Radio, TV &
Hobbies magazine using a 5BP1
(at school in “Leaving”, or year
11 in today’s vernacular). Here
is a picture of the 5BP1s that I
bought from Waltham’s in Melbourne. I believe they were from
WW2 radar sets.
Geoff Champion, Mount Dandenong, Vic.
Solution for unreliable motion-triggered switch
Back in February 2019, Silicon Chip published an article about a small vibration-triggered switch (siliconchip.
au/Article/11410) that overcame the problem of permanently powered accessory sockets in cars that might allow
a battery to be flattened by an accessory being left on. The
switch turned off the power after a suitable delay if no
motion was detected, ie, the car had stopped.
The idea appealed to me as I had a car with this exact
feature (problem!). I ordered a kit from Silicon Chip and
duly built one but could never get it to work reliably. I
often returned to the car to find that the amateur transceiver it powered was still on.
Fast forward to 2022 and a new car with the same problem – unswitched accessory outlets! I decided to revisit
your design and try again with a new kit, as I wanted to
switch a low-power navigation device. However, I had the
same problem: an unreliable switch-off. Even after purchasing new vibration sensors and very carefully installing them, in case I had done some damage to the originals, the problem persisted.
Measurement of the voltage at the negative end of
the 47µF capacitors to ground showed the correct 12V
decreasing to less than 1V over the time-out period, at
which point the circuit turned off.
However, now and then, the voltage did not drop and
stubbornly stayed at 12V. A good thump of the board and
Australia's electronics magazine
siliconchip.com.au
the voltage would decrease, and the circuit turned off
after the time delay.
The sensor data sheet shows the contacts are rated
at 20mA, and my thought is that the contacts were
micro-welding themselves closed with the instantaneous
short circuit current from the 47µF capacitors.
I placed a 100Ω resistor in series with the contacts to
limit the peak current, which has, so far, resulted in reliable operation of the switch. I tried using 680Ω as that
would limit the current to the 20mA specification but the
value was too high to properly discharge the capacitor,
resulting in a shorter turn-off delay.
I am not aware of any updates or errata for this project.
Any thoughts? Thanks for a great magazine.
Nigel Dudley, Ocean Beach, WA.
Response: we think your diagnosis is spot on. We noticed
that the prototypes would occasionally not switch off, but
we thought it must have been due to the vibration sensor
being damaged in testing. As you describe, we now realise
that it was almost certainly contact welding. Your solution of inserting a series resistance is probably the simplest fix. Thank you for doing the work to figure this out.
An alternative source for switch caps
Regarding the WiFi DC Load project in September and
October 2022 issues (siliconchip.au/Series/388), I found
it somewhat difficult to procure the switch caps for the
four pushbuttons on the control board.
The switches are easy to obtain from Altronics or Jaycar,
but when I went to order the caps, Altronics had no stock in
any colour, and Jaycar doesn’t have anything suitable either.
I found a compatible product, Omron B32-16x0. It is
available in ivory, black, orange or yellow (1600, 1610,
1620, 1630). They are sold by the usual suspects (element14, RS, Mouser and Digi-Key) and some are in stock
in Australia. I thought this information would be worth
sharing with your readers.
Erwin Bejsta, Wodonga, Vic.
Fraud warning for too-cheap SSDs
I am writing to inform you and your readers about an
online SSD scam. One AliExpress vendor alone, “SSD
HDD Wholesale Store”, has taken 3941 orders selling
‘multi-TB hard drives’ for pennies. Other stores have sold
many thousands more. Now vendors are advertising up
to 30TB drives for less than US$30. The feedback appears
to show many happy customers.
The drives show up on the operating system as a bunch
of 2TB drives. In my case, four of them for an 8TB drive.
You can write 2TB to each one. It will take around one
whole day to write 2TB. Just don’t expect the data to be
there when you read it. It won’t.
It uses a USB 3.0 socket, but the control chips report
they are USB 2.0. The write speed is around 6MB/s. It
writes in small bursts with a long delay between each
write. Presumably, this is so you will send good feedback
for your apparently good purchase. 66% of the feedback
is 5 stars, while almost 20% is 1 star.
The actual memory chip, as reported by an SSD formatter, is either a 32GB or 64GB device. My 8TB drive
had a mix. While this might be a good size for a thumb
drive, it is less than 1% of what you expect. These drives
have been faked.
6
Silicon Chip
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Silicon Chip
There is no point asking for your money back. It would
not be good PR for AliExpress to make so many refunds;
they must think it’s best to ignore the situation and keep
up the revenue.
The store mentioned above seems to have no other
products for sale. It has only been operating since Feb 23,
2022. The vendor has now sold out. It looks like it was set
just for this scam. These drives are still being advertised
on many other platforms: eBay, Amazon and Alibaba etc.
If it seems too good to be true, it is too good to be true.
I was lulled into a false sense of security by the positive
feedback and the fact that so many vendors were selling
these drives.
The control card reader I used is “ChipGenius_
v4_19_0319.exe”. It tells you everything available to your
operating system, except that the capacity is the real one.
The SSD formatter sizes and formats the SSD memory chip itself. I used “FirstChip_MpTools_20200430_
FC1178_FC1179”. This is published by the control card
manufacturer. Leave the password for Settings blank.
Robin Fleet, Rockingham, WA
Running 3-phase equipment from single-phase mains
Regarding Andre Rousseau’s comment about running
three-phase motors from single-phase AC (August 2022,
page 12), I can confirm that the capacitor phase shift
method does indeed work, probably somewhat better
than you’d expect.
About 40 years ago, a garage mechanic asked me if I
knew any way to test some old three-phase machines he’d
just bought, basically for scrap value. He just wanted to
know if they were still electrically workable, if the bearings were OK and so on, to see if it was worth paying to
have three-phase power installed.
Starting with the bench grinder, I hooked up Active and
Neutral to two of the phases and connected (from memory)
a 6.5µF motor start capacitor to the other phase. I put it
on a Variac, slowly cranked it up, and away it went. Not
only did that confirm it was electrically and mechanically
sound, but it seemed to be perfectly serviceable just like
that! It wasn’t getting hot or showing any signs of distress.
I subsequently hooked up the drill press, lathe and air
compressor the same way, using larger capacitors. Holding a piece of hardwood against the chucks of the drill
and lathe showed they still had plenty of torque. The
compressor seemed to take a bit longer to fill the tank
than we expected, but other than that, it was fine as well.
He never actually got around to installing three-phase
power; for his purposes, they were more than good enough
as they were!
Regarding Bruce Bowman’s letter about water-cooled
amplifiers (August 2022, page 10), I remember reading
in the 1940 edition of Donald Fink’s Principles of Television Engineering how the first generations of VHF TV
transmitters used water-cooled triodes.
The water was pumped into the anode heatsinks via
copper tubes that also served as part of the transmission
line to the antenna. Certain points on a transmission line
are at zero RF voltage; one of those was where the cooling
water was inserted and extracted.
The best they could do then was about 12% efficiency at
50MHz, and the preferred option was to use a temperature-
compensated LC oscillator to drive the output valves!
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November 2022 9
Crystal-based harmonic generators were extremely difficult to design for those frequencies, at least using 1930sera components. Water-cooled CPU and GPU cards for
computers are also ‘a thing’.
Keith Walters, Riverstone, NSW.
A different take on active crossovers
I note the new 2/3-Way Stereo Crossover in the October
issue (siliconchip.com.au/Series/371). A new version of
the fully variable unit from a couple of years ago, more
suited to experimental applications, is a good idea.
It would seem to me that when employing active crossovers, they are best used in a modular manner with amplifiers at the speaker unit, requiring only two cables and
giving optimum performance. Therefore, a single-channel
PCB would be preferable. Each speaker unit can be calibrated using a simple sound level meter and signal source.
From my experience, only a two-amplifier system is
needed, one driving the power-hungry woofer and the
other driving a conventional crossover for the midrange
and tweeter. It also allows a woofer to be simply added
to a quality bookshelf system, increasing performance.
The main application which would definitely require
the current unit is when a single subwoofer is used. Technically, this is a generic domestic trade name for an LFE
(low-frequency effects) speaker for one of the cinema-
based surround sound formats. The LFE is an entirely
separate channel with a theoretical bandwidth of DC to
120Hz at +10dB to the main channels.
LFE is used for audio support and creativity at the
discretion of the movie directors/sound engineers. It is
entirely separate from the main audio field, where each
channel has a theoretical bandwidth of DC to 20kHz and
are not meant to carry LFE. You can find a PDF of the
entire history of LFE on the Dolby Laboratories website.
The main channel speakers (all five in a 5.1 system,
where the .1 is the LFE) are usually full-spectrum threeway drivers, although I think there are very expensive
units that are two-way drivers. The Silicon Chip Senator
speakers (May-June 2016; siliconchip.com.au/Series/300)
also fall into this latter class, and might benefit from an
active crossover treatment.
Kelvin Jones, Kingston, Tas.
Extra generator capacity needed for motor starting
I was intrigued by the questions raised by George Ramsay in the Mailbag section of the July 2022 issue (pages
8 & 10). I have wondered about ‘pure’ sinewave output
compared to ‘modified’; at what point does a switchmode
power supply give up in trying to get the selected voltage
from the modified waveform available?
Now to the real question regarding getting a refrigerator up and running from a ‘genset’ power source. I have
a Petters diesel-powered 4kVA genset. It uses about 1L/h
at 3kVA output.
Older electric motors were pretty easy to start as they
only required a small amount of power to get them going
(for instance, my oldish chest freezer and my old fridge/
freezer, now deceased). My replacement fridge/freezer
won’t even consider starting. Questions to those in the
know about these matters suggest I may need 8-10kVA
output to have enough capacity to start it.
As a case in point, my neighbour recently got skittled
10
Silicon Chip
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by a long-term power outage but needed an instant genset
to get his farm water supply up and running. Stock aren’t
happy about being thirsty. Since he was using a 1.7kVA
pump, he was advised that he would need a genset with
an output of 10-12kVA to get reliable starting. He got one,
and it works well. On that happy note, I leave you.
John Hardisty, Tewkesbury, UK.
Comment: a possible ‘rule of thumb’ is that a motor starting on-load like a compressor or pump needs about ten
times its rated power initially, and can draw more than
its rated power until it gets up to speed, which can take
a second or two. Generators can typically handle a small
short-term overload, so your suggested ratio of 6-7 times
rated power is a reasonable compromise between cost
and capacity.
Kind reader offering up his spare punctuation!
I want to say how much I’m enjoying Silicon Chip these
days, especially Leo’s articles about the magazine’s history
(August & September 2022; siliconchip.au/Series/385). I
was fascinated to finally know how it all happened. I may
be one of your longest readers, being 75 and having been
a reader of RTV&H, then EA and all the other mags since
very early 1960 when my father bought me my first copy.
Around 1967, I wrote a paper letter to EA saying it was
the only magazine I read which lacked a Letters to the
Editor section. Voila, the following month, the Letters
section started. I’m not sure if my letter caused it, but I
like to think it was.
I started my career in broadcast TV engineering in 1966,
so the recent articles on video recording were of great
interest. I specialised in videotape and audio (and a lot
else) at a Perth commercial TV station.
The idea that high-definition video and audio can now
be recorded on a tiny SD card with no moving parts at
such low cost boggles my mind, considering the mechanical and electronic complexity of the machines I worked
on. I clearly remember at an Ampex course being told that
ordinary 625 line PAL required 270Mb/s, and that was
impossible, so forget it. So much for that.
I’m noticing the small changes you’re making and I
strongly approve. I’m also noticing the degree letters after
the names of many of your staff members. Congratulations.
Although I moved to Perth, I visited Sydney many times.
I wish I’d known, as I drove along Bassett St Mona Vale
to my relatives’ house nearby, that your offices were there
as I might have called in to say hello.
Finally, I’m including a supply of !!!...!!! as you may be
running short. Just ask, and I’ll send more!!!!!!
Peter Croft, Butler, WA.
DH30 MAX review feedback
I was bemused by your article on the shortcomings of
the DH30 MAX battery welder in the August 2022 issue
(siliconchip.au/Article/15427). I am reminded of a definition from the 1980s:
Marketing engineer: someone who takes a prototype,
pulls out components one by one until it fails, then
replaces the last one and signs off on it as plainly those
other components were redundant and a waste of money.
It certainly seems that’s what happened in this case.
SC
Dave Horsfall, North Gosford, NSW.
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12
Silicon Chip
Australia's electronics magazine
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Save time
All About Torches
By Dr David Maddison
Illumination so we can be active beyond daylight hours has always been an important
technology. On foot, that usually means a torch. Once a stick with a fire on the
end, modern torches (known elsewhere as “flashlights”) are almost always batterypowered.
Image source: https://unsplash.com/photos/YK8Mvocj6yE
P
can also be gas
or liquid-fuelled lanterns, or
even chemical “glow sticks”
that use chemiluminescence to create light. But this article will focus on
electric torches.
Until the introduction of LEDs,
torches mainly used incandescent
bulbs. Various types were available,
described below.
Batteries used were typically based
on carbon-zinc 1.5V cells or, in later
times, alkaline cells or nicad/NiMH
rechargeables. By the time lithium-ion
rechargeable batteries became commonly available, LEDs were the dominant lighting source.
Some LED torches support
multi-voltage operation, for example,
being powered by a single AA alkaline
cell at 1.5V or a 3.7V Li-ion rechargeable 14500 (same size as AA) cell. But
that only works if the torch electronics
are designed to handle the wide range
of voltages.
ortable lights
Origin of the term “flashlight”
In the UK and its former colonies,
we use the term “torch”, but in
the USA and Canada, the term is
14
Silicon Chip
“flashlight”. The word “flash-light”
predates the invention of battery-
powered devices. It appeared in 1892
but referred to flash photography,
where the flash came from chemicals.
The Flashlight Museum (www.
wordcraft.net/flashlight.html) says
that the origin relates to early torches
that had weak carbon-filament lamps
and weak, low-powered cells with no
switch to keep them on permanently,
as extended operation would quickly
drain the cells. The cells needed to
‘recover’ between uses.
Electrical contact was made by
pressing a spring-loaded contact to
Fig.1: an “Ever Ready”
flashlight from 1899.
Note the momentary
switch in the
middle, hence
“flashlight”.
complete the circuit; hence, the light
would flash.
The first torch
As we noted in our article All About
Batteries (January 2022; siliconchip.
com.au/Series/375), the D cell was
invented in 1896 (and it’s still available today!). It was a dry cell; as there
were no liquids to spill, it was suitable
for portable use in any orientation.
While not the first dry cell, it was the
first that was mass-produced and led
to the torch’s development.
The first torch patent was assigned
to British inventor David Missell who
obtained US Patent 617,592 in 1899
(https://patents.google.com/patent/
US617592A/en and Figs.1 & 2). It
used three D cells in a cardboard
tube with a brass reflector and a carbon filament bulb.
Some were donated to the New
York City police, who liked them,
but the torch was not generally popular because the batteries had a low
capacity and the carbon filament bulb
was not efficient or bright. At the time,
torches were considered an expensive
novelty.
siliconchip.com.au
Torches did not become popular
until the development of the tungsten filament bulb (three times the
efficiency of a carbon filament) in
1904 and the development of better
batteries.
By 1922, there were an estimated
10 million torch users in the United
States. A range of devices was available, including tubular designs, lantern styles that could be set down,
small pocket-size devices and large
lights suitable for long-range use –
see Fig.2.
The first LED torch
Who made the first LED torch is discussed in detail at siliconchip.au/link/
abfm – in summary:
• Rockwell gave out promotional
LED torches in the late 1970s to early
1980s
• Edmund Scientific made a yellow
LED torch in the late 1970s
• Tekna made a red LED torch
around 1980
• HDS Systems in Tucson, Arizona,
USA made a torch with multiple LEDs
in 1997 or 1998.
• Arc Flashlight LLC (website –
www.arcflashlight.com) was the first
to sell high-power Luxeon Star LED
torches around 2001 with the Arc LS
model (see Fig.3). It was the first LED
torch to rival incandescent torches.
The company was in business from
2001 to 2004.
Torch configurations
The key elements of a torch are:
1) a light source and, if applicable, a
reflector, lens and heatsink
2) driving electronics if the torch is
not a direct-drive type
3) a battery
4) a switch
Various other hardware is associated with the entire torch assembly,
such as o-rings, clips, etc. Apart from
the archetypal handheld model, traditionally about the diameter of a D cell,
there are (continued overleaf):
Fig.3: the first commercial LED torch
(the Arc LS) that was competetive
with incandescent torches.
siliconchip.com.au
Fig.2: early torches from the 25th MESCO (Manhattan Electrical Supply Co)
catalog, circa 1910.
Personal recollections on torches
One of my earliest recollections of torches was my father walking me to a
Cub Scout meeting through a dark park with a 3LR12 4.5V-battery powered
light (see photo). They were often used on bicycles at the time but were easily
removable for general use.
Another time, I ascended Mt
Bogong in Victoria and arrived at
the campsite at night. I had decent
lighting, but my walking companion
had an inadequate incandescent
torch powered by two AA cells which
seemed nearly flat.
That taught me several lessons:
the importance of having at least one
form of backup lighting and spare
batteries when in the bush, and the
extreme difficulty of setting up camp
on a dark night without adequate
lighting. Fortunately, having sufficient A vintage bicycle torch powered by
lighting is rarely a problem these days a 3LR12 4.5V battery. By today’s
with the ready availability, low cost, standards, the light was dim and
low weight and high performance of battery life short, but they were still
popular, especially for bicycles.
LED lights.
Australia's electronics magazine
November 2022 15
• headlamps for applications such
as caving or working hands-free
• ‘lanterns’ designed to sit on a flat
surface or hang from something to illuminate an area
• torches with different light
colours such as red to preserve night
vision function for the military, hunters or astronomers
• keychain lights
• hand-cranked torches with a
built-in generator for emergency applications
• firearm mounted lights for hunters, law enforcement or the military
• torches for scuba diving
• lights for hazardous areas such as
mines that are designed not to be an
ignition source
• inspection lights, with the light
on a flexible mounting
• infrared torches for use with night
vision equipment
• ‘shaker lights’, novelty items that
produce light when shaken via a moving magnet (some are fake and have
internal batteries)
Apart from all those, most modern
phones have a torch function.
Light Sources
In addition to incandescent globes
and LEDs, there are other light sources
such as HID lamps (high-intensity discharge, less common now due to the
availability of high-power LEDs) and
the emerging technology of “laser”
torches that use an LEP or laser-
excited phosphor (siliconchip.au/
link/abfn).
Incandescent bulbs
Incandescent torch bulbs are mostly
obsolete now but are still available.
They are mainly defined by their
Fig.4: a P13.5S base torch bulb, in this
case, a Satco S6923 (0.63W, 2.33V). It
has a “B3 1/2” shape, a C2-R filament
and a rated life of 10 hours.
16
Silicon Chip
Battery Warnings
Lithium-ion batteries contain a lot of energy and can be hazardous.
Also, keep button and coin cells away from children and animals as they are
hazardous if swallowed.
voltage rating, power rating, base configuration, glass bulb shape, gas filling
and whether they flash (rare). Some
bulbs are manufactured with LEDs as
direct replacements for conventional
incandescent globes.
Incandescent bulbs can be small,
or large sealed-beam units as used on
older-style car headlights (eg, as used
in the Big Jim torches, described later).
Some higher-performance bulbs
are filled with xenon or krypton gas,
reducing the tendency of the tungsten
filament to evaporate and allowing it
to run at a higher temperature, making
it brighter and more efficient.
Halogen globes are filled with inert
gas and a halogen substance such as
iodine or bromine. A chemical reaction causes evaporated tungsten to be
redeposited on the filament.
Incandescent bulbs and LED bulbs
that replace them (when made) are
available in various base types. For
each base type, various voltage and
power ranges are available. Some common types include:
ANSI P13.5S
Also known as single contact (SC)
miniature flange base (see Fig.4), this
bulb has a flange with a maximum
diameter of 13.5mm. The maximum
distance from the base contact to the
top of the metal barrel is 14mm. It is a
common bulb for older torches.
E10
This is also known as Miniature Edison Screw (MES).
Fig.5: a G1.27 miniature bulb (1.27mm
pin spacing). This 42005 bulb (1.35V,
0.32A) has a T-1 shape as used in
AAA Maglites. Source: www.topbulb.
com
Australia's electronics magazine
BA9S
This base type is commonly used
for older vehicle indicators but also
by some torches and LED replacement bulbs.
Miniature globes, eg, G1.27 base
This bulb (Fig.5) has two pins protruding from the base. The number
after the G indicates the centre-to-
centre spacing between the pins in
millimetres.
Blinking bulb
There were once bulbs that blinked,
driven via a bimetallic strip inside the
globe, which alternately heated and
cooled, making and breaking electrical contact (Fig.6).
They were available for 1.5V, 2.5V,
3.5V or 6V operation and were used
in numerous toys in the 1960s as well
as the Big Jim torch (see below) and
even pinball machines.
The base was typically an E10 and
the current draw was 200mA with a
1Hz flash rate and 50% duty cycle –
see siliconchip.au/link/abfo
Fluorescent tubes
Some torches use a miniature fluorescent tube – see Fig.7. They used to
be somewhat common but are now rare
as LED globes are superior. This style
of torch remains in a specialised form
to create UV or ‘black light’ to cause
fluorescence in certain items such as
currency, minerals, watermarks, biological contamination etc.
Fig.6: a flashing globe from an old
pinball machine with a BA9S base.
Source: www.pinball.center
siliconchip.com.au
Fig.8: construction of a typical 3mm
or 5mm LED as used in basic torches.
LEDs
LEDs (Figs.8-10) tend not to be
removable like incandescent globes as
they do not need routine replacement
and are often an integral part of the
torch. However, enthusiasts do change
them for different types, power ratings, colour temperature tint or other
desired characteristics.
There are slight variations in LEDs
coming from the same production line,
so all LEDs are tested and ‘binned’
into types with similar characteristics, much like other semiconductors.
Major LED manufacturers for
torches are Cree, Luminus, Nichia,
Osram, Philips Lumileds (Luxeon),
Samsung and Seoul Semiconductor.
LED emitters typically have no
markings, so you have to know what
they are or identify them from a chart
such as at https://flashlightwiki.com/
LED_Gallery
High-end LEDs used in torches typically have an efficiency of around
100lm/W (lumens per watt).
Fig.9: a Cree XM-L2 T6 3B emitter
attached to an MCPCB (metal core
printed circuit board), used for the
torch build described in the text.
Fig.11: a 35W HID lamp (Philips
CDM35/T6/830) with a two-pin G12
base, producing 3100 lumens. It is
103mm long and 20mm in diameter.
The bases can be purchased without
emitters to attach your own, or with
the emitter already attached.
runaway heating, so the current has
to be limited using a ballast or other
electronics.
HID torches are still available but
tend to be more expensive than others,
and current high-power LED technology is competitive with them.
High-intensity discharge lamps
HID lamps work by establishing
an electrical arc between two tungsten electrodes inside a quartz or alumina tube. The tube is filled with an
inert gas (argon, neon, krypton and/or
xenon) and a suitable metal or metal
salts (eg, mercury, sodium or halides)
– see Fig.11.
When an arc is struck, the high-
temperature plasma (ionised gas)
generated causes the metal or salts to
evaporate. Within any metal or metal
salt at a high temperature, electrons
jump between energy states, resulting
in light generation. The light usually
includes UV, which is filtered out.
HID lamps are much more efficient
than incandescent lamps but are more
expensive due to the need for fairly
complex control electronics. They
have a negative resistance temperature coefficient, which could lead to
A Phoebus Horizon HID 35W
searchlight (shown below) with 3500
lumen intensity, 1370m throw and
2.5h runtime.
Laser-excited phosphor (LEP)
In an LEP torch, a blue laser beam
is directed onto a special phosphor
coating adhered to a metal plate
(see Figs.12-14 and https://youtu.
be/G0V3p8cc-3I). The laser causes
the phosphor to fluoresce, emitting
Fig.7: a UV torch with a fluorescent
tube. Such ‘black lights’ have various
scientific and law enforcement uses.
Fig.10: how a LED emitter is attached to an MCPCB.
siliconchip.com.au
Australia's electronics magazine
November 2022 17
broad-spectrum white light. The
light emitted is not a laser beam but
is laser-like.
Classic laser light is monochromatic or close to it; the light from an
LEP torch contains all colours. Note
that ‘phosphor’ does not necessarily
refer to the chemical element phosphorous but any substance that emits
light when exposed to radiant energy.
Typically, the blue light from the
laser shines onto an yttrium aluminium garnet (YAG) phosphor, which
absorbs the blue light and re-emits it
as a combination of colours, making
a white beam. This is similar to how
white LEDs function; a blue or UV
LED emits light onto a phosphor mix
which re-emits it as white.
The beam from an LEP torch is
pencil-like and the torch is very efficient. A blue laser is used because it
is easier and more efficient for blue
light to excite phosphors to produce
the desired range of colours in the visible spectrum than other colours such
as red or green.
BMW uses LEP headlights in many
of its vehicles, including the X7. The
lights use less power, have longer
range and enable a smaller headlight
housing than LED lights. You can view
a teardown and repair video on YouTube for a BMW laser headlight titled
“Laser Headlight Teardown and How
Fig.12: how a laser-enhanced
phosphor (LEP) torch works.
to Repair color change” at https://
youtu.be/a5mAdDl5pTA
Power sources
Power usually comes from a battery
(rechargeable or disposable), which
might be recharged via a solar panel
or hand crank for emergencies (only
some types).
Supercapacitor-powered torches are
sometimes seen. They don’t have the
runtime of batteries but they can be
charged very rapidly. You can easily
make your own, and there are many
online instructions; search the web
for “supercapacitor torch”. You can
find two examples at siliconchip.au/
link/abfp and siliconchip.au/link/abfq
Consider that some rechargeable cells, such as certain protected
18650s, are too long to fit in some
Fig.13: the Weltool W4Pro, an LEP
torch. On high, it produces 560lm with
a 2670m throw and two hour runtime.
torch compartments. In this case, a
non-protected cell must be used, but
make sure the torch has low-voltage
shutdown to protect the cell. Also,
some 18650s have flat tops that won’t
make a good (or any) connection with
the torch contacts. In that case, use
button-top cells if they fit.
LED drivers
Most LED torches are not ‘direct
drive’ and include an electronic driver
to regulate the current and/or voltage
delivered to the LED. The electronics
might also provide multiple modes
(eg, low/medium/high brightness),
monitor the battery voltage and LED
temperature, protect against reversed
battery polarity, manage charging and
possibly other tasks.
Fig.14: a W4Pro beamshot. The
narrow, pencil-look beam is typical of
LEP torches.
Fig.15: current vs voltage for
differently-coloured low-power
LEDs. The steep increase in current
with voltage indicates why current
regulation is preferred.
18
Silicon Chip
►
Australia's electronics magazine
siliconchip.com.au
Fig.16: one of the simplest possible
LED torch circuits.
Each type of LED has a maximum
current and power rating. The voltage
across the LED (Vf or forward voltage) varies depending on the colour
and type. UV LEDs have the highest
Vf at 3.1-4.4V; violet 2.8-4.0V; blue
2.5-3.7V; green 1.9-4.0V; yellow 2.12.2V; orange/amber 2.0-2.1V; red 1.62.0V; infrared 1.2-1.7V. White LEDs
typically require around 3.0-3.6V (see
Fig.15).
LEDs are generally not driven with
a fixed voltage because the current
increases exponentially with voltage
once Vf is exceeded, and they could
experience thermal runaway.
There are several ways to regulate
LED power. These include direct drive,
a linear regulator, pulse width modulation (PWM), boost or buck circuits,
or a combination boost/buck circuit to
drive the LED at the correct voltage,
regardless of the input voltage.
One of the simplest LED torch circuits is shown in Fig.16. It is a battery,
LED and a resistor to limit the LED
voltage and current.
Direct drive
In direct drive circuits, the voltage
of the battery or power supply has to
be no greater than the maximum Vf of
the LED. They usually rely on the battery’s internal resistance or power supply to limit the maximum LED power.
This is not an advanced method, but
it can work.
Fig.17: eight AMC7135 regulators plus a microcontroller fit on this small PCB to
provide up to 3.04A (note that some AMC7135s are rated at 380mA rather than
350mA). The micro provides 12 group modes; this board was used for the torch
build described in the panel at the end of the article.
Taking Jaycar Cat ZD0196 as an
example, Vf(typical) = 3.2V and Imax =
100mA. To drive that LED from a 9V
battery, you could use a resistor of R =
(9V – 3.2V) ÷ 0.1A = 58W (round up to
62W to be safe). That assumes Vf(min)
is close to Vf(typical).
For more on driving LEDs directly,
including combinations of LEDs, see:
• siliconchip.au/link/abfr
• siliconchip.au/link/abfs
• electronicsclub.info/leds.htm
You can have fun buying a bag of
3mm or 5mm LEDs and a solderless
breadboard and try connecting the
LEDs in various series/parallel combinations. See the online calculator
at siliconchip.au/link/abft
The different series/parallel combinations give different voltages and
currents for driving the same LEDs (the
product of these, ie, the power will be
mostly constant).
For more information on this, see:
• siliconchip.au/link/abfu
• siliconchip.au/link/abfv
Linear regulation
The term linear regulator might refer
Resistor current limiting
The current to the LED can be limited using a series resistor, although
the LED will dim as the battery discharges, and the resistor can dissipate
a fair bit of power. If Vs(max) is the
maximum supply voltage, Imax is the
LED’s maximum current and Vf(min) is
the minimum Vf at Imax, the resistor
value required can be calculated as R
= (Vs(max) − Vf(min)) ÷ Imax.
siliconchip.com.au
to either current or voltage regulation.
Typically, LEDs are driven with a constant current. If the voltage supplied to
the regulator is higher than Vf, energy
is lost as heat. If the voltage drops
below Vf, the current will be less than
intended, but losses will be low. It is
ideal to supply the regulator with as
close to Vf as possible.
A common current-regulating chip
used in torches is the AMC7135
which can handle up to 350mA. Up
to four can be placed on each side of
a 17mm diameter driver board to give
a total of 2.8A, which suits LEDs like
the XP-L and XM-L2 in torches using
18650 Li-ion batteries (18mm diameter, 65mm long) – see Fig.17.
A microcontroller can be combined
with the linear regulator(s) to control
brightness using PWM (see Fig.18).
PWM (typically using a Mosfet)
Instead of using a linear regulator,
a Mosfet (or BJT) can be switched on
and off by a microcontroller to control
brightness using PWM as described
above. The Mosfet acts as a low-
resistance on/off switch. There is little
voltage across the Mosfet when on, so
it dissipates very little power.
Some sort of current limiting is usually required. Still, it can be arranged
to dissipate less power by operating
it at a reduced duty cycle to achieve
maximum brightness, so the overall
efficiency is improved.
Boost or buck circuit
Fig.18: how PWM is used to vary duty
cycle and thus control average current.
Australia's electronics magazine
An LED can be driven by either a
boost or buck circuit that increases or
decreases the supply voltage to that
most appropriate for the LED.
Some circuits can either boost or
buck. These circuits are most efficient
when the input voltage is close to the
output drive voltage, but they are usually much more efficient than linear
regulation regardless.
November 2022 19
Fig.19: a flow chart
for the generic
Andúril 2 torch
firmware – this is
the ‘simple’ section!
Source: https://
budgetlightforum.
com/node/76941
Driver firmware
Believe it or not, there are operating
systems for torches (see Fig.19). Drivers with microcontrollers require firmware and such software can even be
written or modified by the enthusiast.
The firmware controls the user interface, eg, the program will advance the
brightness every time the on-off button
is quickly clicked.
Popular firmwares include A6,
Andúril, Biscotti, Bistro, Crescendo,
NarsilMulti and RampingIOS. For a lot
more information and links for flashing tools and software, see siliconchip.
au/link/abfx
There is a repository of flashlight
firmware at siliconchip.au/link/abfy
if you are interested in seeing what
it looks like or developing your own.
There is also extensive documentation
for Andúril at siliconchip.au/link/abfz
Example code for the Convoy S2+
torch is at siliconchip.au/link/abg0
Torches of note
example is: siliconchip.au/link/abg1
We are aware of at least one modern
torch that uses this battery. Unusually, it also uses a traditional incandescent globe.
Big Jim
The Big Jim torch was a large light
from the 1960s and possibly earlier
(there is very little documented history on these torches). It used a sealed
beam headlamp, much like some former car headlights.
It was made by Union Carbide or
Eveready and used a large (125.4 ×
132.5 × 73mm) 6V ANSI 918 battery,
IEC 4R25-2, with a capacity of around
18Ah for zinc chloride (RS Pro) models to 33Ah for alkaline (Varta). Within
these were 8 F-size cells. If buying one
of these batteries, note there is a similar
►
For a comprehensive list of LED
drivers, see siliconchip.au/link/abfw
12V battery, Rayovac model 926D or
ANSI 926 equivalent.
Big Jim came in a variety of models.
Some had just the sealed beam main
light, while others also had a flashing red light, using a bi-metal strip as
described earlier.
Torches in this style are still available from the Big Beam Company near
Chicago, USA – see siliconchip.au/
link/abg2
One of that company’s torches from
the 1950s, the Big Beam No. 164, is
remarkably similar to the Union Carbide Big Jim from my collection (see
Figs.21 & 22). This light was subject
to US Patent 2,861,174 of 1958 by
Big Beam, so we assume Union Carbide licensed the design. For further
information on this, see siliconchip.
au/link/abg3
Fig.20: the Varta Palm Light is a modern
European torch that uses a 3LR12 battery. It
has a 3.5h battery life, a throw of 75m and 15lm
brightness. It is a rare example of a modern
torch with an incandescent globe. Source: www.
varta-ag.com/en/consumer/product-categories/
lights/palm-light
Some of the more prominent torches
throughout history are listed below:
The 3LR12 battery was (and is) more
common in Europe and Russia than
in other countries. Some torches still
use this battery – see Fig.20. Adaptors are available for purchase or 3D
printing to enable three AA cells to be
used instead of a 3LR12 battery. One
20
Silicon Chip
►
3LR12 torches
Fig.21: a Big Beam No. 164 from the 1950s.
Source: Made in Chicago Museum
Australia's electronics magazine
siliconchip.com.au
Fig.24: the current
Dolphin LED
torch.
Fig.23: the author’s Convoy S2 torches. The one on the left has 365nm UV LEDs and 1.05A driver. In the middle is
an S2+ with an SST20 4000K LED and 2.8A driver; on the right is an S2+ with SST40 5000K LED and 3.05A driver.
was waterproof and could float, but This battery (IEC 4R25X or 4LR25X)
Convoy S2+
it found acceptance in many applica- has spring terminals and typically
The Convoy S2 and the later version, tions beyond boating.
contains four F-size cells. Typical batthe S2+ are popular and inexpensive
The Dolphin MK1 was known in the tery capacities are 8.5Ah for a Varta
torches for buying, modifying or even USA as the “All American” or “No. “431” Zn-MnO2 (Zinc Chloride) type
building from parts (described later) – 108”. The MK1 is the only one with or 11.9Ah for a Varta “4430” alkaline
see Fig.23. They are not a ‘big brand’ metal retaining clips for the lens bezel type. Typical dimensions are 115mm
but have better quality than their price in the Dolphin model range.
× 68.31m × 68.31m.
would suggest and many favourable
The Dolphin used a 6V lantern batThere is a bit of confusion about the
reviews. If buying one, make sure it is tery which gave it a good run time by date of the MK1 Dolphin. The Austrafrom a reputable seller and not a fake standards of the day, as typical torches lian Museum of Applied Arts & Sci(see the panel on page 27).
from then ran from two D cells (3V). ences website (siliconchip.au/link/
That was before alkaline cells were abg4) lists the design date as 1965.
The Eveready Dolphin torch
widely available; standard cells of the
However, Eveready (siliconchip.au/
Almost all Australians will be famil- time had poor capacity and current link/abg5) has design and manufaciar with the iconic Eveready Dolphin delivery. The Dolphin had a bright and ture dates of 1966. It also states that
torch (Fig.24). It started life in the ‘throwy’ (long range) beam compared Dolphin torches “have been lighting
USA in 1965 and was produced for to other torches.
up the lives of Australian & New Zeasale around the world.
Having a large battery back then land families since 1967, when the first
The Dolphin was initially designed (the 1960s and early 1970s) was the MK1 lantern was launched”.
for the boating community and thus only way to get a reasonable capacity.
The second generation of the torch,
Fig.22: the author’s collection of three Big Jim torches. The left-hand torch
(model 100) is very similar to the Big Beam; the middle torch (model 101)
lacks the red flashing light, while the one with the plastic head (model 101C) is
Australian-made.
siliconchip.com.au
Australia's electronics magazine
Two hand-cranked torches. The
smaller Chinese-made one has a LED,
while the larger one is incandescent
and believed to be of Soviet origin.
November 2022 21
Fig.25: a modern LED Maglite
Solitaire, originally released with a
G1.27 incandescent bulb. Source:
https://maglite.com
Fig.26: the base model PakLite torch
on top of a 9V battery. Several other
models are also available.
Fig.27: the Photon Micro-Light II
LED keychain torch. It is powered by
a CR2032 coin cell, or two stacked
CR2016s.
the MK2, was a project of Eveready
Australia. Eveready contracted the
design to Paul Cockburn of Design
Field Pty Ltd in 1972. It became the
best-selling torch in the world in the
1970s and was manufactured by Eveready worldwide in various locations.
The MK2 dispensed with the metal
clips of the MK1 and featured a more
streamlined look. The MK3 was
released in 1988, according to www.
dolphintorches.com/about/, but the
Powerhouse Museum (siliconchip.
au/link/abg6) states that the MK3 was
designed by Paul Cockburn in 1989.
The MK3 bezel screws on rather than
clipping on.
The MK4 was introduced in 1996,
followed by the MK4.2 in 2000 and
the MK5 in 2003, which featured a
new reflector design, integral rubber mouldings for impact protection
around the lens, an adjustable stand
and better ergonomics.
According to the Powerhouse
Museum, the MK4 and MK5 were
designed by “Design Resource in
Crows Nest, NSW for the US-based
Energizer company” (Energizer Holdings is a division of Eveready).
The MK6 was released in 2007 and
then the MK7 LED in 2012, the first
Dolphin featuring an LED.
Eveready states that 20 million Dolphins have been sold in Australia and
New Zealand over 45 years (1967 to
2012). In 2016, a new LED Dolphin
was introduced, which has no “MK”
designation but is stated to have 200
lumens output, a beam throw of 250m
and a battery life of 65h.
above. In 2012, the LED version of the
Solitaire was introduced, but there are
DIY and commercial LED conversions
for the earlier version.
It is significant because it was a
well-engineered miniature keychain
light. Although the incandescent version was not particularly bright, it was
enough to find a keyhole at night.
Maglite Solitaire AAA
The 1988 Maglite Solitaire AAA
battery model (Fig.25) uses one of the
smallest, if not the smallest incandescent globe to go into a commercial torch; see the G1.27 bulb section
PakLite
This novel torch (see Fig.26 and
https://paklitegear.com/) sits on top of
a 9V battery. It is produced by a family
living off-grid in the mountains of Oregon. It is characterised by light weight,
useful light output and extreme run
time of up to 1200+ hours with a lithium battery on low, 80+ hours on high
or 600+/30+ hours for regular alkaline
batteries.
It can even run on ‘exhausted’ 9V
batteries from sources like smoke
detectors, as it can run down to a very
low voltage. There are many imitations
of this light.
Photon Micro-Light
Fig.28: a classic Maglite six D-cell incandescent xenon torch. Maglite still sells
these. It has a beam distance of 338m, 178 lumens and 28547cd peak intensity.
It is 485mm long and weighs 1417g with a battery. Source: https://maglite.com
This light (see Fig.27) is an extremely
small key chain light with a stated minimum 4.5 lumens output and 18h run
time, weighing 6.27. Depending upon
which beam colour is chosen, it uses
either two CR2016 or one CR2032 cell.
Surefire P60 and other P60 hosts
Fig.29: two Surefire-style torches and a selection of P6-modules, some Surefire,
others after-market; some incandescent, others LED. Source: author’s collection
22
Silicon Chip
Australia's electronics magazine
Surefire introduced their 6 Series
torches in 1988 (Fig.29). The 6C model
produced 60 lumens from two CR123
batteries and was smaller and brighter
than any comparable torch at the time.
The 6P and 6R models were released
in 1989 and featured a P60 incandescent xenon light ‘drop-in’ module of
65 lumens or a P61 module of 120
lumens.
Today, many different P60-style
modules with different light options
are available for various Surefire 6
series style “host” lights. Examples
siliconchip.com.au
include the UltraFire WF501B,
WF502B, WF503B, WF504B, WF502D
(http://flashlightwiki.com/UltraFire)
& Solarforce L2 (http://flashlightwiki.
com/Solarforce).
UltraTac K18
I use this outstanding AAA/10440
cell torch daily (see siliconchip.au/
link/abg7 and Fig.30). 10440 refers
to a rechargeable Li-ion cell in AAA
format.
Fig.30: the UltraTac K18 AAA torch.
It has a maximum brightness of up to
370 lumens (with a 10440 Li-ion cell)
and a maximum run time of 40h at
low brightness.
Upgrading a vintage torch
You can bring new life to a vintage or
antique torch (100+ years). Some people make permanent modifications by
adding LEDs and new battery systems,
but this is regarded as unacceptable by
some for rare lights.
It’s possible to make non-permanent
modifications, such as changing the
incandescent bulb for a ‘drop-in’
direct replacement, which can be
readily purchased for most incandescent bulb types (see Fig.31). Battery
replacements can be made with adaptors, given the lower battery capacity
required for driving LEDs.
For example, you can replace a D
cell with an adaptor containing one,
two or three AA cells.
Fig.31: the author replaced the
incandescent bulb in this vintage
torch with a LED and replaced the D
cells with AAs in adaptors.
Performance standards
for torches
The ANSI/NEMA FL-1 standard is
used for rating torches. It provides
standard ways to measure light output, runtime, peak beam intensity,
beam distance, water resistance and
impact resistance.
Measurement of light output
Lumens (lm), lux (lx) and candela
(cd) are the three most common units
used to characterise lighting sources,
although there are others – see Fig.32.
Torch enthusiasts and manufacturers frequently wish to characterise
torches in terms of overall light output or luminous flux, typically measured in lumens.
Unlike lumens, which measures
overall light output, lux takes into
account the area over which luminous
flux is distributed and is a measure of
illuminance. Lux is lumens per square
meter. Ten lumens over an area of one
square meter would be ten lux, but ten
lumens over ten square meters would
be one lux. Foot-candle is the obsolete
non-SI equivalent unit and is 1lm per
square foot.
siliconchip.com.au
Fig.32: how candela, lumen and lux are measured. Lumens is the most critical
measurement for torches.
Australia's electronics magazine
November 2022 23
Useful Links
• Flashlight Museum: www.wordcraft.net/flashlight.html
• TPAD Direct Thermal Path Technology for LEDs on MCPCBs for more efficient heat
removal: www.cutter.com.au/tpad/
• MCPCBs for sale: https://led-mounting-bases.com/en/310-led-mcpcb
• BudgetLightForum: https://budgetlightforum.com/
• Candle Power Forums: www.candlepowerforums.com
• Flashlight Wiki: https://flashlightwiki.com/Main_Page
Useful Videos
• “Post Vietnam War Flashlight – History” https://youtu.be/UiTGRa6EikE
• “1930s Flashlight Restoration-Niagara Searchlight – Kipkay Restored”
https://youtu.be/VHlVQMbdayw
• “I Bought EVERY Flashlight at Home Depot!” https://youtu.be/bdjHhVhUOWY
• “Flashlight Museum is an illuminating experience (2005)”
https://youtu.be/XdigO6-1MEY (sadly, it appears to have closed)
The candela is a measure of luminous intensity and quantifies the perceived power per unit solid angle
emitted by a point light source in a
particular direction. It is a weighted
measurement that takes into account
the sensitivity of the human eye to various wavelengths (called the luminosity function).
A beam from a 1lm light source distributed evenly within one steradian
(the 3D equivalent to the 2D radian
unit of angular measurement) has a
luminous intensity of one candela. If
the same beam were evenly focused
into half a steradian, the luminous
intensity would be 2cd. A typical wax
candle measures around 1cd.
‘Candlepower’ is an obsolete term,
but today is considered equivalent to
the candela. Sometimes, a torch will be
advertised with a candlepower rating
in the millions (which sounds impressive) because it has a tightly focused
beam, but its overall output in lumens
might be low.
Throw is a measurement of how far
away a torch can usefully light up an
area and can be calculated from its candela rating – see siliconchip.au/link/
abg8 and siliconchip.au/link/abg9
Measuring a torch’s brightness
The most important measurement
related to torches is lumens, which
can be measured using an “integrating sphere” or “goniophotometer”.
Unfortunately, professional equipment to measure lumens can be very
expensive, but there are inexpensive
solutions.
To make this measurement, you (1)
Fig.33: an inexpensive light meter that you can
use to measure lumens. This Neewer meter
shown can measure up to 200,000 lux. You can
find a variety of these types of meters online,
mostly sold at quite reasonable prices.
24
Silicon Chip
Australia's electronics magazine
Fig.34: a DIY lumen measurement
with a hollow foam sphere, as
described by run4jc.
need a way to collect all the light coming from the torch, (2) a way to measure the illuminance and (3) a reference for calibration, such as a torch
with a known accurate lumen rating
from a reputable manufacturer. The
illuminance can be measured using
an inexpensive light meter; searching
eBay for “lux meter” brings up many
models under $50 (see Fig.33).
The light collection device is ideally
a sphere, but it can be a white foam
box, a white foam sphere or even PVC
plumbing fittings. Even a cardboard
box with the inside painted white
will work.
The torch under test is shone into
a hole in one side, and the collected
light is measured (in lux) with a light
meter inside the device. First, the reference torch is measured, and a conversion factor is calculated between
the lux reading and the known number of lumens. This can then be used
to measure unknown torches. Ideally,
the calibration torch brightness is similar to the unknown device.
You can get hollow foam spheres
in Australia from Amazon and eBay;
try Googling “hollow foam ball”. A
method for making an integrating
sphere from a hollow foam sphere is
described at siliconchip.au/link/abga
– see Fig.34. Another hollow sphere
method is described at siliconchip.
au/link/abgb
Brooke Clarke describes the use
of a professional integrating sphere
for flashlight measurements with an
accompanying video at siliconchip.
au/link/abgc
Also see the video by Matt Smith
titled “DIY Lumen Measuring Device.
Integrating Sphere and Lumen Tube”
at https://youtu.be/xOE18kJ5WAU
(refer to Figs.35 & 36).
siliconchip.com.au
Fig.35: a foam packing box can be used as the “integrating
sphere” for lumen measurements. Source: Matt Smith
video (https://youtu.be/xOE18kJ5WAU).
These approaches will be acceptable
for most non-professional purposes,
but you can obtain surprisingly accurate results.
Note that a large proportion of
lumen ratings found on the internet are
inflated, sometimes by a factor of 10
or more. See Matt Smith’s video titled
“Internet Lumens vs Actual Lumens,
and the 100 watt LED test” at https://
youtu.be/XIywzCfvunY
Flood, throw and spill beams
Torch light beams may be more
‘flood’, more ‘throw’ or a combination (see Figs.37 & 38). Flood beams
are better for indoor and local area
Fig.36: using PVC plumbing fittings as the “integrating
sphere”, often called a “LumenToob”. Source: Matt Smith
video.
illumination, such as around a campsite. Throw beams are better for illuminating objects at a distance and tend
to have a central ‘hotspot’. The spill
beam is the light outside the central
hotspot that comes directly from the
emitter and not via the reflector.
Reflectors and lenses
Reflectors are important and, along
with the nature of the bulb, determine
the amount of flood or throw the light
has. Some torches have reflectors with
a variable focus to control this. Generally, smaller diameter torches have
a more flood-like beam because of the
smaller, shallower reflector and larger
lights have more throw because of the
deeper, larger reflector.
Reflectors may be smooth or have
an “orange peel” texture. Orange
peel reflectors give a smoother beam;
smooth ones give a better throw but
have more visible beam artefacts.
Lenses may be plastic or glass; better ones have an anti-reflection (AR)
coating.
TIR lenses are a special type of torch
lens; TIR stands for “total internal
reflection”. These are alternatives to
reflector style lenses and are said to
produce a better quality, fully collimated beam, unlike reflector optics. In
a TIR lens, all light goes through the
What is your EDC?
EDC stands for “everyday carry”
and refers to the torch you usually
carry with you. It might be on a neck
lanyard, a keyring, in a pouch or a
pocket, and there might be more
than one. EDC can also refer to
other tools one might carry, such as
a multi-tool, pocket knife, notebook,
pen, watch, lighter, phone, charger
pack etc.
Fig.37: flood vs throw beams and a combination of both, directed by the
reflector. Not shown here is the ‘spill beam’, light that comes directly from the
light source and does not go via the reflector. Flood vs throw can be varied using
a ‘zoom’ or variable focus feature.
Fig.38: examples of a flood beam (left) and throw beam (right).
Source: www.candlepowerforums.com/threads/spill-vs-flood.252751/
siliconchip.com.au
Australia's electronics magazine
An EDC organiser pouch, filled
with various EDC items, including
an Olight torch. Source: https://
everydaycarry.com/posts/35528/
trending-maxpedition-micropocket-organizer
November 2022 25
lens, but in a reflector, not all light exits
via the reflecting surface (see Fig.39).
Guide to choosing a torch
Fig.42: the components I purchased to build a Convoy S2+ torch. The parts
that came as the ‘torch host’ are at the top, while the ‘pill’ is on the left side of
the middle row. The optional lenses and lighted switch components are in the
bottom row.
When purchasing a torch, there are
many factors to consider, including:
▢ Spend as little or as much as
you want but remember that some
inexpensive torches can be surprisingly good. Read reviews and watch
review videos. An inexpensive torch
we like is the Convoy S2+, described
opposite.
▢ Try to ensure you are getting a
genuine product, not a fake one.
▢ What size torch is required?
▢ What is the required lumen output and number of brightness settings?
▢ How much ‘flood’ or ‘throw’ beam
or combination thereof do you need?
▢ If it has a rechargeable battery,
is recharging convenient in your
intended application or might disposable batteries be better? Some torches
have a built-in USB charging port, so
no dedicated charger is necessary.
▢ Do you want to use standard cells
that can be purchased anywhere, such
as AA, AAA or D, or a less common
specialist type like the 18650?
▢ Does it have a long enough runtime at various power levels for its
intended application, plus extra time
for emergencies? My Convoy S2+ with
an SST40 LED and eight AMC7135
drivers lasts around a week on the
lowest brightness setting with a Sony
VTC6 3000mA 18650 cell, perhaps
longer.
▢ Some torches have a small parasitic battery drain, meaning the battery might be flat when you go to use
it. Check for that. The tail cap can
often be unscrewed to break the circuit for storage.
▢ Is the battery removable? If not,
it could be a problem if it fails or you
want to upgrade it.
▢ Does the torch use special custom batteries? For example, Olight
uses product-specific batteries in some
models.
▢ Is it multi-voltage; eg, can it use
either alkaline or lithium batteries?
▢ Do you need a splash-resistant or
waterproof torch?
▢ Is it shaped so it won’t roll away
on an incline?
▢ Are there points to attach a lanyard?
▢ Does it have a crenulated bezel
(Fig.40)? If the torch is set to a low
setting and placed face-down on a flat
Australia's electronics magazine
siliconchip.com.au
Fig.39: the difference between conventional reflector optics (left) and a TIR lens
(right). Source: LEDiL
Fig.40: a Nitecore SRT7 with a
three-prong stainless steel crenulated
bezel, an optional accessory on this
discontinued model.
26
Silicon Chip
Fig.41: a Lumintop FWAA torch with
a two-way pocket clip that can be
attached to the brim of a hat, into a
pocket or onto a belt.
surface, this allows a small amount
of light to leak out, to provide a low
level of illumination. In some cases,
the bezel can even be used as a glass-
breaking tool to rescue someone from
a car or building.
▢ Can it tail stand? This can be useful to provide “ceiling bounce” light.
▢ What is the switch type, where
is it and is it replaceable? Tail cap
switches can be ‘forward’ (the torch
will momentarily switched on if
the switch is depressed halfway) or
‘reverse’ (momentarily switched off
with a half-depression).
▢ Does it have a pocket clip, and is
it one-way or two-way (Fig.41)?
▢ Does it have a magnet to attach to
magnetic metal?
▢ Does it have a glow-in-the-dark
(GITD) switch or o-ring? If not, GITD
replacement O-rings can be purchased.
▢ How complicated is the user
interface? Can you remember all its
functions, or should you keep instructions with you?
▢ Can it be completely disassembled to modify or repair?
▢ Is there an active “modding” community? Is the torch easily modifiable?
▢ Are spare or other parts available?
▢ Check user reviews
SC
Building your own torch
I purchased the parts shown in Fig.42 to build my own version of a Convoy S2+
from the “Convoy flashlight Store” on AliExpress (https://convoy.aliexpress.
com). These parts can be purchased at many places, but they seem reliable.
The parts are:
Host body: Convoy S2+, which includes an orange peel reflector, pill, o-rings,
glass, battery spring and lanyard for under $15
Driver: 7135 × 8, 17mm 3040mA 12-mode group driver with built-in
temperature control, compatible with lighted switch, for under $9
LED: Cree XML2T6 3B LED for just over $5
Lenses: a range of TIR lenses with different illumination angles, compatible
with XML and XML2 LEDs for about $4 (optional)
Lighted switch: $4.95 (optional)
Postage was a few dollars. Parts and tools I already had include an 18650
Li-ion cell and charger, thermal paste, solder and a soldering iron.
The Cree XM-L2 T6 3B emitter came on an MCPCB (metal core printed circuit
board) base. It handles up to a 3A and 10W and gives 1052lm output. T6 refers
to which luminous flux group it is sorted into (280-300lm <at> 700mA), and 3B
refers to its tint and colour temperature, 6200K cool white.
Fig.43 shows how it is assembled into the pill and its relationship to the
driver. Note solder pads for the emitter and other pads for + and – wires from
the driver.
Glossary of Terms
Beamshot a picture of a torch beam, typically on a wall or in a natural environment and often used for comparisons between lights.
Colour rendering index the ability of a light source to accurately render
the colours of objects it is illuminating (also called CRI). A CRI of 100 is identical to daylight; lower numbers give worse colour rendition.
Donut hole an undesirable dark spot in the centre of a torch beam.
EDC everyday carry (see panel).
GITD glow in the dark.
HA hard anodised; a surface treatment applied to aluminium.
Hotspot the centre part of the beam; a brighter hotspot provides better
throw.
Low voltage shutdown the torch shuts down if the battery voltage gets too
low. Lithium-ion batteries can be ruined if their voltage goes too low; some
such cells have their own low-voltage shutdown.
Memory when the driver remembers the last mode it was in, eg, if you
turned the light off at medium brightness, it would turn on again in that mode.
Pill the part of the torch which is a mounting point and heatsink for the
LED on one side and the driver on the other – see Fig.43.
Fig.43: assembling the Convoy S2+
is pretty straightforward; this shows
how the ‘pill’ goes together. The LED
is on one side and the driver is on the
other, held into the pill by a retaining
ring. The driver wires must be
trimmed and soldered to the LED PCB,
and thermal paste should be added
between the LED PCB and the pill.
siliconchip.com.au
Protected cell a cell with a small PCB to protect against over-charge,
over-discharge and possibly over-current. Not all torches can accept protected lithium cells as they are several millimetres longer than standard cells.
Unprotected cells can be safely used in torches with low voltage shutdown.
Tactical flashlight military-style, but it essentially is a meaningless marketing term (some may disagree!).
Thermal shutdown the torch will shut down if it gets too hot. The driver
usually provides this function.
UI user interface.
Australia's electronics magazine
November 2022 27
TINY LED
ICICLE
by Tim Blythman
This miniature ‘icicle’ is perfect to match the look of a winter Christmas,
despite the summer in Australia. This Icicle Ornament also has two power
connections, making it easy to power a series of them on a single supply.
I
cicle-style Christmas lights are very
popular. With vertical strings of
lights that are often arranged in
groups, they evoke the appearance of
icicles hanging from eaves.
The Tiny Xmas Ornaments from the
November 2020 issue (siliconchip.au/
Article/14636) were a great hit, and we
recently thought that an Icicle shape
would be a great addition. So we’ve
added an Icicle design to the cohort of
tiny Ornaments you can create.
The Icicle has a handy feature
shared with the Reindeer Ornament
published previously in that it has
two power connections (as well as an
onboard cell holder). That makes it
easy to create a long chain and power
it from a single power supply, such as
a 2×AA battery holder.
To keep things simple, we’ve laid
out the LEDs in a simple top-to-bottom
order, the same as the existing Stocking Ornament. The firmware for the
Stocking simply flashes the LEDs in
order from top to bottom. The Icicle
therefore reuses the existing code/HEX
file from the Stocking. The resulting
downward movement evokes water
dripping from the Icicle.
The circuit and parts list are thus
the same as the Reindeer Ornament
(except for a different PCB), and the
firmware is the same as that for the
Stocking. Easy!
We tried a few different LED colours
on our prototypes, and an assortment
of colours looks quite good, but using
all blue or white LEDs (or a mix) creates a striking effect.
For more background, refer to the
article from November 2020 or even
the original Tiny Tree from November
2019 (siliconchip.au/Article/12086).
The 2019 article explains how we
Parts List – Tiny LED Icicle
Wires go out one side of
the Icicle PCB and into
the other side of the next.
Both are in parallel, so the
battery holder can feed in at
either end of the chain.
28
Silicon Chip
Australia's electronics magazine
1 white double-sided PCB coded 16111192,
98.5 × 98.5mm (41 × 127mm upright)
1 PIC12F1571-I/SN (/1572-I/SN) or
PIC16F15213-I/SN (/15214-I/SN) 8-bit
microcontroller, SOIC-8, programmed
with the appropriate version of
16111194.HEX (IC1)
12 SMD LEDs, M3216/1206 or SMA size,
any colour (blue, cyan and/or white
recommended)
1 SMD coin cell holder [BAT-HLD-001]
1 CR2032 or similar 3V coin cell, or 3V
battery pack
1 10kΩ SMD resistor, M3216/1206 size
4 100Ω SMD resistors, M3216/1206 size
1 5-pin right-angle header (CON1; optional;
for power/programming)
1 2-pin right-angle header (CON2; power)
1 length of light-duty figure-8 wire (if daisy
chaining boards; eg, from ribbon cable)
1 M3 x 6mm Nylon screw
2 M3 nuts
SC5579 Kit ($15)
Choose from a variety of ornaments,
each one is supplied with the parts above
(except the coin cell, CON2 & figure-8 wire)
and assorted LEDs to match.
siliconchip.com.au
control 12 LEDs from a tiny 8-pin
microcontroller.
We will be adding the Icicle to the
list of Ornament kits available. You
can order kits from siliconchip.au/
Shop/20/5579 – just be sure to select
the correct colour and type of PCB
(white only for the Icicle). Unlike the
other Ornament kits, which come with
12 each green, red and white LEDs,
the Icicle kits will come with 12 each
blue, cyan and white LEDs.
Construction is simple enough; refer
to the older articles if you need more
details. The main thing to check is
that all the LED cathodes align with
the markings on the PCB; they should
all face the same way (to the left with
it upright). The PIC is the only other
polarised part, although you should
be careful installing the cell holder, to
be sure that it will allow the battery
to be inserted; it only has an opening
on one side.
You don’t need to fit the cell holder
if you are using a battery holder to
power multiple Icicles but mind the
polarity marked on the reverse of the
PCB. We’ve used red and black wires
to make it clear which is which, but
you can use other colours as long as
you don’t get them mixed up.
Programming is not necessary if you
have bought our kit, but if you have
a blank PIC12F1571 or PIC12F1572
microcontroller, you can use a PICkit
3, PICkit 4 or Snap. The PICkit 3 is
not compatible with the newer parts
like the PIC16F15213 or PIC16F15214
(which are generally more available),
so you’ll have to use a PICkit 4 or Snap
for these parts.
The Icicle should start flashing
when programming is complete,
although you might find some LEDs
stuck on if the programmer is still connected. One pin is shared between the
programmer and the LEDs.
If you are building a chain of Icicles, test each individually before
joining them together. They are all
programmed to flash at the same rate,
but minor variations in processor frequency mean they will quickly fall
out of sync.
Finally, secure the coin cell with a
Nylon M3 × 6mm screw and two nuts
against each other to lock them. SC
CAUTION: Coin Cells
Coin cells should be kept well away from
children who may ingest them. Make sure
the cell is secured firmly in place.
siliconchip.com.au
Fig.1: 12 LEDs are driven with just four microcontroller I/O pins using a scheme
called Charlieplexing, explained in the November 2019 article. The Icicle is
similar to the Reindeer as it has an extra connector for daisy-chaining power.
Figs.2 & 3: there are parts on both sides of the PCB, but the front is clear of
markings for a good presentation. Take care that the LEDs line up with their
cathode markings, which are just visible. The LED cathodes all face to the left
(when the Icicle is upright); there is a cathode mark on the PCB silkscreen. On
the reverse, only microcontroller IC1 is polarised.
Australia's electronics magazine
November 2022 29
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.
Digitally controlled preamp with tone controls
The Sanyo LC75341 IC has great features with digital control for volume,
balance, treble, bass, input gain and
channel selection, all in a single package. It only needs a few external parts.
There are four stereo inputs and signals are AC-coupled from them to pins
on the LC75341 (IC2) using 1µF electrolytic capacitors (plastic film types
could also be used). The selected signals are attenuated depending on the
current volume setting and then fed
to the Lout and Rout pins.
These signals feed back to the Lbass
and Rbass inputs via RC filters, allowing the chip to implement its bass
tone control network. The resulting
output signals are then fed to stereo
output connector CON6 via two 2.2µF
AC-coupling capacitors.
The 2.7nF capacitors from the Ltre
and Rtre pins to ground are required
for the LC75341’s treble filter network
to operate, giving control over the
amount of treble in the output signals.
The capacitors between Lin and
Lselo and Rin and Rselo couple the
signals from the input switching circuitry within IC2 to the preamp. This
arrangement allows the signal to be
intercepted and altered if desired,
but in this case, we are just feeding
the selected signals directly back into
the preamp.
Due to its widespread use, I decided
on an ATmega328P for the controller.
Five potentiometers are wired across
the 5V supply rail (VR1-VR5); their
wipers connect to analog inputs on
microcontroller IC1, so it can use its
internal analog-to-digital converter
(ADC) to sense the positions of the pots.
So if you rotate volume control pot
VR1, IC1 senses this and sends a command to IC2 to change the current volume attenuation setting. Similarly,
VR2 controls the left/right balance,
VR3 the amount of treble, VR4 the
amount of bass and VR5 the input gain.
Four-position rotary switch S1 is
connected to a resistor ladder network,
so it has a voltage of around 0V, 1.67V,
3.33V or 5V on its common terminal.
This is fed to the ADC4 input (pin
27) so IC1 can determine the position
of the switch and send commands to
IC2 to select the corresponding stereo input.
The LC75341 is controlled over a
Sanyo ‘CCB bus’, which has similarities to both the SPI and I2C serial buses.
Like I2C, commands are sent to devices
at a specific address. But like SPI, it has
a chip select or chip enable line (CE)
in addition to a data line (MOSI) and
a clock signal (SCK). Addresses (eight
bits) are sent with CE low, followed by
data (32 bits) when CE is high.
I used the Mikroelectronika mikroC
compiler to generate the firmware. The
ATmega328P’s SPI peripheral operates MSB-first (most significant bit;
big endian) while Sanyo CCB requires
LSB-first (least significant bit), so I am
using a bit reverse routine to send the
proper commands.
There is a bit of a trick to implementing the balance control. When you turn
the potentiometer anti-clockwise, you
must adjust the right channel so that
its volume fades while keeping the
The photo at left shows the tone control single-sided PCB with a USBasp AVR programmer connected. The photo at right
shows the same tone control board connected to a power amplifier.
30
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
left volume constant. Similarly, turning the potentiometer clockwise will
reduce the left channel’s volume while
holding the volume of the right channel steady.
The power supply applies 6V AC to
a bridge rectifier formed using diodes
D1-D4 and filtered by a 1000µF capacitor to produce around 7-8V DC, which
is regulated to 5V by linear regulator
siliconchip.com.au
REG1 to power IC1 and IC2. LED1
lights to show the presence of power
at the input of the regulator, LED2 to
show power at the output and LED3
flashes to show that microcontroller
IC1 is operating.
I designed a single-sided PCB for
this project. You can download the
PCB pattern along with the component
layout, firmware HEX file and C source
Australia's electronics magazine
code for this project from siliconchip.
com.au/Shop/6/60 After programming
the chip, set the fuses to the following
values: LFUSE 0x62, HFUSE 0xD9,
EFUSE 0xFC.
The performance of the prototype
built using my PCB is good, with no
observable hum or noise.
Noel A. Rios,
Manila, Philippines ($100).
November 2022 31
ESP32-Camera sentry with object detection via TensorFlow
The ESP32-Camera costs US$6
and includes a 2MP camera and a
2.4GHz WiFi interface that can operate at ranges of up to 200m. When connected to the internet, it can perform
AI-related jobs too.
The ESP32-Camera takes and sends
images to a remote computer via the
internet. The remote computer uses AI
(artificial intelligence) to analyse the
image and determines the class of the
object within. It sends that information back to the ESP32-Camera, which
can then perform object-specific jobs.
We want to use this for safety applications involving conveyor belts,
where the belt must not operate with
any people near it. For this, two cameras are focused across the 200m-long
belt – one from the tail end and the
other from the head end. The moment
they detect any humans on its path,
they will sound an alarm.
If the ESP32-Camera detects a person in its view (from the front or back),
it brings its GPIO14 pin high.
The direct GPIO14 output of
ESP32-Camera pulses due to continuous redrawing of the image boundary. Therefore, that input switches on
NPN transistor Q1, pulling the trigger
input (pin 2) of timer IC1 low. IC1 then
switches on NPN transistor Q2 for up
to 10 seconds, adjusted using trimpot
VR1, activating the relay which triggers the alarm siren.
In the software (which can be downloaded from siliconchip.com.au/
Shop/6/4529), the IP address for the
ESP32-Camera module is fixed but can
32
Silicon Chip
be changed by your requirements. The
ESP32 continuously draws an object
boundary over the image. If it finds two
objects, it draws two boundaries and
so on. The confidence level threshold
can be from 0 to 100%.
Other settings you can change are
the image resolution, whether it is
mirrored, whether the onboard LED is
used as a ‘flash’, image quality, brightness and contrast. Note that the system
will be extremely slow if you increase
the image resolution from 320×240 to
1600×1200. It is better to leave the control at the default resolution first and
change other settings.
The ESP32-Camera board is a 3.3V
device. The Li-ion or LiPo cell provides 3.7V to 4.1V which is reduced to
3.3V using an HT7333 regulator. It has
a dropout voltage of only 90mV and a
quiescent current of just 4μA. I have
disabled brownout protection on the
ESP32, so it will tolerate a marginally
low voltage from the 3.3V regulator.
The LMC555 will operate at a voltage as low as 1.5V, so the relay (3V /
5V DC coil) determines the operating
voltage.
To program the ESP32-Camera
module, you need the latest version
of the Arduino IDE (1.8 or above).
The ESP32-Camera does not have an
inbuilt USB interface. Therefore, one
needs a USB-to-serial adaptor with
its TX wired to the VOR pin (GPIO3),
RX wired to the VOT pin (GPIO1) and
GPIO0 connected to GND for the first
few seconds of uploading after reset,
then released.
Australia's electronics magazine
The coco-ssd model used in this
project, implemented with TensorFlow, can detect a wide range of
objects selected from the pull-down
menu, varying from person to toothbrush. Whatever object is selected, the
ESP32-Camera will look for the specified number of that type of object. If the
number is exceeded, it will command
the relay to switch on the alarm circuit.
This type of collaborative AI model
provides very fast detection.
Other ideas for this circuit include:
• A scarecrow, triggering the alarm
in the presence of birds/dogs/
cats/cows/cars/etc.
• A ‘magic eye’ for your front door,
automatically raising the alarm
when someone arrives.
• A guest counter for a venue.
• Other applications.
Bera Somnath,
Co-author: Sh S K Swain / Lara,
North Karanpura, India. ($100)
siliconchip.com.au
November
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T 2352
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T 2247A
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N 1130F
S 2750
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Magnetic
Battery Bank
Charge your phone
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10,000mAh. 20W
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Q 0594
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90W Car Laptop Charger
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Anderson Style, Car Acc. Socket
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Z 6454
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This cute hedgehog toy kit
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Requires 4 x AAA batteries.
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+ BONUS
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BONUS! Z 6439B micro:bit
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Lab kits
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$
This comprehensive learning lab provides many hours
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VALUE!
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A make-it-yourself AM/FM band radio
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60 in 1
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49
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Keeps bored kids busy.
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K 1154
5 In 1 Smart ‘Coding’ Robot Kit
A six legged robot kit designed to avoid objects
or follow you around the room. Easy to build.
Requires 4 x AAA batteries. Ages 8+
Contains everything
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SAVE $12
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30 in 1
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K 2212
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88
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10 in 1 Electronics Lab
K 2206
Pique a younh engineers interest with 10 fun
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99
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D 0990
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D 0980
$
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One box for all your entertainment.
This kit includes 5m of RGB strip lighting, power
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60 LEDs per metre.
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Includes 3.5mm, S/PDIF, USB & RCA cables.
This fantastic home weather station displays all your local weather data
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Victoria
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B 0011
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LC
Capacitance Range: 1pF to 1200pF+ with
0.1pF resolution
Inductance Range: 100nH to 2500μH+
with 10nH resolution below 10μH
Accuracy: typically better than 2%
Power supply: 3 × AA cells, draws
~35mA during operation
Battery Life: around 72 hours with fresh
alkaline AAs; operates down to 0.6V
per cell
Display: 0.96-inch (24mm diagonal)
OLED screen
3
Meter Mk
This new LC (inductance/capacitance) Meter is a modernised version of a very
old design - the Tektronix T130 from the 1950s. It can measure a wide range of
capacitances and inductances, from less than 1pF to more than 1.2nF, and from
less than 100nH to more than 2.5mH. It displays the results on an OLED screen.
inspired to design this modIthewas
ern LC Meter when I read about
1954 Tektronix Type 130 LC
Meter in the series of Vintage Workbench articles by Alan Hampel from
June to August 2020 (siliconchip.au/
Series/346). It was an impressive feat
of engineering at the time, using all
analog techniques.
While there are many cheap LC
meters available today, their main
drawback is not being able to measure
low values. RF filters often require
accurate values less than 10µH or
10pF.
The Tektronix design had a reference oscillator at 140kHz (Fref). The
measurement oscillator (Ftest) was
initially tuned to the same frequency.
Then, by placing a capacitor across the
tuned circuit, or an inductor in series
with the inductor in the oscillator,
the test oscillator frequency dropped.
Mixing the two signals gave signal
components at frequencies Fref + Ftest
and Fref − Ftest. Selecting the latter
using a low-pass filter, the T-130 used
clever analog techniques to convert
this to a capacitance or inductance
value shown on a moving coil meter.
Their design gave accurate measurements from 1–300pF or 1-300µH.
It was all done using valves; transistors were not available back then.
siliconchip.com.au
My first LC Meter design emulated
much of this principle and worked
reasonably well, but that version had
some deficiencies. It used two variable capacitors, a coarse and fine
adjustment, to set the test frequency
to the exact value before a capacitor
or inductor was measured. This was
time-consuming and fiddly, so I added
an ‘automatic zero’ on power-up.
Also, its construction was complicated, using a large LCD, so I changed
it to use the same OLED screen that
I used for my AM-FM DDS Signal
Generator (May 2022; siliconchip.
au/Article/15306) and 0-110dB RF
Attenuator (July 2022; siliconchip.au/
Article/15385).
The OLED screen is cheaper and
also consumes a lot less power. That
allows the Meter to run for many hours
on three AA cells and operate down to
a total battery voltage of 1.8V (0.6V per
cell) thanks to the use of a step-up regulator. That will save on battery costs.
After making those changes, I had
a Meter that worked well, but I felt it
was still too complicated and used too
many parts, some difficult to source.
The auto-zero function took far too
long, and the accuracy and resolution were worse than I would like.
By Charles Kosina
Australia's electronics magazine
Calibration was problematic as well.
I solved all those problems in my
final design. It somewhat moves away
from the original Tektronix concept
in that it does not start at a particular
frequency. The operating frequency is
now of secondary importance as it gets
cancelled out in the calculations. It is
also self-calibrating, resulting in an
accuracy of about 2% over the whole
capacitance range.
The capacitance range is now 1pF
to more than 1200pF with a resolution
of 0.1pF, while the inductance range
is 100nH to more than 2500μH with a
resolution of 10nH below 10µH.
You might notice that this new
auto-calibrating concept makes it
somewhat similar in operation to our
June 2017 Arduino-based Digital LC
Meter (siliconchip.au/Article/10676),
which was based on the earlier
High-accuracy Digital LC Meter (May
2008; siliconchip.au/Article/1822).
However, those designs use a comparator in the oscillator and that causes
some problems and has limitations.
As you will see when we get to the
circuit, the implementation of this
Meter is somewhat different. It uses a
separate inverter-based oscillator and
has self-calibration features to provide
better accuracy over a wide range of
component values.
November 2022 41
Parts availability
Sourcing components is always a
problem these days, but I went to quite
a bit of effort to ensure that everything was available from element14
at the time of writing. There are a few
parts that are available from multiple
AliExpress sellers at very low prices.
However, for some of these, you may
have to buy multiple quantities. Still,
as the prices are so low, you will end
up with plenty of spares.
Of course, Murphy isn’t resting, and
before this article was published, some
of the critical parts ran out of stock.
The good news is that we realised what
was happening and snapped some up,
so an almost complete kit is available
(see the bottom of the parts list). So if
you can’t source all the parts yourself
or don’t want to, that’s an easy option.
Performance
One primary object of this design
was to produce accurate readings for
low-value inductors. VHF filters generally require inductors in the sub-1µH
(ie, nanohenry) range.
I possess an ancient Q-Meter, a
Meguro MQ-160. The design dates
Table 1 – inductance accuracy
Meguro inductor Measured value
1.0μH 0.98μH
Circuit details
2.5μH 2.53μH
The circuit of the LC Meter is shown
in Fig.1. It is based on a Franklin oscillator comprising two 74HC04 inverters, IC2a and IC2b. The 1MW resistor
across the first inverter puts it into a
linear mode, making it act like a very
high gain inverting amplifier. The second inverter provides the phase shift,
which feeds back into the tuned circuit.
With the nominal onboard 330µH
inductor (L1) and 220pF capacitor, the
oscillation frequency is about 630kHz.
It has a large operating range and will
still oscillate reliably with more than
1200pF added across the tuned circuit
or up to 2.5mH in series.
One advantage of this arrangement
is that the output of IC2b swings
between the supply rails. This means
that it does not need an additional
fast op-amp to boost the signal into a
range that a microcontroller can easily measure.
Four transistors, Q1-Q4, switch
additional capacitors across the tuned
circuit. These capacitors are 1% tolerance types, and by using parallel
5.0μH 4.88μH
7.5μH
7.35μH
10μH 9.94μH
15μH
14.2μH
25μH 24.4μH
35μH
34.6μH
50μH 49.8μH
75μH
75.1μH
100μH 99.8μH
150μH
148μH
250μH 254μH
350μH
357μH
500μH 492μH
750μH
1000μH
750μH
1009μH
1250μH 1250μH
1500μH 1484μH
2500μH 2498μH
made by connecting two coils in series (eg,
150μH = 100μH in series with 50μH)
42
back to the 1940s; the one I have was
made in 1969. It still works quite well,
as long as the valves inside keep functioning.
The MQ-160 came with a box of
14 calibration inductors from 1µH
to 25mH. They are all large air-cored
coils and are really works of art. Their
accuracy would not drift with time, so
they continue to be a good standard.
Using individual and series combinations of my standard Meguro inductors, I obtained the accuracy figures
shown in Table 1.
These assume that my test coils
are accurate, as there is no specific
information in the Meguro manual
about their accuracy. The accuracy
for capacitor values depends on how
close the 1% calibration capacitors
are, and can therefore be assumed to
be no worse than ±2% (and probably
closer to ±1%).
At the measurement frequency of
600kHz or less, ferrite-cored inductors all read low as the ferrite permeability is reduced at lower frequencies.
For example, a nominal 68µH inductor measured 58.5µH at 572kHz, but
a 1µH inductor fared much better and
measured 0.89µH at 630kHz. Air-cored
inductor measurements will not vary
significantly with frequency.
Silicon Chip
Australia's electronics magazine
combinations, we get ten calibration
points. The BFR92P transistors used
here have very low collector-to-base
and collector-to-emitter capacitances,
typically 0.4pF and 0.23pF, respectively, so they will not detract from
the accuracy.
The base resistors for these transistors are 3.3kW, and with 5V applied,
they drive the transistors well into
saturation, providing low-impedance
ground connections for the capacitors.
We need to provide a ‘zero reference’ point for inductance measurement. This is done by connecting L1
to ground and measuring the oscillator frequency. My initial design used
an NPN transistor for this, but once
the inductance under test got close
to 1000µH, the voltage across the
switched-off transistor was such that
its reverse-biased junction conducted
and clipped the waveform.
The solution was to substitute a
small relay (RLY1). That allows the
Meter to measure up to at least 2.5mH.
DPDT switch S2 selects between
capacitance (up) and inductance
(down) measurements. For capacitance measurements, the DUT is
placed across the tuned circuit, while
the DUT is placed in series for inductance measurements. In both cases, the
oscillation frequency will be reduced.
The oscillation frequency is too
high for the microcontroller to measure accurately, so a 74HC161 binary
counter is used to reduce it to less than
100kHz. In the initial design stages,
I was not sure how much division
would be needed, so header JP1 gives
the option to divide by 2, 4, 8 or 16.
In the final design, a division ratio of
eight is used.
Microcontroller and display
The processor used is the
ATMega328P on the Arduino Nano
module (MOD1). I chose it as it is
cheap and readily available from multiple sources, including eBay and AliExpress. It also simplifies the construction substantially.
Its INT0 interrupt pin (pin 20) is
used to count the frequency from
the oscillator. For capacitance measurements, a 250ms window is used
to count pulses. However, this is
increased to two seconds for inductance measurements to obtain enough
resolution down to 10nH.
The OLED screen is controlled over
a two-wire I2C (inter-integrated circuit)
siliconchip.com.au
Fig.1: the primary oscillator is built from inverters IC2a & IC2b. Its frequency is affected by an external capacitor/
inductor at CON1, or onboard calibration capacitors switched by transistors Q1-Q4. Inductor L1 is used for measuring
inductances, switched to ground by RLY1. The Arduino Nano controls and monitors the oscillator, computes the
values and displays them on a small OLED screen.
siliconchip.com.au
Australia's electronics magazine
November 2022 43
I always have a simplified RS-232
serial connection on my boards for
debugging the firmware. In this case,
the three unused 74HC04 inverters
are used, with two in parallel for the
TX pin to provide sufficient drive
strength. The serial interface format
is 38400,8,1,n and lots of debug information is transmitted, which I have
left in, as it does not slow down the
operation.
Power supply
The prototype lacks
the relay and associated
components at lower left, but
otherwise is very similar to
the final design.
serial interface. Because this uses
open-drain style signalling, no voltage translation is needed, just 15kW
pull-up resistors to +3.3V. These values are higher than the usual 4.7kW
to reduce power consumption further. With the short tracks, there is no
problem with noise despite the lower
bias current.
One analog input on the micro is
used to measure the battery voltage,
while the other is used to sense the
three-position function switch, S1.
Momentary switch S3 is used for
starting capacitance calibration or for
inductance measurement.
There is an optional output for a
buzzer at CON4. This gives a beep
when calibration is completed. As this
is its only function, it may be safely
omitted. The series diode is a safety
feature as the connector is the same
as for the battery input. Without the
diode, if the battery was connected to
the wrong socket, it could destroy the
microcontroller!
Fig.2: a plot of the oscillator frequency
shift against external capacitance.
Reading a frequency shift off this plot
will tell you the connected capacitor
value. This can be accurately
approximated with a third-order
polynomial, but linear interpolation
between the points shown is close
enough for our needs.
Fig.3: the inductance vs frequency
shift curve is similar to the
capacitance curve shown in Fig.2,
but it needs second-order curves over
most of its segments to give a good
enough approximation. The exception
is the 0-10μH section, which is close
enough to being linear.
44
Silicon Chip
Australia's electronics magazine
REG1 is an MCP1661 or MP1541
step-up voltage converter. It can
operate with an input voltage below
2V and still provide the required 5V
output. While two cells will provide
enough voltage, by using 3 AA cells,
the minimum voltage is less than 0.7V
per cell. You can use up all those cells
which no longer work in a mouse or
other equipment to power the LC
Meter, saving money.
REG1 works by pulling its switch
pin (pin 1) low, in pulses at 500kHz.
When this pin goes low, current flows
from the battery through inductor L2,
to ground and back to the battery,
charging up L2’s magnetic field.
When the transistor pulling pin 1
low is switched off, current flows from
the battery through L2 and schottky
diode D4 into the 5V supply rail, powering the circuit and charging up the
filter and bypass capacitors. As L2’s
magnetic field collapses, the voltage
at the anode of D4 rises above the battery voltage.
Fig.4: a close-up of the 0-10μH section
of Fig.3, comparing the actual curve to
a linear approximation. The resulting
errors are minor in comparison to
other sources of uncertainty.
siliconchip.com.au
By controlling the duty cycle of
the pulses, REG1 maintains the voltage at its Vfb (feedback) pin close to
1.227V. The division ratio of the 390kW
and 120kW resistors causes this to be
effectively multiplied at the top of the
divider. This results in an output of
1.227V × (390kW + 120kW) ÷ 120kW
= 5.215V.
Measurement calculations
The frequency of a tuned circuit is
given by C = 1 ÷ ω2L and L = 1 ÷ ω2C,
where ω = 2πf. For C in pF, L in µH
and f in MHz, this simplifies to the
useful equations C = 25330 ÷ f2L and
L = 25330 ÷ f2C.
If we know the inductance value by
measuring the frequency, we can calculate the capacitance, but this method
has two problems.
Firstly, an accurate inductor is not
available; the best we can get is ±5%.
Secondly, suitable inductors are on
a ferrite core and, as mentioned earlier, permeability varies substantially
with frequency. It is impractical to
use an air-cored inductor as it would
be too large.
This is where the calibration technique results in accurate measurement. On power-up, the oscillator frequency is measured first with transistors Q1 to Q4 off.
This gives the frequency with no
external capacitance. Then by switching on the transistors in different combinations, we get calibration points of
100pF, 220pF, 320pF, 470pF, 690pF,
790pF, 940pF, 1040pF, 1160pF and
1260pF.
Fig.2 shows the curve derived from
these calibration points with the frequency offset from 0pF. It is possible
to describe this curve with a polynomial equation, but a third-order polynomial is needed to get good accuracy.
This is of the form C(pF) = af3 + bf2 +
cf + d (d = 0).
The first cubed term (f3) results in
huge numbers, well beyond 32-bit
integer calculations. There are ways
of getting around this by cleverly
sequencing the calculations, but I
chose a simpler method. There is not
much of a curve between individual
calibration points, and a linear interpolation gives acceptable accuracy.
Capacitance readings are taken continuously at about half-second intervals. The resolution is 0.1pF for values below 200pF. Above this, only the
integral part of the value is shown, as
siliconchip.com.au
the fraction is unlikely to have significant accuracy.
Inductance measurements
Inductance measurements are made
a bit differently. We don’t have the
privilege of built-in calibration inductors, as any accurate types would have
to be air-cored and far too large.
I measured the oscillator frequency
with each of the calibration inductors
that came with my Meguro Q-Meter,
up to 2500µH, which is close to the
practical limit of the Meter. This gave
me a calibration curve similar to the
one used for capacitance. This curve
may also be approximated by a third-
order polynomial L = 20-12 f3 − 50-8 f2
+ 0.0045 f. With C in pF, L in µH and
f in MHz
Again, this makes 32-bit integer
computation difficult, so I split it into
several segments, some approximated
by quadratics, as shown in Fig.3. I’ve
included a spreadsheet in the download package for this project with the
relevant calculations.
The 0-10µH section of the curve is
so close to a straight line that a linear
equation is very accurate (Fig.4). From
this, we can estimate the likely resolution for low inductance values. To get
the required resolution, the oscillator
must be stable in the measurement
period of four seconds. The measurement readout is stable in practice, with
the 10nH digit remaining constant
between measurements.
Note that this calibration curve
depends on the actual inductance
value of inductor L1, so we have to
correct the difference. This requires
a measure of the value of L1, which
is performed as described in the
“Onboard inductor value calculation” panel.
By comparing the measured value
with the one I used in my prototype,
the offset frequency readings are modified for better accuracy.
Firmware
The firmware is written in BASCOM (BASIC for AVRs), which is
easy to implement and easy to follow. It occupies just over half of the
32KB flash memory on the ATmega328
processor. If you want to know more
about it, download and check out the
source code.
Case preparation
The recommended enclosure is
from Ritec (Altronics Cat H0324) and
includes a clear lid. It has a slightly
indented clear window measuring 98
× 76 mm. The drilling measurements
shown in Fig.5 relate to this window.
The transparent top is relatively
brittle, so be careful if using a centre punch as it can crack the plastic.
Likewise, use a low-speed drill to prevent damage to the top. A step drill
gives the cleanest and most accurate
results.
As these holes have to be very
Fig.5: the locations of the holes in the clear lid of the H0324 plastic box. You
could copy this (or download it from the Silicon Chip website and print it out at
actual size) and use it as a template. See the comment at the end of the body text
explaining that one hole and switch could be omitted.
Australia's electronics magazine
November 2022 45
Onboard inductor value calculation
As the value of inductor L1 will vary with the test frequency due to the permeability of the ferrite core varying, we cannot rely on its nominal value. To get
a good estimate of the inductance in the oscillator circuit, we need to make
some calculations. The capacitance across it is the 220pF plus the stray
capacitance; call this C1. We know that L = 1 ÷ (ω12 × C1), where ω = 2πf (f =
oscillator frequency).
The resonant frequency will change if we add a capacitance C2 in parallel
with C1. As long as it is not too different from the original frequency, the inductance value will be close enough to the same. The new equation becomes:
L = 1 ÷ (ω22 × [C1 + C2])
Combining the above two equations, we get: ω22 × (C1 + C2) = ω12 × C1
This can be rearranged to: (C1 + C2) ÷ C1 = ω12 ÷ ω22
Further manipulation gives us: C1 = C2 ÷ (ω12 ÷ ω22 – 1)
As the 2π factors in ω1 and ω2 cancel out, this becomes:
C1 = C2 ÷ ([f1 ÷ f2]2 – 1)
To more easily calculate this using 32-bit integer arithmetic, we multiply the
numerator and denominator on the right-hand side by f22 to give the equivalent equation: C1 = f22 × C2 ÷ (f12 – f22)
In our case, we know the added capacitance C2, and measuring f1 and f2 gives
us the value of C1. From this, we can calculate L according to the first equation
above, or the simpler version, L = 25330 ÷ f2 × C mentioned in the body text.
This calculation is done during the calibration on power-up, with C2 being the
100pF calibration capacitor. The fact that the frequencies measured are divisions of the actual frequencies does not matter as the ratio remains constant.
accurate, first locate the bottom-left
hole 16mm from the window edges.
Drill this to 3mm and attach the blank
PCB with an M3 screw and nut. Position the PCB to be precisely square,
then drill the other holes in the middle
of the switches. Alternatively, use Fig.5
as a template to mark the four holes
that need to be drilled, then enlarge
the holes to 6.35mm (1/4in) or 6.5mm.
The window has a moulding ‘bump’
in the centre that interferes with the
OLED behind it. Drill this out as well,
to 6.35mm or 6.5mm.
Construction
The LC Meter is built on a 91.5 ×
63.5mm double-sided PCB coded
CSE220503C. Components are
mounted on both sides of the board,
with the connectors and Arduino Nano
module on the back, as shown in the
overlay diagrams, Figs.6 & 7.
The only fine-pitch SMD is the
MPC1661 up-converter. As it is a fivepin device, the orientation is obvious.
Solder it first, followed by the other
ICs. Add a thin layer of flux paste onto
its pads before placing it, tack one pin
and then check carefully that the other
pins are correctly aligned, ideally
using a magnifier. If necessary, re-heat
the tacked joint and nudge it into position. Then solder the other pins.
Clean the flux off the board and
inspect REG1 to verify that all its pins
are soldered properly and none are
bridged. If there are bridges, add a bit
of flux paste and then remove them
with a piece of solder wick.
The remaining 14-pin and 16-pin
chips are relatively easy to solder
but make sure they are orientated
correctly! Follow with the five transistors, four BJTs (Q1-Q4) and one
Mosfet (Q5). They are all in three-pin
SOT-23 packages, so don’t get them
mixed up.
The diodes are in two different package types: plastic SOT-123 (ZD1 & D4)
and cylindrical glass Mini-MELF (D2,
D5). In each case, start by identifying
the striped (cathode) end. You might
need a magnifier to see the stripe on
ZD1 and D4. Then solder them in
place, as shown in Fig.6.
Now fit all the discrete resistors and
capacitors. They are all M2012/0805
(2 × 1.2mm) or M3216/1206 (3.2 ×
1.6mm) size, and none are polarised,
but the resistors should have their
codes marked on top. After that, solder the small SMD relay, taking care
to orientate it correctly. That’s the last
surface-mounting part.
Now add the through-hole components, starting with the lowest-profile
axial devices and working your way
up. The OLED screen plugs into a
4-pin socket strip. Carefully slide off
the plastic on the OLED pins to reduce
Figs.6 & 7: all the SMDs and most of the other parts are on the front of the board. The only one that’s a bit tricky to solder
is REG1; make sure you scrutinise its solder joints before powering the board up. Also watch the orientations of the ICs,
the Arduino Nano module (once it’s plugged in), the relay and the diodes.
46
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
the height above the board. It is then
secured by two M2.5 or M2 screws
with 8mm untapped spacers.
The Arduino Nano and connectors
are on the opposite side of the board.
I also used socket strips for the Nano,
but that is optional. The Nano has 15
pins on each side, so ideally, you’d
use 15-pin strips, but they are not easy
to find. You can use 14-pin headers
inserted towards the top edge of the
board, as the lowest pin on each side
is not electrically connected, or cut
down longer sockets.
The other components on the back
of the board are headers CON2 &
CON4, the optional debugging header
(CON3) and the BNC socket (CON1).
All the switches mount on the front,
and are best fitted last. We’ve specified solder-lug switches rather than
PCB-mounting types, and provided
sufficiently large slots to solder in the
lugs. This is because the solder lug
style switches are more widely available, especially in the wide variety
needed here. Make sure they’re perpendicular to the board before soldering all the lugs.
Clean the board with circuit board
cleaner and inspect all the soldered
joints for any that may have been
missed, and check for shorts between
pins. Finally, place the jumper on JP1
in the position shown in Fig.6.
Assembling it into the case
Presumably, you followed the earlier instructions to prepare the lid with
the aid of the blank PCB. If not, you’ll
have to go back and use a template
made from Fig.5 instead. Then you
can print and prepare the front panel
label, shown in Fig.8.
Print this label on photographic
paper. I placed a transparent 1mm
thick sheet of polycarbonate on top
of the label to protect it, although you
could laminate it instead. Although
the PCB has mounting holes, the toggle switches are adequate to bolt the
unit onto the panel.
The battery holder for the three AA
cells (BAT1) should be attached to the
bottom of the case with double-sided
adhesive tape. While you could solder
its leads directly to the PCB pads for
CON2, that would make disassembly
somewhat tricky. So we’ve specified
a polarised header for CON2 and a
matching plug. Crimp and/or solder
the plug to the battery leads, ensuring
they are not reversed.
siliconchip.com.au
Parts List – LC Meter Mk3
1 double-sided PCB coded CSE220503C, 91.5 × 63.5mm
1 125 × 85 × 55mm IP65 sealed ABS enclosure (clear lid) [Altronics H0324]
1 panel label, 98 × 76mm
1 Arduino Nano microcontroller board (MOD1)
1 0.96-inch OLED display module with I2C interface and SSD1306 controller
(OLED1) [SC6176 (cyan)]
1 Omron G6K-2F-Y-DC5V SMD relay (RLY1)
1 330μH axial RF inductor (L1)
1 3.3μH axial RF inductor (L2)
1 PCB-mount miniature SPDT centre-off toggle switch (S1)
[Altronics S1330; S1332 is PCB-mounting equivalent]
1 PCB-mount miniature DPDT on-on toggle switch (S2)
[Altronics S1345; S1350 is PCB-mounting equivalent]
1 PCB-mount miniature SPDT centre-off momentary toggle switch (S3)
[Altronics S1340; S1333 is PCB-mounting equivalent]
1 PCB-mount miniature SPDT on-on toggle switch (S4)
[Altronics S1310; S1315 is PCB-mounting equivalent]
1 PCB-mount right-angle BNC connector (CON1) [Altronics P0529]
2 2-way polarised vertical pin headers with matching plugs (CON2, CON4)
1 3-way polarised vertical pin header (CON3; optional, for debugging)
1 4-way header socket (for OLED)
2 14-pin or 15-pin header sockets (optional, for mounting Nano)
1 2×4-pin header, 2.54mm pitch (JP1)
1 jumper shunt (JP1)
2 8mm untapped spacers (for mounting OLED)
2 M2 × 12-16mm panhead machine screws and nuts (for mounting OLED)
1 3 x AA battery holder with flying leads (BAT1)
3 AA cells (ideally alkaline)
1 200mm length of foam-core double-sided tape (to attach battery holder)
1 BNC to screw terminal adaptor (optional, to measure components)
1 chassis-mount piezo buzzer (optional) [Altronics S6109, Jaycar AB3462]
Semiconductors
1 74HC161D or 74AC161D synchronous binary counter, SOIC-16 (IC1)
1 74HC04D or 74AC04D hex inverter, SOIC-14 (IC2)
1 MCP1661T-E/OT integrated high-voltage boost regulator
(or MP1541DJ-LF-P boost converter), SOT-23-5 (REG1)
4 BFR92P low-capacitance NPN transistors, SOT-23 (Q1-Q4)
1 2N7002 60V 115mA N-channel Mosfet, SOT-23 (Q5)
1 BZT52C4V7 4.7V 500mW zener diode, SOD-123 (ZD1; optional)
2 LL4148 75V 500mA small signal diodes, SOD-80 (D2, D5)
1 MBR0540 50V 500mA schottky diode, SOD-123 (D4)
Capacitors (all SMD M2012/0805 ceramic)
2 10μF 16V X5R
3 100nF 50V X7R
1 470pF 50V NP0/C0G 1%
1 330pF 50V NP0/C0G 1%
2 220pF 50V NP0/C0G 1%
2 120pF 50V NP0/C0G 5%
1 100pF 50V NP0/C0G 1%
Resistors (all SMD M2012/0805 1%)
1 1MW
1 390kW
1 120kW
6 15kW
2 10kW
4 3.3kW
Optional Adaptor Board
1 double-sided PCB coded CSE200603, 33 × 20.5mm This optional adaptor
1 SMA edge connector
board makes it easier
1 6-pin header socket
to test components.
1 short SMA to BNC cable
KIT (SC6544
SC6544) – $65 + P&P: includes everything in the parts list above that
isn't optional except for the case, AA cells and front panel label.
Australia's electronics magazine
November 2022 47
The battery holder and piezo buzzer
are located in the case so that they don't
interfere with the PCB when the lid is
attached. Note the position of the hole in the
side for the BNC socket.
Before plugging the battery in, very
carefully check that polarity as the
PCB does not have reverse polarity
protection.
Using it
The BNC connector by itself is not
ideal for connecting to separate components. The simplest solution is to
use a BNC plug with screw terminals
and a couple of clip leads to connect
to leaded components. You can connect some parts directly to the screw
terminal. With care, the clip leads
may also connect to M3216/1206 and
M2012/0805 size SMDs.
Depending on the length of leads,
these will add about 100nH to measured inductances. This can be measured by shorting the leads together;
then, you can subtract this from the
inductance reading. That will only
be necessary for values below about
5µH.
An alternative is a small PCB I
designed (coded CSE200603) connected by a short coax cable, BNC to
SMA – see the end of the parts list.
This allows more device options and
includes pads for SMD capacitors.
M3216 and M2012 chip capacitors can
be accurately measured by carefully
holding them down on the pads with
a non-conducting stylus.
The added capacitance of the coax
cable is about 15pF, so it is necessary
to run calibration with the adaptor
connected, cancelling it out. Calibration runs automatically at power-up,
but it can also be triggered manually
by pressing the CAL/START switch.
This requires the L/C switch to be in
48
Silicon Chip
Some example screengrabs when
operating the LC Meter Mk3.
the C position and no external component connected.
To make inductance measurements,
switch to the L position, connect the
unknown coil and press CAL/START.
This will power relay RLY1 for two
seconds to give a reference zero offset.
After that, RLY1 is switched off,
placing the unknown in series with
L1. A lower frequency will be measured and subtracted from the “zero”
point to give an offset frequency. The
inductance is then calculated from this
offset. The inductance will continue to
be measured from then on, each reading taking about four seconds.
If no inductor is connected, the display will show “Reading Error”. In any
case, it’s best to take several readings to
get a consistent result. The calibration
is accurate up to 2,500µH (2.5mH). It
will measure values higher than that,
but the precision of such readings is
unknown.
Future enhancements
The onboard three-position toggle
switch (S1) provides Option 1 and
Option 2 for possible enhancements
in the future. One option I tried was to
double the measurement window for
improved resolution but, in practice,
there was no significant difference,
so I discarded it. That switch may be
omitted to reduce the construction
cost slightly, and the label modified
to remove the options.
Finally, I would like to acknowledge
another regular contributor to Silicon Chip, Andrew Woodfield, for his
helpful suggestions. It was largely his
desire for measuring sub-1µH inductors that I was pressed to improve my
SC
earlier designs.
LC METER MK3
CAL / START
OPTION 1
C
L
NORMAL
OPTION 2
Australia's electronics magazine
ON
Fig.8: the
front panel
label can be
downloaded
from the
Silicon Chip
website and
printed on
photo paper.
There are
two versions
available,
one with
the OPTION
switch at
lower left
(shown
here) and
one without
it.
siliconchip.com.au
Handles 12V <at> 5A (or 10A
with alternative inductors)
by John Clarke
Easy to build and store in
a compact UB5 Jiffy box
Effective noise and
transient suppression
Low standby current
under 5mA
Transient voltage clamping
Low-pass filtering
Fused supply
DC Supply Filter
for vehicles
Many devices will run off 12V DC, so it’s pretty tempting just to plug
them into a vehicle supply (via a cigarette lighter socket or similar),
and away you go. But you’re likely to run into two significant problems
with that: supply noise messing with the device’s performance and
voltage spikes possibly frying it. This Filter solves both those problems.
P
rotect your 12V equipment
from voltage transients that could
cause irreparable damage using this
Vehicle DC Supply Filter. It connects
inline with the DC supply to clamp and
filter transient voltage excursions. It’s
especially useful for audio gear as it
reduces that horrible ignition system
whine that can pass through the vehicle’s electrical system.
While many 12V supplies are transient and noise-free, some are not.
That’s especially true of the 12V (or
24V) supply from a vehicle with the
engine running. In particular, heavy
load switching such as electric radiator fans or air conditioner compressors
switching on or off can produce voltage transients on top of the theoretically smooth 12V DC supply.
Other noise and transient sources
include the vehicle’s alternator, where
alternator brushes produce electrical
noise, and the ignition system with
frequent pulses delivered to the coils
and spark plugs.
siliconchip.com.au
It isn’t just for vehicles, either.
Mains switchmode power supplies
can also have transients on their output, as well as noise. These typically
have high-frequency noise due to the
switching nature of the supply and
can produce transients when the load
is abruptly changed from full load to
a lesser current.
We have found on multiple occasions that modern switchmode plugpacks are unsuitable for powering
sensitive circuits, including signal
generators, preamplifiers and theremins.
While some equipment powered
from such sources can survive damage, others are more sensitive. The
device may fail quickly due to voltage
transients exceeding the internal electronics ratings, or it could fail over an
extended period as sensitive electronic
components accumulate damage with
each voltage transient.
Transients and noise can be reduced
with a low-pass filter, and a transient
Australia's electronics magazine
voltage suppressor can absorb harmful
spikes. The Filter effectively removes
high-frequency signals from the DC
supply. The result is a supply with
much lower noise, less high-frequency
ripple and more minor voltage transients. Filtering can go a long way to
protecting your valuable equipment
from damage.
Our DC Supply Filter is quite compact and can be housed in a small Jiffy
box. Heavy-duty screw terminals are
provided for the input and output connections, plus there is an onboard fuse
and a power-on indicator LED.
Filter design
The circuitry for the Filter is relatively straightforward, as shown in
Fig.1. It uses two inductors and several capacitors. A transient voltage
suppressor (TVS) is included to absorb
excessive voltage spikes.
The TVS specified begins to conduct
at its Vbr (reverse breakdown voltage)
of 14.4V and provides full voltage
November 2022 49
Fig.1: the Filter has two main roles: to reduce high-frequency noise and absorb large spikes. Noise is attenuated by
two cascaded LC filters (47μH/101.1μF) while the TVS between the two shunts to ground any particularly large voltage
spikes that make it past the first filter stage.
clamping at 23.5V, although it would
have to be a mighty spike for it to allow
the voltage to rise much above 16V.
Note that a TVS will conduct a small
leakage current at voltages below its
reverse breakdown voltage. As it turns
out, about half the quiescent current
of this Filter is due to the TVS. But
we need it to protect the downstream
equipment from the worst spikes such
as ‘load dumps’.
If you want to use the Filter at a
higher voltage, like 24V, you will need
to change the TVS to one with a suitable Vbr rating, plus the two electrolytic capacitor working voltages will
need to be increased (to 35V or 50V
for a 24V supply).
For the particular TVS we used, we
measured a leakage current of about
2.6mA from 12V up to 15.6V, at which
point the current increases as it begins
to clamp the voltage. The leakage current through the TVS is something to
The assembled
PCB for the
5A version mounts
within the UB5
enclosure on the
flanged lid using TO-220
insulating bushes as standoffs.
50
Silicon Chip
Australia's electronics magazine
consider if this is going to be the cause
of battery discharge over time.
An extra 2mA (approximately) is
drawn by the power indicator LED.
Typically, when used on a vehicle supply, the overall 4.6mA current should
not discharge the battery except over
a long time.
Returning to the Fig.1 circuit, power
is applied at CON1, and current flows
through the fuse (F1) to a small bypass
capacitor, then the inductor L1, rated
at 47μH and 5A. Following this are
three paralleled capacitors: a 100μF
low-ESR electrolytic, 1μF multi-layer
ceramic and 100nF MKT polyester.
These bypass ripple, noise and transients to ground.
The TVS is connected in parallel with these capacitors to clamp
over-voltage spikes.
We use a mix of capacitors to
improve the filtering action over
a wide range of frequencies. The
non-electrolytic capacitors function
better at higher frequencies, while the
electrolytic capacitor provides reasonable filtering below 100kHz and better
still below 10kHz.
A second identical LC (inductor/
capacitor) low-pass filter follows,
forming a second stage to reduce
noise and ripple going to the output
at CON2.
Note that a radio signal filter design
would likely not include the capacitors across CON2 because they expect
50W source and load impedances. With
our Filter, we expect the source impedance will be close to 0W, and the output impedance can be anywhere from
about 1kW down to as low as 2.9W for
a 5A load with a 14.4V supply.
The capacitance across the output
of the Filter at CON2 gives an effective frequency roll-off that is relatively independent of the external load
siliconchip.com.au
Fig.2: the measured performance of the prototype is quite a bit better than what was predicted by simulation, with noise
and ripple attenuation starting below 1kHz and already below -20dB by 2kHz. -55dB is reached just above 5kHz.
connected to the output. In effect, the
capacitors provide a low impedance
down to below 10Hz.
The LED indicator (LED1) is driven
from the 12V supply via a 4.7kW resistor. The LED does not light if the unit
is not powered or the fuse has blown.
would have made the details of the
transient harder to see.
We also plotted the Filter’s frequency response using the LTspice
simulator and by measurement in
Fig.2. The measurement was checked
down to -55dB at 6kHz, and the
expected roll-off above this frequency
continues as an extrapolation of the
measured roll-off rate.
Testing the Filter
We conducted a test to see how
effectively the Filter reduces voltage
transients using two power supplies.
One supply was set to provide 14.4V
DC and the other 50V DC. The 14.4V
was fed to the filter input via a large
inductor to isolate this from the transient voltage derived from the 50V
supply.
The transient was created by
charging up a 100nF 100V capacitor that was subsequently switched
over to connect to the Filter’s input
momentarily.
The result can be seen in Scope 1.
The top yellow trace shows the input
voltage transient with a peak 26.4V
above the steady 14.4V DC supply.
At the output of the Filter, shown on
the lower cyan trace, there was only
a 600mV increase; that’s a reduction
Scope 1: a demonstration of the
effectiveness of the Filter. We
purposefully created a 26V spike
on top of a 12V supply, causing
some ongoing oscillations at the
Filter’s input. The voltage at the
Filter’s output peaked at only 0.6V
above the DC level.
in transient amplitude by a factor of
44 times.
Note that the oscilloscope traces
were AC-coupled, so the 14.4V DC
applied to the Filter is not seen on the
oscilloscope traces. If we had DC coupled the traces, the sensitivity (volts
per division) would have needed to
be much higher to prevent the traces
from going off-screen at the top. That
Construction
The Filter is built on a double-sided,
plated-through PCB coded 08108221
that measures 77 × 46mm. The 5A
version fits in a standard UB5 plastic
Jiffy box.
If you wish to make a 10A version,
you will need a larger UB3 box. The
part changes required are shown in
the parts list, including the use of a
10A fuse instead of 5A. See the separate panel on winding and mounting
the inductors.
Refer to the overlay diagram, Fig.3,
as a guide to construction.
Begin by soldering the 4.7kW resistor
and low-profile parts such as the TVS
and capacitors. The TVS needs to be
orientated correctly, with the striped
Fig.3: the Filter assembly is straightforward; the components shown here are for the 5A version. Only the TVS, LED
and electrolytic capacitors are polarised. For the 10A version, the inductors will be larger and must be mounted
above the other components on longer leads.
siliconchip.com.au
Australia's electronics magazine
November 2022 51
Parts List – DC Transient Filter (12V, 5A version)
1 double-sided, plated-through PCB coded 08108221, 77 × 46mm
1 panel label, 80 × 47mm (optional)
1 UB5 Jiffy box with flanged lid [Altronics HF0155, Jaycar HB6016]
2 15A 2-way PCB-mount screw terminals (CON1, CON2) [Altronics P2101]
2 47μH 5A chokes (L1, L2) [Altronics L6617, Jaycar LF1274]
1 30A blade fuse holder [Altronics S6040]
1 5A blade fuse (F1)
2 cable glands to suit 4-8mm cable diameter
4 M3 × 10mm countersunk head (CSK) screws
4 M4 hex nuts
4 TO-220 insulating bushes
2 100mm cable ties (5A version only)
1 transient voltage suppressor rated at 1500W with a Vbr of 14.4-15V
(TVS1) [Jaycar ZR1170]
1 3mm LED, any colour (LED1)
2 100nF 63V MKT capacitors
2 1μF 50V multi-layer ceramic capacitors
2 100μF 25V low-ESR electrolytic capacitors
1 4.7kW 1/2W resistor
10A version changes
1 UB3 Jiffy box [Altronics HF0203, Jaycar HB6014]
(instead of UB5 Jiffy box)
2 powdered iron toroidal cores (L1, L2) [Jaycar LO1244]
(instead of 47μF 5A chokes)
1 2m length of 1.25mm enamelled copper wire (for winding L1 & L2)
1 10A blade fuse (F1) (instead of 5A fuse)
Winding L1 and L2 for 10A use
The ratings of pre-wound inductors L1 & L2 limit the standard version of the
Filter to 5A. The circuit can supply up to 10A by using hand-wound inductors
instead.
In this case, L1 and L2 are made by winding 24 turns of 1.25mm diameter
enamelled copper wire on the specified toroidal core. The ends of the wire will
need to be stripped of insulation using a sharp craft knife before soldering.
Keep the ends long enough so the inductors can mount raised off the PCB, as
they will not fit in the space allocated for the 5A inductors.
Ideally, these inductors should be secured high enough to clear the other
PCB-mounted components, but low enough to allow the assembled PCB to
fit inside the enclosure. A horizontal mounting will give the best clearance;
the inductor leads may need extending if they aren’t left sufficiently long. You
can use neutral-cure silicone sealant to secure the inductors to the PCB and
adjacent components.
Fig.4: you can attach
this panel label to the
box lid, so its contents
aren’t a mystery.
The insulating bushes
for the PCB should be
trimmed to fit the lid.
This filter is suitable for use with the Multi-Stage Buck/Boost Charger (October
2022) for battery charging from a vehicle power supply.
52
Silicon Chip
Australia's electronics magazine
end to the top. The two electrolytic
capacitors must have their striped
(negative) side toward the bottom,
with the longer positive leads to the
pads marked with a plus sign on the
PCB, towards the top.
The fuse holder, CON1 and CON2
can be fitted now. Inductors L1 and L2
are installed upright, with the leads
entering the smaller holes adjacent to
each side of the inductors on the PCB.
The cores are held using a cable tie
through each core and around under
the PCB via the larger holes. Ensure
the cable tie joint is on the top side of
the PCB rather than on the underside,
as the PCB needs to sit low in the Jiffy
box to fit.
Depending on your preference, the
LED should be installed either down
close to the PCB or with long enough
leads to protrude through the enclosure.
Mounting it in the enclosure
If using the UB5 Jiffy box, mount
the PCB to the inside of the flanged lid
using countersunk head screws from
the outside, with the PCB raised off
the base with insulating bushes. These
are the type usually used to isolate a
TO-220 transistor (or similar) from its
mounting screw.
Cut a section of the round washer
portion of the bush with side cutters to
allow it to fit on the flanged lid, adjacent to the corner mount mouldings,
as shown in the photo at the bottom
of this page.
Holes at each end of the enclosure
are required for the cable glands. The
PCB has cut-outs to make room for the
gland nuts, so ensure the holes are centred on the enclosure sides. The input
and output wires pass through the
cable glands at each end and are terminated at the screw terminals. Make
sure the wiring polarity is correct, as
the fuse will blow if connected incorrectly to the input.
Draw the wires out through the
glands as the PCB is inserted into
the enclosure, then tighten the gland
nuts to prevent the wires from being
pulled out.
We have designed a panel label that
can be printed and affixed to the enclosure, as shown in Fig.4. A PDF file of
this label can be downloaded from:
siliconchip.au/Shop/11/34
Information on how you can make
labels is available at siliconchip.au/
Help/FrontPanels
SC
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Silicon Chip
Australia's electronics magazine
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November
electronics magazine
2022 55
Raspberry Pi
Pic W
Review by Tim Blythman
The Raspberry Pi Foundation has a habit of making surprise
announcements of new hardware. Although created with education in
mind, their low pricing has made the various single-board computers and
microcontroller boards extremely popular in all sorts of applications. Adding
WiFi support can only increase that popularity!
A
fter nearly ten years of their range
of single-board computers, the
Raspberry Pi Foundation surprised
everyone last year with the release of
its first microcontroller, the RP2040,
and its own microcontroller board,
the Pico. Now the Pico W is available,
building on the already very handy
Pico board, adding all-important WiFi
capability.
Background
The RP2040 is a dual-core ARM
Cortex M0+ processor with 264kiB
of RAM, a 16kiB boot ROM that provides a USB bootloader, plus some
other handy functions. Like many
such 32-bit devices, it runs from 3.3V.
The Pico is a fairly minimal board
implementation that adds a 4MB flash
memory chip and a 3.3V voltage regulator. It breaks out 26 of the RP2040’s
I/O pins into a compact board suitable
for breadboarding or even surface-
mounting on another PCB.
Its target launch price was $6, and
incredibly it is still in stock from multiple vendors at about that price.
While the board is minimal, it is
very capable (especially considering
the price) and could be programmed in
C or MicroPython from launch. Arduino support appeared very quickly
after its debut.
Raspberry Pi is a trademark of the
Raspberry Pi Foundation
It’s the same size as the Pico and
costs only a few dollars more. We can
see the Pico W challenging other WiFi boards
like those based on the ESP32 and ESP8266 due to its
low price and excellent support.
56
Silicon Chip
Australia's electronics magazine
The RP2040 microcontroller was
also available in good numbers and
at a good price (under $2 in single
quantities). It was quickly taken up
by other companies who created their
own spin on the Pico, including variants such as the Arduino Nano RP2040
Connect, one of the many boards that
includes WiFi.
We reviewed the Pico in December
2021 (siliconchip.au/Article/15125)
and found that it is a well-designed
board with a nimble microcontroller
that has a very useful set of features.
With the work of Geoff Graham and
Peter Mather, it was soon possible to
program the Pico in BASIC. This is
the so-called PicoMite (January 2022;
siliconchip.au/Article/15177). The
PicoMite has much in common with
the Micromite, including the ability to
drive an LCD touchscreen.
That led us to create the Pico BackPack in March 2022 (siliconchip.
au/Article/15236). The BackPack is
designed to connect to an LCD touchscreen and includes an RTC (realtime clock) chip, IR receiver, stereo
line-level audio output and a micro
SD card slot. We also showed how to
program the Pico BackPack in four different languages.
The very popular VGA PicoMite followed that in July 2022 (siliconchip.
au/Article/15382). The addition of
a VGA output and a keyboard input
means that the VGA PicoMite is more
siliconchip.com.au
Table 1: GPIO differences between Pico and Pico W
Function
Pico
Pico W
Notes
PSU PS pin
GPIO23
WL_GPIO1
Has 100kΩ pulldown, low is PFM mode, high is PWM mode
USB Vbus sense
GPIO24
WL_GPIO2
Digital input with pulldown
LED
GPIO25
WL_GPIO0
Also broken out to TP5 downstream of resistor
Vsys/3
GPIO29
GPIO29
For Pico W, only when enabled by GPIO25 being high
WiFi CLK
–
GPIO29
WiFi CS
–
GPIO25
Also connected to Mosfet on Pico W to enable ADC readings on GPIO29
WiFi MISO/MOSI
–
GPIO24
Connects to four SDIO pins of CYW43439
WiFi EN
–
GPIO23
Connects to both WL_REG_ON and BT_REG_ON of CYW43439
like a Maximite than a Micromite and
is reminiscent of the computers of
yore, like the Commodore 64.
Enter the Pico W
The Pico W, as you might guess,
is an RP2040-based microcontroller
board to which a WiFi module has
been added. Its target price is $9.
It’s the same size and has much the
same pinout as a Pico, but with a small
metal can at the end opposite the micro
USB socket. That can contains the
WiFi chip. The three-pin SWD (serial
wire debug) header has been moved to
make way for the WiFi antenna.
The Pico W is not the first RP2040
board with WiFi, but given the Raspberry Pi Foundation’s aggressive pricing, it is among the cheapest. It’s similar in price to ‘off-brand’ boards with
ESP8266 or ESP32 microcontrollers,
which also have a similar set of features.
The WiFi module is based on an
Infineon CYW43439 chip, which
boasts 802.11n (2.4GHz) WiFi support and Bluetooth 5.2. However, there
doesn’t appear to be any software support for Bluetooth on the Pico W at
this stage.
The CYW43439 chip has separate
WiFi and Bluetooth subsystems which
each have their own ARM microcontroller core. There are several ways
to communicate with the WiFi Chip
but, importantly, the common SPI
interface has been used on the Pico W.
That means that Bluetooth could be
supported on the Pico W in the future.
Design evolution
Having another chip interfaced to
the RP2040 inevitably leads to the
question of what has been sacrificed,
since some resources will at least need
to be shared if not given up entirely.
The first clue is that all the exposed
siliconchip.com.au
pins are marked the same as the original Pico. The WiFi interface happens
through four GPIO pins that are not
broken out on either board.
These are GPIO23, GPIO24, GPIO25
and GPIO29. On the original Pico,
these all had various internal functions. The Pico W now uses these
to communicate with the WiFi chip.
Some of the original functions are kept,
while others are delegated to GPIO
pins on the WiFi chip. Table 1 summarises these differences.
There are other subtle differences.
The original Pico uses an RT6150
buck/boost regulator to provide the
3.3V rail. This is rated to 800mA and
can work with an input between 1.8V
and 5.5V.
The Pico W uses an RT6154, which
has a similar input voltage range but
can deliver over 2A. Some extra current will be necessary to drive the WiFi
chip; this extra capacity will surely
come in handy elsewhere.
Apart from the pin changes noted
in Table 1, the interfaces to the power
supply are much the same despite the
pin changes. One I/O pin monitors
Vbus to detect the presence of USB
power. At the same time, another is
used to select between the more efficient PFM (pulse frequency modulation) and lower ripple PWM (pulse
width modulation) modes.
In practice, the biggest difference is
how the onboard LED is driven, since
the Pico W uses one of the CYW43439’s
I/O pins to drive it.
On paper, the Pico W appears to
be a mostly compatible and painless
upgrade to the Pico. Some functions
have changed locations, but that is to
be expected.
Hands-on testing
The Pico W was unavailable in Australia until August this year due to
Australia's electronics magazine
delays in the Raspberry Pi Foundation
getting RCM (Regulatory Compliance
Mark) approval. As soon as we could
get one, we tried it out.
We built a Pico BackPack and fitted
it with female headers, allowing us to
change out the two different boards
(fitted with male headers) quickly for
testing. This arrangement also helps
keep the Pico W’s WiFi antenna clear
of the solid copper pours on the BackPack PCB and LCD module. We used
stacked spacers for testing the WiFi
capabilities of the Pico W.
We loaded each of the four UF2 test
files provided for the original Pico
BackPack article onto both the Pico
and Pico W in turn and checked their
operation.
The only difference we noted was
that the Pico W does not flash its LED
when using the PicoMite example
firmware, which was expected due to
pin 25 being used for the WiFi module instead of the LED. Otherwise, all
the test programs worked identically
between the two boards.
So if you can afford the premium
of an upgrade from the Pico to a Pico
W, there aren’t really any downsides.
Next, we decided to see what could
be done with the Pico W’s WiFi.
Using WiFi
The Raspberry Pi Foundation does
a great job of making it easy to get
started; perhaps that is not surprising,
given their educational focus. They
have published online numerous data
sheets, user guides and other resources
such as the full circuit diagrams for
both boards.
Among these documents is a guide
on connecting to the internet with the
Pico W. You can find it at siliconchip.
au/link/abgv
We made good use of that information during our testing. Although the
November 2022 57
WiFi chip on the Pico W uses SPI, it is
in half-duplex mode, using the same
data pin for communication in both
directions.
According to the official C SDK (software development kit) for the Pico and
Pico W, the SPI peripheral is actually
implemented in one of the PIO blocks.
As we mentioned in our original
article on the Pico, PIO blocks are
I/O-orientated state machines that can
run a small program and thus emulate
communication peripherals like SPI or
UART. There are even DVI implementations that can generate signals that
work on HDMI displays.
This means that existing designs
that use the PIO state machines may
need to be modified to work with the
Pico W but presumably, only if the
WiFi features are actually used.
Unfortunately, it looks like the
PicoMite (MMBasic) firmware will
not be updated to include support for
the WiFi chip, as explained at www.
thebackshed.com/forum/ViewTopic.
php?TID=14977
That’s because the WiFi chip on the
Pico W needs a firmware image to be
loaded at runtime, and that alone consumes around 300kB of flash memory, plus RAM at runtime. It would
also require a framework and commands to provide a way to control
the WiFi module through the BASIC
language.
We can see that this would be a lot
of work and perhaps isn’t justified,
especially as it is so easy to interface
to an ESP8266 loaded with an AT command firmware.
Regardless of the language used,
any project that is updated to use the
WiFi feature will undergo considerable changes anyway.
MicroPython support
There are two ways of programming
the Pico W (and the Pico) provided by
the Raspberry Pi Foundation: the C
SDK and MicroPython, a port of the
Python language optimised for microcontrollers.
The Pico W’s MicroPython port
supports WiFi out of the box. It is not
the first microcontroller with WiFi to
work with MicroPython; MicroPython
has long had support for WiFi on the
ESP8266 and ESP32.
There is a prebuilt UF2 image of
MicroPython for the Pico W available. Once uploaded, the following
commands initialise the WiFi chip
and print out a scan of nearby WiFi
networks:
import network
wlan = network.
WLAN(network.STA_IF)
wlan.active(True)
print(wlan.scan())
The Connecting to the Internet guide
mentioned earlier has chapters on
using MicroPython to connect to networks, make HTTP requests and build
HTTP servers, including controlling
Besides the added WiFi
(the metal can), the PCB
trace WiFi antenna has
necessitated the SWD
(serial wire debug)
header being moved
to a different location.
Otherwise, the pins
are in much the same
locations as the original
Pico.
The back of the Pico W
has pin markings that
are identical to those
on the Pico. The six test
points all remain in the
same locations. Like the
Pico, the Pico W comes
without headers; the H
and WH variants cost
more but have presoldered headers.
the onboard LED from a web page.
The guide includes source code for
performing those tasks.
C SDK
Similarly, the Connecting to the
Internet guide has a chapter on using
the WiFi features under the C SDK,
although these depend heavily on
downloadable example projects.
We had previously installed the C
SDK, so we simply had to perform
an update at the command prompt
to get access to the new libraries and
examples. New installs of the C SDK
should already include the most up-todate files.
There are a few command line
switches that need to be used in the
“cmake” command for WiFi support:
-DPICO_BOARD=pico_w
-DWIFI_SSID=“Network Name”
-DWIFI_PASSWORD=“Password”
The first of these sets the board to be
a Pico W; we had not needed to use a
switch previously as the Pico was the
default. If you wish to eliminate confusion, the switch argument for a Pico
is simply “pico”.
The other switches set the SSID and
password parameters for a WiFi network. Doing it this way is much easier
than manually updating many source
files. It also avoids having to store these
credentials in a source file that might
need to be distributed to others.
The release notes for version 1.4.0
of the C SDK describe the updates that
coincided with the release of the Pico
W. You can find them at https://github.
com/raspberrypi/pico-sdk/releases
As for the Pico, the Raspberry Pi
Foundation’s guides assume that you
are using a Raspberry Pi computer to
compile for the Pico W. While not the
quickest way to compile code, the
instructions are clear and work well
in that case.
There is also Pico Setup for Windows, which installs all the programs
needed to compile for the Pico and
Pico W using the C SDK. It can be
downloaded from https://github.com/
ndabas/pico-setup-windows/releases
Although the most recent version of
that software predates the Pico W, the
installer can download more recent
SDK files.
Using the Arduino IDE
We tried two different board profiles
for the Pico in our review from last
58
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
year. There is an ‘official’ board profile
that uses Mbed OS and another profile
(Arduino-Pico) that uses the C SDK.
The first is included as one of the
default options that can be installed
by the Arduino Boards Manager, while
the other needs a link to be added to
the Additional Board Manager URL
field under Preferences.
We found that the latter was actually the first to support the Pico W,
although this is perhaps not surprising as it uses the C SDK from the Raspberry Pi Foundation itself. At the time
of writing, we have not seen an official
Arduino core for the Pico W.
So all our tests with the Arduino
IDE for the Pico W have been with the
Arduino-Pico core: https://github.com/
earlephilhower/arduino-pico
That link includes instructions on
how to install this core into the IDE.
Using the Arduino IDE for the Pico
W was as simple as it gets. After updating or downloading the Board Profile,
we set the board to “Raspberry Pi Pico
W” and uploaded the “ScanNetworks”
example sketch. It then produced a list
of nearby WiFi networks on the Serial
Monitor (see Screen 1).
As a test, we tried the Pico W sandwiched between the BackPack and
LCD PCBs, as well as sitting loose
on our workbench. Most networks
showed a decrease of around 10dB
in the indicated RSSI level compared
to when the Pico W was loose and
unshielded by other boards.
That’s probably not critical for most
applications. Still, it’s worth noting
that using the BackPack and accompanying LCD with the Pico W attached
directly will likely reduce the range or
performance of the WiFi chip.
Comparing WiFi boards
The release of the WiFi-capable
ESP8266 almost a decade ago and support for it being added to the Arduino
IDE suddenly made hobbyist WiFi
projects both cheap and straightforward. At that time, many boards under
$10 appeared on the market.
The Pico W is in the same league
as the ESP8266. The newer ESP32 is
better-equipped and offers the promise of more I/O pins. We made a comparison with these in our original
Pico review.
The Arduino IDE does a great job
of using consistent language across
different hardware, making it easy to
try other devices if you are already
siliconchip.com.au
Screen 1: With excellent support for the Pico W in the Arduino IDE via the
Arduino-Pico core, the example sketch to scan for nearby WiFi networks was
easy to compile and run, producing the expected results.
familiar with the ESP8266 or ESP32.
Those using MicroPython should have
little trouble moving across, too.
In the short term, we expect the Pico
W’s documentation to be its strength
compared to other WiFi-equipped
boards, perhaps drawing in a greater
share of novices.
The continuing parts shortages may
give the upper hand to any board
which is simply available (as long as
pricing remains reasonable), and the
Raspberry Pi Foundation appears to
have ample supplies of the RP2040
chips; however, the early supply of
the Pico W is patchy.
In the long term, we think the different boards will find their own niches.
For example, the RP2040’s PIO appears
to have a lot of untapped potential. The
RP2040 also has two cores, although
some devices in the ESP32 family also
do. We will also keep a close eye on
when Bluetooth becomes usable on
the Pico W.
Conclusion
It’s still relatively early days, and we
expect that there will be some refinement to the various libraries and other
software for the Pico W. There are hints
on some forums that the Bluetooth
Australia's electronics magazine
capabilities of the CYW43439 chip
will be put to use.
Devices like the ESP32 (which is
similarly supported by MicroPython
and the Arduino IDE) already offer
various Bluetooth capabilities, such
as serial and audio over Bluetooth
and also Bluetooth Low Energy (BLE).
Hopefully, the Pico W will gain similar features.
We didn’t run into any problems
using the Pico W on our BackPack
with an LCD touch panel, although
the other PCBs in proximity did seem
to attenuate the WiFi signals slightly.
With MicroPython and the Arduino
IDE long having had support for WiFi
and Bluetooth, it won’t be long before
we see projects using the Pico W in
place of other boards using ESP8266
and ESP32 chips, especially at current
prices. At the time of writing, the Pico
W was available from:
∎ Digi-Key Electronics (SC0918)
siliconchip.au/link/abgw
∎ Core Electronics (CSE08703)
siliconchip.au/link/abgx
Other retailers we expect might
stock the Pico W when it becomes
available in volume include Altronics, element14, Mouser and Little Bird
Electronics.
SC
November 2022 59
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High-end
Part 1: By Phil Prosser
Active Monitor Speakers
With Subwoofer
This hifi system takes a ‘no compromise’ approach to build a truly superlative
sound system that will be at home in a modern living room. We are utilising
high-end components that are readily available while avoiding falling into the
abyss of overly expensive, gold-plated parts. The parts used are not cheap
but this system will still be within reach for many people.
T
his new high-end hifi system will
be presented in three parts. This
first part details the design and construction of the relatively compact
main (left & right) speakers that provide excellent sound quality without
being overly obtrusive.
Because these are active speakers,
they need an amplification solution
that integrates an electronic crossover,
which will be the focus of the second
article. The electronics are housed
in an attractive two rack unit (2RU)
black rack-mount case, including all
the amplification, signal conditioning
and power supply circuitry.
The third article will present a
very high-quality Active Subwoofer
to round out the system. It is ideal to
combine with the speakers presented
here, giving a full-range sound system.
However, nothing locks the subwoofer
into use with these particular speakers;
it would be a fine addition to almost
any sound system.
While you could build these speakers without the sub, I reckon almost
anyone going to the trouble of building these will want to extend the bass
all the way down to 20Hz.
So basically, all three parts are
intended to be combined into one
excellent sound system. Still, I have
taken a modular approach, allowing
you to choose which parts to build.
I was a bit cheeky in the intro when
I said there were no compromises.
There are always compromises – in
this case, one of them is that the system is a little on the expensive side.
While most of our recent loudspeaker systems have aimed to be
‘good value’ systems with excellent
sound quality, this one erred more
on the side of ultimate fidelity without worrying too much about the bottom line.
Still, we aren’t talking sheep stations. The four drivers for the Active
Monitor speakers total just under
$1000, while the subwoofer driver is
another $339. Add in all the other bits
and pieces and you can probably build
the speakers for a little over $1500.
Factor in the electronics, and you’re
looking at perhaps a little over $2000;
that’s far from outrageous for a highend speaker and amplifier system.
Another compromise we often make
in our loudspeaker systems is to prefer larger enclosures. That helps us
achieve excellent sound quality at a
reasonable price. But for this system,
I decided that many people these days
do not want huge loudspeakers in their
living spaces.
So I have tried to keep with the modern principle of keeping the speakers
as small as possible without ruining
the sound quality. That is part of the
reason they are a bit more expensive.
It does have the significant advantage
that they are far less likely to be vetoed
by any people who might have the
power to say “no”!
Photos 1 & 2: the SB
Acoustics tweeter (left) and
mid-bass woofer (right) used
in the Active Monitor speakers.
They are quality units with a broad
range of frequencies at which they can
both operate, giving us many choices for
the crossover frequency and slope.
Note that these photos are not to scale.
62
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
Features & Specifications
∎ Modestly-sized bi-amplified monitor speakers plus a subwoofer
∎ Frequency response: 25Hz-20kHz, ±3dB (20Hz-20kHz, +3,-12dB; see Fig.8
and the following article on the Active Subwoofer)
∎ Distortion: <1%, 20Hz-10kHz (typically <0.3% for normal levels; see Fig.9)
∎ Over 400W total power (2×50W tweeters + 2×50W woofers + 1×200W
subwoofer)
∎ Active crossover <at> 2.7kHz (woofer/tweeter) & 90Hz (subwoofer/woofer)
∎ High-end Satori drivers used throughout
∎ Good time alignment between woofers and tweeters
∎ Excellent off-axis response
Driver lineup
For this system, I have chosen
drivers from the SB Acoustics Satori
series, their premium product line.
The ‘Active Monitor’ speakers utilise:
Satori MW16P-8 bass mid-range: a
165mm (6.5in) driver utilising papyrus fibres in the cone with a rubber
surround and a copper sleeve on the
pole piece. That sleeve helps to reduce
inductance change with cone position
and reduces flux modulation and distortion. In this design, it operates down
to 90Hz in the active implementation
and ~40Hz without the subwoofer.
Satori TW29R-B tweeter: a 29mm
ring radiator with a frequency response
within ±2dB over 1-20kHz. It has a low
resonant frequency of 600Hz and a
very well-behaved impedance. Distortion over the frequency range of interest is very low indeed.
Does that sound good? Wait a
moment; a whole octave is missing
from this equation, but it is delivered
by the active subwoofer using the
SB34SWNRX-S75-6. It is a 12-inch
driver, although it is actually 346mm
in diameter, with a 3in (75mm) voice
coil, one of the real measures of
continuous power handling of a driver.
It has a resonant frequency of 19Hz
and a 22mm peak-to-peak linear cone
excursion. In an 80-litre enclosure
tuned to 25Hz, this driver will deliver
solid bass to 25Hz (-3dB) and operate
in its linear region right down to 20Hz
at up to 200W.
The parts combine to form a stereo
system of the highest quality. Both
my measurements and listening tests
reflect that.
The electronic configuration of this
system is shown in Fig.1. Once built,
you just need to plug it into your preamp and away you go.
Let’s now turn our attention to
the Active Monitor speakers that are
the subject of this article. They are a
‘pigeon pair’ with the Active Crossover Amplifier that will be presented
next month. Being active speakers, we
dispense with the cost and complexity
of passive crossover components. We
also benefit from an amplifier directly
driving each driver and the control
that provides.
If you use the Active Monitor speakers without the intended subwoofer,
you can achieve a low-frequency cutoff
The finished speakers shown with subwoofer and Philips CD player. The speakers can be mounted on top of 800mm tall
stands, as shown here, bringing them to about ear height when seated (see the parts list).
siliconchip.com.au
Australia's electronics magazine
November 2022 63
Projects used in a stereo Active Monitor Speaker system
4 x Hummingbird Amplifier – December 2021; siliconchip.au/Article/15126
3-Way Active Crossover – October-November 2021; siliconchip.au/Series/371
Multi-Channel Speaker Protector (4-CH) – January 2022; siliconchip.au/Article/15171
Power Supply – to be described next month
Projects used in the Optional Subwoofer
Ultra-LD Amplifier Mk3 Amplifier – March-May 2012; siliconchip.au/Series/27
OR Ultra-LD Amplifier Mk4 – August-October 2015; siliconchip.au/Series/289
Multi-Channel Speaker Protector (4-CH) – January 2022
Power Supply – to be described in two months
of about 45Hz, but note that you will
have to adjust the active crossover for
that. 45Hz is OK, but by adding the
active subwoofer, you will experience the entire audible spectrum from
about 20Hz to 20kHz. Few speakers
can deliver that, especially with low
distortion.
The drivers are very high-quality
units and, as you will see, their performance is outstanding. While their
price is not stratospheric, the quality
of these components does mean the
cost of building this system is relatively high.
The drivers used have excellent
frequency responses and are well
regarded for their subjective performance. See the panel titled “Subjective vs objective performance” for
some insight into how I approached
this design.
Working on a speaker system that
costs thousands of dollars to build, I
feel that I am obliged to bring both a
scientific and analytic approach. But
I also need to use a somewhat subjective and emotional assessment to tune
the final result. Both approaches have
a place in this exercise.
Photos 1 & 2 show the two drivers
used in the Active Monitor speakers,
while Figs.2 & 3 are plots of their individual frequency responses in a sealed
box at 1m.
Those figures show that, in terms of
simple frequency response, there is a
very wide crossover region throughout which both the woofer and tweeter
have a flat response and do not exhibit
unwanted behaviour such as breaking up, unmanageable resonances,
glitches and the likes. From this measure, these drivers are a good match.
The 30° off-axis measurement provided by the factory shows that for a
2-3kHz crossover point, both drivers
remain well-matched and provide
good off-axis coverage.
Editor’s note: a good off-axis
response is an essential feature of a
hifi loudspeaker unless you only ever
listen from a single point in a room!
The ‘woofer’ actually performs
extremely well out to 10kHz looking
at amplitude alone, but does show
signs of breaking up in the 4.5-5kHz
region.
Fig.1: this block diagram shows the configuration of the speaker system. A single rack-mount case houses the
power supply, four amplifiers for the Active Monitors, the speaker protector and the active crossover. The line-level
subwoofer output drives the active subwoofer, which has an internal power supply and amplifier.
64
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
These drivers are a paper cone type
with Neodymium magnets and the
build quality is excellent. That is evident in the comparison of two drivers
shown opposite in Fig.4. Modelling
this driver indicates that a 21L enclosure tuned between 29Hz and 35Hz
covers Butterworth-Chebyshev alignments. (Butterworth is a response with
a ripple-free passband, while Chebyshev allows a little passband ripple for
a faster roll-off).
Reducing this volume a touch to 18L
and stuffing it well allows us to keep
the size of the enclosure under control
at the cost of the -3dB point moving
up a few hertz, to 44Hz. Given that
we are designing the system to have a
subwoofer, this is a moot point. This
slight reduction in volume means we
can keep the depth of the enclosure
within reasonable limits.
Driver alignment
The relative placement of the
tweeter and woofer is critical to the
operation of the speaker, especially
through the crossover region. Aside
from the obvious function of filtering signals for each driver, the crossover needs to do this in a manner that
results in a flat frequency response
through the crossover region.
There is a critical interplay between
driver placement and the operation
of the crossover, shown in Fig.5. The
result of this misalignment of the
acoustic centre of the tweeter and
woofer is a skewing of the beam pattern of the speaker downwards (about
5° in our case) and a null at the crossover frequency about 5° above horizontal.
These effects occur for signal frequencies in the crossover region and
result in a dip in the speaker’s frequency response. If you are not aware
siliconchip.com.au
Amplitude (dB)
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-40
100
200
500
1K
2K
5K
Frequency (Hz)
10K
20K
Fig.2: the SB Acoustics tweeter’s frequency response, measured 1m away. The
top-end roll-off is almost entirely due to filtering on the front end of the ADC
used to make these measurements.
0
-10
Amplitude (dB)
The MW16P-8 woofer
0
-20
-30
-40
50
50
100
200
500
1K
Frequency (Hz)
2K
5K
10K
20K
Fig.3: the SB Acoustics mid-bass woofer’s frequency response in a sealed box,
measured 1m away. The top end above about 5kHz looks good, but there is
breakup occurring in this region. The roll-off below about 200Hz is due to the
enclosure, while the ripple in the low end is due to room modes. No effort has
been made to make the plot pretty or smooth. The response over the 200Hz3kHz region is excellent.
10
0
-10
Amplitude (dB)
The tweeter response extends well
beyond 20kHz. Cone breakup is not
evident until above 20kHz, and is
well-controlled. So crossing from the
woofer to the tweeter in the 2-3kHz
region will:
1 - Provide a fairly continuous horizontal coverage from the speaker
2 - Have the potential to have a
very flat frequency response
3 - Not excite breakup modes in
the woofer
4 - Operate the tweeter several
octaves above its resonance (600Hz)
-20
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-40
-50
-60
1K
2K
3K
4K
5K
6K
7K
8K 9K 10k
12K
14K 16K 18K 20K
Frequency (Hz)
Fig.4: a frequency response plot comparing two woofers. I suspect that some of
that difference is me standing a little too close to the measurement system! It is
also very pleasing to note that the response is extremely smooth and flat. The
ripple visible below about 1kHz is entirely room modes.
of this, it can make designing a crossover very confusing!
There are a few ways designers
tackle this problem. The most direct
manner is to increase the output in
Australia's electronics magazine
this crossover region by playing with
crossover frequencies and shifting
the phase at crossover by pushing the
tweeter crossover frequency down.
That approach can work but has the
November 2022 65
effect of putting more energy into the
room at off-axis angles.
Editor’s note: I reiterate my earlier
point that little change in sound quality or frequency response off-axis is
very desirable.
Another approach is to offset the
drivers. There are several ways to
approach this; a famous example is
the Duntech speakers from the nineties, which used stepped baffles and
acoustic treatment to reduce diffraction from the edges.
My solution is a bit of a mix of the
two approaches. If this sounds like I
am hedging my bets, I kind of am. I
have opted for a gently-sloped baffle
that somewhat offsets the tweeter back
from the woofer (see Fig.6). I have also
recessed the tweeter, which is good for
avoiding diffraction around the transition of the tweeter face plate to the
front panel.
The woofer is not recessed; I simply
applied felt around it to help reduce
the visual and acoustic impact of this
choice.
It would have otherwise been
Fig.5: the drivers have different depths, so their ‘acoustic centres’ are not aligned
when installed on a flat panel. Around the crossover frequency, both drivers
are producing signals, and the phase shift due to this misalignment causes
undesirable reinforcement and cancellation at different locations in the room.
necessary to slope the front panel back
by 8° to get the offset between tweeter
and woofer perfect.
My tests show that the result is quite
good. By recessing the tweeter, we get
away with a modest 5° tilt on the front
panel while keeping the drivers in time
alignment. To my eye, the sloped front
makes a pleasing change from a rectangular cube for a speaker. Still, the
effect is subtle enough that you won’t
even spot the front panel tilt in many
of the photos.
The crossover
I have set the crossover frequency
to 2.7kHz, implemented by an active
crossover in the amplifier. I have also
implemented ‘baffle step correction’
in the amplifier. This accounts for
the effect of acoustic radiation from
the speaker transitioning from omni-
directional at low frequencies to directional at high frequencies.
The transition frequency is a function of the driver and its location on
the front panel. The step can be as
much as 6dB, but in our case, a boost
of 3dB at frequencies below 250Hz
works well.
As the speakers are bi-amplified,
each driver is powered directly from
its own amplifier. However, I have
included a large 100μF DC blocking
capacitor (Jaycar Cat RY6920) in series
with the tweeters as the last line of
defence against faults or crossed wiring.
This capacitor has no effect in regular operation but will save your bacon
should LF or DC signals somehow
make their way to the tweeters.
If substituting this part, make sure
you use a high-voltage, high-current
capacitor; many small 50V-rated bipolar capacitors do not have the ripple
current rating for use in loudspeakers.
Performance
Fig.6: by tilting the front panel and using some other tricks, we bring the
‘acoustic centres’ into horizontal alignment, so the signals around the
crossover frequency coincide, and we avoid constructive and destructive
interference.
66
Silicon Chip
Australia's electronics magazine
Measuring the system’s overall frequency response was an exercise to
minimise room reflections. The final
plot (Fig.7) is a composite showing two
measurements, one with the speaker
on a stand and measured at 1m, the
second plot with the speaker facing
upwards. Both plots are smoothed
one-third octave to eliminate the usual
‘fuzz’ you get on these plots.
It might look a bit lumpy, but loudspeaker systems are notoriously difficult to characterise in this way. As
speakers go, this is actually remarkably
siliconchip.com.au
flat when measured indoors, on average from around 25Hz up to 20kHz.
Fig.8 is a frequency plot measurement made outside over grass near the
shed. For a stand 80cm tall and 1m
from the microphone (with the speaker
cone at about 0.9m), the “bounce path”
is 2.06m (2 × √0.9m2 + 0.5m2). The
direct path is 1.0m, the difference
being 1.05m. Because it’s measured
outdoors the -3dB point is shown at
35Hz rather than 25Hz quoted above.
Subjective vs objective performance
The engineer in me always thinks, “if you can’t measure it, then you can’t
hear it”. Ultimately, this is true. But the question is: what exactly do we
need to measure to determine what makes one speaker sound better than
another?
I have run tests to see what I can hear compared to what I can measure.
I have been surprised at the results, concluding that the ‘character’ of a
speaker comprises not only the gross frequency response but is also influenced by less overt parameters such as the stored energy in the driver, its
breakup modes and distortion profile.
The lessons my experience brings to the Active Monitor speakers are:
■ We should operate the drivers well within their linear regions
■ I took note of trusted reviewers’ opinions of the drivers
■ I considered the stored energy (waterfall plots) of the drivers
■ I sought to match the beam patterns of the drivers via the crossover
■ I prefer higher crossover rates where practical
■ I stuck to drivers with few breakup modes and definitely avoided exciting
them
■ After designing the system using proper engineering principles, I still
needed to listen to the result and then tune or tweak it until I was happy
with the sound
■ I shouldn’t be afraid to tune a speaker, but I should consider why I am
making any given change
siliconchip.com.au
Amplitude (dB)
The cabinet material you choose
comes down to the finish you want,
your skill at woodworking and cost.
I recommend you use MDF, plywood
or chipboard. All these materials
will work fine for the Active Monitor
Speakers.
I prefer MDF over ply. MDF is
denser and has a reputation as a
“deader” material than chipboard. But
be warned, it is also heavier and makes
an extraordinary amount of dust when
cut and routed. Wear a mask while
working with it; breathing this dust
can be harmful to your health.
My woodworking skill is modest,
and in building the prototypes, I have
intentionally stuck to tools that most
people would have. The tools I recommend using are:
1 – Circular saw
with the cut angle adjustable to 5°
I used a cordless circular saw and it
worked great. My old mains-powered
unit would also have been fine for the
job. A younger or skilled person could
possibly make these cuts with a hand
saw, but they would be nowhere near
as clean or accurate.
2 – Jigsaw
Used for a couple of cuts, especially
180
120
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60
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Fig.7: two frequency response plots of the overall system. Depending on where
and how the speaker is located, we can move the low-frequency dip around and
usually work out what is causing it. The only way to avoid it entirely would
be to stick the speaker up a tall ladder, but that’s a bit awkward! So it’s best to
ignore the very bottom of the frequency response as it was taken outdoors.
10
0
Amplitude (dB)
Building the
Active Monitor speakers
10
Phase (deg)
For sound travelling at 343m/s or
so, the half wavelength frequency is
163Hz, which is pretty close to the dip
in that figure. That shows this is a test
setup phenomenon, not the speakers.
-10
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20
50
100
200
500
1K
Frequency (Hz)
2K
5K
10K
20K
Fig.8: a frequency response measurement of the speaker system in a relatively
open grassy area. That dip at 159Hz is because the measurements were taken
outside with the sub arbitrarily placed.
Australia's electronics magazine
November 2022 67
in the braces. You could use a small
handsaw instead, but it would be a
miserable task.
3 – Cordless drill/screwdriver
You will also need various drill
bits and a Philips No.2 driver bit for
the screws.
4 – Router and bits plus a circle jig
You will need a 10mm round over
bit (or similar size), a 6mm round
over bit (or similar size) and a 16mm
straight cut bit.
5 – Sash clamps
You’ll need at least two; many more
if you choose to glue the enclosures
only (not glue & screw).
6 – Sanding disc with 120 grit paper
This will be used to smooth the
edges before routing. It is possible
to do this by hand if your assembly
is clean.
7 – 120-400 grit sandpaper and block
Buy lots of 120, 240 and 400 grit
sandpaper (you can buy it as 5m rolls).
Change paper frequently to reduce the
amount of elbow grease required.
8 – Builders’ bog
To smooth over gaps.
9 – 100mm roller, short nap
For applying the acrylic primer.
Assembly tips
If possible, attach your vacuum
cleaner to your router. If you don’t
do this, don’t say I didn’t warn you!
It’s also important to work in a well-
ventilated area to help prevent inhalation of sawdust.
Work out what final finish you are
aiming for before you start. This will
affect your construction method and
Fig.9: a distortion
plot for the overall
system. These
levels are very low
for a loudspeaker
system, where
0.5% is considered
good. It is excellent
between 50Hz and
1kHz, with the
distortion generally
below 0.33%.
The distortion is
primarily second
harmonic; the third
harmonic is very
low, which is why
these speakers
sound so good.
planning. I chose to go for a smooth,
painted finish. This choice was driven
by cost, my existing décor, and to allow
me to demonstrate that you can produce a good speaker finish at home
with no special tools.
I have laid out the design with
rebated joints, allowing you to glue
and clamp or glue and screw the enclosure together. It requires some precision in routing, but once your jig has
been set up, that is reasonably easy to
achieve. If you do not have a router,
fear not. Rejig the panel sizes to use
butt joints and screw them on the end
grain (with pre-drilled holes!).
Fig.10 shows the cuts for a 2400mm
x 1200mm sheet of 16mm-thick MDF
(or two or three smaller sheets). I could
have brought the sheet home in a ute
and made all the cuts myself, but
instead, I asked the nice people at my
Photo 3: my simple jig allows quick
and repeatable 90° (and angled)
cuts and routed lines to be made.
This saved hours of fiddling with
clamps at the cost of a few timber
off-cuts. You can use this with a
saw or router but be prepared to
throw away your ‘alignment edge’
every time you change the angle.
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local hardware store to cut two vertical
strips 188mm wide, two 210mm wide
and two 358mm wide. I took the extra
as an off-cut.
That lot slid easily into a VW golf
hatchback, and everything, including
cutting, was $50 – the cuts came free.
There aren’t many free things in life,
so you might as well take what you
can get!
Figs.11, 12 & 13 show the details
of the various panels that make up
the enclosures for the Active Monitor
speakers. Cutting the panels from the
strips is relatively straightforward; just
note that accuracy here will pay dividends in final assembly. Some things
to keep in mind are:
• The front panel and the internal
brace are sloped back by 5°. I set my
circular saw to an angle of 5° and admit
to using some bog to smooth these joins
in my assembly.
• All rebates are routed to a depth
of 5mm. Do a test cut or two and get
this right; do not cut too deep, or your
panels will need trimming to fit.
• If you need to trim a panel, plane
or use a disc sander – you do not want
to lop off large chunks of timber.
• Keep track of your left and right
panels as they have the routing on
opposite sides!
I used an extremely simple jig to
allow simple right-angle and 5° cuts
and routed lines to be made, as shown
in Photo 3.
Once you have cut the panels to
size, mark and route the rebate for the
tweeter, which is 104mm in diameter
and 5mm deep. Check that the tweeter
fits your circle by routing an off-cut.
Next, cut the tweeter and woofer
holes, noting that there are two notches
siliconchip.com.au
Making circular rebates for the tweeters
You need a router circle jig to make neat rebates
for the tweeters, as they will be visible. You can
buy a circle jig for most brands of routers, but you
can also make one.
Get a flat sheet of aluminium about 100mm wide
and 250mm long and drill a hole near one end
that’s larger than your biggest router bit. Measure
and drill mounting holes for the router relative to
that and countersink them so the screws will not
scratch the timber.
Next, drill a series of 3mm holes to provide
various radii from the router bit and countersink
them from the top.
Attach the jig to a centre hole on your workpiece
using a countersunk M3 machine screw with an
extra nut between the jig and the workpiece to keep
it stable, and voila, you have a circle jig. Just make
sure to test it on offcuts to select the ideal hole in
the jig before doing the final rebate.
Fig.10: here’s how to cut the full set of Active Monitor panels from one or two MDF sheets. Smaller sheets could be used,
or as described in the text, take advantage of the free cutting service offered by many hardware stores. Cut these as
accurately as possible, then route and cut the indicated holes in the panels for the drivers, ports and holes in the brace.
siliconchip.com.au
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November 2022 69
in the tweeter cutout to accommodate
the connection terminals. Once the
front panel is finished, you can cut
the holes in the brace. I marked these
and then used a jigsaw. There is nothing terribly special about the dimensions on these cutouts, but you want to
leave sufficient material to strengthen
the enclosure.
Finally, cut out the speaker terminal
hole. Again, a jigsaw is handy but not
essential. Also make the cutouts for
the input terminals and speaker port
on the rear panel.
Now route all the rebates. I recommend setting up a jig as this will save
you a lot of time and give you consistent route line locations.
Cabinet assembly
Whether you plan to simply glue
and clamp or glue and screw the enclosures, do a dry assembly to check that
all the joints are neat and fit correctly.
Make any adjustments now, so that
everything sits flush.
If you are planning to screw the panels together, be prepared to drill 2.5mm
pilot holes for your screws and countersink the heads. If your timberwork
is neat and achieves a clean and tight
fit together on dry assembly, simply
gluing the enclosures together is something you could consider.
Apply a generous layer of glue to
both surfaces and use masking tape
to hold panels in place if you find
yourself looking for an extra hand.
Wipe away excess glue as you assemble them, keeping everything relatively clean.
With the rebates and internal brace,
which sit horizontally between the
front and rear panels, the boxes should
fit nicely together. Jiggle the panels
into their final places and add sash
clamps to hold the lot together while
the glue sets. To ‘clamp’ the top and
Fig.11: details of the Active Monitor front and rear panels. Note the notches for the tweeter terminals, the rebate to recess
the tweeter and the rectangular areas routed out of the inside for the internal brace.
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siliconchip.com.au
bottom panels down, I sat the assembled speaker on the floor and put some
bricks and a hefty box of transformers
on top of it, as shown in Photo 4.
Once clamped, take a damp cloth
and wipe all excess glue from the
joints. This is an essential step as sanding PVA glue is extremely difficult.
Applying the finish
No matter how you choose to finish your speakers, the most important
thing is preparation. Once the glue
had set, I used a sanding disc to sand
back all external joints to flush. I then
used ‘bog’ to fill any gaps between
joints, being extremely careful not to
overfill. The sand-and-fill process was
Fig.12: details of the top and bottom panels, and the internal brace. The brace fits horizontally between the drivers and
ensures good rigidity. The bottom panel is larger than the top due to the angled front.
Fig.13: details of the side panels, which are trapezoidal to fit the tilted front panel. The routed areas are where the front
and rear panels attach as well as the horizontal internal brace.
siliconchip.com.au
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November 2022 71
Photo 4:
one Active
Monitor
speaker box,
glued and
clamped,
waiting to
dry. This sat
for 24 hours
before further
work was
undertaken.
repeated, moving through 120 grit to
240 grit sandpaper until the boxes
were totally smooth.
You will see in the photos that I
rounded the speakers’ edges. The front
edges have a 10mm radius curve to
the edge, while the sides have a 6mm
radius. The front edges are rounded to
reduce diffraction, although if your finish demands a square edge, that will be
OK. My earlier prototypes had square
edges and did not show significant
refraction-related problems.
Next, I used a roller and acrylic
primer to seal the timber, paying particular attention to the end grain. We
need this sealed; otherwise, it will
absorb paint and be visible through
the top coat. The primer had an
orange-peel effect which required yet
more sanding with 240 grit paper to
make the finish smooth, as can be seen
in Photo 5.
After the acrylic primer had been
sanded totally smooth, I applied a
spray primer. This sealed any patches
of MDF showing through. I sanded
that again using 400 grit paper and
then applied two top coats with a
light sanding using 400 grit paper in
between. I used “satin black”, which
is more matte than gloss. Gloss is the
worst case for showing any flaws.
Luckily, the results were excellent. Photo 6 shows the least flattering aspect of the speaker, with a slight
imperfection along the top rebate joint
at the rear. I almost filled and re-coated
this to make them perfect, but the
reality is this is only visible from this
angle, so I considered the extra effort
unwarranted.
Installing the drivers
Set the speaker port to 100-110mm
in length. This does not need to be
super exact; a 90 to 115mm range is
acceptable. The specified Altronics
port is 110mm long with the adjustable extension removed. Install and
screw the port in, as shown in Photo 7.
The connector is the ideal place to
mount the protection capacitor for
the tweeter. The 100μF capacitor will
protect against the application of DC
and provide a small measure of protection against modest levels of fullrange signal. However, it will not protect against prolonged high-level low-
frequency material.
To prepare the connector, you must
take the bridging straps off before soldering anything to the tabs.
I hot-melt glued the capacitor to the
input connector and wired it directly
in series with the tweeter wire. I used
1mm2 (17AWG) heavy-duty speaker
cable for the tweeter and woofer connection. Make sure you cut these long
enough that you can solder them to the
drivers when you install them.
I started with 600mm lengths, soldered them to the input terminals and
trimmed them to length when I connected the drivers – see Photo 8. Mark
the woofer and tweeter connections so
Photo 5: the primed Active Monitor speakers drying in front of the air
conditioner. These were later sanded smooth before applying spray
primer, then sanded again before the top coat.
Photo 6: the
ultimate finish,
shown at the least
flattering angle (see
the top rear). A final
smear of filler and a
couple of top coats would
resolve this, but I figured
it wouldn’t be visible in the
listening room.
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Australia's electronics magazine
you do not get them confused. I also
suggest labelling the connectors on the
exterior of the box so that in the future,
when you have forgotten how you built
these, the connections are clear.
Poke the speaker wires into the
enclosure, put foam tape around the
terminal cutout, then screw it down
with four wood screws.
Next, cut two strips of thick wadding about 1m long, fold one and stuff
it above the brace, then the second one
below it. The aim is to loosely fill the
enclosure with wadding to damp rear
radiation into the enclosure.
The drivers have pre-installed foam
gaskets. Solder the tweeter wires
to the tweeter, being careful to get
the phasing correct. Now screw the
tweeter in and follow by installing
the woofer. Secure the drivers with
16mm screws.
Finally, I installed the felt. It is best
to cut the circles after it has been stuck
to the front panel but cut the straight
lines using a ruler and sharp knife
before installing. The pattern I used
is shown in Fig.14.
This is required as we are mounting the woofer flush to the front panel;
the felt neatens the appearance and
allows the woofer to be moved forward, improving time alignment and
reducing diffraction.
Depending on the felt you can
source, you might need two layers.
Ultimately, you want the felt flush
with the woofer frame.
Parts List – Active Monitor Speakers (per pair)
1 Amplifier/Crossover (to be described next month)
1 active subwoofer (optional; but recommended; described next month)
2 SB Acoustics Satori MW16P-8 165mm mid-woofers
[Wagner Electronics – siliconchip.au/link/abfi]
2 SB Acoustics Satori TW29R-B 29mm ring tweeters ➊
[Wagner Electronics – siliconchip.au/link/abfj]
2 100μF 100V bipolar crossover capacitors [Jaycar RY6920] ➋
2 35mm adjustable speaker ports [Altronics C3638]
2 bi-wire speaker terminals with two independent inputs [Altronics P2019]
1 2400 × 1200 × 16mm sheet of MDF or similar, cut as per Fig.10
30 16mm-long 8G wood screws
1 2m length of 1mm2 (17AWG) figure-8 speaker [Altronics W1936]
2 5mm-thick sheets of dark felt, 300 × 200mm
1 5m length of 5-10mm wide soft foam sealing tape (for sealing driver and
terminal holes)
1 2m × 1m acoustic wadding blanket [Lincraft “king size thick wadding”]
1 300mL tube of PVA glue
1 500mL tin of acrylic primer paint
2 350g cans of spray primer paint
2 350g cans of spray paint (for two or more top coats)
➊ If you’re ordering the drivers from Wagner and want to build the
subwoofer, you can get the SB34SWNRX-S75-6 subwoofer driver at the
same time (siliconchip.au/link/abfk).
➋ Increasing the value up to 220μF is beneficial but not required. Make sure
the capacitors can handle the currents involved.
Parts for optional stands (per pair, 800mm tall)
2 2m lengths of 120 × 19mm DAR pine
2 300 × 300 × 16mm sheets of MDF or similar
2 200 × 140 × 16mm sheets of MDF or similar
8 75mm-long 10G wood screws
8 50mm-long 10G wood screws
1 250mL tin of acrylic primer paint
1 350g can of spray primer paint
1 350g can of spray paint (for two or more top coats)
Fig.14: cut the felt to
this shape and glue
it to the front of the
speaker. It serves
two purposes: to
prevent sound from
refracting from the
edges of the drivers
and to hide the
difference in the
mounting styles of
the two drivers.
Photo 7: the rear of the speaker,
showing the texture you get if you
don’t sand the undercoat. This also
gives you a good view of the vent and
the terminals.
siliconchip.com.au
Australia's electronics magazine
November 2022 73
Speaker stands
Where and how you use your Active
Monitor speakers is a personal choice.
That said, positioning is important;
having them at ear level is a good idea.
My speakers are in a listening
room and I wanted some stands to
set them at the right height. I made
suitable speaker stands from off-cuts
of MDF and 120 × 19mm DAR pine
timber. I used angled braces to make
them both stronger and more visually
interesting.
Fig.15 shows how you can make
some of these simply and cheaply. I cut
the timber as shown, primed, sanded
and applied a top coat in a similar
manner to the Active Monitor speakers. The overall height of the stands as
specified is 800mm; you can tweak the
height to suit your needs.
Testing
We’re getting a bit ahead of ourselves
Fig.15: the details of the low-cost but sturdy and attractive stands I designed for the Active Monitor speakers. You can
probably cut the base and top plates from off-cuts of the material used to make the speakers.
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siliconchip.com.au
-27
150
-30
100
-33
50
-36
0
-39
-50
-42
-100
-45
1.0K
1.5k
2.0k
2.5k
3.0k
3.5k
Frequency (Hz)
4.0k
4.5k 5.0k 5.5k 6.0k
6.5k 7.0k 7.5k 8.0k 8.5k 9.0k 9.5k
Phase (deg)
Amplitude (dB)
here because you’ll need to build the
amplifier/crossover system described
in the article next month to test your
new speakers properly. Still, this is
an appropriate place to discuss how
to check that everything has gone
together properly, so let’s proceed on
the assumption that you have already
built the electronics.
A good test for a crossover and
speaker alignment is to invert the
tweeter phase and see if there is a dip
at the crossover frequency. Fig.16
shows a 10dB dip in the response at
the crossover frequency when I invert
the phase of the tweeter. This indicates
that the time alignment is correct and
that everything in the system is working as planned.
-150
Fig.16: a major dip is seen in the frequency response when the tweeter phase
is inverted. This sound cancellation shows that everything is well aligned and
working as expected.
Calibration and use
Assuming you are setting the output level controls on the 3-Way Active
Crossover, I recommend you use an
oscillator and AC voltmeter. The oscillator could be your PC audio output.
Be a little cautious using DVMs as an
AC voltmeter as some do not respond
to signals above 400Hz, so check you
get sensible readings. The steps are:
1 - Unplug your Active Monitor
speakers from the Active Crossover
Amplifier.
2 - Set the woofer level to maximum.
3 - Set your oscillator to generate
400Hz at 1V RMS.
4 - Measure the woofer output of
the active crossover or amplifier. These
should be 0.65V/12.6V RMS respectively; ±1dB precision on these is 0.580.73V & 11.2-14.1V.
5 - Now set your oscillator to 5kHz.
Check that your meter still reads 1V
RMS at the input to the Active Crossover Amplifier.
6 - Adjust the tweeter volume control to get 0.24V/4.7V RMS on the
active crossover or amplifier’s tweeter
output; ±1dB precision on these is
0.21-0.27V/4.17-5.25V.
7 - Set your oscillator to 40Hz and
check that your meter still reads 1V
RMS at the input to the Active Crossover Amplifier.
8 - Adjust the subwoofer volume
control to get 0.59V RMS on the subwoofer output; ±1dB precision on this
is 0.48-0.61V.
It is probably best to set the subwoofer output by ear as there can be
huge differences between listening
rooms. Adjust the level up until it
siliconchip.com.au
Photo 8: I used hot melt glue to attach the DC block capacitor for the tweeter to
the back of the speaker terminal. I then soldered 600mm of heavy-duty speaker
wire to the terminals, ready for attachment to the drivers.
sounds ‘bassy’, then back it off until
the sound is dry. The right level is in
between those settings. If you have an
SPL meter, use it, just be aware that
your room will create all sorts of interesting peaks and dips.
Some say that two subs can help fill
these, but it is an expensive proposition. Still, there’s absolutely nothing
stopping you using both subwoofer
outputs from the Active Crossover
Amplifier to drive one sub each. In
that case, you’ll initially want to set the
subwoofer output closer to 0.4V RMS.
I adjusted the baffle step correction to achieve optimal subjective
sound quality in my listening room.
You might wish to tweak this to suit
your room.
This is because the baffle step corrects how much sound is heard at the
listening spot – but remember that diffraction merely redirects the sound off
Australia's electronics magazine
to the side, and the sound is still in
the listening room. So each room may
demand a different correction.
Increasing the 2.2kW resistor will
reduce the amount of baffle step correction (and reduce the frequency at
which the correction kicks in). The
recommended value should be correct
in many situations, but you may like
to experiment with it.
I trust that you will enjoy building
and tweaking, then listening to these
very high-quality speakers and possibly making your own version inspired
by some of these ideas.
Next month
The second article next month will
describe the Active Crossover Amplifier system for driving the Active Monitor speakers. After that, we’ll have an
article on building the matching High
Performance Subwoofer.
SC
November 2022 75
Using WiFi with the
GPS-Synchronised Analog Clock
By Geoff Graham
ur new GPS-Synchronised Analog
O
Clock Driver featured in the September issue has been a great success,
it with the new GPS Synchronised
Clock. If you want the full details, read
the original article at siliconchip.au/
Article/15466
The recommended WeMos D1 Mini
WiFi module is available from many
sources, including Altronics (Cat
Z6441) and Jaycar (Cat XC3802), as
well as on eBay, AliExpress etc.
The original module is made by a
Chinese company called Lolin, but
many clones exist. While they may
look different, they have the same
form-factor and pinout and work just
as well.
When buying the module, make sure
it is the D1 Mini version. There are
other variations called D1 but without
the Mini suffix; they are much larger
and will not fit in the space reserved
for the GPS module.
with hundreds built. It was so popular
that there was a two-week backlog of
kits until early October (kits are now
back in stock).
However, some constructors have
reported difficulties with the GPS
module being unable to get a signal.
This is usually because the GPS signal is blocked or heavily attenuated
when used in a multi-level house or
building, a building with a steel roof
or even heavy rain.
The solution is Tim Blythman’s
“Clayton’s GPS”, described in the April
2018 issue (siliconchip.au/Article/
11039). This is a WiFi module that
emulates a GPS module, but it gets the
time from a public time server on the
internet using the network time protocol (NTP).
Besides the WiFi module, it does
not require any extra components and
is a drop-in replacement for the GPS
module specified in the September
article. You could swap back and forth
between the two, and the clock would
not notice the difference.
This article briefly describes how
to set up the WiFi module and use
Loading the firmware
To make the D1 Mini emulate a
GPS module, you need to load the
appropriate firmware, which can be
downloaded from siliconchip.com.
au/Shop/6/52 The following description is based on the Windows operating system.
You can load the firmware using
other operating systems, but that will
require the Arduino IDE software.
That process is described in the original Clayton’s GPS article from April
2018.
First, plug the D1 Mini into a USB
port on your Windows computer.
It will connect as a serial-over-USB
device. No device driver is required
for Windows 10 or 11. Open Device
Manager and you should see it listed
as “USB-SERIAL CH340” – see Fig 1.
Note the COM port number, which is
COM23 in this example.
Next, run the program file named
“ESP8266Flasher.exe”, which is
included in the firmware download.
This is an easy-to-use programmer for
ESP8266 devices developed by www.
nodemcu.com
When you start the programmer,
it will guess the COM port number
(see Fig.2), so the first thing that you
should do is check that it has selected
the correct number for the D1 Mini.
Then you need to click on the Config
tab and enter the path to the firmware
file, “ NTP_client_for_ESP8266_GPS_
OUTV12.bin”.
Leave the starting address at
0x00000 (hexadecimal value) and do
not change any of the settings in the
Advanced tab. Finally, return to the
Fig.1: when you plug the D1 Mini into a computer running Windows, Device
Manager will show the COM port allocated to it.
►
Fig.2: ESP8266Flasher.exe is an easy-to-use programmer for the D1 Mini. It has
correctly guessed the module COM port here, but you should still check it.
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siliconchip.com.au
Operation tab and click the Flash(F)
button.
The programmer will load the firmware. While that is happening, the blue
LED on the D1 Mini should flicker rapidly. When the programmer has finished, it should show a green tick on
the bottom left corner of the program,
indicating that it was successful. If
you do not see that, click on the Log
tab and scroll to the end of the log to
view any error messages.
NTP GPS Source Setup:
Current Baudrate:9600
1.Set 4800 Baudrate
2.Set 9600 Baudrate
3.Set SSID. Current:SSID
4.Set Password. Current:PASSWORD
5.Set NTP Server. Current:pool.ntp.org
6.Set Dummy Coords. Current:3351.000,S,15112.000,E
9.Exit and save
Enter a number:
❚
Fig.4: the WiFi
module fits neatly
in the space
usually occupied
by the GPS module,
and only three
connections are
required.
Configuring the firmware
After successfully loading the firmware, disconnect and then reconnect
the USB cable. That will reboot the
module, and the blue LED on the top
of the module should illuminate and
stay on.
Open a terminal emulator like Tera
Term (https://tera-term.en.lo4d.com),
set the baud rate to 9600 and connect
to the COM port used by the D1 Mini.
You will see the output of the module,
which will be emulating a GPS module that cannot find a signal.
Using the terminal emulator, enter
the tilde (~) character on your keyboard and you should see the setup
menu as shown in Fig.3.
Change the SSID and Password to
suit your network, then save and exit
the configuration menu by pressing
9. None of the other settings need to
be changed.
Finally, disconnect and reconnect
the USB cable, and the D1 Mini module should start up with the blue LED
coming on solidly. That indicates the
firmware is connecting to your WiFi
network, accessing the internet and
contacting a public time server. The
blue LED will change to a brief flash
every second when the firmware has
received the current time.
If you reconnect with your terminal
emulator, you will see that the module is now producing GPS-compatible
messages indicating the correct (UTC)
time.
Installing the module
The module fits neatly into the
space reserved for the GPS module
on the clock controller PCB, as shown
in Fig.4.
Only three wires are needed: the
pin labelled 5V on the module connects to the solder pad labelled “RE”
on the controller board; pin G on the
module to pad “BK” on the main PCB;
Inductor part code mix-up
The 10 × 10mm inductor (L1) used to build the prototype, RS Components 496-0401,
fit the PCB nicely and worked well. As such, we provided the part code from that item’s
description in the parts list (EPCOS B82462-A4).
We now know that the correct part code is B82464-A4 (that code appears on the RS
page, just further down). By the time customers clued us in, we had supplied hundreds
of EPCOS B82462-A4 inductors in kits from another supplier.
They are electrically compatible, just smaller at 6 × 6mm. If ordering that part from
RS, you will need to use the part code we gave in the parts list, as that is what they use,
but from any other supplier, use the correct part code (B82464-A4-472M).
If you already have the part (eg, you got it as part of a kit), we recommend you solder one side to a pad on the PCB, then use a component lead off-cut to bridge the gap
between the other side and the opposite PCB pad. Many constructors have successfully built the kit that way.
To make construction easier, we will be supplying a redesigned PCB that will accept
either size of inductor. Those new PCBs should be available by the time you are reading
this and will be included in future kits.
siliconchip.com.au
Fig.3: this is the
configuration menu
for the module. You
need to change the
SSID and Password
entries, but the
remainder of the
settings can be left
as they are.
Australia's electronics magazine
and pin TX on the module to pad “BU”
on the PCB.
Finally, attach the D1 Mini to the
controller board using double-sided
tape.
When you insert cells into the clock,
you should see the module’s blue LED
illuminate for a few seconds while
it accesses the internet, changing to
a flash when it gets the correct time.
Almost immediately, the clock controller’s microcontroller will power
down the module (because it has the
correct time) and the LED on the controller board will start a long flash
every second. That indicates that it is
waiting for the next hour or half-hour
to start the clock running.
That’s it! You can hang your clock on
the wall, and it will keep accurate time
for as long as it can reach the internet
via your WiFi network.
Incidentally, your clock will keep
going even if you turn off your WiFi
(for example, if you go on holiday).
Then, when you re-enable your WiFi,
the clock will get the correct time when
it next tries to synchronise (within 24
hours) and immediately correct any
error that accumulated while you
were away.
D1 Mini module kit (SC6472)
We will be offering the D1 Mini as
an option for the current kits instead
of the GPS module – note that the D1
Mini will require programming. SC
November 2022 77
Using Electronic Modules with Jim Rowe
PM (particulate matter)
“Dust” Sensors
In this last article on low-cost air quality sensors, we look more closely at
particulate matter (PM) sensors, also called “dust” or “smoke” sensors.
A
s mentioned in the first of these
articles, PM sensors fall into three
groups based on the size of the particles they are designed to detect: less
than 10μm (PM10), less than 2.5μm
(PM2.5) and less than 1μm (PM1.0).
Currently, PM2.5 types are the most
common in the low-cost section of the
market, so we’ll concentrate on modules that support it.
The basic principle of the most
common type of PM sensor is shown
in Fig.1. This was described in the
first article but we’ll briefly go over
it again. A small fan pulls air from
the surrounding environment into a
channel which passes through a sensing chamber. A laser sends a focused
beam of light through the chamber,
and any particles in the air scatter the
light towards the sides of the chamber.
One or more photodiodes detect
this scattered light on the sides of the
chamber. Any light not scattered by
particles passes through the chamber
to be absorbed by the ‘beam dump’.
By controlling the fan speed and
thus moving the air through the sensing chamber at a known rate of volume and measuring the photodiodes’
output, the concentration of particles
in the air can be calculated.
The result is in terms of μg/m3
(micrograms per cubic metre), because
the traditional and most accurate way
of measuring PM is the ‘gravimetric’
method. This involves using a preweighed clean filter to collect particles from the air over a 24-hour sampling period, then weighing the filter
again to determine the total mass of the
accumulated particles in micrograms.
The concentration is then obtained
by dividing this figure by the total volume of air that passed through the filter
during the 24-hour sampling period.
Available PM modules
There are several low-cost PM sensors currently available, including the
Grove-Laser Sensor module, based on
the Seeed Studio HM3301 sensor from
Shenzhen, China, and the SN-GCJA5
sensor made by Panasonic Photo and
Lighting Co in Osaka, Japan.
The first is a fan-type sensor, as
shown in Fig.1. But other types of
PM sensor modules do not have an
internal fan, including the Panasonic
SN-GCJA5 and the XC3780 from Jaycar,
The Grove-Laser air sensor module is based on the Seeed
HM3301 particulate matter sensor. The sensor itself measures 38
x 40 x 15mm and the module comes with a suitable cable.
Fig.1: the basic operating principle of a particular matter (PM) sensor. Air is drawn through a chamber with a laser beam,
and any laser light scattered by particles in the air is picked up by one or more photodiodes.
78
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siliconchip.com.au
Fig.2: the components of the HM3301 sensor. The part at left is basically identical
to what’s shown in Fig.1, while the section at right shows the electronics that pick
up the scattered light level and turn it into a digital measurement.
based on the Sharp GP2Y1010AU sensor. We will look at all three of these
sensor modules in this article.
The Grove-Laser module
The Seeed Studio HM3301 sensor
comes inside a compact plastic and
metal case measuring 38 × 40 × 15mm.
In addition to the fan, laser and photodiodes, it has built-in electronics that
provide fan control, photodiode signal
amplification, filtering, multi-channel
data acquisition and an MCU (microcontroller unit) for data processing.
The output is via a two-wire I2C serial
interface.
In the Grove-Laser module, the
HM3301 sensor is mounted on a PCB
measuring 80 × 40mm, with a four-pin
connector at one end for connections
to a 3.3-5V power supply and the I2C
lines for connection to a PC or an external MCU. The effective PM2.5 measuring range of the module is 1-500μg/m3,
although it can measure up to a maximum level of 1000μg/m3.
This module is available from
Australian distributor Pakronics in
Rosanna, Vic for $46.06 plus shipping
and GST, totalling $62.07.
Fig.2 shows a functional block diagram of what’s inside the HM3301 sensor. The actual PM measuring section
with the fan, laser, detection chamber,
and photodiode detector is on the left.
On the right is the electronics section
with its filter/amplifier, multi-channel
acquisition and internal MCU for digital signal processing and the I2C data
communication interface.
Since the HM3301 sensor operates
from a 3.3-5V DC supply and has a
standard I2C interface, connecting
the module to an Arduino module or
similar is relatively straightforward. A
sample connection scheme is shown
in Fig.3.
Note that although the HM3301
sensor itself has no internal pull-up
resistors on the SDA or SCL lines, the
Grove-Laser module provides pull-up
resistors plus logic-level converters on
its PCB. That’s why the connections
shown in Fig.3 are so straightforward.
Of course, wiring the module up is
only part of the story. You also need
software that can communicate with it
and display the results. So if you want
to use it with an Arduino, you’ll need
both a matching library and a sketch
designed to communicate with the
HM3301 sensor using it.
When I went to the “Reference”
section of the Arduino website and
scrolled down through the Libraries/
Sensors list, I found a library that had
clearly been produced to do the job:
“grove-laser-pm2.5-sensor-hm3301”.
And when I clicked on “Read the documentation” on its page, it took me to
GitHub, where I found both the documentation and a link to download the
library (v1.0.2).
After downloading and installing
the library, I found that it came with an
example program called “basic_demo.
ino”. After verifying and uploading
that program ‘sketch’ to an Arduino
Uno connected to the Grove-Laser
Fig.3: connecting the
Grove HM3301 module
to an Arduino is
simple. All it needs is
a ground connection,
a 5V DC supply and
the SDA and SCL pins
connected to an I2C
bus.
Fig.4: HM3301 sample output
siliconchip.com.au
08:46:39.046 -> sensor num: 0
08:46:39.046 -> PM1.0 concentration(CF=1,Standard
particulate matter, unit:ug/m3): 404
08:46:39.046 -> PM2.5 concentration(CF=1,Standard
particulate matter, unit:ug/m3): 850
08:46:39.046 -> PM10 concentration(CF=1,Standard
particulate matter, unit:ug/m3): 1356
08:46:39.046 -> PM1.0 concentration(Atmospheric
environment,unit:ug/m3): 266
08:46:39.046 -> PM2.5 concentration(Atmospheric
environment,unit:ug/m3): 524
08:46:39.046 -> PM10 concentration(Atmospheric
environment,unit:ug/m3): 776
module as per Fig.3, the Arduino IDE’s
Serial Monitor (set to a baud rate of
115,200) sprang into life.
I immediately saw the text shown in
Fig.4, with two sets of PM1.0, PM2.5
and PM10 measurements appearing
every five seconds.
The example output shown in Fig.4
is higher than normal (it should be just
above zero). That’s because I struck
a match and blew it out just before
that, blowing the smoke towards the
HM3301 sensor. The readings jumped
up quite quickly but went back to normal after about 10 seconds.
So while it’s not particularly low in
cost, the Grove-Laser PM module is
easy to use and seems quite sensitive.
Panasonic SN-GCJA5 sensor
similar to the HM3301 sensor innards
shown in Fig.2, apart from not having any internal fan to move the air
through the detection chamber.
Since it has an I2C interface, it connects to an MCU like the Arduino in
much the same way as the Grove-Laser
module, as shown in Fig.6. But there’s
one small but significant problem: connections to the SN-GCJA5 sensor are
all made via a tiny 5-pin ‘pico’ connector at one end, but a connection
cable with a matching plug is not supplied with it.
So if you want to use – or even try
out – the sensor, you first need to
obtain a matching cable.
Panasonic’s data sheet for the
SN-GCJA5 sensor states that its connector is made by JST (Japan Solderless Terminals) Manufacturing
Company, and has the type number SM05B-GHS-TB(LF)(SN). I had
a lot of trouble finding any compatible cables – most cables I found with
similar connectors turned out to have
pins either 1.0mm or 1.5mm apart, not
the 1.25mm of the JST SM05B-GHSTB(LF)(SN).
Just as I was on the brink of concluding that I would not be able
to try out the SN-GCJA5 sensor,
Silicon Chip’s Editor emailed me to
say that he believed he had found
a supplier of compatible cables on
AliExpress (www.aliexpress.com/
item/33005797784.html). I quickly
checked them out and then ordered
a pack of 10 (the smallest quantity).
These cost $18.20 including postage
and GST, and they took quite a few
weeks to arrive.
But they did finally arrive, and I
used one (or half of one, to be precise)
to hook up the sensor to an Arduino
and try it out.
It was again necessary to find a suitable Arduino library to communicate
with the SN-GCJA5. Luckily, I found
one in the Reference section on the
Arduino website, under siliconchip.
au/link/abep
When I downloaded this library
and installed it, I found that it again
included some example sketches. The
first of these was called “Example1_
BasicReadings.ino”. When I verified
and uploaded this sketch to the Arduino Uno connected to the SN-GCJA5
sensor, as shown in Fig.6, it finally
sprang into life. Once again, I had to
set the Arduino IDE Serial Monitor to
115,200 baud.
You can see the output of the sketch
►
The Panasonic SN-GCJA5 sensor
is again mounted inside a compact
moulded plastic box that measures
37 × 37 × 12mm and weighs 13g. As
with the HM3301 sensor, it includes
electronics to control the laser and
amplify and filter the signals from the
photodiodes, plus an MCU for data
processing.
The output is via either an I2C or
a UART TX terminal. The effective
measuring range of this module is
0-2000μg/m3.
The Panasonic SN-GCJA5 sensor is
currently available in Australia from
element14 for $33.56 plus delivery
and GST, giving a total of $53.42 (less
if you buy it along with enough other
stuff, such as a second sensor, to get
free delivery).
Fig.5 shows what is inside the
SN-GCJA5 sensor. As you can see, it’s
External connections to
the SN-GCJA5 sensor
are via a tiny 5-way JST
connector with 1.25mm
pin spacing. No matching
cable is supplied, which
is a bit of a problem as
they are hard to find!
Fig.5: the Panasonic SN-GCJA5-PM sensor does not use a fan. It
instead relies on passive diffusion of air through its sensing channel.
Otherwise, its structure is similar to the HM3301 shown in Fig.2.
The Panasonic SN-GCJA5 particulate matter sensor is in a small
moulded plastic case measuring 37 x 37 x 12mm. In addition to
the laser and photodetector, it contains all of the electronics and
provides both I2C and UART digital outputs.
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Australia's electronics magazine
siliconchip.com.au
Fig.6: connecting the Panasonic SN-GCJA5
module to an Arduino is again simple. All you
need to do is connect a 5V DC supply, a ground
connection and the I2C bus via the SCL and SDA
pins. Pin 1 isn’t used for anything, nor does it
have any function.
Fig.7: SN-GCJA5 sample output
08:03:23.189
08:03:23.189
08:03:23.189
7.5, 10,
08:03:23.236
08:04:18.209
08:04:28.238
146,4,
08:04:48.249
08:05:58.231
in Fig.7. It gives three PM readings
(1.0, 2.5 and 10) at the start of each
sample line, followed by six Count
figures (labelled 0.5, 1, 2.5, 5, 7.5 and
10). The first three figures are the ‘mass
densities’ for the three main particle
categories, while the later figures are
‘particle counts’ for all six particle size
categories.
Looking at Fig.7, the first values outputted are pretty low, they then shoot
up to much higher levels after I lit a
match about 150mm from the sensor and then blew it out, blowing the
smoke towards the sensor.
So the Panasonic SN-GCJA5 sensor does work, and even works quite
well, once you manage to find a suitable cable to connect to it. It would be
-> Panaosnic SN-GCJA5 Example
-> Sensor started
-> PM:1.0, 2.5, 10, Counts: 0.5, 1, 2.5, 5,
-> 2.79,3.12,3.50,5,32,4,0,0,0,
-> 57.99,135.45,448.29,39,598,801,13,71,2,
-> 1370.39,1730.99,2392,60,440,3824,3759,37,
-> 139.76,154.51,173.83,513,1210,153,1,2,0,
-> 62.35,73.86,83.09,200,591,120,1,0,0,
a lot easier if they supplied a matching cable!
The Jaycar XC3780 sensor
As mentioned earlier, Jaycar’s
XC3780 dust sensor module is based
on the Sharp GP2Y1010AU fanless
sensor. The sensor itself is pretty compact, measuring 46 × 30 × 17.5mm,
and the XC3780 module is only a little larger, at 62 × 35 × 19mm. 7.5mm
diameter holes in the top and bottom
of the sensor (and the PCB) allow air
containing any particulate matter, dust
or smoke to diffuse through the sensor.
At the time of writing, the XC3780
module is available from Jaycar stores
for $23.95 or their online Techstore for
$31.95, including delivery.
Because the sensor’s mini six-pin
SIL connector is on the top of the
case, the XC3780 module comes with
a short six-wire cable connecting it to
a matching mini SIL connector on the
end of the module’s PCB. There are
some passive components at the same
end of the board plus a four-pin SIL
header with standard 0.1in/2.54mm
spacing, to simplify connection to an
external MCU.
Fig.8 shows the components inside
the GP2Y1010AU sensor itself, and as
you can see, it’s similar to Fig.5 apart
from not having a microcontroller to
digitise and process the output signal.
In this case, the analog output signal
“VO” is simply made available at pin 5.
Note that the centre amplifier
The Jaycar XC3780 module is based on the Sharp
GP2Y1010AU dust sensor. Being fanless, it relies on air
diffusing through 7.5mm diameter holes in the top and
bottom of the sensor’s case. It has a varying DC voltage
output rather than digital outputs, so conversion into a
dust density figure is done by software running on the
controlling MCU.
siliconchip.com.au
Australia's electronics magazine
November 2022 81
Fig.8: the main difference between this GP2Y1010AU ‘dust’ sensor and the
Panasonic sensor shown in Fig.5 is that this one lacks any digital control
electronics; it only includes analog signal processing. Therefore, the driving
microcontroller module must power the LED via pins 1-3, measure the
voltage at output pin 5 and convert that into a particle level.
Fig.9: this curve shows the transfer function between the output voltage of
the GP2Y1010AU sensor and the corresponding dust density in mg/m3. A
table (or similar) representing the points in this plot needs to be loaded into
the microcontroller to perform this conversion.
Fig.10: there aren’t many components on the Jaycar XC3780 module besides
the Sharp sensor. All they do is filter the power supply to the module,
provide a power-on indication via LED1 and route the necessary signals to a
standard four-pin header for connection to an MCU.
82
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Australia's electronics magazine
section has a small adjustable resistor or trimpot to adjust the sensor’s
effective sensitivity. But the Sharp
data sheet for the GP2Y1010AU sensor warns that this trimpot is set to
make the sensor conform to its specification before shipment. As a result,
they advise against further adjustment
of the trimpot.
This specification is summarised in
Fig.9, which shows how the output
voltage (VO) varies with dust density.
VO is close to 0.9V with zero dust in
the air, rising relatively linearly to
about 3.25V at a dust density of 0.4mg/
m3 before flattening off at about 3.55V
for a dust density of 0.53mg/m3. It then
rises very slowly to about 3.6V for a
dust density of 0.8mg/m3. Note that
1mg = 1000μg.
The complete circuit of the XC3780
module is shown in Fig.10, and there
are only a few passive components on
the PCB apart from the GP2Y1010AU
sensor itself. The 150W resistor and
220μF capacitor provide decoupling
and smoothing for the supply to the
sensor’s internal LED, while the 1kW
resistor and LED1 indicate when the
module is powered up.
Connecting the XC3780 module to
an Arduino is quite straightforward, as
shown in Fig.11. The GND and VCC
pins of the module can be connected to
the GND and +5V pins of the Arduino.
The LED pin should be connected to
the IO3 (D3) pin of the Arduino while
the VO/OUT pin goes to the Arduino’s
ADC0 (A0) input.
These are the connections needed to
ensure that the XC3780 module works
correctly when a specific sketch runs
on the Arduino. That sketch uses a
particular library to control the LED
inside the GP2Y1010AU and convert
its DC output voltage into the equivalent dust density.
I found this library on the Arduino website in the reference → libraries → sensors section. Called PMsensor, it was written by JongHyun Woo,
and the latest version is 1.1.0. When I
downloaded this library (“PMsensor-
master.zip”) and installed it in my
Arduino IDE, I found that it came with
an example sketch called “PMsensor_
demo.ino”.
This sketch provides almost no
information on the correct connections
for the sensor’s LED and VOUT lines,
or the correct baud rate to use for the
Arduino link back to the PC. However,
after examining the code in the sketch,
siliconchip.com.au
I determined that the proper connections were those shown in Fig.11, and
the correct baud rate was 9600 baud. I
then powered it up and got the result
shown in Fig.12.
I decided to adapt JongHyun Woo’s
sketch into one with more helpful
information in a ‘header’ section. I
called this new sketch “SC_PMsensor_
demo.ino” and it is available to download for free from siliconchip.com.au/
Shop/6/62
As you can see from Fig.12, this
sketch simply pulses the sensor’s internal LED once per second, then reads
its output voltage and converts it into
an equivalent dust density reading.
This is then printed in the lines reading “Filter : XXX.XX”.
You may have noticed in Fig.12 that
at the top of the listing, the readings
are low. But then they started rising
because I struck a match and blew it
out with the smoke passing over the
top of the sensor.
Precisely what these figures mean
is not too clear, though. They could
represent the dust density in μg/m3
(micrograms per cubic metre), or they
might not.
So the XC3780 dust sensor can be
connected fairly easily to an MCU like
an Arduino, and it does work using
JongHyun Woo’s library and demo
sketch. But the accuracy and significance of its readings are a tad indeterminate.
The bottom line
Overall, I prefer the Grove-Laser
module based on the HM3301 fan
sensor. It is the most expensive of the
three, but not unreasonably so, considering its ease of use and the apparent
accuracy of its readings.
I would have to rate the Panasonic
SN-GCJA5 sensor as the next best;
although it seems to give fairly accurate readings, it lacks a fan and also
has the disadvantage of not coming
with a matching cable.
The Jaycar XC3780 module is only
about half the cost of the other two
modules/sensors and is the easiest
to get.
But the fact that it needs software
running in the Arduino to convert its
DC output voltage into dust density
makes me a little less confident in
the accuracy of its readings. Still, it
would be fine if all you needed were
relative readings, eg, to use it as a kind
of smoke alarm.
SC
siliconchip.com.au
Fig.11: connecting the Jaycar
XC3780 module to an MCU is
straightforward. Various pin
connections could be used, but this
is the routing needed for the test
sketch to work. It uses one digital
pin (to control its internal LED)
and one analog pin (for sensing the
output voltage).
Fig.12: XC3780 sample output
15:15:25.825
15:15:25.825
15:15:26.762
15:15:26.809
15:15:26.809
15:15:27.793
15:15:27.840
15:15:27.840
15:15:28.824
15:15:28.824
15:15:28.871
15:15:29.808
15:15:32.854
15:15:32.901
15:15:33.839
15:15:40.962
15:15:40.962
15:15:41.946
->
->
->
->
->
->
->
->
->
->
->
->
->
->
->
->
->
->
Read PM2.5
Filter: 11.15
=========================
Read PM2.5
Filter: 30.79
=========================
Read PM2.5
Filter: 78.10
=========================
Read PM2.5
Filter: 120.76
=========================
Read PM2.5
Filter: 253.01
=========================
Read PM2.5
Filter: 396.47
=========================
We assume the readings are in μg/m3 but the documentation is a bit vague
Useful links
Suppliers:
• www.pakronics.com.au
• https://au.element14.com/3523840
• www.jaycar.com.au
Software libraries:
• www.arduino.cc/reference/en/libraries/grove-laser-pm2.5sensor-hm3301
• https://github.com/Seeed-Studio/Seeed_PM2_5_sensor_HM3301
• www.arduino.cc/reference/en/libraries/pmsensor/
• https://github.com/ekkai/PMsensor
• https://github.com/sparkfun/SparkFun_Particle_Sensor_SN-GCJA5_
Arduino_Library
Panasonic SN-GCJA5 data sheet: siliconchip.au/link/aber
Sharp dust sensor application note: siliconchip.au/link/abeq
Australia's electronics magazine
November 2022 83
Vintage Radio
Philips Minstrel radios
By Assoc. Prof. Graham Parslow
The Minstrel series of radios from Philips in the
early 1950s was intended to be affordable and
cheerful. Comparable kitchen radios are the Astor
Mickey, HMV Little Nipper, AWA model 467MA
and Healing model 404. The Philips Minstrel cost
£21, similar to its four-valve competitors.
84
Silicon Chip
Australia's electronics magazine
I
managed to get a copy of the
original advertisement showing
the nine beautiful colours that
the cabinet came in via Glen Oriss, a
member of the Facebook group The
Real Bakelite and Antique Radio Page.
As well as the models noted in the
introduction, Philips also competed
against themselves with the Jubilee
model 122. But this comparable fourvalve radio was much more conservatively styled in dark Bakelite.
The performance of these radios is
excellent on local stations due to the
progressive refinement of the three
valves in the radio circuit (the fourth
valve is the high-tension rectifier).
More expensive five-valve sets added
audio preamplification and are usually
indistinguishable in performance for
city locations.
The Minstrel radios were moulded
from solid-colour plastics. These new
polymers were used in many items in
the 1950s when plastic was fantastic.
Before these plastics, light colours
were often produced as factory-
painted Bakelite.
The standard Minstrel is the model
138. When they added a clock, it
became the Chronoradio model 145.
The circuit and construction of the
two models are otherwise almost identical; the clock radio has an additional
socket on the chassis that allows the
synchronous-motor clock to connect
to the 240V 50Hz mains and switch
the radio on at set times.
The clock radio has a low profile
4-inch speaker (100mm) mounted at
the top and delivers sound through a
grille moulded into the top of the case.
This produces reasonable sound, but
not as good as the 5-inch (125mm)
speaker mounted at the front of model
138.
The station markings on the dial
depended on the target states for sale.
The blue radio pictured opposite features WA and SA stations. The clock
radio included at the end of the article
has all states on the one dial.
Circuit details
The original circuit for the model
138 clock radio is shown in Fig.1.
The aerial coils of the 1950s were
well-evolved to make the best of
whatever aerial was connected. The
Radiotron Designer’s Handbook 4th
Edition from 1957 says, in the summary of design for aerial coils:
“It can be seen that the common
siliconchip.com.au
Fig.1: the circuit for the Philips Minstrel Four 138 radio is
nearly identical to the model 145. The 145 has one less tap on
the secondary of the power transformer (L14 is removed) and
some of the resistors have been changed by ~10% in value. An excerpt
from the model 145 circuit showing the clock portion is shown on the
left-side with a grey fill.
loose coupled primary and secondary for MW radios is most satisfactory
because it readily lends itself, with
minor modifications, to applications
using balanced or unbalanced aerial
systems.”
Random lengths of wire connected
to a domestic radio certainly fit into
the unbalanced category.
In looking at the aerial coil circuit
for this radio, I was motivated to dig a
bit deeper to work out what the hook
shape at the top of pin 2 indicates.
Whatever it is, it was logical that it
would be equivalent to many other
front-ends that connect a 15pF capacitor between pins 2 and 3.
C1 (100pF) makes a resonant circuit
with L1, and ideally, that resonant frequency will be below 550kHz at the
bottom of the MW band. This avoids an
impedance peak in the MW band that
would give uneven matching between
primary and secondary over the span
of the band. Even so, the signal coupling will deteriorate as tuning goes
from 550kHz to 1600kHz.
Adding a small capacitor between
pins 2 and 3 boosts the signal at higher
frequencies to even out the sensitivity
over the MW band.
I went to my salvage shelf and found
another Philips radio with the same
siliconchip.com.au
aerial coil and removed it. I melted
off the protective wax covering using
a heat gun to reveal the wire connections shown in Fig.2.
The primary of this transformer
measured 25W and the secondary 2W.
At first, this seems a paradox until
looking at the wire gauge in the different coils. The primary has many
more turns of fine-gauge wire, giving a
higher inductance than the secondary,
so its resonance with a 100pF capacitor (C1) is below 550kHz.
The separation between the primary and secondaries (loose coupling)
makes the tuning characteristics more
robust to whatever aerial is connected
to the primary.
This Minstrel is originally blue; the colour is solid through the case. Re-sprayed
radios can usually be detected by having a different colour inside the case.
Australia's electronics magazine
November 2022 85
100pF
3
4
4
2
Aerial coil with
wax coating
Secondary
To pin 1
Primary
3
Loop of gimmick wire
between secondary
coils connects to pin 2
To pin 2
Connection
between
loops of the
secondary
Fig.2: an aerial coil taken from another Philips radio. The protective wax
coating was melted off to reveal the connections shown above.
At last, the nature of that hooked
line (a gimmick) on the circuit diagram
from pin 2 to 3 was revealed. It is a loop
of wire sandwiched between the secondary coils and provides capacitive
coupling to augment the higher MW
band frequencies.
Valve lineup
V1, the mixer valve, is a 6AN7,
possibly the most common valve for
this application through the 1950s.
Philips released this 9-pin miniature
triode-hexode valve in 1949, so it was
new technology for the Minstrel. The
local oscillator (L3 and L4) is an Armstrong type with feedback from the triode anode to sustain oscillation.
The double-gang tuning capacitor
is the compact brass-plate type introduced by Philips in the early 1950s
and used right up to the early Philips
transistor radios.
The compact IF coils in the Minstrel
were another new standard for Philips
radios that would span the 1950s.
These IF transformers are configured
to tune both the primary and secondary with slugs adjusted at the top. They
are a cause for some apprehension
because the IF coils are set in resin, so
the common occurrence of open circuits due to spot corrosion condemns
them to the bin.
V2, the pentode IF amplifier and
twin diode detector, is a 6N8. This is
also a Philips-designed valve, released
in 1949. The 6N8 is not reflexed as an
audio amplifier, so the detected signal
is passed directly to the 6M5 output
pentode via potentiometer R7 (0.5MW).
Unsurprisingly, the 6M5 (V3) is
another Philips design released in
1949. At the anode voltage of around
210V used in the Minstrel, the audio
output from the 6M5 is comfortably
2W. This is a fair match to the 5-inch
(125mm) round speaker made by
Philips that fits snugly into the moulding in the case.
R13 (160W) generates a negative bias
for the 6M5 of -6.5V. R13 also serves to
generate a negative grid bias voltage for
the 6AN7 and 6N8. The first two valves
additionally receive negative feedback
(AGC) from the audio detector. Follow
the circuit from the intersection of R4
and R5 to trace the AGC.
Because of R13, the AGC does not
work on weak signals and comes into
The front of the model 138 chassis, with the power transformer visible on
top.
86
Silicon Chip
Australia's electronics magazine
effect as signal strength increases (ie,
this set has delayed AGC).
The high-tension (HT) circuit is
conventional using a 6V4 valve (V4).
The Minstrels were assembled at Hendon in Adelaide, and the components
were largely Australian-made (including valves) with occasional European
imported stock.
A European-made EZ82, equivalent to the 6V4, can also be found in
these sets. Interestingly, the indirectly-
heated 6V4 valve has the heater powered by its own 6.3V transformer winding. This allows the heater and cathode
to be connected to avoid any high tension arc-over between these elements.
Later Minstrels had an alternative
transformer with only one 6.3V winding and no connection between the
cathode and heater.
There is no tone control and no feedback from the speaker to modify the
tone and maintain stability. Even so,
the sound is cheerful.
The radios typically consume
28-30W; included in that figure is the
power for a single dial lamp.
The hardware
Disassembling a Philips radio is
invariably a challenge. A minor nuisance with the Minstrel is that the
captive speaker obliges the connecting wires to be desoldered.
A trap for the unwary is to overlook disconnecting the dial cursor
from the dial string before pulling the
chassis out. Forcing the chassis out
breaks the dial string, and restringing these radios is one of life’s greater
challenges, particularly without the
stringing diagram.
The underside of the model 138
chassis, showing the output
transformer.
siliconchip.com.au
When the chassis is out, these units
are relatively easy to work on because
they are happy to stand up resting on
the power transformer at the bottom.
The filter electrolytics (2 x 24μF) are
both mounted in a single can.
With the original paper capacitors
in place, the 6N8 and 6M5 bases are
inaccessible. Fortunately, it is only a
minor chore to replace the old units
with small modern capacitors and continue with a complete re-cap.
Two Minstrel radios I have worked
on had C10 measuring negligible
capacitance, preventing the frontend tuning circuit from functioning.
C10 is an Earth return from pin 4 of
the aerial coil. It is soldered into a
cramped position with one lead tightly
folded back, probably pulling an endcap away from the internal foil with
time and heat.
Case restoration
One Minstrel that I acquired on
eBay was apparently posted via the
post office branch that assesses survivability after ‘robust’ handling. It
was packed in a cardboard carton with
only crumpled newspaper pages for
padding. The outcome was instructive (or should that be ‘destructive’?).
Fortunately, I was able to glue the
shards of the case back in place reasonably well with thin-CA (cyanoacrylate) glue. After that, I applied a twopart epoxy body filler, then abraded it
back to a smooth finish. I then sprayed
it with an undercoat, sanded it back
and repeated. I needed to make four
applications before I was happy with
the adhesion and quality of the surface.
I then finished the radio in powder
While the case arrived cracked, it glued back together quite well.
blue, a slightly lighter shade than the
original Philips blue.
In the end, there was no external
hint of the distress suffered by the case.
The inside of the case was left cream
so that it could not be passed off at a
future time as an original blue radio.
The clock radio
All major manufacturers offered a
clock variant of their low-end models
so that they could serve as a kitchen or
bedroom set. The clock radio shown
below did not work when I received
it, due to a faulty capacitor C10, which
was not a surprise.
However, another unexpected fault
was a 27kW resistor installed as a
replacement for two 50kW resistors
in parallel (R2 and R3). This determines the screen voltage to the 6AN7
and 6N8, and the screens should be
55V. On this radio, it measured only
40V. Replacing it with an 18kW resistor restored the correct screen voltage.
The clock is accommodated by moving the speaker to the top and using a
low-profile clock. There are no markings to indicate where those clocks
were sourced or made. Most Australian clock radios use a Smiths synchronous movement that is too bulky
for the limited space at the front of
this radio.
The 4-inch Alnico speaker in the
clock radio was carefully chosen to fit
between the chassis and clock at the
top of the case. To be fair, the installed
speaker did an adequate job for kitchen
or bedroom listening. I tried replacing the original speaker with others
that had better specifications, but they
fouled the clock.
The conservative Minstrel case was
utterly compliant with the norm at
the time – a rectangular shape with
rounded edges. The distinctive niche
of the Minstrel radios was to introduce
the world of coloured plastics to radios
SC
made by Philips in Australia.
The Philips
model 145
radio also
includes a
clock on
the dial.
siliconchip.com.au
Australia's electronics magazine
November 2022 87
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PRE-PROGRAMMED MICROS
For a complete list, go to siliconchip.com.au/Shop/9
$10 MICROS
$15 MICROS
24LC32A-I/SN
ATmega328P
ATmega328P-AUR
ATtiny85V-10PU
ATtiny816
PIC10F202-E/OT
PIC10LF322-I/OT
PIC12F1572-I/SN
PIC12F617-I/P
Digital FX Unit (Apr21)
Si473x FM/AM/SW Digital Radio (Jul21), 110dB RF Attenuator (Jul22)
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; versions), Nano TV Pong (Aug21)
Model Railway Level Crossing (two required – $15/pair) (Jul21)
Range Extender UHF-to-IR (Jan22)
PIC12F617-I/SN
Model Railway Carriage Lights (Nov21)
PIC12F675-I/P
Heater Controller (Apr18), Useless Box IC3 (Dec18)
Train Chuff Sound Generator (Oct22)
PIC12F675-I/SN
Tiny LED Xmas Tree (Nov19)
PIC16F1455-I/P
Digital Interface Module (Nov18), GPS Finesaver (Jun19)
Digital Lighting Controller Slave (Dec20), Auto Train Controller (Oct22)
PIC16F1455-I/SL Ol’ Timer II (Jul20), Battery Multi Logger (Feb21)
PIC16LF1455-I/P New GPS-Synchronised Analog Clock (Sep22)
PIC16F1459-I/P
20A DC Motor Speed Controller (Jul21)
Fan Controller & Loudspeaker Protector (Feb22)
Secure Remote Mains Switch Receiver (Jul22)
PIC16F1459-I/SO Multimeter Calibrator (Jul22), Buck/Boost Charger Adaptor (Oct22)
PIC16F15214-I/SN Improved SMD Test Tweezers (Apr22), Tiny LED Icicle (Nov22)
PIC16F1705-I/P
Flexible Digital Lighting Controller (Oct20)
Digital Lighting Controller Translator (Dec21)
PIC16LF15323-I/SL Secure Remote Mains Switch Transmitter (Jul22)
ATSAML10E16A-AUT
PIC16F18877-I/P
PIC16F88-I/P
High-Current Battery Balancer (Mar21)
USB Cable Tester (Nov21)
UHF Repeater (May19), Six Input Audio Selector (Sep19)
Battery Charge Controller (Dec19 / Jun22)
Railway Semaphore (Apr22)
PIC24FJ256GA702-I/SS
Wide-Range Ohmmeter (Aug22)
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)
RCL Box (Jun20), Digital Lighting Controller Micromite Master (Nov20)
Advanced GPS Computer (Jun21), Touchscreen Digital Preamp (Sep21)
PIC32MX170F256B-I/SO
Battery Multi Logger (Feb21), Battery Manager BackPack (Aug21)
PIC32MX270F256B-50I/SP ASCII Video Terminal (Jul14), USB M&K Adaptor (Feb19)
$20 MICROS
ATmega644PA-AU
PIC32MX470F512H-I/PT
PIC32MX470F512H-120/PT
PIC32MX470F512L-120/PT
PIC32MX795F512H-80I/PT
AM-FM DDS Signal Generator (May22)
Stereo Echo/Reverb (Feb 14), Digital Effects Unit (Oct14)
Micromite Explore 64 (Aug 16), Micromite Plus (Nov16)
Micromite Explore 100 (Sep16)
Touchscreen Audio Recorder (Jun14)
dsPIC33FJ64MC802-E/SP
dsPIC33FJ128GP306-I/PT
1.5kW Induction Motor Speed Controller (Aug13)
CLASSiC DAC (Feb13)
$25 MICROS
$30 MICROS
PIC32MZ2048EFH064-I/PT DSP Crossover/Equaliser (May19), Low-Distortion DDS (Feb20)
DIY Reflow Oven Controller (Apr20), Dual Hybrid Supply (Feb22)
KITS, SPECIALISED COMPONENTS ETC
VARIOUS MODULES & PARTS
siliconchip.com.au/Shop/
WIDE-RANGE OHMMETER (CAT SC4663)
(AUG 22)
VGA PICOMITE KIT (CAT SC6417)
(JUL 22)
MULTIMETER CALIBRATOR KIT (CAT SC6406)
(JUL 22)
110dB RF ATTENUATOR SHORT-FORM KIT (CAT SC6420)
(JUL 22)
Specify the Icicle style – comes with 12 white, cyan & blue LEDs and all required
components (except the coin cell, CON2 & figure-8 wire for daisy chaining)
$15.00
BUCK-BOOST LED DRIVER KIT (CAT SC6292)
(JUN 22)
NEW GPS(/WIFI)-SYNCHRONISED ANALOG CLOCK
SPECTRAL SOUND MIDI SYNTH KIT (CAT SC6261)
(JUN 22)
IMPROVED SMD TEST TWEEZERS KIT (CAT SC5934)
(APR 22)
RASPBERRY PI PICO BACKPACK KIT (CAT SC6075)
(MAR 22)
500W AMPLIFIER HARD-TO-GET PARTS (CAT SC6019)
(APR 22)
CAPACITOR DISCHARGE WELDER
(MAR 22)
- INA282AIDR + 20mW shunt (30V 2A Bench Supply, Oct22, SC6578)
- ISD1820-based recording module (Auto Train Controller, Oct22, SC5081)
- 70W LED panel (cool white, SC6307 | warm white, SC6308)
- 0.96in SSD1306-based yellow/blue OLED (AM-FM DDS, May22, SC6421)
- Pulse-type rotary encoder (AM-FM DDS, May22, SC5601)
- DS3231 real-time clock SOIC-16 IC (Pico BackPack, Mar22)
LC METER MK3
(NOV 22)
Short Form Kit: includes the PCB and all non-optional onboard parts, except
the case, front panel label and power supply (Cat SC6544; see page 47)
- Cyan/blue 0.96-inch OLED (Cat SC6176)
TINY LED ICICLE KIT (CAT SC5579)
$10.00
$7.50
$19.50
$10.00
$3.00
$7.50
$65.00
$10.00
(SEP & NOV 22)
(OCT 22)
Includes everything in the parts list (see page 64) except the Buck/Boost LED Driver
(see adjacent; Cat SC6292)
$40.00
- laser-cut acrylic cover panel (SC6567)
$2.50
- cyan/blue 1.3-inch OLED (SC5026)
$15.00
- white 1.3-inch OLED (SC6511)
$15.00
MINI LED DRIVER
(SEP 22)
Complete Kit: includes everything in the parts list (Cat SC6405; see page 81)
- XL6009 4A DC-DC boost module (Cat SC6546; red PCB)
WiFi PROGRAMMABLE DC LOAD
$25.00
$6.00
(SEP 22)
Short Form Kit: includes all SMDs, the power Mosfets, four 0.02W 3W resistors
and the VXO7805 regulator module (Cat SC6399; see page 39)
- laser-cut 3mm clear acrylic side panel (SC6514)
- 3.5-inch TFT LCD touchscreen (Cat SC5062)
Complete kit with everything needed to assemble the board, you just require a few
external parts such as a power supply, keyboard and monitor
$35.00
Complete kit with everything needed to assemble the board
Includes the PCB, programmed micro, OLED and all other on-board parts
(NOV 22)
GPS-Version Kit: includes everything in the parts list with the VK2828 GPS module
(Cat SC6472; see Sep22 p63)
$55.00
WiFi-Version Kit: includes everything in the parts list with the D1 Mini module instead
(Cat SC6472; D1 Mini is supplied not programmed, see Nov22 p76)
$55.00
- VK2828U7G5LF GPS module with antenna and cable (Cat SC3362)
$25.00
BUCK/BOOST CHARGER ADAPTOR KIT (CAT SC6512)
Partial Kit: includes the PCB, programmed micro, all SMDs, most semiconductors,
PPS capacitors and calibration resistors
$75.00
- 16x2 alphanumeric LCD with blue backlighting (Cat 5759)
$10.00
$85.00
$7.50
$35.00
Complete kit with everything needed to assemble the board
Complete kit including all programmed PICs (no case or power supply)
$45.00
$75.00
$80.00
$200.00
Complete kit with PCBs, all onboard parts, new microcontroller and gold-plated header
pins to use for the tips. Does not include a lithium coin cell
$35.00
Complete kit, includes all parts except the optional DS3231 IC
$80.00
All the parts marked with a red dot in the parts list, including the 12 output transistors,
driver transistors, VAS transistors, input pair (2SA1312), BAV21 & UF4003 diodes,
TL431 ICs, 75pF capacitor, E96 series resistors and 10kW 1W resistor
$200.00
Parts for the Power Supply – includes the power supply PCB, IC1-3, D1, the 1W
shunt and sole SMD capacitor (Cat SC6224)
Parts for the ESM – includes one ESM PCB, IC8, Q3 & Q4 (IRFB7434G), D9 plus
the SMD capacitors and resistors (Cat SC6225) → 8-14 sets typically needed
SMD TRAINER COMPLETE KIT (CAT SC5260)
(DEC 21)
Includes PCB & all on-board components, except for a TQFP-64 footprint device
$25.00
$20.00
$20.00
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PRINTED CIRCUIT BOARDS & CASE PIECES
PRINTED CIRCUIT BOARD TO SUIT PROJECT
TINY LED XMAS TREE (GREEN/RED/WHITE)
HIGH POWER LINEAR BENCH SUPPLY
↳ HEATSINK SPACER (BLACK)
DIGITAL PANEL METER / USB DISPLAY
↳ ACRYLIC BEZEL (BLACK)
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
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
DATE
NOV19
NOV19
NOV19
NOV19
NOV19
JAN20
JAN20
JAN20
JAN20
JAN20
FEB20
FEB20
MAR20
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MAR20
APR20
APR20
APR20
APR20
MAY20
MAY20
JUN20
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JUN20
JUL20
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JUL20
JUL20
JUL20
AUG20
NOV20
AUG20
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SEP20
SEP20
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OCT20
OCT20
OCT20
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DEC20
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JAN21
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FEB21
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MAR21
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APR21
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APR21
APR21
APR21
MAY21
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JUN21
JUN21
JUN21
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JUL21
JUL21
PCB CODE
Price
16111191
$2.50
18111181
$10.00
SC5168
$5.00
18111182
$2.50
SC5167
$2.50
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
07107201
$10.00
SC5500
$10.00
19104201
$5.00
SC5448
$7.50
15005201
$5.00
15005202
$5.00
01106201
$12.50
01106202
$7.50
18105201
$2.50
04106201
$5.00
04105201
$7.50
04105202
$5.00
08110201
$5.00
01110201
$2.50
01110202
$1.50
24106121
$5.00
16110202
$20.00
16110203
$20.00
16111191-9 $3.00
16109201
$12.50
16109202
$12.50
16110201
$5.00
16110204
$2.50
11111201
$7.50
11111202
$2.50
16110205
$5.00
CSE200902A $10.00
01109201
$5.00
16112201
$2.50
11106201
$5.00
23011201
$10.00
18106201
$5.00
14102211
$12.50
24102211
$2.50
10102211
$7.50
01102211
$7.50
01102212
$7.50
23101211
$5.00
23101212
$10.00
18104211
$10.00
18104212
$7.50
10103211
$7.50
05102211
$7.50
24106211
$5.00
24106212
$7.50
08105211
$35.00
CSE210301C $7.50
11006211
$7.50
For a complete list, go to siliconchip.com.au/Shop/8
PRINTED CIRCUIT BOARD TO SUIT PROJECT
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
8-LED METRONOME
10-LED METRONOME
REMOTE CONTROL RANGE EXTENDER UHF-TO-IR
↳ IR-TO-UHF
6-CHANNEL LOUDSPEAKER PROTECTOR
↳ 4-CHANNEL
FAN CONTROLLER & LOUDSPEAKER PROTECTOR
SOLID STATE TESLA COIL (SET OF 2 PCBs)
REMOTE GATE CONTROLLER
DUAL HYBRID POWER SUPPLY SET (2 REGULATORS)
↳ REGULATOR
↳ FRONT PANEL
↳ CPU
↳ LCD ADAPTOR
↳ ACRYLIC LCD BEZEL
RASPBERRY PI PICO BACKPACK
AMPLIFIER CLIPPING DETECTOR
CAPACITOR DISCHARGE WELDER POWER SUPPLY
↳ CONTROL PCB
↳ ENERGY STORAGE MODULE (ESM) PCB
500W AMPLIFIER
MODEL RAILWAY SEMAPHORE CONTROL PCB
↳ SIGNAL FLAG (RED)
AM-FM DDS SIGNAL GENERATOR
SLOT MACHINE
HIGH-POWER BUCK-BOOST LED DRIVER
ARDUINO PROGRAMMABLE LOAD
SPECTRAL SOUND MIDI SYNTHESISER
REV. UNIVERSAL BATTERY CHARGE CONTROLLER
VGA PICOMITE
SECURE REMOTE MAINS SWITCH RECEIVER
↳ TRANSMITTER (1.0MM THICKNESS)
MULTIMETER CALIBRATOR
110dB RF ATTENUATOR
WIDE-RANGE OHMMETER
WiFi PROGRAMMABLE DC LOAD MAIN PCB
↳ DAUGHTER BOARD
↳ CONTROL BOARD
MINI LED DRIVER
NEW GPS-SYNCHRONISED ANALOG CLOCK
BUCK/BOOST CHARGER ADAPTOR
30V 2A BENCH SUPPLY MAIN PCB
↳ FRONT PANEL CONTROL PCB
AUTO TRAIN CONTROLLER
↳ TRAIN CHUFF SOUND GENERATOR
PIC16F18xxx BREAKOUT BOARD (DIP-VERSION)
↳ SOIC-VERSION
AVR64DD32 BREAKOUT BOARD
DATE
JUL21
AUG21
AUG21
AUG21
AUG21
AUG21
AUG21
SEP21
SEP21
OCT21
OCT21
OCT21
NOV21
NOV21
NOV21
DEC21
DEC21
DEC21
JAN22
JAN22
JAN22
JAN22
JAN22
JAN22
FEB22
FEB22
FEB22
FEB22
FEB22
FEB22
FEB22
FEB22
FEB22
MAR22
MAR22
MAR22
MAR22
MAR22
APR22
APR22
APR22
MAY22
MAY22
JUN22
JUN22
JUN22
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JUL22
JUL22
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JUL22
JUL22
AUG22
SEP22
SEP22
SEP22
SEP22
SEP22
OCT22
OCT22
OCT22
OCT22
OCT22
OCT22
OCT22
OCT22
PCB CODE
09108211
07108211
11104211
11104212
08105212
23101213
23101214
01103191
01103192
01109211
12110121
04106211/2
04108211
04108212
09109211
01111211
16110206
29106211
23111211
23111212
15109211
15109212
01101221
01101222
01102221
26112211/2
11009121
SC6204
18107211
18107212
01106193
01106196
SC6309
07101221
01112211
29103221
29103222
29103223
01107021
09103221
09103222
CSE211002
08105221
16103221
04105221
01106221
04107192
07107221
10109211
10109212
04107221
CSE211003
04109221
04108221
04108222
18104212
16106221
19109221
14108221
04105221
04105222
09109221
09109222
24110222
24110225
24110223
Price
$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
$5.00
$7.50
$2.50
$2.50
$7.50
$5.00
$5.00
$7.50
$20.00
$25.00
$7.50
$2.50
$5.00
$2.50
$5.00
$5.00
$2.50
$5.00
$5.00
$5.00
$25.00
$2.50
$2.50
$7.50
$5.00
$5.00
$5.00
$7.50
$7.50
$5.00
$7.50
$2.50
$5.00
$5.00
$7.50
$7.50
$5.00
$10.00
$2.50
$5.00
$5.00
$7.50
$2.50
$2.50
$2.50
$2.50
$2.50
$2.50
LC METER MK3
↳ ADAPTOR BOARD
DC TRANSIENT SUPPLY FILTER
TINY LED ICICLE (WHITE)
AUDIO/RF SIGNAL TRACER
HEAVY-DUTY 240VAC MOTOR SPEED CONTROLLER
NOV22
NOV22
NOV22
NOV22
JUN97
NOV97
CSE220503C
CSE200603
08108221
16111192
04106971
10311971
$7.50
$2.50
$5.00
$2.50
$5.00
$7.50
NEW PCBs
We also sell the Silicon Chip PDFs on USB, RTV&H USB, Vintage Radio USB and more at siliconchip.com.au/Shop/3
0-30V 0-2A
Part 2
by
John Clarke
bench supply
This new Bench Supply, introduced last month, is basic yet feature-packed,
including full onboard metering and an adjustable current limit. It’s pretty easy
and cheap to build, so it is suitable for relative beginners. You will find it handy for
various purposes, including powering circuits for testing or development. It also fits
neatly into a compact and attractive instrument case. So let’s get to building it.
P
art of the reason for the
30V and 2A limits is that
they allow us to use an inexpensive and modestly-sized transformer that fits neatly alongside the
regulator board in a compact 160 × 180
× 70mm benchtop instrument case. It’s
small enough to stay out of your way
but powerful enough for many jobs.
You could even stack two or three
to have a few different voltages available or connect two in series to form
a split supply. Just keep in mind that
their current limits will be enforced
separately, so if there is a fault, it’s
possible that one Supply would go
into current limiting while the other(s) wouldn’t.
While this is a mains-based project, anyone who is good at following
instructions and with reasonable soldering skills should be able to build
it safely. Just make sure you perform
all the wiring as described using correctly rated wire, and don’t skip any
of the required insulation or cable ties.
90
Silicon Chip
Before we get to construction, a
word about the metering. We tested
some low-cost volt/ammeters from
eBay but found that they were too inaccurate, which is why we specified the
part from Core Electronics. Use caution if you want to substitute another
meter, as its readings could be way off.
As with many projects, the first step
in construction is soldering the majority of the components to the printed
circuit boards.
Construction
Most of the parts for the Supply
mount on two PCBs. The main 76 ×
140mm PCB is coded 04105221 and
includes most of the components,
while the smaller 56 × 61mm PCB
coded 04105222 has the front panel
parts such as voltage and current setting potentiometers, indicator LEDs
and load switch. A 14-way ribbon
cable fitted with insulation displacement connectors (IDCs) connects the
two PCBs.
Australia's electronics magazine
As explained last month, there is the
option to use a single 2.5kW multi-turn
potentiometer for VR1 or a standard
single-turn 5kW potentiometer in conjunction with a 5kW multi-turn trimpot (VR2). If you are using the 2.5kW
multi-turn potentiometer, VR2 is not
used and must be left off the PCB.
During the following process, refer
to the PCB overlay diagrams (Figs.5 &
6) to see which parts go where.
Begin construction with the main
PCB by fitting the two surface-mount
components. These are the INA282
shunt monitor (IC2) and the 20mW
resistor. For the resistor, we have made
provision on the PCB for either two
10mW resistors in series or a single
20mW resistor. Both the resistor and
IC are relatively easy to solder.
Find the pin 1 orientation marker
on the INA282. This can be a dot on
the top face, a notch at the pin 1 end
of the device, or a chamfer along the
pin 1 to 4 edge of the package.
Position the IC over the pads and
siliconchip.com.au
Fig.5: fit the components
to the main PCB as
shown here, watching
the orientations of the
polarised parts. VR2 is
not shown as it is only
needed if VR1 is 5kW; in
that case, install it with
the adjustment screw
towards the top of the
board like the other
trimpots. Leave Q1 and
REG1 off until the case
has been prepared (see
text). Ensure the sockets
for CON1 and CON2 are
rotated so the wires exit
on the correct side per
the photos.
Figs.6(a) & (b): this board
carries the front panel
controls and indicator
LEDs. Potentiometer
VR3 is held to the
board using PCB pins,
and its terminals are
also connected via PCB
pins. VR1 is attached
using brackets on either
side of its body and
connected to its three
pads (labelled “Anti
CW”, “Wiper” and
“CW”) via short lengths
of wire.
solder a corner pin using a fine-tipped
soldering iron. Once soldered, check
the alignment against the remaining
IC pin leads and PCB pads. Remelt the
solder and realign the IC if necessary
until each pin aligns with its pad, then
solder the remaining pins to the PCB.
Any solder bridges can be fixed using
solder wick with flux paste to draw up
the excess solder.
The surface-mounting resistor can
be soldered similarly, one end at a
time. Straighten the resistor by remelting the solder and nudging it after
the first end is soldered should it be
skewed.
The next components to be installed
are the through-hole (axial) resistors.
The resistors have colour bands, but it
is a good idea to check the values using
a multimeter too. Leave the larger 1W
resistor for last.
Fit the four types of diodes next.
They are all polarised and must be oriented as shown in Fig.5 and the screen
printing on the PCB. Use the smaller
siliconchip.com.au
glass-encapsulated 1N4148 diodes for
D5, D6 and D9. D1, D3, D4, D7, D8 and
D10 are the larger 1N4004 devices,
while D2 is a larger still 1N5404 diode.
The three remaining diodes are
zener diodes ZD1, ZD2 and ZD3,
which are in larger glass packages. ZD1
is 33V (1N4752) while ZD2 and ZD3
are 12V (1N4742) types. Ensure each
is installed in the correct position.
Operational amplifier (op amp)
IC1 can now be installed, taking care
to orientate it correctly. This can be
mounted using a socket or directly
on the PCB.
Follow with transistors Q2-Q6 and
REG2. These all are in TO-92 plastic
packages, so be sure the correct device
is installed in each location. Q2 is a
2N7000 while Q3-Q5 are BC547s and
Q6 is a BC327. REG2 is the LM336-2.5.
Mount the trimpots next. These
are top-adjust multi-turn types; two
are 10kW (VR6 and VR7), one or two
are 5kW (VR2 and VR4), while VR5 is
100W. The 10kW trimpots might be
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labelled 103, the 5kW trimpots as 502
and the 100W trimpot as 101. Be sure
to orientate these with the adjustment
screws as shown in Fig.5. Note that if
using a 2.5kW multi-turn pot for VR1,
VR2 is not fitted.
Now install rectifier bridge BR1; the
diagonally cut corner is the positive
side, so make sure that faces as shown.
You can install the four-way pluggable terminals for CON1 and CON2
now. Ensure these are oriented correctly by inserting the plugs into the
sockets first, then rotating them so that
CON1’s screw heads face toward the
edge of the PCB and CON2’s screw
heads are toward CON3. Then solder
the terminals in place, followed by box
header CON3, orientated as shown.
There are 12 test points located
around the PCB. You can fit PC stakes/
pins in each or leave them bare and
use your multimeter probe directly
onto the PCB pad instead. It is easier
to have a PC stake at TP GND so that
you can use an alligator or crocodile
November 2022 91
The main and both sides
of the front panel PCB are
shown here at 75% of actual size.
Shown opposite is an internal photo of
the completed Supply minus both PCBs, so
you can more clearly see where the various other
parts mount and how the wiring is run. Note the
locations of the three plugs in the lower portion,
ready to plug into the main PCB.
clip for measurements with respect to
0V. If fitting the PC pins, do that now.
Mount the capacitors next. The
100nF, 10nF and 1μF ceramic types
can be installed either way, but most of
the electrolytic capacitors are polarised
and must be inserted with the polarity
shown. The positive side usually has a
longer lead, while there is a stripe on
the negative side of the can. The 10μF
capacitor marked NP is non-polarised
and can insert either way around.
Now mount relay RLY1 and two-way
header CON7. Leave Q1 and REG1 off
for now.
Front panel PCB assembly
The front panel PCB has components mounted on both sides. The
potentiometers, switch and LEDs are
on the top, while CON4-CON6 are
mounted on the underside.
It is easier to solder in the 14-way
box header (CON4) first so that you
have full access to solder its pins on
the top side of the PCB. It is installed
on the underside of the PCB; ensure
it is oriented correctly, as shown in
Fig.6(b), before soldering it in place.
Next, install the six PC stakes for
VR1 and the three for VR2. Then fit
CON5 on the underside of the PCB,
with its wire entries towards the nearest PCB edge.
92
Silicon Chip
Mount switch S2 on the top side
of the PCB. This sets the height position for the potentiometers and LEDs;
however, LED1 and LED2 are mounted
after the front panel holes are drilled
and LED bezels are inserted.
Fit VR2 next, but first cut its shaft
so that the length from the top of the
threaded mounting boss to the end of
the shaft is 15mm. VR2 is supported
by PC stakes soldered to the potentiometer body.
You need to scrape off the passivation coating in the area where the PC
stakes will be soldered so that the solder will adhere. Solder it so that the
top of the threaded section matches
that of switch S2.
Once it is in place, make the electrical connections to the potentiometer
using PC stakes.
Mounting VR1
The mounting method for VR1
depends on whether you are using
a single-turn or multi-turn pot. The
circular cut-out allows the multi-turn
potentiometer to pass through the
hole. Solder right-angle brackets to the
back of the PCB and use a cable tie to
position the pot as shown above. Connect short wires from the pot terminals
to the wiper, anticlockwise and clockwise terminals on the PCB.
Australia's electronics magazine
Similarly, if using a single-turn pot,
it is held in position by right-angle
brackets soldered to the pot body and
the PCB. The brackets need to be soldered to the PCB such that they reach
the pot body and there is some overhang from the cut-out. Again, you will
have to scrape off the passivation coating from the pot body where you will
solder the brackets.
For a single-turn pot, solder its terminals directly to the PC stake connection points.
Making the ribbon cable
Fig.7 shows how the IDC line sockets are attached to the ribbon cable.
Ensure the 14-way wire and sockets are oriented correctly, with the
notches positioned as shown, before
compressing the connectors. You can
do this by placing a small piece of soft
timber (such as radiata pine) over each
side of the connector and compressing
it with a G clamp or bench vice.
Alternatively, you can buy a specialised IDC crimping tool.
Metalwork
Now it’s time to drill and shape
holes in the baseplate of the enclosure
and the heatsink, as shown in Fig.8.
Rectangular and similarly-shaped
cut-outs can be made by drilling a
siliconchip.com.au
series of small holes around the inside
perimeter, then knocking out the centre piece and filing the job to a smooth
straight finish. The power switch hole
must be sized so that it stays clipped
in when inserted into the cut-out, so
take care when shaping it.
The banana sockets have ovalshaped holes (“F”) that can be made
by first drilling round holes and then
using a round file to elongate them.
There are four holes for mounting
the regulator, power transistor and
thermal switch on the rear panel; these
are the holes marked “A” not near
the mains input socket. After drilling
them, clean them up around the edges
on both sides with a deburring tool or
a larger drill bit, so there are no sharp
edges around the rims.
This will avoid puncturing the insulation pads for the regulator and transistor and allow the heatsink to sit flat
against the rear panel for maximum
heat transfer.
It would give even better heat transfer to the heatsink if you cut out a rectangular hole for the transistor, so the
transistor and its insulating pad can
be mounted directly against the heatsink instead of the rear panel of the
case. However, we found that mounting onto the rear panel provided sufficient heat transfer to the heatsink,
satisfactory for most Supply use cases.
Still, if you require a high current at
low voltages for an extended period,
having this cut-out will reduce the
transistor temperature.
Once the drilling and cutting are
finished, temporarily install the mains
IEC input connector and then place the
heatsink against the back panel with
its side about 1mm away from the IEC
connector and the top edge in line with
the top edge of the rear panel. Mark out
the positions for the transistor, regulator and thermal switch holes on the
heatsink through those already in the
back panel.
Make sure all the holes will be
within the central mounting area of
the heatsink and not through the fins,
or the screws won’t fit. Once you’ve
Fig.7: fit the IDC line sockets to the cable as shown here. This way, pin 1 is correct on both sockets but having them on
opposite sides makes routing the cable easier once everything is in the case. Note that some sockets don’t come with
the third locking bar over the top, in which case the ribbon cable isn’t looped.
siliconchip.com.au
Australia's electronics magazine
November 2022 93
Fig.8: the shapes and sizes of some of the cut-outs are critical, so file them to shape carefully and periodically test to see if
the parts fit in the holes. For example, the panel meter will fall out if its hole is too large, as will the rocker switch. For the
binding posts (marked “F”), drill round holes, then elongate them to ovals using a round file.
checked that, drill them in the heatsink, then deburr them for a smooth
finish on the heatsink.
Case assembly
Attach the four 6.3mm-long
M3-tapped spacers to the corners of
the main PCB using 5mm M3 machine
screws. Next, insert the power transistor and the regulator leads into their
allocated holes in the PCB. Slide the
PCB so the transistor and regulator can
later be attached to the rear panel via
the pre-drilled holes using machine
screws (temporarily secure the transistor and regulator to the rear panel
with M3 screws and nuts).
Adjust the leads so that the device
tabs sit flat against the rear of the case
then, making sure the PCB is straight
and not skewed in the case and the
standoffs are directly on the base,
94
Silicon Chip
solder the leads to the PCB on the
top side.
Next, mark out the locations for the
standoff mounting holes in the base
of the case. Also mark out the mounting holes for the transformer. This sits
between the left edge of the PCB and
the left edge of the case, leaving equal
clearance on both sides. The transformer is also positioned centrally
between the front and rear of the case.
Once that is done, remove the transistor and regulator mounting screws.
Solder the transistor and regulator
leads on the underside of the PCB.
Now drill out the holes for the PCB
and transformer (see Fig.9 for the component layout in the case). Also, drill
the Earth lug holes in the base and
scrape away the paint from around the
holes so the Earth connections will be
against the metal, not the paint.
Australia's electronics magazine
Attaching the heatsink
The heatsink is a little taller than
the enclosure. There are two ways of
preventing the heatsink from touching the workbench, as the enclosure
mounting feet are not tall enough to
prevent this from happening.
One option is to add extra spacers
between the feet and the case, such
as two M3 Nylon washers under each
foot to raise the enclosure a little. This
prevents the heatsink from touching
the bench. Use the longer self-tapping
screws supplied with the enclosure to
secure the mounting feet.
The second method is to cut the bottom of the heatsink off, so it is 67mm
tall. That can be done with a hacksaw
or a metal cutting saw.
After you’ve sorted that out, apply
a smear of heatsink compound to
the rear of the heatsink. Press it onto
siliconchip.com.au
the rear panel in its correct position
and install the thermal cut-out using
15mm-long M3 machine screw and
nuts. Leave the screws loose for the
moment, so there is movement to
adjust the mounting.
Insert the 20mm screws for the
transistor and regulator through the
heatsink, then feed them through the
rear panel. Place the TO-3P silicone
washer for Q1 and TO-220 washer
for the regulator onto the screw ends.
Now you can re-mount the PCB, with
the mounting screws for the regulator
and transistor passing through the
device holes.
Push the insulation bush into the
regulator mounting hole before attaching it with a hex nut. For the transistor,
add a steel washer against the device
before attaching the nut. Secure the
PCB to the base with M3 × 5mm screws
and then tighten up the screws for the
thermal cut-out, transistor and regulator, ensuring the heatsink stays square
against the rear panel.
The main PCB is attached to the
base using four M3 × 5mm screws with
Nylon washers. The washers allow
the screws to tighten into the standoffs without touching the screws that
enter from the top.
Front panel label
The panel label (see Fig.10) can be
made using overhead projector film,
printed as a mirror image so the ink/
toner will be between the enclosure
and film when affixed. Use projector
film that is suitable for your printer
(either inkjet or laser) and affix it using
clear neutral-cure silicone sealant.
Roof and gutter silicone is suitable.
Squeegee out the lumps and air bubbles before it cures. Once cured, cut
out the holes through the film with a
hobby or craft knife.
For other options and more detail on
making labels, see the page on our website: siliconchip.au/Help/FrontPanels
Insert the two LED bezels for the
Fig.9: the internal case layout and
wiring. Take care that your unit is
wired up exactly as shown here,
especially the mains wiring, and don’t
skimp on the cable ties, insulation
or Earthing. See the notes in the text
about the transformer secondaries;
they might be labelled backwards,
in which case you’ll have to reverse
the connections. The transformer is
shown here closer to the front of the
case than in reality.
siliconchip.com.au
Australia's electronics magazine
November 2022 95
LEDs into the front panel and place
the LEDs into the holes from the top
side of the PCB, taking care to orientate
them with the longer lead to the anode
(“A”) side. Push the LEDs down onto
the PCB but do not solder the leads yet.
Break off the locating spigot on
potentiometer VR3 (and single-turn
potentiometer VR1, if used) and mount
them onto the front panel with the
washer on the pot side and nut on the
outside. Then mount the on/off switch
with one nut on first, to set the depth
that the panel sits into the threaded
section, then place the second nut on
the outside to hold it in place.
Move the LEDs off the PCB, insert
them into the bezels and solder the
LEDs in place.
The front panel PCB is held in position by the switches and potentiometers; there is no need for extra support.
If you wish, you can add 15mm-long
standoffs at a couple of the corners.
Now attach the pot knobs. For VR2,
ensure the pointer is correctly positioned so it points to the end stops on
the front panel label at both rotation
extremes.
Remaining parts
Mount the IEC connector to the rear
panel using M3 × 15mm screws and
nuts, and the transformer to the base
using M4 × 10mm screws, star washers and nuts.
The panel meter can be installed
next. This is intended to slide and
clip into the panel cut-out, but the
top and bottom clips will not compress because they impinge on the
seven-segment displays.
The solution is to lever out the side
clips to allow the internal PCB and
displays to come out of the surround,
then insert the surround through the
front panel. The top and bottom clips
can now be compressed so the meter
can sit in the front panel. Once it’s in
place, reinstall the meter internals.
Mains wiring
All mains wiring must be done using
mains-rated cable. Be sure that brown
wire is used for Active while the blue
wire is used for Neutral. The green/yellow-striped wire is for the Earth wiring
only (see the wiring diagram, Fig.9).
Connect up the mains leads to the
IEC connector and use a cable tie to
secure the wires together and insulate
using the rubber boot after it is cut so
that the main section is 30mm long.
This is so there is room for the transformer. Pass the wires through the boot
before fitting it.
The Earth wire from the IEC connector must go straight to the Earth
mounting point on the case. This is
attached using a crimp eyelet secured
to the base with a 10mm M4 screw, star
washer and two M4 nuts. If you haven’t already done so, you must scrape
the paint away from around the hole to
ensure the Earth connects to the metal
of the case and not just the paint.
The wires connect to the mains
switch using female spade crimp
connectors. Be sure to cable tie the
wires together to prevent any broken
wires from coming adrift. Additionally, cover the spade connections with
25mm diameter heatshrink tubing.
Connect the transformer secondaries to CON1 using 7.5A-rated wire.
Note that there is an anomaly for the
transformer secondary outputs. The
photos shown for the transformer on
Fig.10: this
front panel
label can be
downloaded as
a PDF from the
Silicon Chip
website and
printed out to
form a label for
the case.
There is an
alternative
label without
voltage
markings
to suit a
multi-turn
potentiometer.
96
Silicon Chip
Australia's electronics magazine
siliconchip.com.au
These four
close-up views
show how the
panel meter,
mains switch,
mains input
socket and
thermal switch
are wired up
and insulated.
the Jaycar website have the terminals
for the 0, 9, 12, 15, 18, 21, 24 and 30V
as shown in our wiring diagram.
But on our sample transformer from
Jaycar, the windings only produced the
expected AC voltages when the order
of the taps (including the 0V and 30V
ends) were reversed.
The discrepancy wouldn’t matter if
the taps were symmetrical, but they are
not, and the resulting voltages are quite
different depending on which end is
defined as the 0V tap. It is important
to have the 0V tap correct to get the
required sequence of 0, 9, 12, 15, 18,
21, 24 and 30V. Otherwise, you will
get 0, 6, 9, 12, 15, 18, 21 & 30V.
To make sure you have the correct
windings, use a multimeter set to measure AC volts to probe the secondaries and carefully check their voltages
with power applied.
Apply power by connecting the IEC
plug to the mains with the IEC plug
inserted into the IEC connector at the
rear of the power supply. The fuse will
need to be installed in the IEC connector. Check that the neon lamp in
the switch lights up when the power
switch is on.
Find the two ends of the windings
first; that should give the full 30V AC.
Then check the secondary taps off each
end to find the following voltage. It
should be 9V AC at the 0V end and 6V
AC at the 30V end. These voltages may
be around 10% higher due to mains
voltage variations and the fact that the
transformer is unloaded.
Once you’ve verified which is the
0V end, switch off power and wire up
the secondaries as per Fig.9.
The Supply should look like this once you have finished fitting all the
parts and wiring them up. After checking it works, all that remains is
to attach the lid using two of the supplied screws on either side.
siliconchip.com.au
Australia's electronics magazine
November 2022 97
Next, connect the IDC cable between
the two boards and wire up the meter.
The supply ground for the meter is not
connected and can be either cut short
or connected to the NC terminal at the
centre of CON5. That centre terminal
is used as a wire keeper; it makes no
electrical connection.
Attach the banana sockets to the
front panel, wire them up to CON2
(black for negative, red for positive)
and connect the Earth terminal to the
chassis.
Testing and calibration
Before applying power, check your
wiring carefully and ensure all mains
connections are correct. If you are
using a socket for IC1, insert it now
with the proper orientation. Take care
that none of its leads fold under its
body during insertion.
Wind VR1 fully anti-clockwise
and VR3 a little clockwise from fully
anti-clockwise. This sets the Supply to
its minimum output voltage at a low
current. Wind VR6 fully clockwise by
turning it until a faint click is heard, or
if you don’t hear a click, wind for 20
turns in the clockwise direction. This
prevents the regulator output voltage
from going negative initially before
being set up correctly.
Switch power on, and the voltmeter should show around 1.2-1.3 V.
Check that you can increase the output
Summary of test points
TP1
is the negative voltage applied to REG1 via VR1 and VR2. It is
measured with respect to GND (or V- at CON2) and can range from -1.2V
to -1.3V. VR6 is adjusted to provide a 0V output at V+ on CON2 when VR1
is fully anti-clockwise.
TP2
is the -2.49V reference. It is measured with respect to GND (or
V- at CON2) and adjusted via VR7.
TP3
is the current limit setting, measured between TP3 and TP10 at
CON6, that ranges from 0V to 2V when correctly adjusted. The upper and
lower thresholds are adjusted by VR4 and VR5, respectively. CON6 allows
the current limit setting of VR2 to be measured using a multimeter or other
floating voltmeter.
TP4
is the raw negative supply and should read around -8V to -9V relative to GND.
TP5
is the output of current monitor IC2, giving 1V per amp of load
current, measured with respect to TP2 (-2.490V).
TP6
is the negative voltage applied to IC1a. TP1, the output of IC1a,
should be within a few millivolts of TP6. See above for the significance of
TP1.
TP7
should be near 0V, rising toward 0.6V when power is switched
off, measured with respect to GND. This is the AC detection voltage for the
relay switching. 0V = AC detected, 0.6V = no AC detected.
TP8
should rise from 0V to 13.6V with respect to GND over several seconds when power is first applied and drop quickly to near 0V when
power is switched off. The time the voltage takes to rise from 0V to 13.6V
is the switch-on delay.
TP9
should be at about 12V with respect to GND, generated by zener
diode ZD2.
TP10
is the current setting offset to compensate current readings at
TP5 (see TP3 above).
TP 25V is the positive supply and should measure around 25V with respect
to GND.
98
Silicon Chip
Australia's electronics magazine
voltage by rotating VR1 clockwise.
Take care not to increase the output
above 35V as the output capacitor is
only rated to handle 35V.
If the Supply does not appear to be
working at this stage, recheck your
construction. In particular, check that
there is about -8V (or similar) at TP4
and about 25V at TP25V. Check that
TP1 is around 0V.
Once the voltages appear correct, it
is time to make adjustments. Firstly,
the precision reference needs to be set.
Measure the voltage between TP GND
(or the negative output terminal on the
front panel) and TP2, and adjust VR7
for a reading of -2.490V.
Once adjusted, the regulator can
be set to produce a minimum of 0V.
This is done by initially winding VR1
fully anti-clockwise and measuring
between the Supply’s output terminals. Adjust VR6 anti-clockwise until
the reading just reaches 0V.
Next, we set the maximum 30V
output range. This is only if you are
using a single-turn potentiometer for
VR1. For the multi-turn potentiometer,
ignore this step since VR2 is not fitted.
For the multi-turn pot, the maximum
voltage will be close to 30V when VR1
is wound fully clockwise, possibly a
little more.
Carefully adjust VR1 clockwise and
stop where the voltage is 30V or when
the pot is fully clockwise, whichever
comes first. If the pot has reached full
clockwise rotation and the voltage is
less than 30V, adjust VR2 clockwise
until you get a 30V output. If 30V is
reached before full rotation, adjust
VR2 anti-clockwise and VR1 clockwise a little each time until 30V is
reached with VR1 fully clockwise.
The current limit range is adjusted
by rotating VR3 fully clockwise and
measuring between TP2 and TP3.
Adjust VR4 to obtain 2V. That sets the
maximum current to 2A.
The minimum current setting alters
the lower end of VR3 to cancel out
the offset voltage of IC2. To set this,
rotate VR3 fully anti-clockwise, then
measure between TP5 and TP10 and
adjust VR5 for 0V.
It shouldn’t be necessary to readjust
VR4 again for the maximum current
limit as the voltage adjustment made
with VR5 will only change the maximum current setting by about 20mV,
which is insignificant compared to the
original setting at 2A. But you could
tweak it again if you want to.
SC
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SERVICEMAN’S LOG
Toys with a serious purpose
Dave Thompson
You might think I’m running out of things to repair because I’m working
on toys again. But actually, while this device appears to be made of child’s
toys, it has a serious medical use. It is used to check the hearing of young
children who can’t yet talk (or don’t like to) but this particular example
didn’t survive the tender mercies of one particular delivery service...
It will come as no surprise to many that I sometimes get
weird and wonderful devices through my humble workshop. Word somehow leaks out through the concrete-jungle
telegraph that I am willing to look at anything, always with
a view to (hopefully) repair it.
A few weeks ago, a long-time Silicon Chip reader from
another part of the country contacted me about a device
he had designed and built many moons ago that needed
some electronics-based love and attention.
Darryl was an audiologist in one chapter of his life, and
as an electronics enthusiast, he had designed and built
several VRA (visual reinforcement audiometry) devices
to assist with testing very young children’s hearing. The
usual traditional tone-testing we all know as adults is not
so easily performed on toddlers.
These so-called ‘puppet boxes’ are utilised as an audio-
visual testing aid. In this case, the ‘box’ itself is in the form
of a large, round, carpet-covered timber tube about 1.8m
high and 50cm in diameter. The front ‘face’ of the tube
is covered by a dark Perspex cover almost to the bottom,
where there is a panel covering the electronics.
100
Silicon Chip
There are three levels to this box, all isolated and separated from each other. In each of the levels is a different
animatronic ‘toy’ which, when activated, is illuminated
by an LED spotlight in the top-left corner of that section.
A hand controller – a jiffy-type box with three press-tomake, release-to-break switches on a long lead activates
each of the toys.
The ant, the gorilla and the elephant
In this box, starting in the top section, is a large ant in
a forest-type setting. He speaks a phrase and his bug-eyes
move and blink when the appropriate button on the hand
controller is pressed. The animation and light activates for
about 15 seconds before going dark again.
The middle level contains a furry gorilla toy, set in a
yachting scene; this toy dances and his mouth opens and
closes along (roughly) to a popular 90s novelty song.
The bottom section has a pink plush elephant, which
animates with its legs moving in time to a typical child’s
‘crawling song’. In practice, I suppose it doesn’t really
matter what toys are there and what they do; they are just
something to grab the attention of the child.
I was certainly entertained and admit to pressing those
buttons a lot – once I’d fixed it. I now know the lyrics to a
crawling song, so life is full of surprises!
In use, a child being tested is ‘trained’ to respond to
a test tone they hear through headphones by watching
a visual stimulus every time they hear the tone. The
audiologist plays a tone and activates the puppet box at
the same time. The child looks at the animated toy and
‘learns’ that when they hear the tone, they’ll see the toy
light up and move.
As the audiologist changes the tone frequency and the
volume level, they can build a picture of that child’s hearing and diagnose accordingly. It’s a time-honoured method
of testing children’s hearing.
The idea of the puppet box is relatively simple, and the
implementation in this case very clever; I suppose any animated toy could do the job, and all we need is a suitable
power supply, some lights and a timer board to control it
all. The majority of us would likely never see such a thing,
unless we had a very young child in need of having their
hearing tested.
I’ve certainly never seen one before, even though I’ve
had many hearing tests over the years, so all this has been
an education for me.
Australia's electronics magazine
siliconchip.com.au
The VRA in my workshop is a classic example of someone with electronics knowledge and the vision to create
something practical and useful using that knowledge.
These things should have become an industry standard.
They might very well be, for all I know – no doubt some
company makes and sells them for exorbitant amounts of
money. Still, for whatever reason, this box, and several
others like it Darryl made, have stayed a relatively ‘local’
solution to this problem.
Damaged in transit
The problems with this unit started when the puppet
box was shipped from ‘up north’ to ‘down south’. When
it arrived, it no longer worked. According to the people
involved, the packaging showed no signs of trauma, and
the unit was intact, but there was obviously something
quite wrong with it.
The sections lit up with the button press, but the only
toy moving was the elephant. While I got audio from the
others, the ant and the gorilla were not animating at all,
though their LED spot lights did activate.
The recipient of the box got in touch with Darryl and
then he got hold of me. Me being in the same town down
here as the customer likely sweetened the deal. He asked
me if I could take a look at it, rather than ship it all the
way back ‘up north’.
Of course, I said yes, and really, what else could I do?
The chance to work on something new and unique is many
a serviceman’s dream (well, it is mine anyway).
The box arrived at the workshop nicely bound up in a
woollen rug, although that was not the original shipping
material. After unwrapping, it seemed intact and undamaged when viewed from the outside. However, after plugging it in, connecting the hand controller and trying it,
there was obviously something wrong.
The ant and the gorilla toys looked to be sprawled on the
floor of their respective compartments, and there was no
movement at all visible
when the compartment
lights came on. The elephant at the bottom also
looked a bit skewed, but
it did at least have some
music and motion when
the relevant button was
pushed.
The first thing to do
was remove the smoked
black Perspex cover,
exposing the toys. It was
held on with standard
super-screws, countersunk into the plastic.
Some kind of sealant
had been applied around
the bevelled edges of the
screen, perhaps to remove
any sharp machining
edges that might catch a
small hand.
With the screen off, I
could see what was going
on. The ant was meant to
siliconchip.com.au
Items Covered This Month
•
•
•
•
•
Toys with a serious purpose
A Sony tuner with a side of gum
Washing machine and mixer repair
Repairing a Toyota wheelchair lift
Restoring a Porsche 928
Dave Thompson runs PC Anytime in Christchurch, NZ.
Website: www.pcanytime.co.nz
Email: dave<at>pcanytime.co.nz
Cartoonist – Louis Decrevel
Website: loueee.com
be standing upright and be glued to the back of the compartment, while his ‘feet’ were fixed to the timber ‘floor’
of the section to hold it into position. The glue holding it
upright had torn away from the wrap-around cardboard
picture background, so the toy was just folded up headfirst like a rag-doll on the floor.
I unwound him and stood him up and pressed the button. This time, his eyes rolled and blinked and he said
his lines quite happily. A simple fix for this one then;
all I had to do was clean him up and glue his backpack
back into place on the background to secure him in the
right place.
One sick gorilla
The gorilla section was a bit different. He’d come well
adrift and was crumpled onto the floor. He’d been tacked/
glued in three places to hold him upright – all these points
had been torn away, as evidenced by the paper stuck to
the glued areas. The box had evidently suffered quite an
impact – at least enough to knock these guys free.
The gorilla didn’t move at all, so something electrical
had gone wrong. He did, however, emit the opening notes
of that novelty song,
but it sounded like a
stuck record, playing
the same sound-bite
over and over.
A check with Darryl confirmed that
it should play the
whole song for the
allotted time, while
the gorilla would
usually dance and
‘mouth’ the words.
Apparently, something else was amiss
here.
All the toys were
originally battery-
powered. Power for
this box – and the
toys and lights –
was derived from
a battery charger
mounted into the
cavity in the base of
the unit.
Australia's electronics magazine
November 2022 101
Switched permanently to the 6V setting, the charger was
working because all the compartment LED lights activated
on the press of the button. Two of the toys moved, however
weirdly, so the juice was making it through to all but the ape.
The lights and animation were all controlled by a common timer, so they all operated for the same duration. It was
mounted on top of the charger. The ammeter on the charger indicated when the toys were powered – again, except
for the gorilla, which was not surprising as it seemed to be
the most affected by the drop.
The toy was easy enough to remove – one foot was still
glued to the base, so I carefully got a box-cutter style knife
blade in between the glue and card and gently separated
the two. Once free of that, I then had to desolder the power
leads, which went directly to the battery compartment and
were soldered to the contacts there.
With the toy removed, I pressed the button and my trusty
multimeter showed roughly 6V getting to the now-bare
wires, so whatever was wrong was inside the toy.
Fortunately, the manufacturer had installed a zip in the
bottom of the plush, and when opened, this revealed the
internal mechanism. A large torso-shaped plastic clamshell
box was held together with four screws, and with these
removed, the two halves came away easily.
Access was very tight – the plush would only pull back
a limited amount, as a cable tie secured the neck area to
the actuator case. I had to cut and remove that tie to allow
deeper access, and as there were linkages to the arms, the
head and the mouth, I had to be careful I didn’t damage
those.
More damage inside
Inside the actuator was the sound and movement controller module. This was made from two small PCBs joined at
right angles, screwed to the plastic case, with one containing a COB (chip-on-board) IC that likely had the song programmed into it. There were a few other surface-mounted
components which I assumed controlled the animatronics.
The bottom half of the case also contained a reasonably
complex plastic gearbox and an electric motor. The motor
is a typical small DC motor that powers countless toys. Its
102
Silicon Chip
leads were adrift, explaining why there was no movement.
I applied a bench power supply at 5V to that motor
directly and sure enough, it fired into action, so that was
the likely problem. A suppressor capacitor was also connected across the motor’s terminals – this had broken away
on one side, so a quick hunt through my spares box had
that replaced and the connections remade and solidly soldered in place.
A press of the button proved the gorilla now jiggled and
animated, but his mouth didn’t move (it should) and that
song was still just a machine-gun-style delivery of one note.
I didn’t think I’d be able to do anything about the lack of
music, but I could look into that gearbox and see why the
mouth didn’t articulate.
After stripping the gearbox assembly from the toy (which
meant pressing a few pin-hinges out), I could see an actuator shaft that should have operated the mouth had snapped
at a join in the neck area. It was a clean break and there
was plenty of meat there for a glue job, so I hunted through
my adhesives collection for some plastic-welding cement.
This material is standard PVC or similar, and a test drop
of glue onto an open area confirmed that it would indeed
weld those bits together. Once glued and held for a few
minutes (nothing seems to go on as long as waiting for glue
to harden), I carefully reassembled the gearbox, motor and
linkages and left it overnight before powering it up.
The next morning, I held the gorilla roughly in place and
pressed the button. Success! He did a little dance, and his
mouth snapped open and closed. The ‘music’ wasn’t happening properly, but Darryl mentioned that as long as there
was some noise, it would suffice for the purpose.
I suppose we could have sourced another toy, or even
grabbed a sound module from a charity shop talking toy,
but a quick look showed that animated toys are really
expensive these days. I learned over the phone that most
donated toys go pretty quickly from the Salvos and Vinnies stores.
Shaving the gorilla (no, really!)
After zipping him back up, I cleaned off as much of the
old hot-melt glue originally used to hold the gorilla in from
his fur coat as I could. I wouldn’t like to have to get this
glue out of a real coat, because it makes a nasty mess! Shaving it partially was the only way to remove the bulk of it.
I used the rest of the glue as a template to fit the limbs
back into their original positions, which were pretty obvious due to the torn-away card. I also used the same glue
to reattach the elephant toy to the bottom, which was a
little askew on its mounts, but still working as intended.
After a bit of tidying up of wire runs and the dog-eared
and torn panoramic picture backgrounds, I was satisfied it
was all working as well as it ever would. Due to the extra
dollops of glue liberally applied to the toys, I’m reasonably
sure they won’t be coming loose again. [I’m sure the post
office would accept your challenge – Editor]. If they do, I
think we’ll have bigger problems!
The only thing left to do was to replace the front cover
and give the box a good workout. As it has been in the
workshop for a couple of weeks, all my visiting customers see it and, of course, ask what it is and how it works.
I pass them the hand controller and everyone seems to
have fun making the toys animate; it makes for a good
conversation piece.
Australia's electronics magazine
siliconchip.com.au
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It would have gone back by now, but the designer and
the customer are talking about modding it for use with foot-
operated switches as well. That would require finding some
single-pole press-to-make, release-to-break stomp-box type
switches (sometimes called momentary switches), some of
which I think Darryl has already sourced.
I initially thought readily-available musicians’ foot
switches would be ideal, as they are designed to be trodden on. However, they are usually quite expensive and are
typically multi-pole, press-to-make, press-to-break types
used for switching effects in and out of the signal chain.
Anyway, with the right switches in hand, it will be a
relatively simple matter of taking off the power supply
cover again and adding another paralleled multi-pin plug
to the existing facia.
As the audiologist may want to have the switches in a
different room to the box (usually, they are in the same
room), we’ll have to find a way to utilise jack panels on
the walls. Still, that’s for another day – at least now, the
box can be returned to normal service and delight kids
of all ages.
One Sony tuner with a side of gum
B. H., of Little Mountain, Qld ran into one of those situations where, while diagnosing a fault, the measurements
didn’t seem to make sense. Luckily, he managed to figure
out the reason for those discrepancies...
I inherited a Sony tuner that played for many years, but
within the span of one week, its FM output diminished
to zero. I thought the most likely culprit was the first RF
transistor. This unit is beautifully made and is of the PLL
type, which was very novel back in 1981. After googling
for many days, I could not find a schematic, so I started
from the beginning.
This unit is not unusual; the RF input stage is followed by
the mixer/oscillator, then a dual transistorised IF stage, followed by an IC that turned out to be the PLL FM IF decoder,
which includes another six stages of IF amplification.
Three ceramic filters are associated with the transistor
amplifiers. However, I couldn’t find a bias voltage at the
base or emitter of either transistor. I also checked the voltages on the connected resistors.
They had used red gum to stop some flying leads from
interfering with the station pointer dial mechanism. This
blob covered a resistor and solder joint.
I removed the red gum to access the resistor, which I
believed to be the bias provider. The resistor had the correct value on the component side, but the solder joint on
the copper side was peculiar. I could measure a positive
Servicing Stories Wanted
Do you have any good servicing stories that you would like
to share in The Serviceman column in SILICON CHIP? If so,
why not send those stories in to us? It doesn’t matter what
the story is about as long as it’s in some way related to the
electronics or electrical industries, to computers or even to
cars and similar.
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Please be sure to include your full name and address details.
104
Silicon Chip
voltage on the resistor lead, but the surrounding solder
tested 0V, suggesting a dry joint.
Re-soldering it made no difference; the pad and resistor wire were still 14V apart. It all looked proper on closer
inspection; the wire was surrounded by solder with the
correct colour. But I could not find any continuity between
the wire and the solder.
I think the gum from the PCB component side must
have corroded the tin coating of the resistor wire all the
way down into the solder joint, isolating the resistor from
the solder. Replacing the resistor with one soldered on the
copper side of the PCB fixed it.
Washing machine and mixer repair
P. M., of Christchurch, New Zealand made three successful repairs on very different pieces of equipment lately...
The first was my washing machine, which has been reliable for more than ten years. Recently, I switched it on and
instead of the usual bright display of LEDs showing the
wash program and time, the LEDs were dull and flashing
slowly. Switching it off and on again didn’t help.
A Google search first turned up some unhelpful suggestions, but then there was one that seemed to be on the right
track. The post mentioned a faulty 10µF 450V electrolytic
capacitor on the main board and that person had found a
replacement at Jaycar.
I was planning to go to Jaycar later that day, so I added
the capacitor to my list. The post also mentioned cutting
a hole through some plastic with a hole saw to get to the
part, which sounded a bit extreme to me at first.
The machine’s top must be removed to get to the main
board. Once away from the wall, after removing a few
screws and some plugs, out comes the main board. The
board sits in a plastic tray filled with clear sealant covering most of the components. The capacitor was visible in
the middle of the board and was obviously faulty as the
top had bulged open.
The problem was that the solder side of the board was
face-down in the plastic tray, and I didn’t want to disturb
the sealant holding it all there. The hole saw was starting
to make sense now, but still seemed a little risky. Instead,
I drilled a series of small holes to make a circle that I could
nibble out to make a hole to access the solder joints of the
capacitor.
I was glad I did this as there were more components on
the solder side of the board, and hitting any of them with
the hole saw would not end well. I could now replace the
capacitor and used silicone sealant to refit the plastic piece
I had removed.
As I was putting it all back together, I remembered the
original poster had said to be careful not to pinch the rubber hose at the back of the machine when refitting the top
cover. This was valuable advice, as when I looked at the
hose, it was indeed pinched under the top. This hose is
part of the water level sensor, and if I had not freed it, the
machine would have overflowed the first time it was used.
Unsurprisingly, when I fired it back up, it was working
correctly again.
Secondly, I repair a lot of analog audio mixers of various
sizes; some of the most common problems are faulty faders. Those slots in the panel for the faders allow ingress of
all manner of dirt and liquid spills. In most of these units,
everything is mounted on one large circuit board, including
Australia's electronics magazine
siliconchip.com.au
the faders, so access means removing all the knobs, nuts
and screws to get the board out.
I have found that in many cases, there is sufficient space
at the front edge of the board to wiggle the fader out once
it has been desoldered, and a new one can be refitted the
same way.
The mixer I worked on recently did not have this space,
but I still managed to get the faulty fader out. Getting the
replacement in would be a different story until I had an idea.
I fed a piece of fine wire through the fader slot from the
top of the panel and wiggled it around until I got it past
the PCB. I then tied the wire to the fader’s shaft and used
it to slowly guide the fader to its location, where I could
then push it back into the holes in the board, resolder it
and test it. That saved me a lot of work.
Thirdly, a friend sent me his large stereo amplifier that
had stopped working after a heavy session. After a bit of
probing, I discovered the power transformer’s primary
winding was open circuit. It is not uncommon for Japanese-
manufactured equipment to have a thermal fuse inside the
power transformer in series with the primary winding.
These fuses are non-resetting, so the unit will no longer
work after they trip.
At first, I could not see the fuse; they are often buried
inside the bobbin that holds the windings.
After snipping away some small pieces of the bobbin,
I could just see the fuse at the bottom of a slot roughly
5mm wide and 40mm deep. With a suitable probe, I could
determine that this was where I needed to connect to the
winding, but how could I connect to it when my soldering iron would not fit in the slot without melting everything around it?
Then I remembered that my soldering gun uses a piece
of looped copper wire as an element and it is not very
wide. I dropped a small grain-of-wheat lamp into the slot
and powered it from my bench power supply so I could
see. I was then able to solder a wire to the fuse to complete the circuit.
That got it back into business, but as I had defeated the
thermal fuse, I checked to ensure a conventional suitably-
rated fuse was in line with the transformer. The thermal
fuse is an extra line of defence, but there are millions of
power transformers out there that do not have one. I have
even seen some transformers with an extra wire to bypass
the thermal fuse should it fail.
Repairing a wheelchair lift inside a car
J. W., of Hillarys, WA is another regular contributor to
this column. His latest entry involves repairing a wheelchair lift built into a Toyota Regius van...
A friend rang recently and asked if I could have a look
at his daughter’s wheelchair lift. He said that the lift was
not going back to the home position in the back of the van.
He had contacted several local auto electricians, but they
were not interested in looking at it, as it was a Japanese
import with no service information available. So I went
around to have a look.
The system was a genuine Toyota accessory and seemed
well-built (much like their cars). If the carriage was taken
too low, it would start to lift the van!
The lift has large motor driving screws that lower and
raise the platform, and that part was working as it should
(see the photo at upper right).
siliconchip.com.au
The wheelchair lift attached to a Toyota Regius van.
Once the platform was back at the level of the van floor,
two smaller motors and a second set of screws was supposed to drive it into the home position. This was not
happening.
The system was all-electric and controlled by four relays
& four microswitches. The main control assembly was easy
to unbolt and inspect. It had three large onboard relays plus
a smaller one.
The large ones were not enclosed, so I could see them
operating; they seemed to be working OK. I unplugged and
tested the small relay, and it was also functional.
Next, I decided to start checking the microswitches. Two
were easy to access and tested OK. The other two, which
switched power from the large motor to the smaller motors
and stopped the platform in the home position, were challenging to access.
After some deliberation and standing on my head in the
back of the van, my friend figured out that we needed to
take off the runner plate as that would let me access the
microswitches and wiring.
After that, I tested the final two switches, which were
fine. I then lay on the van’s floor and used a torch to look
at the wiring to the platform, which was hidden in part
of the frame. It was encased in black plastic cable chain.
Sticking out of the cable chain was a broken wire. I managed to effect a repair by joining the broken ends using a
small section of new wire.
The break had occurred because the plastic cable chain
had broken at one end, so the wiring was not supported.
I managed to cut some flexible conduit and fit it over the
broken section, which did not actually need to be flexible. We then put the whole system back together, and it
worked as it should.
The whole process took many hours over several days.
My friend and I were relieved finally to have the lift back
in the van and working again.
Restoration of a Porsche 928 (Central Warning System)
D. T., of Sylvania Southgate, NSW previously wrote
about repairing a Porsche 928 demister control relay (February 2022, pages 88-90). He’s still working on restoring
that car, but this time, it’s the warning system that’s on
the fritz...
Australia's electronics magazine
November 2022 105
During my restoration of a 1982 Porsche 928, I came to
the Central Warning System (CWS). In addition to all the
usual warning lights in the instrument cluster, the 928
CWS integrates all the warnings that the car generates into
one central warning light, also in the instrument cluster.
As well as illuminating this light if there is a major problem like oil pressure, high temperature or low fuel, it will
also light up with less common things like a low washer
bottle level or worn brake pads.
This warning light repeatedly flashes a specific number
of times, with the number indicating what the problem
is. Low-importance warnings can be cleared by pressing
a button, but high-importance warnings can’t. The central
warning light is also duplicated in the centre console – the
two lights are connected in parallel. I guess that way, if the
driver doesn’t notice it, the passenger might.
Finally, the CWS also turns all the instrument cluster
warning lights on each time you start the car, so you can
verify they’re working correctly.
Electrically, the CWS sits between the sensors and the
dashboard warning lights. The less-expensive model of the
car had a simple adaptor fitted in place of the CWS that
connected the sensors directly to the dash warning lights
in the traditional way.
With it plugged in, there was no response from any of the
instrument cluster warning lights or the light in the centre
console. I found that the light in the centre console was
shorted out with a piece of wire deliberately soldered across
it – I guess at some stage in the past, the CWS has failed,
and this was the easiest way to eliminate the warnings!
The indicator panel cleaned up with the short removed,
but I wasn’t surprised when it didn’t change anything –
with a short across the lamp, the driver was probably toast.
The next step was to open the CWS unit. I’ve found the
Porsche 928 modules to be quite serviceable in the past,
and this one was no exception. After I bent a few tabs, the
internals slid out of the aluminium housing to reveal a sandwiched pair of PCBs with plenty of parts – all through-hole,
and all discretes except for one 14-pin DIP IC.
The IC was an SN8400 with a TI logo, but I couldn’t find
any data on it. I decided it’s nothing like an embedded
microprocessor – this car was designed in the mid-1970s,
and they didn’t exist then. There were plenty of transistors
onboard, of seven or eight different types, with all but two
being in TO-92 plastic packages. Some I could find data
on, but most not.
When I tipped the housing over, a blackened 1W resistor
fell out. It only took a minute to figure out where on the
board the resistor came from, and tracing showed it drove
the two central warning lights – no doubt it overheated and
melted the solder because of the external short. The driver
transistor connected to it also had a crack in it.
I didn’t recognise the number on the transistor and
couldn’t find any data on it, but I measured a few others with the same marking and decided a BC547 would
probably do. Having fixed those two items, I now had the
central warning lights stuck on, but no instrument cluster
warning lights.
Next, I looked at the electros. There were some standard-
looking aluminium electros which all looked OK, but there
were also some plastic-cased 22μF units that had brown
residue around the top. Brown residue is never good on
electros. Funnily enough, it wasn’t anywhere near any
106
Silicon Chip
seam in the case, but all the plastic-cased electros had it
to some degree.
I tried measuring them in-circuit with my Fluke, but I
haven’t really used the capacitance measurement facility
on the meter before and was dubious about it, especially
since I was measuring in-circuit. I wasn’t surprised when
I measured something other than the marked value.
I decided to remove one and measure it out of circuit and
it measured low – about 8μF. Not really being sure how
they were used, I thought I might as well replace them all.
I now had a flashing central warning light, but the flashing was inconsistent, bordering on gibberish. I thought it
might be because multiple valid warnings were present (for
example, the fuel tank and washer fluid were both empty).
However, posts on a Porsche forum said that it managed
this OK when it was working correctly.
The next step was to check all the transistor junctions
using the Fluke’s diode tester. I felt more confident about
this than I did with the capacitors – the voltage across a PN
junction should never exceed about 0.7V at low currents.
Plus, there were enough of each type of transistor on the
boards, so I could guess what was normal and what wasn’t.
Some types gave high base-emitter readings of about
1.3V. I decided these were Darlingtons with two diode
drops between the base and emitter.
I found two transistors I didn’t like. One I replaced with
a BC547, but the other was one of these Darlingtons. I spent
a bit of time looking around to try to find something to
replace it with, but TO-92 Darlingtons aren’t that common
even when there isn’t a silicon shortage, so in the end, I
replaced that device with a pair of BC547s connected as
a Darlington.
After that, I had a consistent flash indicating I had no
petrol, and the instrument cluster lights started working.
Afterwards, I measured the aluminium electros I’d replaced
on the bench and saw a range of values, some very low,
under 1μF. Interestingly, when I measured the new ones
in-circuit, they all measured about 22μF – chalk another
one up for the Fluke.
Editor’s note: the SN8400 is likely a quad NAND gate like
the SN7400 but with a different (possibly wider) operating
SC
temperature range to better suit vehicular use.
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Suitable parts for the
WiFi DC Load
Thanks to Richard Palmer for
the WiFi DC Load project (September & October 2022; siliconchip.au/
Series/388) and thanks for all the component links you supplied. I have some
questions about the remaining parts.
The case is described as metal. Is
it actually all metal, or are the front
panels plastic? I’ve found cases on
eBay described as “270mm x 210mm
x 140mm Blue Metal Enclosure” with
the material described as ‘metal & plastic’ listed for $45.47 with free delivery.
There’s another similar one available,
also ‘metal & plastic’. The seller is
“silaluna88” and the brand “Uxcell”.
Are those the right items?
From the text, I take it that the relay
is chassis mounted, with a contact rating of at least 30A. I assume a minimum contactor operating voltage of
150V DC with a suggested opening
time of no more than 10ms and a 5V or
12V coil. I can source a PTRH-1C-12ST5-X relay that seems suitable, except
the coil operating power is 0.9W.
The following components are not
available until 2023: MCP4725A0T-E/
CH and ADS1115IDGSR. What about
the wirewound resistors – can I substitute MSR3-0R02F1 with better specs?
(B. P.)
● Those are suitable enclosures; the
front panel is metal. The relay current
is determined by the BC817 driving
transistor’s 500mA limit. That should
be plenty to drive your suggested
relay coil.
Its mounting lugs would be an
improvement on the one I used in
the prototype, a 30A “Arduino module” with an onboard driver transistor
found on eBay (siliconchip.au/link/
abh6 or siliconchip.au/link/abh7).
The relay operating time is a secondary concern for short-circuit protection as the software detects over-
current within around 1ms, switching
the Mosfets off in less than 2ms. The
relay is most useful for reverse voltage protection, where the Mosfets can
108
Silicon Chip
conduct more than 100A each when
reverse-biased, as well as over-voltage
protection.
In both cases, the load’s design is
conservative and should easily survive
the 10ms relay operating time.
Both the ADS1115 and MCP4725 are
available as part of Arduino modules
on eBay. I have successfully floated
devices off these modules in the prototype when unable to source them from
other suppliers. Sometimes the ADC
module actually contains an ADS1015,
but the loss of accuracy is manageable
in this application.
Alternatively, you can get those
two parts along with all the other
SMDs and some other useful parts in
the Silicon Chip kit (siliconchip.au/
Shop/20/6399).
Tweeter and subwoofer
drivers for isoundBar
Concerning the tweeter part number
specified for the isoundBar (August
2022; siliconchip.au/Article/15426), I
have conducted an exhaustive search
of the Vifa/Peerless (Tymphany) catalogue, and the model BC25SC55-04
is the only one to be found. I believe
the 4Ω tweeter will work perfectly
well in this instance. This tweeter is
also stocked by Altronics (Cat C3019).
Further to the tweeter in-cabinet
placement, I have reviewed the quoted
published axial response diagrams. In
my view, the high-frequency response
would be disappointing unless the
room in which the soundbar is to be
used has side walls fairly close to the
position of the television and soundbar.
My solution would be to modify the arrangement of the midrange
speakers so that the tweeters could
be positioned facing the front and the
outer midrange speaker be relocated
inboard. I would flip the second midrange speaker 180° on the designated
panel. The associated port for this
isobaric subsystem would need to be
relocated adjacent to the repositioned
front-facing tweeter.
Australia's electronics magazine
As for the subwoofer option, I’m
afraid that Ryda states it to be obsolete/
discontinued. Only US eBay sellers
appear to be offering it, so cost-plus
freight makes it unaffordable. (R. K.,
Cessnock, NSW)
● Allan Linton-Smith responds: you
are right; I used the BC25SC55-04
tweeters, not -06.
The so-called ‘mid-range’ front-
facing speakers are actually full-range
and have an excellent frequency
response up to 20kHz. All the frequency response measurements published in the article were taken with
the microphones positioned directly
in front of the isoundBar.
There is no need to add tweeters
for more front-firing high-frequency
sound, so I do not recommend you
place the tweeters on the front panel.
Otherwise, the sound will be very
‘bright’ and higher frequencies will
predominate.
The tweeters are deliberately positioned at each end to give a ‘spacedout’ effect. Most TVs are located in
rooms with adjacent walls, and some
high-frequency sound waves will be
reflected off the back wall, ceiling etc.
This helps to avoid a muted off-axis
response.
Even in the large, open Silicon Chip
office, this spatial effect was noticeable, and it was tuneable by using the
tweeter level control to suit personal
preferences.
Unfortunately, the JBL subwoofer
has been enormously popular and is
now difficult to get. We have obtained
a sub with almost identical specifications from a local eBay supplier named
“Boss Audio D10F” for $130 (eBay:
siliconchip.au/link/abh8). You will
probably have to be quick!
Questions for the
isoundBar project
I am considering building the
isoundBar project (siliconchip.au/
Article/15426), but I have a few questions. How do you control the overall volume without having to climb
siliconchip.com.au
Does winding wire diameter affect inductance?
Thank you very much for your response to my question regarding the diameter of
enamelled wire for winding T1 and L6 for the Super-9 FM Radio Receiver. I wasn’t
aware of the errata feature on your website (siliconchip.au/Articles/Errata).
As I am ignorant of the physics underlying RF transformers and inductors, I’d
like to ask a question on this subject regarding the selection of wire diameters for
T1 and L6 in the radio.
It appears that the diameter of the wire is not a critical factor in the
electromagnetic equation regarding RF; instead, the number of turns is the relevant
factor, notwithstanding the physical limitations that need to be considered. After
an extensive internet search, I could not find enamelled wire of 0.125mm diameter
in small enough quantity to make it realistically affordable.
Still, I found 0.12mm and 0.13mm diameter wires readily available. Given what
I understand now, I assume that either of those two diameters would work OK.
As an alternative, I have an assortment of enamelled wire I have salvaged from
transformers, so would the principle of ‘close enough is good enough’ apply to the
subject inductors? Thank you in advance for any advice you can give me regarding
my questions above. (C. B., Bonville, NSW)
● Yes, 0.12mm or 0.13mm are within manufacturing tolerance of 0.125mm
diameter, so either would be expected to give identical results.
The diameter has a small effect on inductor properties as it determines how thick
the windings become and therefore, the exact diameter of the turns (especially
towards the outside if there are multiple layers). Still, you are correct that the number
of turns is the primary concern, along with the resistance and current-carrying
capacity of the wire (neither being terribly important in this case).
In this case, the properties of the inductor are not critical, so you can get away
with using a range of different wire diameters. The erratum we published doesn’t say
that you need to change the number of turns depending on whether you are using
0.125mm and 0.25mm diameter wire, so you can almost certainly use anything
between those values with satisfactory results.
around the back of the unit? Many
TVs are mounted on a plinth and, in
our case, I would have to put the TV
on top of the soundbar.
I am considering making an extension so that the soundbar has larger
dimensions to allow the top-mounted
bass unit to be clear of the TV plinth.
Where does the amplifier control
panel mount? On the outside or inside
of the enclosure? It is not clear from
the article. Are the ports covered with
speaker cloth? Finally, the parts list
calls for a sheet of 4mm plywood.
Could I use MDF instead? (J. C., Pelican Waters, Qld)
● Allan Linton-Smith replies: I usually plug the sound bar into the 3.5mm
headphone socket on the TV and then
use the TV remote for volume control
after setting up the balance between
treble, L & R and woofers. You can also
pair it with your TV with Bluetooth if
it recognises it (mine doesn’t).
Yes, you could make it larger externally but be careful; if your TV is
heavy, it could warp the top. If the
woofer is blocked, it might be best to
use the external subwoofer.
The control panel is mounted internally and I used 3mm machine screws
siliconchip.com.au
and nuts to secure it. The picture
on p58 shows the little screws but
they are not obvious, as you noted.
Yes, I covered the whole thing with
speaker cloth so it would not stick
out visually.
I initially used 3mm MDF but had
problems because the panels got
mouldy during our wet period and I
had to throw them away. They also
proved very weak and vibrated occasionally. The 4mm plywood feels and
sounds a lot better.
Incorrect isoundBar
timber length
When reading the isoundBar project (siliconchip.au/Article/15426), I
thought it was just what I needed, so I
have ordered the speakers and amplifier as specified. On reading the parts
list and looking at the dimensions of
the cut-outs, though, there appear to
be some inconsistencies.
The diagram on page 51 shows the
front and rear panels to be 1240mm
wide, yet the parts list includes three
lengths of 1200mm pine.
The plan view of the construction
on page 53 shows that the front and
Australia's electronics magazine
rear panels need to be 1240mm long.
An alternative would be to have the
end panels be 200mm long and mount
them outside the front and rear panels.
That would then tie in with the front
and rear panels being 1200mm wide,
adding the two 20mm thicknesses of
the end panels of 20mm for a total
width of 1240mm.
Could you advise the correct dimensions, or have they been corrected in
the next issue? (C. G., Beckenham, WA)
● Allan Linton-Smith replies: you
will have seen the erratum stating
that those lengths of timber should
be 1.24m, not 1.2m, as you have surmised. It is a good idea to adjust the
side panels for those who may have
already purchased the 1.2m lengths.
The original idea was to have a
soundbar the same width as several
common sizes of TV, but I settled on
making it as wide as a 55-inch TV,
typically 1232mm. You can make the
soundbar bigger to look better with
wider TVs, but not smaller because the
performance will be compromised. For
a 65-inch TV, make it 1454mm wide
(or a bit more), and for 75 inches, use
a width of at least 1677mm.
Limited VGA PicoMite
colour resolution
I am building the VGA PicoMite
project (July 2022; siliconchip.au/
Article/15382) and I like that it is a
low-cost computer with many useful features. However, I noticed that
when switched to colour mode, the
VGA resolution drops from 640 × 480
to 320 × 240.
I guess the 640 x 480 monochrome
frame buffer takes up 640 × 480 ÷ 8 =
37.5kiB and the 320 × 240 4-bit frame
buffer also takes up 320 × 240 ÷ 2 =
37.5kiB. Still, with 262kiB of RAM, the
Pi Pico should have enough RAM for a
640 × 480 colour framebuffer (150kiB)
with more than 100kiB left.
Is there a reason that a 640 × 480
colour mode is not possible? (P. B.,
Turramurra, NSW)
● Geoff Graham responds: I asked this
of Peter Mather, who ported MMBasic
to the RP2040 chip.
A lot of RAM was needed to improve
performance, so there was a trade-off
with the RAM needed to buffer the
video. Another hurdle is the banked
RAM architecture.
The RP2040 processor does not
have flash memory on the chip, so the
November 2022 109
firmware and the BASIC program must
be accessed over a quad SPI bus (very
slow). To alleviate this, the core components of MMBasic are loaded into
RAM and executed from there. Other
tricks were used to get the performance
up such as a RAM based hash table for
indexing BASIC variables.
The result is that the performance
(per MHz clock) is about the same as
the other implementations of MMBasic, despite the slow access to the flash
memory.
However, a significant portion of the
Pico’s RAM is therefore unavailable
for other uses. This is the RAM budget used in the final version:
44kB of memory-buffered firmware
38kB of video memory
32kB of variable hash table
4kB of stack for the 1st core
4kB of stack for the 2nd core
2kB for the main heap
32kB for general variables including
function hash buffer
100kB for the MMBasic heap
8kB for miscellaneous uses
SMD Test Tweezers
display cut off
I have recently built the Improved
SMD Test Tweezers (April 2022 issue;
siliconchip.au/Article/15276) and find
them extremely useful and practical,
especially with the increasing usage
of small SMD components in projects
today. My only problem is that the
right-most character on the screen is
cut off. Is it possible to reduce the font
size and move the displayed text to the
left? (J. A., Townsville, Qld)
● We’ve had reports of this occurring
for some other users but did not see
it with any of our prototypes. We suspect there may be some OLED modules
that map their columns differently,
meaning that there is not a universal
fix. OLED modules with and without
this problem may not be easily distinguishable, either.
We’re working on another update
of the Tweezers using a larger display
(which will not have this problem as
it maps all rows and columns), and it
will also have a better power-saving
mode as it will completely shut down
the OLED at its supply.
With a more capable microcontroller, we plan to give the next version
a better set of test routines as well as
extra buttons to simplify control and
calibration.
110
Silicon Chip
Readers wishing to experiment
could try changing the value of
OLED_X_OFFSET in the oled.h file
and then recompiling the code.
Control pot values for
Hybrid Power Supply
Thank you for your fine efforts
in producing the Intelligent Hybrid
Power Supply (February & March
2022; siliconchip.au/Series/377). The
regulator PCB is a work of art in itself.
I intend to create one manual board
only for the simplicity of my needs.
I have a couple of points that need
clarification.
Please nominate the value of the
two panel-mounted pots connected
to CON5 and CON6, as there is no
reference to their values in the text. I
intend to connect a multi-turn pot to
V-Set, but they are not cheap.
Secondly, there appears to be a ghost
component in Fig.10 on page 85 of
the March 2022 issue. Below REG4 is
a polarised 10µF capacitor as per the
circuit diagram. To its immediate right
appears another spurious 10µF capacitor with its designation written vertically. There is no provision for this
capacitor on the PCB I bought.
Lastly, in the circuit diagram (Fig.7),
I am wondering about the function
of transistors Q8, Q10 and Q11. I
could find no reference to them in
the text. They appear to provide some
Darlington-
based constant current
load to the pre-regulator IC, but there
must be more to it than that.
Thanks once again for your fine
efforts, and those of your colleagues
from this 75-year-young hobbyist. (C.
D., Glenside, SA)
● Phil Prosser responds: the potentiometers I used when running in ‘manual’ mode were 1kΩ types. This results
in a 5mA current through them and
25mW dissipation. Other values could
be used, but 1kΩ seems safe.
Multi-turn pots are very expensive.
I suggest that you start with a single-
turn pot, as the old-school power supply I have been using for years has a
single-turn pot, and I have never had
trouble with it.
The ‘ghost cap’ is left over from an
earlier version of this board. When
the diagram was revised, with a
new copper track layout and some
changed component locations, it
appears that redundant capacitor was
not removed.
Australia's electronics magazine
There is no more to the circuit block
involving Q8, Q10 & Q11 than a simple load for the switchmode regulator.
If the circuit was built without them,
I suspect it would work, but having
them there ensures that the minimal
load specification is always met.
Battery Condition
Checker running at 48V
Some years ago, I built your LeadAcid/SLA Battery Condition Checker
(August 2009 issue; siliconchip.au/
Article/1535). It’s an awesome tool; I
still use it today. I am wondering how
difficult it would be to change the 24V
setting to 48V. (Ian, via email)
● For 48V operation, change the 220Ω
resistor at the bottom of the divider
chain connected to switch S3a to two
110Ω resistors in series. The middle
tap of the 110Ω resistors can then be
connected to the common terminal of
S3a for use with a 48V battery.
Another change you’ll need to
make is to add a 24V zener diode in
series with D11 at the input to the
LM2940 regulator (REG1) with its
anode to D11’s anode, to reduce the
input voltage to a safer level for the
regulator. That added zener diode
will need to be shorted out for 6-24V
operation.
You could add a DPDT switch so that
it shorts out that zener diode in one
position, while connecting the common terminal of S3a to pin 2 of IC4.
In the other position, it would remove
the short across the zener diode, disconnect S3a’s common terminal and
instead, connect pin 2 of IC4 to the
junction of the 110Ω resistors. That
switch will then select between 6-24V
operation and 48V mode.
Depending on the Mosfets used for
Q4-Q7, consider using higher voltage
rated types at, say, 100V. You might
get away with the 55V types specified, provided the 48V battery terminal
voltage will never exceed 54V during
testing (a freshly charged 48V battery
might be above 54V for a short period
after charging).
Capacitor Discharge
Ignition questions
I have obtained copies of High
Energy Multi-Spark CDI series (December 2014 & January 2015; siliconchip.
au/Series/279).
continued on page 112
siliconchip.com.au
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Silicon Chip magazine regularly describes projects which employ a mains power supply or produce high voltage. All such projects
should be considered dangerous or even lethal if not used safely. Readers are warned that high voltage wiring should be carried
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siliconchip.com.au
Australia's electronics magazine
November 2022 111
The design seems very good but
would require considerable effort (and
probably extra cost) for little benefit
for my circumstances. All that I need
is a simple, reliable spark.
I know that I will have to buy a 12V
coil and battery; I just need the electronics to control the spark. I can use
the existing trigger but will need circuitry to couple it to the control module. My questions are:
1. Is a PCB available for the December 2005 Universal High Energy Electronic System, code 05112051?
2. Is there a kit available for that
project, or would I have to buy components separately?
3. Is a PCB available for the reluctor circuit?
4. Are there any components that
are not available now. If so, what are
the alternatives?
5. Are the above all available from
your Shop?
(T. H., Wallington, Vic)
● We do not recommend building the
2005/6 version of the High Energy
Ignition system as there are no longer
any kits or PCBs available. However, a
Advertising Index
Altronics.................................33-40
Control Devices............................. 9
Dave Thompson........................ 111
Digi-Key Electronics...................... 3
Emona Instruments.................. IBC
Hare & Forbes........................... 107
Jaycar.......................IFC, 11, 53-55,
..................................60-61, 99, 103
Keith Rippon Kit Assembly....... 111
revised version of that project was published in the November & December
2012 issues (siliconchip.au/Series/18),
and the PCB is still available; see
siliconchip.au/Shop/?article=464
Kits for that project may also still be
available. Check with Jaycar regarding
their kit KC5513; their website currently says “Limited quantities available in store”, and if available, it is on
sale at $19.80.
As well as the PCB, we sell the hardto-get parts such as IGBT and programmed PIC, available via the link
above. The other parts are commonly
available. The reluctor circuitry is
catered for on the PCB supplied.
Replacement SOT-223
LDO regulators
I am in the process of making the
PIC/AVR Programming Adaptor Board
(May & June 2012; siliconchip.au/
Series/24), but I can’t seem to find any
AP1117E33 3.3V low-dropout linear
regulators. Can I use an MCP17993302H/DB or LDI1117-3.3H instead?
(L. P., Sydenham, NSW)
● There are many different kinds of
compatible LDO regulators in SOT-223
packages with 1117 in their part code.
The 3.3V version of the LDI1117 you
mentioned should work. Another common compatible type is the AMS1117.
The MCP1799 will not work without modifying the PCB because it has a
different pinout (Vin, GND, Vout rather
than GND, Vout, Vin).
About power supply in
Circuit Notebook
I want to build the “Fully adjustable
power supply” circuit published in the
Circuit Notebook column, March 2004
(siliconchip.au/Article/3427).
I assume the 33Ω resistor needs to
be rated at 5W. I do not have an 18V
supply at 5A. Can I use a transformer
secondary rated at 15V 6A, giving
approximately 21V when rectified? I
could use a 1W 18V zener and dropping resistor to power the TL071. Is
there any erratum for this circuit? (R.
M., Melville, WA)
● The 33Ω resistor can be a 1/2W or
even 1/4W type as its dissipation will
be less than 30mW. There will only
be a maximum of about 0.7V across it
(the base-emitter forward voltage of
transistor Q1).
Yes, you can use your proposed
20V DC supply to power that circuit.
The TL071 can run from a supply of
up to 30V, so no extra zener clamp is
required.
Replacing components
on a failed Turbo Timer
I have a burnt-out resistor on my
Turbo Timer circuit board (November
1998; siliconchip.au/Article/4649).
It is labelled “33R [680R]”. Can you
please confirm the value of the resistor I have to replace it with? (S. M.,
via email)
● The resistor should be 33Ω 1/2W.
However, zener diode ZD1 and the 555
timer IC are possibly destroyed as well.
The burned-out resistor would have
been caused by a voltage transient that
shorted the zener diode and possibly
harmed the 555 timer.
Check if there is a short circuit
across ZD1. We suspect that it will
measure near 0Ω with a multimeter. All three components should be
replaced.
SC
Lazer Security........................... 111
LD Electronics........................... 111
Microchip Technology......... 5, OBC
Mouser Electronics..................... 13
Ocean Controls............................. 8
Rohde & Schwarz.......................... 7
Silicon Chip Shop.................88-89
Silvertone.................................... 12
The Loudspeaker Kit.com.......... 10
Tronixlabs.................................. 111
Wagner Electronics....................... 6
112
Silicon Chip
Errata and Next Issue
LEDsales................................... 111
isoundBar with Built-in Woofer, August 2022: the part code given
for the Peerless tweeters should have been BC25SC55-04 instead of
BC25SC55-06. Also, the sheet of 19-20mm thick plywood in the parts list
is arguably not required as all the pieces can be cut from the DAR pine
lengths.
Motion-sensing 12V Power Switch, February 2019: it has been reported
that the vibration switches can become unreliable (stuck ‘on’) due to
contact welding when it closes. To solve this, solder a 100Ω resistor in
series with one of the sensor leads (we suggest the thinner one). This
value seems to work well but note that it is a compromise as it must be
low enough to discharge the capacitor quickly but high enough to avoid
contact welding.
Next Issue: the December 2022 issue is due on sale in newsagents by
Monday, November 28th. Expect postal delivery of subscription copies in
Australia between November 28th and December 12th.
Australia's electronics magazine
siliconchip.com.au
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