This is only a preview of the January 2015 issue of Silicon Chip. You can view 36 of the 104 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 "The Micromite Mk.2":
Items relevant to "Isolating High Voltage Probe for Oscilloscopes":
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January 2015 1
Contents
Vol.28, No.1; January 2015
SILICON
CHIP
www.siliconchip.com.au
Features
12 Interfacing To The Brain
Interfacing to the human brain might seem the stuff of science fiction but a great
deal of work is being done in this area, as well as work on animals and insects.
You can even do it yourself – by Dr David Maddison
20 The Micromite Mk.2
Interfacing To The Human Brain: It’s
Happening – Page 12.
Introduced in our May 2014 issue, the Micromite is a small 28-pin chip running
a powerful BASIC interpreter. Now we have the Micromite Mk.2 with more
memory, more functions, higher speed and a host of other improvements – by
Geoff Graham
84 Review: Tektronix RSA306 Real Time Spectrum Analyser
This spectrum analyser hooks up to a late-model PC, laptop or tablet via a
“SuperSpeed” USB 3.0 cable and offers virtually all the features of a real-time
spectrum analyser at a fraction of the cost – by Jim Rowe
Pro jects To Build
26 Isolating High-Voltage Probe For Oscilloscopes
Measure AC mains and other high-voltages safely on your oscilloscope with this
low-cost unit. It has three switchable input voltage ranges, wide bandwidth and
high voltage isolation between input and output – by Jim Rowe & Nicholas Vinen
Isolating HighVoltage Probe For
Oscilloscopes –
Page 26.
38 High-Energy Multi-Spark CDI For Performance Cars, Pt.2
Second article gives the full assembly details for six different versions to suit
your car’s ignition trigger source and describes the installation – by John Clarke
64 Currawong 2 x 10W Stereo Valve Amplifier, Pt.3
Final article describes the optional remote volume control, the laser-cut acrylic
cover and the testing procedure – by Nicholas Vinen
76 Beginner’s Project: The PicoMiniCube
It’s powered by three 1.5V batteries and uses a PIC microcontroller to drive
27 LEDs to give an eye-catching 3D display. It’s perfect for school projects and
costs less than $28 – by Phillip Tallents & Ross Tester
Building & Installing The HighEnergy Multi-Spark CDI – Page 38.
Special Columns
44 Circuit Notebook
(1) Using A Micromite To Control A PCF8563 Real-Time Clock; (2) Engine
Immobiliser Uses An RFID Tag; (3) 4-Digit Thermometer; (4) USB OTG
Charging Cable
58 Serviceman’s Log
DIY printer repairs can easily go wrong – by Dave Thompson
90 Salvage It
Want to salvage and reuse common-mode chokes (CMCs) from faulty
switchmode power supplies? Here’s how – by Ken Kranz
94 Vintage Radio
The Stromberg-Carlson 5A26 radio – by Associate Professor Graham Parslow
Departments
2 Publisher’s Letter
4 Mailbag
siliconchip.com.auShowcase
57 Product
83 Subscriptions
89 Online Shop
99 Ask Silicon Chip
103 Market Centre
104 Advertising Index
The PicoMiniCube: A Fun
Beginner’s Project – Page 76.
January 2015 1
SILICON
CHIP
www.siliconchip.com.au
Publisher & Editor-in-Chief
Leo Simpson, B.Bus., FAICD
Production Manager
Greg Swain, B.Sc. (Hons.)
Technical Editor
John Clarke, B.E.(Elec.)
Technical Staff
Ross Tester
Jim Rowe, B.A., B.Sc
Nicholas Vinen
Photography
Ross Tester
Reader Services
Ann Morris
Advertising Enquiries
Glyn Smith
Phone (02) 9939 3295
Mobile 0431 792 293
glyn<at>siliconchip.com.au
Regular Contributors
Brendan Akhurst
Rodney Champness, VK3UG
Kevin Poulter
Stan Swan
Dave Thompson
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a year by Silicon Chip Publications
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2 Silicon Chip
Publisher’s Letter
Petrol power tools are anathema
Now that we are in the middle of the Australian
summer, part of the weekend ritual seems to be that
everyone in suburbia needs to drag out their mowers
and related paraphernalia to inflict a lot of unnecessary noise on the neighbours. Most of these mowers,
whipper-snipper lawn edgers and leaf blowers are
2-stroke and are inevitably noisier and more polluting
than the usually more expensive 4-stroke equivalent,
if one is available.
But this noisy and polluting ritual is no longer necessary – you can use electric mowers and power tools instead. For some years
now, I have used a mains-powered electric mower. I love it. It is much lighter
than my not-so-old 2-stroke monster and indeed I can carry it up stairs and over
fences with one hand! Nor is there any fiddling about with 2-stroke mixture,
priming the carby and then pulling the retractable start. My petrol mower would
typically start on the first try (due to regular maintenance!) but there are many
men and women for whom starting such a mower is a virtually insurmountable
physical hurdle, if it cannot be started quickly – they are simply not fit enough!
Not only is the electric mower no problem to start, it is much quieter. In
fact, I don’t need to resort to protective ear muffs. That brings about another
advantage because not having to wear ear muffs means that you don’t get so
hot while you are doing the mowing. Nor do I have to put up with the smoky,
smelly exhaust of a 2-stroke motor. In fact, mowing the lawn is a breeze and I
have no qualms about doing it in the late afternoon after work (during daylight
saving) because I know that the mower’s noise will not disturb the neighbours.
(I know that because two of my neighbours now have electric mowers too!)
There is one disadvantage in using a mains-powered electric mower and that
is the power cord. You have to be vigilant at all times to make sure that the
mower does not run over and cut the power cord. That has never happened to
me fortunately but at the end of each run along the lawns, I have to swing the
cord right out of the way, to make sure that it is well clear for the next run back
in the opposite direction.
But if I was buying an electric mower today, I would not necessarily purchase
a mains-powered version; I would carefully consider a lithium battery-powered
model. These are still more expensive than mains-powered models but they are
much lighter than the nickel-cadmium battery-powered models of only a couple
of years ago. On the other hand, if you only have a small lawn, there are now
small battery powered mowers which are very cheap. Mind you, actual mowing
time capability does seem to be less than typically claimed and the way around
this can be to buy a second battery pack (expensive!) or buy another power tool
of the same brand with the same battery pack.
I also have a mains-powered electric leaf blower but sadly, I have to report
that it is probably just as noisy as a petrol-powered job, albeit with the inconvenience of a power cord. I still prefer it though, because it does not have a smelly
exhaust. Fortunately, I only use it about once a month so it is not a regular part
of the weekend ritual.
So if you are a “weekend warrior”, you should seriously consider pensioning
off your petrol-powered mower and garden power tools. Not only is there less
chance of losing your temper while trying to start the intractable beast(s), you will
find the whole job much more enjoyable. You stay cool and your neighbours will
like you better too. They may even follow your lead and change over to electric
power as well. Isn’t that a pleasant prospect? Have a quiet, peaceful weekend.
Leo Simpson
siliconchip.com.au
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January 2015 3
MAILBAG
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 may edit and
has the right to reproduce in electronic form and communicate these letters. This also applies to
submissions to “Ask SILICON CHIP” and “Circuit Notebook”.
Alcohol ignition
interlock devices
I wish to comment on the use of ignition interlock devices, as discussed on
pages 10 & 11 of the November 2014
issue. Some time in the mid 1980s I got
involved in the preliminary investigation of an alcohol ignition interlock
device. I had about 20 subjects, each of
whom willingly consumed measured
amounts of alcohol, after which I tried
to measure their BAC (Breath Alcohol
Content).
Indeed there was a difference between sexes but the differences between males were even greater! The
correlations between my readings and
actual blood alcohol content readings
were surprisingly low.
The next problem I encountered
was that of sensor contamination. The
breath content of the previous test
person would linger on and would add
to that the next test person. Many a
flushing technique, some quite inventive, were tried but we settled on a test
person who had not consumed alcohol
to test-blow the device. I admit this is
not a terribly scientific approach.
The sensor worked within 10%
when artificial breath (compressed air)
mixed with alcohol fumes was used.
The sensor was correct in detecting
alcohol levels.
Then, one day, the non-alcoholic
test person blew 0.2%. He had just
consumed a sandwich, purchased in
the local milk bar! Of course the test
was repeated many times but in the
end I had to admit defeat and cancel
the project. The sandwich, by the way,
was the standard composition of salad,
onions, beetroot etc. Draw your own
conclusions.
Ben Heij,
Little Mountain, Qld.
New software for
Signal Hound spectrum analyser
As the owner of a Signal Hound
SA44b and TG44 tracking generator
since 2011, I was interested to read
your review in the October 2014 issue of SILICON CHIP. There’s no doubt
that the hardware is a minor miracle,
especially at the price and I have
found it extremely useful in my homeconstruction activities.
There have been problems though,
especially when using the matching
TG44 tracking generator. Often the
output level from the TG would not
match that indicated and any attempt
to change settings or abort a sweep
could cause a crash. The “slow, high
resolution” mode is very useful for
‘digging down’ into narrow crystal
filters to reveal detailed responses etc
but this mode is unstable and can crash
with very little provocation.
To Signal Hound’s credit, they have
revised the software several times and
things have improved, but the basic
problems never seemed to go away.
However, you may be interested to
learn that new code has been written
from scratch and is now undergoing
final tweaks before a January 2015
release.
To get the new software just right,
Signal Hound have canvassed the users of the SA44b and carefully noted
their concerns over ergonomics and
stability and the new software looks
much slicker, quicker and userfriendly than before. There’s a preview
video on You Tube at http://youtu.be/
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4 Silicon Chip
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I hope this is of assistance to all
those who may be considering the
purchase of the SA44b.
Andy Howlett, G1HBE,
Cheshire, UK.
MEN system
comments
The series on Earthing to waterpipes was quite interesting. I am not a
“sparkie” (but I do confess to replacing
single GPOs with doubles) so I did not
know that earthing to a pipe is illegal.
As for Sydney Water taking on the
responsibility of correct Earthing, I
would say that it is because their employees and contractors are amongst
those most at risk. In the meantime,
I am still wondering where the Earth
stake is where I live. It’s a new complex
with a single meter board (padlocked,
so I cannot check my usage) and no
earth bond near it.
Finally, with respect to the Courtesy
Light Delay published in the October
2104 issue, I can’t but notice how
they’ve advanced over the years. The
first one I built was from an Electron-
Old wireless microphones
may not be illegal in some areas
I have been following with some
interest the information and articles
in SILICON CHIP about wireless microphones. The local church in our
town has a fairly old system though
still functional, with one mic and
a diversity receiver operating on
202.8MHz. In one of the articles
in the magazine, it was stated that
after 1st January 2015, wireless mics
working in the VHF spectrum would
not be legal.
I searched the ACMA website and
could find no reference confirming
this, so I sent an email to the ACMA
asking if we could still use our system after the cut-off date in light
ics Australia circuit and consisted of
a 2N3055 and an RC timer, wrapped
in insulation tape and stuffed down
the “B” pillar via the switch hole, on
my old Ford Cortina (this was in the
1970s). Now we’re looking at microprocessors for a similar function.
Dave Horsfall,
North Gosford, NSW.
of the fact that the frequency was
not occupied by a digital television
station in Adelaide. There are no
stations on channels 9 and 9A in
Adelaide.
The reply came back very promptly (the morning of the next business
day) from a Spectrum Engineering
Manager, saying that as the channels
were vacant and there are no plans
for TV stations on these channels in
Adelaide, we could continue to use
our system. There are DAB+ radio
stations in Adelaide on 203.872207.120MHz so our wireless mic
won’t affect, and hasn’t been affected
by, digital radio either.
Keith Gooley,
One Tree Hill, SA.
Potential shorted turn in
Currawong power transformers
I refer to the second article on the
Currawong Stereo 10W Valve Amplifier in the December 2014 addition of
SILICON CHIP. I would like to point out
a potential trap and save someone from
cooking the two power transformers.
As shown on pages 91 & 93, Earth
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January 2015 5
Mailbag: continued
Helping to put you in Control
LogBox RHT 32K Readings
IP65 dual channel data logger with built-in temperature &
humidity sensor. It can be easily
programmed and configured via a
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connects to a USB port under
Windows® software or PDA IrDA interface.
Replacabe internal lithium (3.6V ½ AA)
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Price:$159 +GST
Any-Direction Microswitch
Industrial microswitch with springy
actuator triggers when the actuator
is pushed or deflected in any direction. This makes it trivial to mount
in a wide variety of situations.
SKU: HES-204
Price:$12.95 +GST
10-Port USB Charging Hub
10 dedicated USB ports with a
massive 60 W built in power in
a compact design. 2 selectable
types of charging current, 1 A or
2 A, 240 VAC powered.
SKU: UHB-003
Price:$89.95 +GST
USB Serial Stepper Controller
Four axis stepper motor
controller fitted with USB and
RS-485 ports. Takes simple
serial commands and produces ramped frequency profiles
for stepper or servo motor
control. Revised version can
be 8 to 35 VDC powered and has analog
inputs.
SKU: KTA-290
Price:$79 +GST
Power Multiplexer Carrier
The Texas Instruments
TPS2113A autoswitching
power multiplexer allows you
to switch seamlessly between
two power sources of 2.8 V to
5.5 V, while blocking reverse
current into either source & and the board
also breaks out a USB Micro-B connector
that can be used to supply one of the rails.
It has an adjustable current up to 2 A.
SKU: POL-2596
Price:$9.95 +GST
Bluetooth 4.0 BLE Shield
Bluetooth Low Energy (BLE)
shield for Arduino based on the
Nordic Semiconductor nRF8001.
This shield lets your Arduino
talk to your smartphone or
other Bluetooth 4.0 equipped
devices. 3.3 V or 5 V powered.
SKU: SDA-001
Price:$34.95 +GST
New MeanWell Slim Line Series
MeanWell has recently announced the released of their
highly anticipated new slim
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For OEM/Wholesale prices
Contact Ocean Controls
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6 Silicon Chip
True science is
always questioned
I just read with interest both my
letter and Robert Suhr’s in the Mailbag pages of the November 2014 issue. He may have been angry enough
to have stopped his subscription
but you have recently gained me
as a subscriber for sticking to true
questioning of science.
While I once believed in the dangers of Global Warming , I have given
this the due diligence to investigate
the so-called “science” and what it
was based on. Climate science has
become a farce, with government
grants being withheld and jobs
being on the line if government
political agenda using science was
not backed. Valid scientists are of
different opinions to the warmists. A
study of the IPCC themselves makes
interesting reading. See this link at
http://tinyurl.com/SillyCon-Scam2
How on earth can it be called science when the numbers they collate
can back any conclusion they wish
to pull out of their collective hats?
There are far-fetched conclusions of
acidification of rising oceans, claims
of extinctions when actual science
is not yet truly understood and they
readily jump to unproven conclusions. And the Australian Bureau
of Meteorology has “homogenised”
wires are connected to the bolts holding the transformers. In this case, all is
OK as they are mounted in the timber
plinth. But if someone was to mount
them on a metal chassis, this would
be when disaster strikes.
I did this on an amplifier I built years
back, thinking it was a good idea to
connect the Earth wires like this. When
I switched on with no load connected,
there was a loud hum followed by a
wisp of smoke just as I switched off. I
could not work out why as the transformers secondary windings were not
yet connected; I was just checking out
the transformer to see if all the voltages
were OK.
After looking at it for a while the
penny dropped; the Earth wires make
a complete turn of thick wire with no
temperatures previous to 1906 (currently being investigated by parliament – see http://jennifermarohasy.
com/temperatures/).
Marohasy’s research has put her in
dispute with the BoM over a paper
she published with John Abbot at
Central Queensland University in
the journal Atmospheric Research,
concerning the best data to use for
rainfall forecasting (she is a biologist and a sceptic of the thesis that
human activity is bringing about
global warming). BoM challenged
the findings of the Marohasy-Abbot
paper but the international journal
rejected the BoM rebuttal, which
had been prepared by some of the
bureau’s top scientists.
Sea levels are not rising as they are
mostly within the bounds of errors of
measurements. Elusive numbers are
used and actually found to be inside
normal margins by an Australian
scientist, Doug Lord, who was made
redundant after disagreeing with the
government’s claim of a 100-metre
sea level rise and he was a climate
change believer. Other CSIRO scientists have quit due to disagreements
based on the institute’s policy.
I fully support the Editor of SILICON CHIP.
John Vance,
Wangaratta, Vic.
resistance to the magnetic field of the
transformer and thereby overload it.
David Francis,
Kilburn, SA.
Comment: you are absolutely correct.
Earthing the transformer bolts in an
already earthed metal chassis constitutes a classic shorted turn which
could easily burn out the primary
winding when power is applied.
In the case of the Currawong though,
the immediate effect would be to blow
the 1A slow-blow fuse in the IEC mains
socket so no damage would be done
but there would inevitably be some
head-scratching by novice constructors.
Nor is it really necessary to have
the bolts earthed in the timber plinth,
especially as the transformers should
siliconchip.com.au
siliconchip.com.au
January 2015 7
Mailbag: continued
SIGNAL HOUND
USB-based spectrum analyzers
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SA44B: $1,320 inc GST
•
•
•
•
•
Up to 4.4GHz
Preamp for improved
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Thermometer for
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AM/FM/SSB/CW demod
USB 2.0 interface
SA12B: $2,948 inc GST
•
•
•
Up to 12.4GHz plus all
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AM/FM/SSB/CW demod
USB 2.0 interface
The BB60C supercedes the
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The BB60C streams 140
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Sweep speeds of 24 GHz/sec.
The BB60C also adds new
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Streaming bandwidths
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Vendor and Third-Party
Software Available.
Ideal tool for lab and test bench
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ham radio enthusiasts and
hobbyists. Tracking generators
also available.
Silvertone Electronics
1/8 Fitzhardinge St
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Ph: (02) 6931 8252
contact<at>silvertone.com.au
8 Silicon Chip
Alternative 433MHz module
is ideal for sniffing
With respect to the query about
433MHz sniffing on page 99 of the
September 2014 issue, Jaycar’s new
ZW-3102 433MHz data receiver
(based around Princeton Tech’s
PT4302 RF IC), is pin-for-pin compatible with their traditional ASK
module. Aside from their intended
data duties, band “sniffing” persuasion gives piezo-based audio
that also seems superior in both in
volume and clarity to their classic
Keymark offering.
The module especially scores over
Dorji’s cheaper 433MHz receiver
for its ability to work down to 2.4V.
Such a flexible supply nicely suits
powering by a single Li coin cell,
single LiFePO4 cell, two alkaline
AA cells etc.
It’s shown itself to be significantly
more sensitive than the old module.
Semi line-of-sight signals (through
light vegetation and wooden buildings) from a 25mW tone-sending
Dorji transmitter were still audible
when some 100m away.
Data sheet sleuthing reveals a signal strength point at PT4302 pin 14,
which conveniently runs to a good
be mounted with a large rubber washer
(which is supplied) underneath the
large steel washer. And in the case of
an earthed steel chassis, there would
be no need at all to separately earth the
transformer mounting bolts because
they would be earthed by the steel
chassis itself.
PWM motor whine can be
fixed with an LC filter
In the “Ask SILICON CHIP” section of
December 2014, on page 114, reader
J. E. has a problem with whine from
a PWM-driven fan. I have designed a
number of PWM motor controllers and
initially experienced the same problem years ago but it is easily solved
with an LC low-pass filter.
A bobbin style inductor of 100µH to
220µH is inserted between the driving
Mosfet or transistor and the motor,
followed by a capacitor across the
solder point at SMD capacitor C5. A
wire can be run from this to a duplicated module data pin that’s freshly
isolated (by PCB track cutting).
The voltage swing here suits useful RSSI work, as it varies between
0.9V with just band noise and ~1.4V
with a strong nearby signal. DMM
monitoring here could allow keen
insights into transmitter, propagation path and antenna performance.
A simple LED (perhaps wired via a
boosting Darlington transistor) however could be enough for proximity
and visual checking on such suspect
transmitters as 433MHz wireless
doorbells.
As these ZW3102 modules are
available off the shelf at any Jaycar
store they may be worthwhile for general 433MHz use, even though they’re
more costly than other offerings.
Stan Swan,
Wellington, NZ.
motor wires close to the inductor. The
capacitor is sized so that its reactance
is substantially less than the inductor
at the PWM frequency, eg 1/10th.
Most people will not be familiar
with the maths so the easy way is to try
various values until the motor is quiet.
My designs have used values ranging
from 100µH & 1µF to 220µH & 220µF,
with low-ESR capacitors.
George Ramsay,
Holland Park, Qld.
Choice of line output
transformer in Currawong
Your Currawong Stereo Valve Amplifier is interesting. Last year, I used
a line transformer to repair a 1960s
Electronics Australia Playmaster
Unit 4 Stereo Amplifier that had an
open-circuit in one of the output
transformers.
After reading the articles by Paul
siliconchip.com.au
Cambie, Grant Wills and Roly Roper in OzValveAmps on
using line output transformers, I decided to have a go at
fixing the old Playmaster unit as I had a spare Altronics
M1130 40W transformer. Even though the originals were
only rated at about 10W, they were much heavier (940g
compared with 540g for the M1130). The M1130 fitted easily and even the hole spacings matched. I used an 8-ohm
load on the 2-ohm output to run it as 8kΩ (plate loading).
The original circuit specified 9kΩ but I decided that this
was near enough.
The stereo unit probably gives the best possible comparison as you can hear both channels at the same time,
rather than try to remember what it sounded like. My wife
and I independently concluded that the M1130 channel
had more treble and slightly less bass than the channel
with the original Ferguson OP412 output transformer. The
M1130 actually ran cooler than the original.
As a replacement for an unobtainable part, the line
transformer is an excellent way to keep a 50-year old
amplifier running but I think that you have tried to be a
little too cheap in the Currawong. I built a pair of 807 valve
amplifiers based on the “Triode Connected 807 Amplifier”
described in Radio & Hobbies 1948 (the sound quality is
stunning) and a large guitar amplifier with EL34s and there
is no substitute for copper wire in the output transformers.
As the OzValveAmps article suggests, the small M1115
transformers will probably run quite warm and the 40W
M1130 would match a pair of 6L6s.
Leo Simpson has resisted publishing valve amplifiers
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Mailbag: continued
TempMaster Mk.3
works very well
Well done on the excellent TempMaster Mk3 (SILICON CHIP, August
2014) kit! I’d recently purchased a
deep freezer from a well-known German retailer at what I thought was a
bargain price. The freezer had a 3.5
star rating and from all my research
that was about the best to expect
from freezers.
Unfortunately, every time I walked
past the unit, it always seemed to be
continuously running, irrespective
for decades because they just cannot
match modern amplifier designs on
sound quality, price, safety and ease
of construction. Unfortunately, I don’t
think that your choice of output transformer in the Currawong amplifier will
help convince him or many of your
readers. Your design does limit most
of the safety risks and a circuit board
is a thousand times easier than pointto-point wiring.
Wabeco Australia
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of what setting the thermostat was
at. I ended up measuring the temperature and found it to be at -36°C
(or even lower at times), which was
way too far from the optimum -18°C.
I ended up building the TempMaster Mk3 and fitted it to the freezer. In
no time flat, it was a breeze to set the
temperature to the optimum -18°C.
I’m looking forward to the lower
running costs thanks to this great
project. Keep them coming!
Peter Kutas,
Shortland, NSW.
I know this from experience as the
two 807 amplifiers look like mirror
images but the valve pins and therefore the circuits are not. It actually
took longer to build the second one
as I had to completely “unthink” the
first circuit.
The blue LEDs in the Currawong
might not be needed. When I first built
my amplifier, the 807s emitted a beautiful eerie blue glow, probably with lots
German made
Highest precision
5 year warranty
of UV (the 6L6 or KT66s might also).
This glow has faded over 10 years.
Unfortunately, the eight valves
alone will push the price to $300
and the other components and board
will add hundreds more. There is no
advantage saving $25 by using the
cheapest transformers (the M1130 are
each about $12 more) or even $100
(compared with genuine output transformers such as Hammond or those
made in Australia).
It would be sad if you disappointed
a generation of hobbyists who have
heard just how good a valve amplifier
can sound. I don’t mean good valve
amplifier sound, I mean good amplifier sound. Why not run a series of
comparisons to see if my suggestions
do actually improve the final sound?
You suggest that different transformers
could be used to raise the output; why
not give your builders some definite
evidence.
As well as hifi enthusiasts, I am sure
that there are hundreds of guitarists
drooling over the prospect of a “toob”
guitar amplifier design. Custom tone
control and selective distortion are
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10 Silicon Chip
siliconchip.com.au
High-power LED modules
can be over-rated
more important than flat response and S/N ratio. A guitar
amplifier design would be very popular and less likely
to disappoint. Thanks very much. I hope the amplifier
design does go well.
Dave Dobeson,
Berowra Heights, NSW.
Comment: we think your choice would probably be OK
if you were not using an ultra-linear connection. The
Playmaster Unit 4 did use an ultra-linear circuit, so we
would regard the M1130 line transformer as not the best
transformer substitution and we would recommend the
one we used in the Currawong. We did obtain a sample of
the Altronics M1130 transformer and we concluded that
we could not achieve symmetrical screen connections.
The line transformers we used run warm but not hot
to the touch.
Ultimately, the very best valve amplifiers were designed
on similar lines to the Currawong. Examples are the Mullard 5-10, 5-20 and Twin-Ten. All of these used ultra-linear
push-pull operation and typically achieved total harmonic
distortion below 0.1%. That was regarded as a benchmark
and if we can achieve comparable or better results in the
Currawong, the audible sound quality should be in line
with those results.
We don’t deny that a better (far more expensive) output
transformer may improve the performance but we also
think that any audible improvement would be relatively
small.
It is true that the blue LEDs are not necessary. We only
included them for cosmetic effect. However, the blue or
indigo glow from some power valves is not all that common and typically does fade as the valve ages.
Finally, we do think that the Currawong sounds quite on
a par with other good valve amplifiers. But it is no match
for the exceptional sound quality of the SILICON CHIP 20W
SC
Class-A or Ultra-LD solid-state amplifiers.
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Those that are interested in building their own highpowered LED lighting will be aware that LED modules
of up to 100W are available. I recently purchased one
of these via eBay and confirmed its operation and left
positive feedback. It was only later after I had modified a heatsink to suit it to allow me to run the device
at full power that I became aware that it was, in fact,
a 50W unit.
Despite plenty of power being available, it would
only draw around 1.5A at its maximum rated voltage
of 35V when it was rated at around 3A at that voltage.
Unfortunately, many or even most of these devices
seem not to have any identifying marks on them so that
you can easily to determine their power rating or other
specifications. Having had generally good experience
on eBay with well-selected sellers, I am inclined to
think it was an honest mistake because the seller was
similarly unable to identify the device.
Dr David Maddison,
Toorak, Vic.
January 2015 11
INTERF
TO THE
by DR DAVID MADDISON
S
While interfacing to the human brain might
seem the stuff of science fiction, there is much
work being done in this area, as well as work on
animals and insects. You can even do it yourself
and it can have many practical aspects.
cience fiction is full of scenarios in which a person’s
own brain is interfaced directly to a computer or a
machine (or another person) and is used to interact
with, or control it.
Examples include the people in The Matrix trilogy, the
Daleks in Dr Who and the Borg in Star Trek.
And who can forget that 1983 sci-fi film Brainstorm, the
whole theme of which was the development, use (and misuse) of a Brain-Computer Interface (BCI). BrainStorm can be
viewed on YouTube at http://youtu.be/cOGAEAJ4xJE
In this article we will primarily focus on methods of interfacing the human brain with computers and machines,
so called brain-computer interfaces or BCIs. Australia is
a world leader in the Cochlear implant but these devices
do not interface directly to the brain. Rather, they connect
to existing nerve fibres and are in the related category of
neuroprosthetics.
A brain-computer interface can be defined as a system
for reading information from the brain to enable control of
a machine or the transmission of an item of communication
or thought. It is also a system of feeding information into
the brain to enable the brain to interpret a sensation from
some external sensory device.
In other words, information is transmitted to and from
the brain to a machine without the engagement of the usual
senses, the peripheral nervous system or limbs.
Reading the brain
To interface the brain to a computer, information has
to be first read from the brain. There are several means by
which information can be acquired from a brain for the
purpose of brain-computer interfacing.
Electroencephalography (EEG) has the advantage that it
is relatively cheap and simple to do and can provide useful information in a clinical setting. It is also non-invasive
and so is amenable to a wide variety of brain computer
interfacing techniques, provided useful information can
be obtained. There is a distinct advantage that changes in
brain activity can be read very rapidly compared to other
slower methods that rely on a change of blood flow, such as
functional magnetic resonance imaging (fMRI), for example.
EEG also has a number of disadvantages. A scalp-reAn EEG headset, as used in a clinical
setting. Worldwide, the location of
EEG electrodes is standardised
according to the so-called 10-20
system (see right) whereby
electrodes are positioned
according to anatomical
landmarks. Results from
different researchers will
therefore correspond to
the same electrode locations
(there are also higher resolution
electrode placement schemes such
as the 10-5 system and others). In clinical applications
typically 19 electrodes are used plus an earth and
system voltage reference. The voltages measured are of
the order of microvolts and are amplified by 1,000 to
100,000 times.
12 Silicon Chip
siliconchip.com.au
FACING
BRAIN
... yes, it is
really happening!
corded EEG represents a coarse measure of brain activity
due to the poor electrical conduction and thickness of the
skull and the subsequent dispersion of electrical signals.
It only measures the collective excitation of large numbers
of neurons behaving in a synchronised manner that also
happen to be oriented in the correct direction to provide an
electrical signal that conducts toward the scalp. Individual
neurons or small groups of neurons cannot be read directly.
The EEG output consists of rhythmic signals in various
frequency ranges and also transient activity. Typically (but
not always) these rhythmic signals are classified in terms
of a number of frequency bands. These are usually Delta
(<4Hz), Theta (4-7Hz), Alpha (8-15Hz), Beta (16-31Hz),
Gamma (32+Hz) and Mu (8-12Hz). All these bands are associated with a certain biological significance and activities
in the brain.
Electrocorticography
Electrocorticography (ECoG) is a form of EEG in which
the electrodes are placed on the surface of the brain (cerebral cortex). It has the advantage that much higher spacial
resolutions can be obtained and the sampling of much
smaller groups of neurons. Different types of electrodes
can also be used.
Of course, it has the distinct disadvantage that it is intrusive and requires the skull to be opened. For the purposes
of brain computer interfacing it would only be done (at this
point in time) for life-critical applications such enabling a
quadriplegic to operate a robotic arm or wheelchair.
Electrical activity in the brain
The brain consists of specialised cells called neurons
and glial cells. The neurons are the cells responsible for
information processing while the glial cells mostly have
support roles.
Neurons are electrically active and can communicate
with other cells in the brain by a branched conducting
fibre called an axon that extends from the body of the cell
and which can communicate with many other nearby or
far away neurons. Neuron to neuron communication constitutes the essence of how the brain works.
The architecture of this connectivity between neurons
Research conducted at the Brain Institute at the University
of Utah showing three types of electrocortical arrays in
simultaneous use. The numbered electrodes are part of an ECoG
array sitting on the surface of a human brain, the green wires
terminate in a micro-ECoG grid and the black square with the
gold-coloured electrodes is a “Utah Electrode Array” (UEA)
which has an even finer resolution than the micro-ECoG grid. In
this work the electrodes are used to discover and remove areas
of the brain responsible for epileptic seizures but data read
from such electrodes can also be used, for example, to convert
speech-related brain signals into words, control machinery
such as a robot arm, a wheelchair or even an aircraft or to work
in any other application requiring a direct brain-computer
interface. Note that while it is obviously an invasive procedure
to have such electrodes implanted beneath the skull, these
particular electrodes sit on the surface of the brain and do not
penetrate it where damage may be done in sensitive areas.
siliconchip.com.au
January 2015 13
Synaptic transmission of information showing neuron body
(soma) and attached dendrites and axons. Information
enters a neuron via a dendrite and leaves via an axon.
Neurotransmitter molecules pass across the synaptic gap.
Each electrical impulse will cause a connected neuron to
be either excited or inhibited. The collective excitement or
inhibition of very large numbers of neurons is what can be
detected by an EEG signal.
is known as a neural network.
The way axons transmit electrical signals is by means of
electrochemical pulses involving sodium and potassium
ions being transported in different directions through the
neural cell membrane. These electrochemical pulses are
known as action potentials and typically last less than one
millisecond and propagate at speeds of 1 to 100 metres
per second.
Some neurons are inactive most of the time while others may be constantly active and fire at a rate of 5 to 50
times per second. A neuron’s axon is connected to other
neurons via junctions called synapses which make contact
with another part of the neuron’s body called the dendrite.
There is a very high level of connectedness; each axon may
have many thousand synaptic connections to neurons or
possibly other cell types.
According to the latest estimates the human brain has an
average of 86 billion neurons and 100 trillion synapses. The
axons are the “wires” that connect most of the functional
elements of the brain with each other.
Once an electrical signal or action potential arrives at a
synapse, specialised chemicals known as neurotransmitters are released and these bind with the target neuron or
other cell.
Many different neurotransmitters exist (around 100 have
been identified so far) and can exert many different simple
14 Silicon Chip
or complex influences on the target (or post synaptic) neuron but fundamentally will cause the post synaptic neuron
to be either inhibited or excited.
As each neuron is connected to large numbers of other
neurons the total numbers of inhibitory or excitatory signals
received will determine whether that neuron will either
not fire or fire and not pass or pass information to the next
neuron in the network, and so on.
Many of these synaptic junctions are dynamically reconfigurable by changing the nature of the signals that travel
through them and are thought to be involved in learning
and memory.
Since the connections are not “set in stone”, some reconfiguration of the brain is possible and this is the basis
of neuroplasticity, the ability of the brain to reconfigure
itself to compensate for damage.
This plasticity has only been seriously recognised in
recent years and also suggests that electrode placement for
the purpose of brain-computer interfacing is not extremely
critical. It suggests that the brain will eventually be able to
learn how to control an interface no matter where in the
brain it is located (within reason) by a sufficient amount
of learning.
Electrical signals in the brain or action potentials are
the way neurons communicate with each other. Action
potentials are subject to some basic but important rules.
Firstly, there is a minimum threshold voltage below which
no signal will be propagated along an axon so electrical
“noise” will not cause signals to propagate.
Secondly, it is “all or nothing”; each action potential has
the same strength, independent of the strength of a stimulus.
Thirdly, there is a refractory period after the action potential
in which no further action potentials can be generated. This
helps ensure that the action potential propagates in only
one direction and not back to its point of origin.
Most people are familiar with the terms “grey matter”
and “white matter”. If one takes a cross-section of a human
brain, it will be seen that the outer layers are dark in colour
(grey) while the inner parts are light in colour (white). The
difference arises from the fact that axons are lighter in colour due to their insulating myelin sheaths while neurons
are darker in colour. These colour differences show that
the outer parts of the brain contain mostly neurons and
the inner parts of the brain contain mainly axons or the
“wiring” of the brain.
Non-invasive brain interface
While EEG and other methods can be used to read information from the brain, the information has to be meaningful
and somehow express the subject’s intent if they are to do
something useful like control a machine. Like any new
task, practice is necessary so that the appropriate synaptic connections can be strengthened in order to learn the
desired behaviour. The following methods describe ways
BCI devices can be controlled without intrusive implanted
electrodes.
An EEG signal can be influenced by imagined movements
and biofeedback methods whereby an individual learns
with many training sessions to influence an EEG signal in
a way that can be detected and used to drive a machine.
Silent vocalisation of words can also be sensed and used
to drive the interface.
The Steady State Visual Evoked Potential (SSVEP) is
siliconchip.com.au
a control system whereby a subject looks at one or more
flashing screens or symbols. The signal from the flash is
relatively easy to detect in an EEG signal and the intent
of the subject can be inferred from the frequency of the
flashing area they are looking at. It may be annoying for
people to use, however.
The P300 wave, or more specifically now known as
two waves, the P3a and P3b, are another way information
can be read from the brain. These occur after a low probability event is observed and recognised among a series of
“standard” events. These waves are useful to monitor for
brain-computer interfacing because they are relatively consistent across most people and using them can be learned
with minimal training.
One example of using this brainwave for communication in the disabled is the use of a P300 matrix speller. A
test subject is presented with a 6x6 matrix of letters and
numbers and individual rows and columns are illuminated
in a pseudo-random manner. The subject selects a letter by
concentrating on the character they want and their P300
wave is detected at that time.
Using this method with a scalp EEG results in letter selection rates of 1.4 to 4.5 characters per minute. This was
able to be increased to 17 characters per minute by Peter
Brunner and others in 2011 with an implanted 96-electrode
array. Hybrid systems have also been developed combining
the SSVEP mentioned above and the P300. See YouTube
video http://youtu.be/08GNE6OdNcs “Emotiv BCI2000
Video.mp4”.
Writing information to the brain
Mentioned above were several methods that could be
used to read information from the brain. It is also possible
to “write” information to the brain. This can be done via
implanted electrode arrays, transcranial magnetic stimulation (TMS) where a powerful magnetic field is pulsed
through the skull or focused ultrasound (FUS) where a
focused ultrasound beam is transmitted through the skull.
All these methods excite groups of neurons within their
field of influence and cause them to fire.
The earliest experiments with interfacing animal brains
to machines happened in 1969. The experiment was by E.E.
Fetz at the University of Washington School of Medicine
in Seattle and involved training a monkey to move a biofeedback meter needle by activating neurons in its motor
cortex, the region of the brain responsible for the execution
of movement. The activity of these neurons was read from
an implanted tungsten micro-electrode.
Following work by Fetz in interfacing a monkey brain to
a machine, in the 1980s Apostolos Georgopoulos at Johns
Hopkins University found a mathematical relationship
between the electrical signals from motor cortex neurons
and the direction the animal wished to move.
This lead to the development of computer models that relate movement to neural signals and are the basis of models
that now translate complex neural signals into commands
to operate machines such as robot arms.
Monkey controls robot arm
Professor Miguel Nicolelis from Duke University in North
Carolina was the first to interface a monkey brain to a robot
arm which it could move.
By 2000 the group had managed to reproduce a monkey’s
siliconchip.com.au
A monkey using a brain-controlled robotic arm to grab
food to feed itself. The monkeys were able to effortlessly
control the robot arm as though it were a natural part of
themselves.
arm motion in a robot arm by monitoring neural signals
from the monkey. The monkey had no direct control over
the arm, it just reproduced its movements.
Subsequently, monkeys first trained to reach and grab
objects on a computer screen using a joystick. This joystick
also controlled a robot arm which the monkeys could not
see. They were learning the simply task of moving things
in two dimensions on the computer screen before being
shown the actual robot arm which could move in three
dimensions which the monkeys learned to control.
In this work an electrode array monitored an area on the
motor cortex of around 50 to 200 neurons.
Other groups have done similar work and a group lead by
Andrew Schwartz at the University of Pittsburgh in 2008
interfaced a monkey to a robot arm with an electrode array which recorded signals from 15-30 neurons and which
enabled the monkey to feed itself.
A video of a monkey operating a robot arm can be seen
at http://youtu.be/gnWSah4RD2E “Monkey controls robotic
arm with brain computer interface”.
Visual imagery from the brain
Although the stuff of science fiction, scientists are mak-
Open-source brain computer interface
There is a successfully funded Kickstarter project called
OpenBCI to develop an open source platform to enable anyone with an interest to monitor their own or another person’s
brainwaves via a wearable EEG monitor with a view to developing products controlled by the brain. Each board supports
eight electrodes but
these can be daisychained together to
increase the electrode count.
Apart from the
electronics and
software there is
also a 3D printable headset to
mount the electronics package. See
http://openbci.
com/
January 2015 15
can be seen at http://youtu.be/nsjDnYxJ0bo “Movie reconstruction from human brain activity”.
Reading the subject matter of dreams
Image (top row) presented to a cat and reconstruction
(bottom) of that image as read from the brain using
electrodes implanted in a region of the brain that processes
visual information.
ing good progress in reading visual imagery from inside
the brain. Examples include reading images seen by the
eye directly from the brain and also determining some
content of dreams.
In one of the first demonstrations of reading visual imagery from a brain a cat had electrodes implanted in its
brain and it was made to watch various scenes. The data
from the electrodes was processed with some basic mathematical filtering and the original image was reconstructed.
It certainly seems from the reconstructed images, however, that the animal imposed its own cat-like interpretation
on the features on the human face.
This work was done in 1999 at the University of California, Berkeley with a research team lead by Professor Yang
Dan. Naturally, this brain reading was invasive by virtue of
the fact that electrodes needed to be implanted on the brain.
Apart from cats, visual imagery has also been read from
human brains. This work was done in 2011 by scientists
at the University of California, Berkeley lead by Professor
Jack Gallant. In this case non-invasive function magnetic
resonance imaging (fMRI) techniques and computational
modelling were used to read and interpret brain activity.
Subjects watched video clips and the moving images were
read from their brains.
To extract this video information from the brains of
experimental subjects they had to lay still inside a fMRI
machine while watching two different sets of trailers from
Hollywood movies. The fMRI machine was used to measure
the blood flow through the visual cortex of the brain which
is the part responsible for vision. The fMRI data was then
broken down into three dimensional versions of pixels
known as “voxels”.
One of the researchers said “We built a model for each
voxel that describes how shape and motion information in
the movie is mapped into brain activity”. As the video was
being played to the subject the change in each voxel, corresponding to changes in brain activity in that region, was
correlated with the video image being presented at the time.
A problem of using fMRI for this type of work is that
the blood flow which fMRI measures changes much more
slowly than the electrical neural signals. This problem
was overcome by the development of a two stage model
that separately describes the neural signals and blood flow.
However, the scientists who did this work were careful
to point out at the time that the technology to read people’s
thoughts is many decades away. A video of the experiment
16 Silicon Chip
Japanese researchers Yukiyasu Kamitani and colleagues
at the Advanced Telecommunications Research Institute
International in Kyoto, Japan have been working on reading
the subject matter of people’s dreams.
In work published in 2013 they showed that they could
tell what a person was dreaming about. The research involved asking volunteers to have a mid-afternoon nap in
a fMRI machine and when they had reached the earliest
stages of sleep (stage 1 or 2) they were woken and asked
to give a verbal report of what they were dreaming about.
This was repeated at least 200 times for each subject.
Next, these verbal dream reports were analysed by researchers who reduced them to key words and concepts.
Researchers next went online to build a vast visual database
of images that mostly closely corresponded to the subject
matter of the verbal reports provided by the dreamers.
Researchers then did further fMRI scans on the dreamers while they were awake and asked them to watch the
images that had been collected that corresponded to the
subject matter reported from their 200 plus dream sessions.
This enabled brain activity patterns to be read from that
individual that corresponded to the visual imagery they
were watching. These activity patterns were used to train
a decoder computer to correlate patterns of brain activity
with certain types of visual imagery.
After the decoder was trained it was possible to enter
measured brain activity and it could then correlate that with
the visual imagery now known to produce this pattern and
thus the subject matter of the dream could be predicted.
The predictive capacity of the system was quite coarse.
For example, it could tell if someone was dreaming of driving in a car but not what type of car. Also, the decoder has to
be trained individually for each person. It cannot be used to
read dream subject matter without individualised training.
See YouTube video http://youtu.be/inaH_i_TjV4 “Dream
decoding from human brain”.
Transmitting thoughts from one person to
another
In early 2014, a team lead by Alvaro Pascual-Leone, Director of the at the Berenson-Allen Center for Noninvasive
Brain Stimulation at Beth Israel Deaconess Medical Center
(BIDMC) and Professor of Neurology at Harvard Medical
School in Boston succeeded in reading a thought from one
person and transmitting it to another person 8,000km away
via the Internet.
Together with researchers in France and Spain, the
thoughts of a person in India were transmitted to a person
in France. The words transmitted were the greetings “hola”
and “ciao”. In reality it was not words that were transmitted but a binary code. The sender evoked imagery of using
either their hands or feet. The brainwaves of the sender in
India were read by an EEG and it was determined if they
were imagining using either their hands or feet.
Hands corresponded to a “0” and feet to a “1”. The chosen
number was transmitted over the Internet to France and
the receiver’s brain was stimulated via the process of transcranial magnetic stimulation (TMS). The TMS stimulation
was interpreted as a flash of light (phosphene) for a 1 and
siliconchip.com.au
no flash for a 0 and thus the simple message was decoded.
Connecting two rat brains together
The brains of two rats were electronically linked such that
what one rat did was duplicated by another rat at a distant
site. A team lead by Miguel Nicolelis of Duke University in
North Carolina and collaborators in Brazil published this
work in early 2013.
One rat called the “encoder” learned various tasks and
signals from a cortical micro-electrode array implanted in
it were monitored. The electrical signals from the encoder
rat’s brain were then transmitted to the same area of a
“decoder” rat’s brain.
The encoder’s electrode arrays consisted of 32 electrodes
connected to the rat’s primary motor cortex of the brain
which is responsible for movement. The decoder rats had
4 to 6 micro-stimulation electrodes implanted in the same
area.
When the decoder rat received signals from the encoder
rat’s brain it interpreted the action meant by those signals
and performed the same task (pressing the same lever) as
the encoder rat. Even when the decoder rat was untrained
and unfamiliar with the task the decoder rats would press
the correct lever around two thirds of the time which while
not perfect is still a remarkable result.
The encoder rat was located in Brazil while the decoder
rat was located in the USA. A video of the experiment can
be seen at http://youtu.be/w_qbkYDlhDY “Brain-to-brain
interface transmits brain activity directly from one rat to
another”
Human-to-animal control
Transmitting a thought from one person to another is
impressive but so too is transmitting a command from a
person to animal. Seung-Schik Yoo of Harvard Medical
School in Boston lead the team. A person was connected
to an EEG machine and used the technique of steady state
visual evoked potential (SSVEP) to trigger a signal for a rat
to move its tail. The rat’s brain was stimulated in the area
that controls tail movement by the technique of focused
ultrasound (FUS) and the rat moved its tail.
The experiment can be seen at https://www.youtube.
com/watch?v=VaJjHgyHnEc “Human moves rat’s tail with
thoughts alone”. See also http://youtu.be/TpFdM_e76Fw
“LEGO goes with the brain: A robot
remotely controlled with steady-state
visual evoked potentials”,
Still images taken from video showing the presented image
(top) and the corresonding image read from a human brain
using functional magnetic resonance imaging (fMRI).
(From http://spectrum.ieee.org/geek-life/tools-toys/this-isyour-brain-on-fmri)
(sic) in which a robot is controlled by a person using SSVEP techniques.
Human-to-human control
Researchers at the University of Washington have enabled one person to control motion in another person. The
first person thought of an action to move their hand to
press a button but did not actually move their hand. The
electrical activity in the brain associated with this intention was recorded with an EEG headset and transmitted
via the Internet.
The brain of a receiving subject was stimulated via the
process of transcranial magnetic stimulation (TMS) which
induced an electrical signal in the brain of the subject over
an area responsible for hand movement causing them to
physically move their hand to press a button.
This may sound scary in some senses but it is important
to note that this work is currently at a very basic level and
there is no indication that mass mind control or robot-like
zombie people will be walking our streets any time soon.
See http://youtu.be/rNRDc714W5I “Direct Brain-to-Brain
Communication in Humans: A Pilot Study”.
Human vision & movement
An obvious application for interfacing the brain is to
provide vision for blind people. Retinal implants (“bionic
eyes”) are one such approach but if this is not suitable
the vision areas of the brain can be stimulated directly.
Data from a camera is processed and sent to an electrode
array implanted on the visual cortex of the brain. Where
Scheme by which a thought was
transmitted from one person to another
over the Internet. From http://abcnews.
go.com/Technology/scientists-transmitthoughts-brain/story?id=25319813
siliconchip.com.au
January 2015 17
this has been done the subjects have gained some limited
level of functionality to enable them to do basic tasks and
even driving a car slowly in a car park was demonstrated
in one instance.
BCIs have been used to help disabled people control
computer cursors for communication, wheelchairs and robotic arms to help them with household tasks. See YouTube
videos http://youtu.be/mJQ0HqThU4c “Two-Dimensional
Cursor Control Using EEG”, http://youtu.be/qQ7AJnVKc_g
“Mind Typing and PC Control with Brain-Computer Interface (BCI)”, http://youtu.be/gvR0kHm9fwo “BCI driving a
wheelchair” and http://youtu.be/76lIQtE8oDY “One Giant
Bite: Woman with Quadriplegia Feeds Herself Chocolate
Using Mind-Controlled Robot Arm”.
Neurogaming
Neurogaming is a new computer gaming modality where
characters and games are controlled by BCI technology
as well as other sensors such as heart rate monitors, eyetrackers and sensors to detect muscle movement. Such
technology can also be used for virtual reality training for
different professionals and has also been suggested for the
treatment of various disorders such as PTSD, ADHD and
other behavioural and cognitive disorders.
Future uses
Anything that requires human input for control is open
to the possibility of direct control via a brain-computer
interface. For precise and high levels of control it may be
necessary to have implanted electrode arrays since at the
moment scalp EEG readings are fairly coarse in nature
although if training with EEG headsets started at a young
age, better results might be achievable.
The military also have some interest in controlling fighter
jets and other machines with the mind (whether the pilot
is in the cockpit or a remote operator). Firefox (1982) was
a science fiction movie which features an aircraft with a
mind-controlled weapons system but the English-speaking
pilot tasked to retrieve the plane could not get it to work
until he realised he had to think in Russian, not English.
Brain-controlled toys
A number of toys have been produced or are under
development which are controlled by the brain. One such
toy is a radio-controlled helicopter called the Puzzlebox
Orbit which us controlled via a NeuroSky EEG headset
(see below).
Instructions for a do-it yourself conversion of a cheap
radio controlled helicopter to mind control using consumer
EEG headsets is described at http://www.instructables.com/
id/Brain-Controlled-RC-Helicopter/
Note that on that web page on the right hand column you
will see links to other brain control DIY projects.
Consumer EEG headsets
Interfacing the brain is not just restricted to laboratories.
There are a large number of consumer grade EEG headsets
available for the purpose of brain computer interfacing.
They are all capable of measuring a number of mental states
and some can measure facial muscle movement and eye
movement as well. A full description of these devices is
not possible here but you may wish to research them yourselves. These devices have between 1 and 14 electrodes.
Some of these headsets are also appropriate for professional
use and research.
The devices include: Emotiv EPOC, Emotiv Insight,
HiBrain, iFocusBand, Mindball, Mindflex, MindSet, MindWave, Muse, MyndPlay BrainB, Neural Impulse Actuator
(discontinued and detected muscle movement only),
NeuroSky, OpenBCI (this is an open hardware project,
see box), Star Wars Force Trainer (discontinued), Xwave
headset (discontinued) and Xwave Sonic (discontinued).
Of particular interest is that Emotiv Systems is a Sydneybased company with international offices, founded by former Young Australian of the Year, Tan Le. For an overview
of some features of one of the Emotiv headset models see the
YouTube video at http://youtu.be/bposG6XHXvU “Emotiv’s
New Neuro-Headset”.
A lot of open-source software has been developed to
support the output of some of these and other EEG devices.
An example is OpenViBE, which is a general purpose and
highly capable software platform for real-time acquisition,
processing and classification of brain waves for all aspects
of brain-computer interfaces including biofeedback, robotinterfacing, diagnosis, biofeedback and game control.
OpenViBE can be used by anyone even if they are not
familiar with programming. Several open-source Matlab
toolboxes have also been developed for interpreting data
Scheme for brain to brain interface with human
subjects. A sender imagines hand movement to
press a fire button but does not actually move his
hand. The intent to press the button is detected
via EEG signals and the signal is transmitted
via the Internet. The person receiving the
signal is stimulated to press a button as their
brain is stimulated via transcranial magnetic
stimulation (TMS). (From www.washington.edu/
news/2013/08/27/researcher-controls-colleaguesmotions-in-1st-human-brain-to-brain-interface/).
18 Silicon Chip
siliconchip.com.au
from various EEG devices.
With any EEG device, receiving unwanted electrical noise
from muscles can be a problem with these devices so a
special effort has to be made to avoid unwanted movement,
especially of the facial area, when using these devices.
SILICON CHIP readers may be interested in experimenting
with some of these devices and software tools.
Many of these devices can be connected to smart phones
for purposes such as meditation, biofeedback or playing
games (neurogaming) or other possible purposes such as
assisting the disabled to communicate, for research, software usability testing and so-called neuromarketing where
a person’s reaction to advertising material is monitored.
BCI2000
In addition to the open source software mentioned above
to analyse EEG signals, BCI2000 (www.schalklab.org/research/bci2000) is an open-source suite of software for all
aspects of brain-computer interface research and can be
used for data acquisition, stimulus of neurons and brain
monitoring applications.
It is free for non-profit and educational use and supports
numerous types of instrumentation and runs on Windows,
OS X and Linux.
It has been under development since 2000 by the BrainComputer Interface R&D Program at the Wadsworth Center
of the New York State Department of Health in Albany,
New York with substantial contributions from various
other groups.
BCI2000 is designed to easily interface with various
equipment and software in real time via a network-based
interface so that, for example, a robot arm running its own
software could be made to be easily controlled by neural
signals processed by BCI2000. In addition, Matlab scripts
can be executed within BCI2000.
BCI2000 has an additional benefit that all data is stored
in a standardised format along with the system configuration and event markers so that it can easily be shared with
other researchers.
To see an example of BCI2000 in use see http://youtu.be/
suKTlrzaU9g “Playing the Game ‘Pong’ with EEG”. Here
a 32-channel EEG is acquired and analysed from each of
two subjects to extract control signals which move the
electronic game paddles.
Ethical issues
As with any new technology certain ethical issues need
to be considered, especially with intrusive brain interfaces
such as cortical electrode arrays. While few would question the need for such intrusive interfaces in life-critical
applications such as controlling a wheelchair or robot
arm, one might question the appropriateness of such an
interface for a non-critical application such as connecting
to the Internet.
On the other hand many would argue that a person is
entitled to do as they will with their own body as long as
that person pays for it.
Other issues relate to the reversibility or otherwise of
intrusive BCI interface procedures. Most implants, no matter what type, leave some sort of permanent impact on the
body and may not be removable without doing damage.
What issues arise if better models of interface are developed
and old ones need to be removed?
siliconchip.com.au
Cyborg Roaches!
We make no judgement
on the ethics of doing
this but some people
have built their own
remote controlled
living cockroaches
with parts from a kit
as featured in this video.
http://youtu.be/V2zNOP6RqRk “Amazing! Real Creating a Cyborg Cockroach (Bugs Robot)”.
It is not known whether this would work with typical Australian cockroaches.
It is not a joke! Note that the developer does consider
ethical issues and addresses them on their web page at
https://backyardbrains.com/products/roboroach
Alternative therapies also need to be considered. For
example, with advances in stem cell research it is conceivable that in the near term future spinal cords could be
repaired and the necessity to have an electrode implant for
brain control of a wheelchair might become unnecessary
(but people already in receipt of such implants might be
able to re-purpose them).
Conclusion
Brain-computer interfacing has an exciting future and it
is likely that the first major uses will be to assist disabled
people to communicate and move.
Neurogaming, like much computer gaming is likely to
have many spin-offs such as virtual reality and treatment
of various disorders. Later developments might include
control of cars, aircraft and many other machines as well.
Some people may consider the technology “inhuman”
and may choose to preserve what they see as their humanity. Controlling animals with BCI may bring many benefits
such as in search and rescue but may also raise ethical
challenges.
Neuroplasticity ensures that most people should be able
to learn to use BCI and most likely do useful things with
non-intrusive BCI such as EEG headsets. Other ethical challenges are raised due to appropriateness of the technology
for certain uses and cost.
In the medium to long term future the rights of people
not to have their mind read (should that prove to be possible) need to be seriously considered. BCI is potentially
very useful for the disabled but biological cures using stem
cells for conditions such as a severed spinal cord may be
better and not far off.
The nightmare scenarios from science fiction seem a long
SC
way off, if they happen at all.
YouTube videos of interest:
Visual Image Reconstruction from Human Brain:
http://youtu.be/daY7uO0eftA
A Remote Controlled Rat: http://youtu.be/G-jTkqHSWlg
Cyborg insects: http://youtu.be/dSCLBG9KeX4
Computer records animal vision in Laboratory – UC Berkeley:
http://youtu.be/piyY-UtyDZw
January 2015 19
The Micromite
Mk.2
More memory, more functions
& much faster than before!
Introduced in the May 2014 issue of SILICON CHIP, the Micromite
is a small 28-pin chip running a powerful BASIC interpreter. Now
we introduce the Micromite Mk.2 with more memory, higher speed
and a host of other improvements. It’s all due to the relentless
march of semiconductor technology.
By Geoff Graham
T
HE SEMICONDUCTOR industry
does move fast. Just after the introduction of the Micromite back in
May 2014, the manufacturer of the
PIC32MX150F128 microcontroller
used in the device surprised us with
a new version of the chip. Designated
the PIC32MX170F256, it has the same
capabilities as the original but has
double the amount of RAM and flash
memory. Even better, it only costs 40
cents more.
We had gone to a lot of effort to
squeeze the MMBasic interpreter into
the original chip. However, as soon
as we saw the new chip, we started
thinking of implementing some of
the features that were missed out in
the original version. The result is the
Micromite Mk2. It does everything the
original Micromite did but it does it
much faster, with a lot more memory
and a lot more features.
The original Micromite is still fine
for everyday jobs; it’s just that it now
has a newer and faster cousin.
The Micromite
Just in case you missed the May
2014 issue, the Micromite is a PIC32MX150F128 microcontroller programmed with our BASIC interpreter
called MMBasic. This microcontroller
comes in two package styles: (1) a 28pin plastic dual-in-line (DIL) package
which can be plugged into a breadboard or IC socket; and (2) a 44-pin
surface mount (SMD) package.
The 28-pin Micromite has 19 I/O
pins which can be configured by the
The Micromite Mk.2 is just a Microchip PIC32MX170F256 microcontroller
programmed with Version 4.6 of our MMBasic interpreter. You can buy the
microcontroller in both 28-pin and 44-pin versions and once programmed it
turns into an easy to use controller that you can employ for a host of tasks,
eg, servo control, infrared remote control, distance sensors, temperature
sensors and much more.
20 Silicon Chip
BASIC program to be digital inputs
or outputs, analog inputs, frequency
measurement inputs and more. The
44-pin chip has 33 I/O pins with the
same characteristics.
The BASIC interpreter running on
the Micromite is a high-level implementation of the language. It supports floating point and strings, long
variable names, arrays with multiple
dimensions, user defined subroutines/
functions and a host of other advanced
programming features.
Programs are stored in the chip’s internal flash memory and can be edited
on the chip using the inbuilt full-screen
editor and a serial link. A program can
be configured to run immediately on
power-up so that the Micromite acts
as a pre-programmed custom chip and
the user need not know anything about
what’s running inside.
Perhaps the most powerful feature
of the Micromite is the range of communications protocols that it supports.
These include I2C, asynchronous ser
ial, RS232, IEEE 485, SPI and 1-Wire.
Using these, your program can communicate with other chips and sensors
and can send data to test equipment.
The new chip
As stated, the Micromite Mk.2 uses
the new PIC32MX170F256 series. For
people who struggle to decode these
siliconchip.com.au
part numbers, “PIC32” refers to the
32-bit family of Microchip processors,
“MX170” is the chip’s part number
and “F256” refers to the amount of
flash memory in the chip (256K bytes
in this case).
The MX170 comes in a number of
variations with different packages, pin
numbers and maximum speeds. Table
1 lists the versions suitable for the
Micromite Mk.2 and their characteristics. The recommended part number
is the PIC32MX170F256B-50I/SP. This
has a top speed of 50MHz and is in a
plastic DIL package with 28 pins.
If you purchase one of these from
Microchip, it will cost you around
$US4 (plus freight). You then need a
programmer such as a PICKit3 to load
the MMBasic firmware and turn it
into a Micromite Mk2. Alternatively,
if you only need a few chips, a more
convenient option is to purchase the
chip fully-programmed from the SILICON CHIP OnlineShop for $15.00 plus
postage.
More memory & much faster
One of the great features of the
Micromite Mk2 is that the free space
for your BASIC programs has been
increased to 58KB and the amount
of free RAM is now 52KB. This is a
huge increase on the original Micromite which had just 20KB and 22KB
respectively.
Previously, you could run quite
large programs. Now you can run
truly enormous programs with plenty
of comments and other components
that consume the program space. In
addition, the extra RAM allows your
programs to build large arrays for manipulating numbers and large buffers
for moving data around.
Another feature of the Micromite
Mk2 is that it is much faster than the
previous version. The chip used in
the original Micromite had a limited
amount of flash memory, so when we
squeezed the MMBasic interpreter
into this chip, we had to optimise it
to conserve space. And that slowed
down the interpreter.
With double the amount of flash
memory in the Micromite Mk2, we
have the luxury of optimising the interpreter for speed. So now programs on
the Micromite Mk2 will run about 40%
faster than on the previous Micromite
running at the same clock speed.
In fact, the Micromite Mk2 has
more memory and runs faster than the
siliconchip.com.au
Fig.1: the DHT-22 is a combined
+3-5V DC
temperature & humidity sensor
that is supported by MMBasic
in the Micromite Mk2. Using
ANY MICROMITE
just one command you can
I/O PIN
get both the temperature and
humidity with no complicated
programming required. Note
that the DHT-22 is also known
as the RHT03 or AM2302.
popular Maximite and Colour Maximite computers described in the March
2011 and September 2012 issues of
SILICON CHIP.
Big numbers
The original Micromite used floating point numbers (often abbreviated
to “float”) for all arithmetic. Floating
point is good because it allows you to
have numbers with a decimal point
such as “12.4”. However, the problem
with floating point numbers is that
they only store an approximation of
the number when the number has more
than six or seven significant digits.
Despite this issue, floating point
is still the best for general purpose
computing. It is rare that you need
more than six digits of accuracy in
everyday life and operations like
division always do what you expect
4.7k
when you are using floating point. On
the other hand, when you are working in an embedded controller environment, you often need more precision than floating point numbers can
provide.
Because of this, we have given the
Micromite Mk.2 the ability to store and
manipulate numbers as 64-bit signed
integers. These can be used to accurately count and manipulate numbers
up to nine million million million
(or ±9,223,372,036,854,775,807 to be
precise), which is a very large number
indeed.
The downside of an integer is that
it cannot store fractions (ie, numbers
after the decimal point). Any calculation that produces a fractional result
will be rounded up or down to the
nearest whole number when assigned
to an integer.
New Features In The Micromite Mk.2
• The same hex file works with both 28-pin and 44-pin chips.
• The amount of free memory for programs is increased by 300%.
• Programs will run about 40% faster at the same CPU speed.
• 64-bit integers can be used to store and manipulate numbers as large as 19 digits.
• 64-bit integer arithmetic is about 25% faster than floating point.
• A full SELECT...CASE decision structure has been implemented.
• Compiled C or assembler programs can be embedded in the BASIC program.
• The temperature and humidity can be read from a DHT22 sensor.
• The frequency of the internal clock can be trimmed for better timekeeping.
• The >> and << operators can shift bits in a number to the right or left.
• The processor can be put to sleep for a specified number of seconds.
• The gate time used when making frequency measurements can be specified.
• Internal pull-up or pull-down resistor can be enabled for any input pin.
• Voltage measurements can be corrected for variations in the supply voltage.
• The console can be used with RS232 signals without a converter.
• The TIMER function will now count up for over 200 million years.
• The SPI function can now send/receive data in 32-bit blocks (in addition to eight and 16
bits).
• Additional features to prevent common programming errors.
• The manual has been updated and it includes a full bookmark listing.
January 2015 21
(%) as a suffix to a variable name. For
example:
+3.3V (FROM PICkit3)
PICkit3
ICSP CON.
Count% = Count% + 1
10k
1
1
MCLR
27
2
Vcc
Because this expression uses 64-bit
integers, it will be able to count up to
a number with 19 digits with perfect
accuracy. Even doing nothing else, a
Micromite Mk2 running at full speed
would take millions of years of counting to reach this limit.
28
3
GND
PGD
PCC
4
4
5
5
6
(NC)
28-PIN
MICROMITE
8
20
47 µF 6V
19
13
CERAMIC
OR
TANTALUM
LOADING FIRMWARE
Fig.2: here’s how to connect a blank 28-pin chip to a PICkit3 programmer
to load the MMBasic firmware for the Micromite Mk2. Once connected,
you use MPLAB IPE (free from Microchip) to program the device. Note
that the 47µF capacitor is critical and must be a tantalum or multilayer
ceramic type.
+3.3V (FROM PICkit3)
17
28
40
10k
PICkit3
ICSP CON.
MCLR
Vcc
GND
PGD
PCC
NC
1
18
2
44–PIN
MICROMITE
3
4
21
5
22
7
6
47 µF TANTALUM
OR 10 µF CERAMIC
6
16
29
39
LOADING FIRMWARE
Fig.3: the 44-pin version of the chip is programmed using a PICkit3 programmer as shown here.
An illustration of where 64-bit integers come in handy is when you are
dealing with latitude and longitude.
For example, you might be planning
a project which needs to capture these
two numbers from a GPS module and
use them to calculate the distance
between two points.
The problem comes about because
latitude and longitude need to be
stored with more than six digits of
accuracy. For instance, the longitude
of Sydney is 151.2094° and a floating
point variable will only store that
number as an approximation. This
is a significant issue because even a
slight variance in the stored number
could represent an error amounting to
several kilometres.
However, you could store the latitude and longitude in hundredths of a
22 Silicon Chip
second and use 64-bit integers to handle the number (Sydney’s latitude in
hundredths of a second is 54,435,384).
Because integers retain the full precision of the number, the location will
be accurate to better than one metre.
There are many other cases where
large and precise numbers are required; eg, when working with frequency synthesisers.
Calculations involving integers are
also faster than floating point calculations (by about 25%) and there is
nothing stopping you from using them
exclusively in your programs if you
need a bit more speed. The only drawback is that integers cannot store fractions, only whole numbers. For many
programs though, that is not an issue.
In MMBasic, 64-bit integers are
specified by adding the percent symbol
Mixed arithmetic
With the introduction of two types
of numbers (floating point and integers), you might be wondering how
MMBasic handles the two when they
are mixed in a calculation. Well, in
general, this is done automatically
and is transparent to the programmer.
For example, if you assign a floating point to an integer, MMBasic will
automatically convert it to an integer,
including rounding the fractional
component to the nearest integer. The
opposite action will convert an integer
to a float.
Because floating point numbers can
handle a wider range of numbers, the
interpreter will automatically promote
an integer to a float when the two are
mixed in an expression. For example,
in the following program fragment,
the value of B% will be automatically
converted to floating point with the
result that 123.45 will be stored in Nbr:
A = 23.34
B% = 100
Nbr = A + B%
If all numbers in an expression are
integers, then they will be left as integers and an integer will be returned.
The only exception to this is division
using the normal divide operator (/). In
this case, both sides of the expression
will be promoted to a floating point
number and a floating point number
will be returned.
For integer division, you should use
the integer divide operator (\). It will
leave both sides of the expression as
integers (or convert them if they are
floats) and return an integer while
truncating any fractional part.
If you use constant numbers (eg,
23.45, 100, etc) in an expression, they
will be treated as a floating point number if they contain a decimal point and
an integer if they do not.
Functions in MMBasic return integers or floating point depending on
their characteristics. For example, the
function to get the length of a string
(LEN) will return an integer while
siliconchip.com.au
TAN() will return a floating point. As
another example, PIN() will return a
float if it is measuring voltage but an
integer if it is counting the pulses in
an input signal.
BASIC CONNECTIONS
1
28
27
CFunctions
Another new feature in the Micromite Mk2 is the ability to define
program modules written in C or MIPS
assembler. These modules can be easily called by your BASIC program and
can be used to implement functions
that cannot be implemented in BASIC.
Typically, you use CFunctions to
access special features of the PIC32
chip or where speed of execution is
required. As an example, the firmware zip file for the Micromite Mk2
(available on the SILICON CHIP website)
includes a CFunction that will add up
to eight additional serial I/O ports.
This isn’t something that you could
do in BASIC alone, as the interpreter
is not fast enough for this type of bit
manipulation operation.
However, by adding the code for the
CFunction to your BASIC program,
you can have the best of both worlds
– the easy-to-program BASIC language
and the high-speed ability of a function
written in C.
A few caveats are in order here.
Writing in the C language is nowhere
near as easy as writing in BASIC and
the environment of the CFunction
is limited. For example, you cannot
interact with MMBasic (except in
limited ways) or call standard library
functions. However, CFunctions are
handy for small functions that cannot
be accomplished using BASIC.
Example CFunctions
The zip file containing the Micromite Mk.2 firmware includes a number
of example CFunctions. These include
sending serial data, receiving serial
data, discovering the chip type that
the program is running on (28-pin or
44-pin) and discovering the current
clock speed.
By using pre-compiled functions
like these, you will be able to add
functionality to your programs without having to know anything about
the internals of the CFunction. Hopefully, other people will write more
CFunctions and expand the library
in the future.
If you do want to delve into writing
CFunctions yourself, the Micromite
Mk.2 zip file includes a link to a 74siliconchip.com.au
+2.3 TO +3.6V
(25mA)
(CAN BE 2 x AA
CELLS OR A
NOMINAL 3.3V
POWER SUPPLY)
SERIAL CONSOLE:
VT100 TERMINAL OR
USB TO TTL CONVERTER
(38,400 BAUD, 8 BITS,
NO PARITY, 1 STOP BIT,
TTL VOLTAGE LEVELS)
8
MICROMITE
20
47 µF 6V
Rx
SERIAL
TERMINAL Tx
DATA FROM MICROMITE
DATA TO MICROMITE
GND
11
12
13
19
CERAMIC
OR
TANTALUM
Fig.4: to use the Micromite Mk.2, you need to connect it to a VT100 emulator
such as the ASCII Video Terminal described in SILICON CHIP in July 2014.
Alternatively, you can connect it to a PC via a USB-Serial bridge. You can
then use programs such as Tera Term or MMEdit to create programs and
download them to the Micromite (see text). As before, the 47µF capacitor is
critical and must be a tantalum or multilayer ceramic type.
page tutorial which goes into all the
details.
Select...Case
One often requested feature in
MMBasic is the SELECT...CASE statement. Given the expanded flash memory capacity of the new chip, we have
now been able to add this.
This is generally used as a replacement for the IF...THEN...ELSEIF construct. The SELECT...CASE statement
is much easier to use and makes the
intentions of the program much more
obvious to the casual reader (which
might be you in a few years time). The
structure is:
SELECT CASE value
CASE testexp [[, testexp] ...]
<statements>
<statements>
CASE ELSE
<statements>
<statements>
END SELECT
The “value” is the value to be tested
against each following CASE statement, while “testexp” can be a wide
range of test expressions. For example,
you can say 5 to 8 which will match
the numbers 5, 6, 7 and 8. You can say
>5 which will match any value greater
than 5. There are many more tests that
you can make and they are detailed in
the user manual.
Reduced programming errors
While the BASIC programming lan-
Fig.5: the terminal emulator that
you use to connect to the Micromite
Module (via USB) should be set
to 38,400 baud, eight bits data, no
parity and one stop bit. This screen
grab shows what the set-up dialog in
Tera Term should look like with the
correct values entered. Note that your
port number will almost certainly be
different to that shown because it will
change with the physical USB port.
guage has the reputation for being easy
to learn it also has a darker reputation
for creating some difficult to debug
programs. The new Micromite Mk2
has a number of additional features to
help eliminate many of the more common programming errors and make it
easier to debug the final program.
For some time, MMBasic has had
structured programming elements like
multi-line IF...THEN constructs and
subroutines/functions. These have
mostly eliminated the need to use
the GOTO command which has the
January 2015 23
Fig.6: MMEDIT
was written by
Jim Hiley and can
be installed on a
Windows or Linux
PC. It allows
you to edit your
program on the
PC and then, with
a single mouse
click, transfer it to
the Micromite for
testing.
potential to create truly impossibleto-understand programs.
New in the Micromite Mk2 is the
OPTION EXPLICIT command. This
instructs the interpreter to not automatically create a variable when it is
encountered in the program.
Previously, when MMBasic found
an expression like nbr = 1234, it would
automatically create the variable nbr
and then assign the number 1234 to it.
This is fine for quick and dirty programs but in a larger program, disaster
can strike if the variable was misspelt.
For example, if the programmer
accidentally misspelt the above variable as nmbr, the interpreter would
automatically (and silently) create it
with the value of zero. The programmer, who expected it to contain 1234,
might miss this subtle change in testing, with the result that the program
contained a potentially serious flaw.
Now the programmer can specify
OPTION EXPLICIT which will throw
an error when the new variable is
encountered without being explicitly
declared beforehand. The way you
do this is with the DIM command.
For example, at the beginning of the
program you can state:
DIM AS INTEGER nbr
This tells the interpreter that nbr is a
Where To Get The
Micromite Mk2
A pre-programmed Micromite Mk2
chip (28-pin version) is available
for $15 plus p&p from the SILICON
CHIP Online Shop (includes the
47μF capacitor). MMBasic and a
User Manual are also available on
the SILICON CHIP website (free of
charge).
24 Silicon Chip
valid variable (and is an integer). Then,
if the program used a reference to nmbr,
an error message will be shown (variable not declared).
Another common class of bugs can
occur when the type suffix is left off
a variable. The type suffix indicates
the type of variable – for example “$”
indicates a string and so data$ would
be a string. If the suffix was accidentally left off during program entry,
the type of variable would then be a
number, which is significantly different from that which the programmer
had intended.
To prevent this type of error, the
programmer can specify OPTION
DEFAULT NONE which tells MMBasic
that variables must have a type suffix
or the type must be explicitly specified
in the DIM command. In fact, placing
both OPTION EXPLICIT and OPTION
DEFAULT NONE at the start of your
program is good programming practice
and will draw attention to a wide range
of common programming errors.
The OPTION DEFAULT command
also allows you to specify the default
type for a variable without a suffix.
This can be convenient for a short
program where you are only using
integers (for example); you can then
specify OPTION DEFAULT INTEGER
and gain the speed benefit of integers
with the shortcut of not having to
specify a suffix.
It does fly in the face of what we
were talking about above but it is acceptable for short programs that only
use the one type of variable.
Constants
Another source of bugs is the use
of literal numbers as constants in a
program. Let’s say that you are building a single-cell battery charger using
the Micromite and you need to detect
when the cut-off voltage has been
reached. Your program might use
something like this:
IF PIN(15) > 1.8 THEN ...
But what does pin 15 connect to
and what does 1.8 represent? In a
year or two when you need to modify
the program, you will have probably
forgotten.
You could always use a variable
called “MaxV” and set it to the threshold voltage but that runs the danger
of being accidentally changed somewhere else in the program. A much
better option is to use the new CONST
command. For example:
CONST BattV = 15, MaxV = 1.8
Then the above program line would
read:
IF PIN(BattV) > MaxV THEN . . .
which is much more understandable
to the casual reader.
Another benefit of constants defined
by the CONST command is that you
can use them through your program
and if you need to change the value
of one particular constant you can do
it easily in the one place.
DHT22 sensor
The DHT22 sensor is a module that
will measure temperature and humidity and can be purchased for less than
$5 on eBay. Support for the DHT22
has been added to the Micromite Mk2
and it provides a convenient method
of measuring these two key weather
parameters.
Connecting the DHT22 is straightforward (see Fig.1) and getting the
temperature and humidity into your
BASIC program is just as easy. The
command is:
DHT22 pin, tVar, hVar
where pin is the I/O pin used to connect to the DHT22 and tVar and hVar
are floating point variables. After this
command has been run, tVar and hVar
will be updated with the measured
temperature and humidity, with a
resolution of one decimal place.
Another useful addition to the Micromite Mk2 is the ability to specify
an internal pull-up or pull-down resistor on any input. Using a pull-up,
for instance, allows you to connect a
switch directly to an input pin. When
the switch is open, the pull-up resistor will keep the input high but when
the switch is closed, the input will be
pulled low.
Overall, there have been almost 50
siliconchip.com.au
new features and enhancements in
the Micromite Mk2 and a summary of
these is listed in the panel at the start
of this article. For the full list, download the updated firmware from the
SILICON CHIP website and refer to the
detailed change log which is included
in the zip file.
The zip file also includes the Micromite Mk2 User Manual which goes into
far more detail than we can provide
here. It runs to almost 80 pages and
includes a detailed description of
each command and function. About
half the manual is devoted to tutorials
and explanations so it also provides
an easy learning path for beginners
to the Micromite and programming
using BASIC.
Programming the chip
As we said earlier, the easy way to
get going with the Micromite Mk2 is to
purchase the chip fully programmed
with the MMBasic language from
the SILICON CHIP website – www.
siliconchip.com.au There are also
some web based companies such as
micromite.org and www.circuitgizmos.com who also supply the chip
fully programmed.
As previously stated, another option
is to purchase a blank chip directly
from Microchip (www.microchipdirect.com) or their distributors (element14, RS Components, etc) and
program it yourself.
To program the chip you need the
Micromite Mk2 firmware (download it
from the SILICON CHIP website) and a
PIC32 programmer such as the PICkit3
from Microchip. There are also many
PICkit3 clones available on eBay and
other sites for as cheap as US$30 and
they seem to do the job just as well as
the genuine product.
In order to use the PICkit3, you need
to download and install MPLAB X
from Microchip. This includes a full
development environment for Microchip products but the part of interest
is the programmer called MPLAB X
IPE (IPE stands for Integrated Programming Environment). This is usually
installed as an icon on your desktop
(in Windows) and double-clicking on
it will put you into the programmer.
Figs.2 & 3 show how the PICkit3
You can use a USB-to-serial
bridge like the one shown
here to connect the Micromite
Mk.2 to a USB port on a PC.
Once connected, you can use
Tera Term or MMEdit to write
programs for the Micromite and
download them via this device.
Table 1: Micromite Mk2 Microcontrollers
CPU
Package & Speed
PIC32MX170F256B-50I/SP
28-pin DIL package. Guaranteed to run at 48MHz
PIC32MX170F256B-50I/SO
28-pin SOIC package. Guaranteed to run at 48MHz
PIC32MX170F256D-50I/PT
44-pin surface mount package. Guaranteed to run at 48MHz
PIC32MX170F256B-I/SP
28-pin DIL package. Guaranteed to run at 40MHz
PIC32MX170F256B-I/SO
28-pin SOIC package. Guaranteed to run at 40MHz
PIC32MX170F256D-I/PT
44-pin surface mount package. Guaranteed to run at 40MHz
This table lists the PIC microcontrollers that are suitable for use as a Micromite
Mk.2. From our testing, the chips rated at 40MHz also ran at 48MHz (at room
temperatures), so they are a viable choice if you cannot find the higher speed
versions.
is connected to the chip. The 47µF
capacitor is critical and should be a
tantalum or multilayer ceramic type
with an ESR (Equivalent Series Resistance) of less than 1Ω. Do not use an
electrolytic as the microcontroller may
intermittently restart without warning.
Using the Micromite Mk2
To write and test your BASIC programs on the Micromite Mk2, you first
need to connect a VT100 terminal
emulator to the console pins as shown
in Fig.4. The emulator should have
a TTL serial interface set at 38,400
baud (Fig.5).
You have two choices here: you
can build the ASCII Video Terminal
described in SILICON CHIP, July 2014 or
you could use a USB-serial bridge as
shown in the accompanying photo. A
USB-serial bridge will convert the USB
interface on a PC to a TTL level serial
interface which can directly connect
to the Micromite Mk2.
Note that the 47µF capacitor in Fig.4
is again critical (see the comments
above related to this component).
Issues Getting Dog-Eared?
If you are using a USB-serial bridge,
you then need to run a terminal emulator on your PC and we recommend
Tera Term for Windows. Another excellent choice is MMEdit written by
SILICON CHIP reader Jim Healy and this
can be downloaded from www.c-com.
com.au/MMedit.htm
MMEdit contains a terminal emulator but it is also a powerful editor for
MMBasic programs with features such
as automatic formatting and colourcoded key words.
Using either Tera Term or MMEdit,
you can develop and test your program
and when you are finished, set the
program to automatically run when
the chip is powered up.
As a closing thought, consider
that this little $4 chip has double the
memory of the first personal computers which were programmed in BASIC
(the Tandy TRS-80, Apple II, etc) and
runs more than 50 times faster. That
really is amazing.
Finally, for firmware updates and
handy hints, check the author’s website at geoffg.net/micromite.html SC
Keep your copies safe with our handy binders
Order online from www.siliconchip.com.au or fill in and mail the handy order form in this issue or ring (02)
9939 3295 and quote your credit card number.
siliconchip.com.au
January 2015 25
By JIM ROWE and
NICHOLAS VINEN
Isolating High Voltage
Probe for Oscilloscopes
Here’s a low-cost project which will allow you to use your oscilloscope to
observe and measure AC mains and other high voltage waveforms safely.
It has three switchable input voltage ranges, wide bandwidth and high
voltage isolation between input and output.
O
bserving and measuring waveforms on the AC mains and in
other high voltage circuitry
is quite dangerous using a standard
oscilloscope or with the usual passive
probes.
And by “dangerous” we mean not
only risking a possibly lethal electric
shock to yourself, but also risking serious damage to your scope.
The danger arises mainly because
the “earthy” side of all scope inputs is
connected to the scope’s internal frame,
which is normally itself earthed via the
mains cable.
And it needs to be earthed in this
way, both for correct operation and for
the safety of the operator – you. (An
unearthed or “floating” scope is an ac26 Silicon Chip
cident/disaster waiting to happen, so
never be tempted!)
So the earthy side of all scope inputs is connected back to mains earth,
which clearly poses a problem when
you want to make measurements in
circuits where everything is operating
at a high or significant voltage with
respect to earth.
After all, where do you attach the
“earth clip” of the scope probe?
For example, in a circuit connected
directly to the 230VAC mains, you
can’t connect the earth clip to the Active line because this will at least blow
one or more fuses and may even start a
fire which destroys either the scope or
various components in the circuit you
want to make measurements in.
On the other hand you can’t clip it
to the Neutral line either, because this
is often itself floating at a significant
voltage with respect to earth.
Another problem arises because the
input attenuator on each channel of
most scopes can only be switched to
a maximum setting of 5V/division,
which corresponds to 50V/division
when a 10:1 divider probe is being
used.
Because there are usually only 10
vertical divisions on the display, this
means that only waveforms of up to
500V p-p (peak-to-peak) can be displayed in their entirety.
Since the peak-to-peak amplitude of
a 230VAC mains waveform is around
650V, this means that it simply can’t be
siliconchip.com.au
The differential probe connects to the circuit being tested using a pair of
standard multimeter probes, alligator clip leads or similar. The output
signal is optically isolated and connects to the oscilloscope (or other
test instrument) via a BNC lead. Three different attenuation factors are
available; 10:1, 100:1 or 500:1, to suit the voltages being measured. The
higher attenuation settings offer the best bandwidth, up to 1MHz.
displayed or measured properly.
it is not possible to achieve meaningful $385 and they rapidly move up into
Things are even worse when it comes measurements.
the four-digit range.
to making measurements in circuits
Even if the scope does offer a difWe estimate that you should be able
connected to the 3-phase 400VAC
ferential mode, the resulting waveform to build this new design for less than
mains (415VAC with 240VAC mains).
may not be a true portrayal because the $100.
It’s true that 100:1 passive probes scope’s common mode rejection may
are available and these can be used to not be adequate when measuring high The new probe
extend a scope’s upper voltage limit to voltage circuits.
Unlike other scope probes this one
a nominal 500V/division or 5kV p-p.
The best way of solving all of these is not meant to be held in the hand but
But this type of probe does nothing to problems is to use a special probe with sits on the bench – with its insulated
solve the main problem: where do you full high voltage isolation built in, like input leads running to the circuit under
connect the probe’s earth clip?
the one we’re describing in this article. test and its output connected to one
With most modern scopes having at
By the way, we know that this type input channel of the scope via a BNCleast two input channels, there is usu- of probe is available commercially. But to-BNC cable.
ally only one way around this problem. the cheapest we could find was about
It’s housed in a small ABS instruThat’s to use two
ment box measur100:1 divider probes,
ing 150mm long,
one for each input
80mm wide and
channel, and re- An isolating high voltage probe for oscilloscopes, providing three voltage division ranges.
30mm high.
÷500 (optionally, ÷200), ÷100, ÷10
move the earth lead Division ranges:
All of the probe’s
2.0M|| ~10pF
and clip from both Input resistance:
circuitry, including
probes.
the two 9V alkaline
Linearity:
±0.05%
Then the two Bandwidth (see Fig.3):
batteries it uses for
10:1 range: DC to 500kHz (±0.5dB)
channels are used in
power, is housed
100:1 range: DC to 1MHz (±1dB)
differential mode, to
inside the box.
500:1 range: DC to 900kHz (+0.2,-1dB)
display and measure
The input leads
Residual noise:
typically 1.4mV RMS, 2.5mV peak-to-peak
the voltage differplug into insulated
Input-output isolation resistance:
>10G (500V)
ence between the
“banana” sockets
two tips. But unless Maximum working isolation voltage: 1.4kV peak (1kV RMS)
at one end of the
2.1kV peak (60 seconds)
the scope provides a Isolation test voltage:
box, while the BNC
8kV peak (10 seconds)
differential (subtrac- Maximum transient I/O voltage:
output connector
2 x 9V alkaline batteries
tion) mode (Ch1-Ch2 Power supply:
emerges from the
6.0mA from battery 1, 1.0mA from battery 2
or Ch2-Ch1) display, Typical operating current drain:
other end.
Specifications
siliconchip.com.au
January 2015 27
On the top of the
output photodiode.
Vcc1
Vcc2
box are the two main
The close matchcontrols: a small
ing of the two phoLINEAR ANALOG
OPTOCOUPLER
rocker switch to turn
todiodes means that
the probe’s power on
when the LED is
V
IC1
l
and off and a rotary
passing a current IF
switch used to select
and emitting radiaI
one of three volttion to both photoI
I
IC2
age division ranges:
diodes, the current
V
÷500, ÷100 and ÷10.
IPD1 passed by the
R2
R1
The important
feedback photopoint to grasp is
diode will have a
OUTPUT CIRCUIT
INPUT CIRCUIT
that inside the box,
value very close
GROUND
GROUND
there’s a high voltage
to that of the curFig.1: the simplified probe circuit. Op amp IC1 drives an LED in the opto“galvanic isolation coupler with feedback from one of the photodiodes. IC2 generates the output rent IPD2 passed by
barrier” between the signal from an identical, isolated photodiode. Note that I
the isolated outPD1 ≈ IPD2.
input and output
put photodiode.
circuitry.
By passing current
This allows the input leads to be optocoupler), the other is located back IPD1 through resistor R1 to produce
connected to circuits operating at many on the same side as the LED itself.
a voltage proportional to the LED
hundreds of volts above (or below)
This allows the second photodi- current IF, we can use the resulting
earth, despite the fact that the probe’s ode to be used to provide linearising voltage to provide input amplifier IC1
output is directly connected to the feedback, as a “proxy” for the isolated with negative feedback. This linearises
earthed input of a scope – and without
causing any distress or damage.
10pF
In fact the isolation barrier inside
+
1.5kV
CON1
the probe is able to withstand a peak
K
62k
620k
620k
560k
D1
“working” voltage of 1414V, or 2100V
100nF
1N5711
for up to one minute (60 second), or
62k
500V
500V
500V
A
Q1
as high as 8000V peak for transients
0.5W 0.5W 0.5W
INPUT
8
BC549
3
÷10 RANGE
10pF
of less than 10 seconds in duration.
100pF
56k
B
1
S1a
IC1a
150V
÷100
2
And if you’re curious about the isola500V
tion resistance between the inputs and
INPUT
4.7pF
330W
SOCKETS
220pF
1nF
÷500
16k
the output, this is more than 10G(10
K
(÷200)
(1nF)
(10k)
IC1: LM6132BIN
Gigaohms or 10,000M).
D2
F
PD1
FEEDBACK PIN
PHOTODIODE
I S O L AT I O N B A R R I E R
AlGaAs LED
IN
ISOLATED PIN
PHOTODIODE
PD2
OUT
28 Silicon Chip
E
1N5711
How it works
The probe achieves this impressive
performance because of a very special
component: a high linearity analog
optocoupler.
Understanding what this is and how
it works is the key to understanding
how the probe works as a whole, as
we’ll see shortly.
For the present, though, refer to Fig.1
which shows a basic linear analog
isolation amplifier based on one of
these devices.
The linear analog optocoupler is
like a conventional digital optocoupler
except that it has two PIN photodiodes
sensing the infrared (IR) radiation emitted by the high performance AlGaAs
LED. The two photodiodes are very
closely matched in terms of their optical sensitivity and linearity.
The only difference between these
”identical twin” photodiodes is that
while one of them is located on the
far side of the device’s internal voltaic
isolation barrier (like the output photodiode or transistor in a conventional
C
2.0k
(1nF)
4.7nF
(1nF)
(10k)
2.0k
(link)
CON2
A
USE VALUES IN BLUE
FOR 200:1 MAXIMUM
DIVISION RATIO OMIT EXTRA
CAPACITOR FOR 500:1
INPUT AMPLIFIER/BUFFER
200k
IC1, IC2
BC549
B
E
C
= INPUT SIDE GROUND
4
8
1
D1-D4
A
K
ON/OFF
S2a
MAXIMUM INPUT VOLTAGES
(DC + AC, CON1 TO CON2)
FOR THE THREE INPUT RANGES
RANGE
MAXIMUM VOLTS
÷10
80Vp-p (28V RMS)
÷100
800Vp-p (280V RMS)
÷200
±800V peak (560V RMS)
÷500
±1414V peak (1000V RMS)*
*SET BY THE WORKING ISOLATION
VOLTAGE RATINGS OF OPTO1 & S2
SC
Ó2015
10k
INPUT
HALF-SUPPLY
BUFFER
5
6
9V
BATTERY1
100mF
16V
D3
1N4004
6
4
100nF
7
IC1b
10k
150W
100mF
16V
ISOLATING HIGH VOLTAGE PROBE FOR SCOPES
siliconchip.com.au
the operation of the input circuitry in
converting input voltage VIN into LED
current IF and hence the IR radiation
passing over the isolation barrier.
Since the output photodiode’s current IPD2 is virtually the same as IPD1,
we are then able to use resistor R2 to
convert this current back into a voltage
VOUT which is also directly proportional to VIN.
(IC2 is then used to buffer VOUT, to
ensure that any load connected to the
output does not upset this linearity.)
In fact the resulting linear relationship between VOUT and VIN turns out
to be very close to the ratio of R2 to
R1, multiplied by the optocoupler’s
“transfer gain” K3 (where K3 = IPD2/
IPD1). So
+3
500:1
10:1
-1
0
-2
-3
90
-4
-5
180
-6
-7
270
-8
-9
50 100 200
500 1k
(ISOLATION BARRIER)
100nF
56k
FEEDBACK PIN
PHOTODIODE
6
4
l
2
1
IR LED
TO SCOPE
INPUT
5
8
3
ISOLATED PIN
PHOTODIODE
1nF
(ISOLATION BARRIER)
IC2: TLV2372IP
V1
LED1
BLUE
OUTPUT BUFFER
A
l
V2
V2+
OUTPUT
HALF-SUPPLY
BUFFER
(ISOLATION BARRIER)
10k
5
OFFSET VR2
ADJUST 2k
9V
BATTERY2
V1
6
10k
100mF
16V
IC3b
IC
2b
4
100nF
100mF
16V
D4
1N4004
100mF
16V
7
150W
V2
Fig.2: the complete probe circuit. The voltage being monitored is attenuated
by a resistor/capacitor ladder and the selected tap connects to input pin 3 of
IC1 via rotary switch S1. IC1b and IC2b provide half-supply rails to allow
signals with bidirectional voltage swings to be probed.
siliconchip.com.au
360
50k 100k 200k 500k 1M
A = VOUT / VIN = (R2/R1)
It also turns out that we can compensate for any small deviation of the
optocoupler’s K3 away from unity,
simply by “tweaking” the value of R2.
So the overall gain of the isolation
amplifier can be adjusted to be exactly
unity, or whatever other figure we want
it to be. So we achieve linear analog
voltage gain while at the same time
passing over a high voltage isolation
barrier.
Performance
= OUTPUT SIDE GROUND
K
S2b
V1+
100mF
16V
VR1
50k
GAIN
CALIBRATE
CON3
100W
1
IC2a
2
180k
5k 10k 20k
linear analog optocouplers have a
transfer gain K3 of very close to unity
(1.0); within a few percent.
So the overall gain of the basic linear
isolation amplifier of Fig.1 simplifies
down to:
V2+
OPTO1
IC2 HCNR201
HCNR201
LINEAR
OPTOISOLATOR
2k
Frequency (Hz)
Fig.3: frequency response of the probe for each attenuation setting. The response
is flattest at 500:1 but there is slightly more bandwidth at 100:1. The output/
input signal phase shift for each setting is shown dashed, using the right y-axis.
Because of the close matching between their twin photodiodes, most
3
0
-10
10 20
VOUT/VIN = K3.(R2/R1)
V1+
100:1
+1
Phase Shift (Degrees)
Output/Input Relative Amplitude (db)
+2
We tested our prototype by measuring signals under a number of different
circumstances. The ‘litmus test’ was
connecting the probe across the motor
of a drill plugged into our 230V/10A
Speed Controller For Universal Motors
(February-March 2014).
The result is shown in Scope1. This
is gratifying as it gives a clear picture
of the voltage across the load, despite
the fact that it’s floating at mains potential and with the fast rise/fall times
displayed correctly. In fact, this result
is almost identical to what we get with
a commercial differential probe.
With its ~1MHz bandwidth, our
probe can be used to view signals with
a higher switching frequency than this.
For example, it could be used to view
January 2015 29
the probe to unity.
At the probe’s front-end circuitry,
the 200k resistor connected between
pin 2 of IC1a and the input circuit’s
negative rail is the equivalent of feedback resistor R1 in Fig.1.
As you can see the anode of OPTO1’s
feedback photodiode (pin 4) also connects to the 200kresistor, as in Fig.1.
Note that the value of the 330
current-limiting resistor is important
since its ratio with the 200kresistor
sets the current gain of the optocoupler and this affects the open-loop
bandwidth of the surrounding circuit
(ie, including IC1a). Increasing this resistor value reduces output overshoot
but also reduces overall bandwidth.
The 4.7pF capacitor also has an
effect on bandwidth (in combination
with the 330resistor) and is required
for the circuit to be stable, due to the
phase shift inherent in the DC feedback
path via the opto-coupler.
Scope1: the voltage across a drill powered by our 230V/10A Speed Controller for
Universal Motors, showing a rectified mains waveform chopped at about 1kHz.
The spikes are generated by the circuit; they are not measurement artefacts.
a floating Mosfet gate drive.
We did try it out connected across
the output of our Induction Motor
Speed Controller (April/May 2012)
which has a much higher switching
frequency, 36kHz.
While we were able to get a reasonable picture of the output waveform
(Scope3 shows it “zoomed out”), the
bandwidth of our probe is a little too
low to show the very short pulses as a
square wave. The voltage rise and fall
times are simply too fast.
The output photodiode of OPTO1 is
connected to the non-inverting input
(pin 3) of output amplifier IC2a, in
exactly the same way as in Fig.1. Trimpot VR1 with its series 180kresistor
takes the place of R2 in Fig.1, with
VR1 allowing the exact value of R2 to
be adjusted to set the overall gain of
Input voltage divider
The non-inverting input of IC1a
(pin 3) is connected to input connectors CON1 and CON2 via a switched
voltage divider, to provide the probe’s
three division ranges.
The switching is done by S1a, one
pole of a 4-pole, 3-position rotary
switch (the other poles are unused).
The input divider is arranged so that
it provides a fixed input resistance of
The full probe circuit
Now refer to the full circuit of Fig.2.
The specific linear analog optocoupler
device we’re using is the HCNR201,
made by US firm Avago Technologies.
This has very impressive features:
•
•
•
•
•
•
•
Low non-linearity: <0.01%
Transfer gain: 1.00 ±5%
Wide bandwidth: >1MHz
Isolation: UL 5000V RMS for one minute
Maximum working voltage: 1414V peak
I/O test voltage: 2121V peak for 60s
I/O transient over-voltage: 8000V for 10s
The IR LED of optocoupler OPTO1
is driven by op amp IC1a via transistor
Q1. The transistor is used as an emitter
follower to provide the required current drive for the optocoupler’s LED,
since IC1 is a low power device with
low current drive capability.
30 Silicon Chip
Scope2: a 1kHz scope compensation square wave as measured using the
differential probe on its 10:1 setting. There are brief overshoot spikes at each
edge but otherwise the shape is square with no ringing or distortion.
siliconchip.com.au
+
+
+
+
+
OPTO1
+
+
siliconchip.com.au
HCNR201
+
5711
/500
IC2
TLE2022
5711
4004
10k
10k
+
+
C 2014
/100
62k
150W
560k
/10
(500V 0.5W)
2Mon all three ranges.
9V BATTERY
A series of capacitors
(FOR
CIRCUITRY ON
have been connected in
(500V 0.5W)
OUTPUT SIDE OF
620k
parallel with the divider
ISOLATION BARRIER)
resistors. These are re620k
VR1
50k
S1
100mF
100mF
100mF
100mF ADJUST GAIN
RANGE
quired for a number of
+IN
–
10pF 500V
180k
reasons.
BATTERY 2
OUTPUT TO
10pF
OUTPUT
150W
SCOPE
1.5kV
D3
Firstly, they swamp the
100nF
100nF
D1
100pF
100mF
input capacitance of IC1a
S2
150V
CON3
(exacerbated by the capacIC1
OFF/ON
LM6132
62k
itance of D1 & D2), which
100nF
56k
would otherwise form a
100W
4.7pF
16k
D2
4.7nF
–IN
100nF
100mF
1nF
1nF
low-pass RC filter with the
200k
A
K
10k
220pF
2.0k
2.0k
NOTE:
NOTE:AAPIECE
PIECE
Q1
resistive divider network,
330W
LED1
BC549
OF
OF0.8mm
0.8mmTHICK
THICK
10k
VR2
2k
seriously limiting the
9V BATTERY
PRESSBOARD
PRESSBOARD
ADJUST OFFSET
SHEET
SHEET100
100xx23mm
23mm
56k
available bandwidth.
(FOR CIRCUITRY ON
(CUT
(CUT&&BENT
BENTAS
ASIN
INFIG.8)
FIG.7)ISIS
4004
INPUT SIDE OF
They also keep the AC
USED
USEDTO
TOPROVIDE
PROVIDEEXTRA
EXTRA
D4
STRAIN
ISOLATION BARRIER)
–
impedance “seen” by IC1a
ISOLATION
ISOLATIONBETWEEN
BETWEENINPUT
INPUT
BATTERY 1 RELIEF
AND
ANDOUTPUT
OUTPUTCIRCUITRY
CIRCUITRY
low, minimising noise and
RF/hum pick-up.
An extra 10pF capacitor placed across the top
620kresistor in the divider provides some extra
compensation to cancel
out the input capacitance
of IC1a.
Regarding the voltage
ratings of these components, 90% of the voltage
applied across inputs
CON1 & CON2 appears
across the top three resistors and parallel capacitor.
Given the 1414V peak
rating of the device, the
resistors must therefore
be able to handle at least
500V and the 10pF capacitor, 1.5kV. Similarly, the Fig.4 (top): the component overlay, which matches the near-same-size photo of the early proto100pF capacitor sees 9% type PCB (above). Note that the PCB is double-sided – make sure you solder the components to
of the total voltage and the correct side! S2 is not yet soldered in place in the photo but is shown in situ above.
thus must be rated for at
So each section operates from its
least 150V.
the opto-coupler just below 1MHz (ie,
Diodes D1 and D2 provide over- its roll-off point). This gives a flatter own 9V alkaline battery, with the input
section running from battery 1 and the
voltage protection for IC1a, ensuring frequency response (Fig.3).
that input pin 3 cannot swing higher
Note that we’ve also shown some output section from battery 2.
We are using op amps 1C1b and IC2b
than 0.4V above the input circuit’s alternative divider component values
positive supply rail (V1+) or lower in the circuit. If used, these change the as buffers to give each supply its own
than 0.4V below its negative rail (V1-). ÷500 range to ÷200. This results in a half-supply “reference ground”. The
This prevents IC1 from damage should better signal-to-noise ratio but with buffers are very similar, in each case
you accidentally connect the probe a more limited input voltage range using a resistive divider to establish a
battery “centre tap”, with the ICs coninputs to high voltages when switch before saturation (see table in Fig.2).
S1 is switched to the low voltage (÷10)
Note that the resulting 800V peak nected as voltage followers to provide
range.
rating is sufficient for working with the necessary current capability.
(The 150 resistors and 100µF caThe 100resistor at IC2a’s output even 3-phase mains.
pacitors are to ensure that the voltage
isolates this buffer from any cable
followers remain stable.)
capacitance or input capacitance of Power supply
In the case of the input circuitry,
the scope.
Importantly, the input and output
We’ve also added a 1nF capacitor circuits of the probe must be operated the purpose of IC1b is to establish a
to form an RC low-pass filter here, to from separate power supplies, since “reference ground” voltage level for
compensate for a peak in the frequency they are on opposite sides of the isola- the negative input connector CON2,
so that when there is no input to the
response of the circuit surrounding tion barrier.
January 2015 31
if a battery happens to be connected
backwards while S2 is on (easy enough
to do, at least briefly), the diode will
limit the voltage applied to IC1 or IC2
to no more than -1V, protecting it from
damage.
LED1 is fitted to make it harder to
forget to turn the unit off when you’ve
finished using it. As it’s a high-brightness blue LED, it only requires 100µA
to operate, so it doesn’t add much to
the battery drain during operation.
Building the probe
Scope3: the voltage across two outputs of the Induction Motor Speed Controller
with an incandescent lamp as a load. The scope performs a sort of averaging
when zoomed out like this, revealing the PWM-modulated sinewave shape.
probe the non-inverting input of IC1a
is biased midway between the V1+ and
V1– rails. This allows the input circuit
to operate the IR LED inside OPTO1
at close to “half brightness”, while
also allowing IC1a to cope with the
maximum possible AC voltage swing.
On the output side, IC2b is again
there to provide a half-supply reference ground, for the output connector
CON3. And by making the exact reference voltage variable using trimpot
VR2, we allow cancelling of any output
offset voltage that might be caused by
differences between the photodiodes
inside OPTO1 at the quiescent current level.
9
Although the two supplies are on
opposite sides of the probe’s isolation
barrier, we switch them on and off in
tandem using S2a and S2b, the two
poles of a 250VAC-rated rocker switch.
Typical mains-rated switches of
this type are rated to withstand 1000V
RMS, which just happens to be exactly
what OPTO1 is able to withstand.
To be safe, we’ve added some extra
insulation between the leads connecting to the switch (as we’ll explain
soon).
Diodes D3 and D4 are connected to
the switch such that the are reversebiased normally and thus do not
affect circuit performance at all. But
(SIDE VIEW)
TIN THESE ENDS
ONLY
As mentioned earlier, all of the components and circuitry of the probe are
built into a small ABS instrument case
measuring 150 x 80 x 30mm.
In fact everything except the two 9V
batteries, on/off switch S2 and input
jacks CON1 and CON2 is mounted on
a single PCB measuring 122 x 70mm
and coded 04108141. The board has
cutouts on each side to provide spaces
for the two 9V batteries, as you can
see from the overlay diagram of Fig.4.
On/off switch S2 mounts on the
top of the case on the centre line and
about 1/3 of the distance up from the
output end, with short insulated and
splayed leads connecting its lugs to
the matching pads on the PCB.
The two insulated input jacks CON1
and CON2 mount in the input end
panel of the case with their connection lugs wired to the matching pads
on that end of the PCB.
Output BNC connector CON3 is
mounted directly onto the PCB at the
centre of the output end, with trimpots
VR1 and VR2 spaced equally on either
side. The trimpots are then easily
adjusted using a small screwdriver
or alignment tool, through matching
holes in that end of the case.
(END VIEW)
(END VIEW)
WHITE DOT
MAKE SOLDER
JOINTS SMALL
AND SMOOTH
HEATSHRINK
SLEEVES
11.5
1
CUT 4 x 50mm LONG PIECES OF
HOOKUP WIRE, STRIPPING INSULATION
4mm FROM ONE END & 37mm FROM
THE OTHER END & LEAVING 9mm OF
INSULATION ON EACH WIRE. TIN THE
SHORT BARED ENDS OF ALL FOUR WIRES
2
IDENTIFY THE SWITCH
LUGS TO WHICH THE
WIRES WILL BE SOLDERED,
ON BOTH SIDES OF
THE SWITCH
3
SOLDER THE SHORT END OF EACH
WIRE TO A SWITCH LUG, MAKING
EACH JOINT SMALL & SMOOTH. THEN
SPLAY EACH PAIR OF LEADS OUTWARDS
TO SPACE THEM 11.5mm APART
Fig.5: follow these steps in soldering leads to, then securing, S2 to the PCB.
32 Silicon Chip
4
CUT 4 x 11mm LONG PIECES OF 3mm
DIAMETER HEATSHRINK TUBING AND
SLIP OVER EACH WIRE & SWITCH LUG.
THEN SHRINK THEM IN TIGHTLY USING
A HOT AIR GUN OR THE SHANK OF
A SOLDERING IRON.
siliconchip.com.au
To wire up the probe PCB, fit the
components in the usual order: first the
resistors (including VR1 & VR2), followed by the four diodes, the smaller
capacitors and the six 100F electrolytics – taking care to fit the diodes and
electrolytics with the correct polarity.
Take care not to get the two types of
diode mixed up.
Next, mount transistor Q1, followed
by the range switch S1, after cutting
its spindle at a distance of 12mm from
the end of the threaded ferrule. Then
fit the switch to the PCB, taking care
to use the orientation shown in Fig.4.
Next fit IC1 and IC2, again making
sure you orientate each one as shown.
The next component to be added to
the PCB is the HCNR201 linear analog
optocoupler (OPTO1).
Although it comes in an 8-pin DIL
package, it has wider pin spacing than
usual: 0.4” (10.16mm) rather than 0.3”
or 7.62mm. It’s fitted to the PCB with
the “notch” end towards the top.
After this fit BNC output connector
CON3 at the right centre of the PCB,
midway between trimpots VR1 and
VR2, followed by the four PCB terminal pins used to make the connections
between the two battery snap leads
and the PCB.
Two of these pins are soldered into
the pads just below the cutout for Battery 1 at upper left, while the other
two go just to the left of the cutout at
lower right, for Battery 2. You can see
these quite clearly in Fig.4.
Mount LED1 with the bottom of its
lens 20mm from the top of the PCB.
This will be with virtually the full
lead length.
Finally, cut the two battery snap
leads themselves to about 45-50mm
long (measured from the snap) and
strip back about 5mm of the insulation
from the wire ends.
Thread the wires through the stress
relief holes provided on the PCB and
solder them to the terminal pins, again
as shown in Fig.4.
Your probe PCB assembly should
now be complete, and can be placed
aside while you prepare the box.
Preparing the box
There are no holes to be drilled in
the bottom half of the case. All of the
holes are drilled and/or reamed in the
top half and in the two removable end
panels. But as there are only nine holes
in all, this shouldn’t be a problem. The
size and location of all of the holes are
siliconchip.com.au
Parts List – Isolating High Voltage Probe
for Oscilloscopes
1 PCB, code 04108141, 70 x 122mm
1 ABS instrument box, 150 x 80 x 30mm [Jaycar HB-6034]
1 4-pole 3-position rotary switch, (S1)
1 knob to suit S1, <25mm diameter
1 DPDT, 250VAC-rated rocker switch, single hole mounting (S2) [Jaycar SK-0994]
2 banana sockets, fully insulated, 1 red, 1 black (CON1, CON2)
1 PCB-BNC socket (CON3)
1 6mm long untapped spacer
1 15mm long M3 tapped Nylon spacer
1 15mm long M3 Nylon machine screw (cut from a 25mm long screw)
1 6mm long M3 machine screw
2 16.5mm long untapped spacers (cut from 25mm long spacers)
2 25mm long 6G or 7G countersunk self tapping screws
4 3.5mm ID flat washers
2 9V alkaline batteries
2 battery snap leads to suit
4 PCB terminal pins
1 100 x 26mm piece of 0.8mm Pressboard or Presspahn/Elephantide sheet
Semiconductors
1 LM6132AIN/BIN dual high speed op amp (IC1) [element14 order code 9493980]
1 TLE2022CPE4 dual low current op amp (IC2) [element14 order code 1234686]
1 HCNR201-050E high speed linear optocoupler (OPTO1) [Digi-Key 516-2379-5-ND]
1 BC549 NPN transistor (Q1)
1 3mm blue LED (LED1)
2 1N5711 Schottky diodes (D1,D2)
2 1N4004 1A diodes (D3,D4)
Capacitors
Changes for 200:1 option:
6 100F 10V/16V PC electrolytic
• Delete 220pF & 4.7nF ceramic
4 100nF multilayer monolithic ceramic
capacitors
1 4.7nF 50V disc ceramic
• Add three more 1nF ceramic capacitors
2 1nF 50V disc ceramic
• Delete 16k& two 2kresistors
1 220pF 50V disc ceramic
• Add two more 10kresistors
1 100pF 150V* disc ceramic
2 10pF 1.5kV* disc ceramic
1 4.7pF C0G/NP0 disc ceramic
* 7.62mm lead spacing; 3kV types suitable
Resistors (1% metal film 1/4W unless specified)
2 620k500V 1% 1/2W
1 560k500V 1% 1/2W (eg, Vishay HVR37)
1 200k 1 180k 2 62k 2 56k 1 16k
4 10k 2 2.0k 1 330 2 150 1 100
1 50kmulti-turn horizontal adjustable trimpot (VR1)
1 2kmulti-turn horizontal adjustable trimpot (VR2)
shown in a drilling guide PDF which
can be downloaded from siliconchip.
com.au
After drilling the smaller holes and
reaming the larger holes to size, use a
jeweller’s file or a sharp hobby knife to
remove any burrs left around each hole
on both the inside and the outside.
To make a “dress” front panel for
the probe you can make a photocopy
of our artwork in Fig.8 (or download
it from siliconchip.com.au) and then
laminate it in a plastic sleeve for protection. After this it can be trimmed
to size and attached to the top of the
case using double-sided adhesive tape.
Then cut holes in the dress panel for
fitting the top PCB mounting screw, S2
and the control spindle for S1, using a
sharp hobby knife and guided by the
holes you have already cut and reamed
in the case underneath.
Making the isolation barrier
Before you begin fitting everything
into the case, you need to prepare the
isolation barrier which will provide
additional isolation between the input
and output circuitry and their batteries.
The barrier is cut from a 100 x 26mm
January 2015 33
15mm LONG M3 NYLON SCREW
(CUT FROM ONE 25mm LONG)
EPOXY FILLET
6mm LONG
UNTAPPED
SPACER
PRESSBOARD
ISOLATION
BARRIER
S2
OFF/ON
LED1
EPOXY FILLET
220p
15mm LONG M3
TAPPED NYLON SPACER
RANGE
Q1
BC548
S1
4.7nF
9V BATTERY
BATTERY 2
IC2
6mm LONG M3 SCREW
OUTPUT TO
SCOPE
+
IC1
CON1
16.5mm LONG UNTAPPED SPACERS
(CUT FROM 25mm LONG)
IC3
25mm LONG 6G CSK HEAD SELF TAPPING SCREWS
(BOTTOM OF BOX)
CON3
4004
2x 3.5mm ID FLAT
WASHERS ON EACH SCREW
CUT OFF THESE
SPACERS
Fig.6: how it all fits into the case, as if looking through the side. Opposite is a photo of the completed unit.
rectangle of 0.8mm thick pressboard
sheet (similar to Presspahn Elephantide), using the upper diagram of Fig.7
as a guide, and then bent up as shown
in the lower diagram.
Preparing S2
The next step is to prepare on/off
switch S2 by fitting it with the four
well-insulated wires which will connect it to the PCB. As you can see from
Fig 5.1 this needs four 50mm lengths
of insulated wire, each with the insulation stripped by 4mm from one end
but 37mm from the other end. (The
long bared ends are to make assembly
easier later.)
We are using the two centre lugs and
those at the ends opposite to the white
dot on the red rocker actuator at the top
of S2, as shown on the left in Fig 5.2.
After soldering the short ends of the
four wires to these switch lugs, each
pair of wires is splayed away from the
other pair as shown Fig 5.3, so that the
pairs are spaced about 11.5mm apart.
Then cut four 11mm-long lengths of
3mm diameter heatshrink tubing, and
push each of these sleeves up one of
the wires as far as it will go – that is,
over the switch lug and the solder joint
and until its top end is hard against the
rear of the switch body (see Fig 5.4).
After this use a hot air gun or the
hot shank of your soldering iron to
shrink each of the sleeves firmly into
position around the wires and switch
lugs. Then your “S2 switch assembly”
should be complete, and ready to be
fitted into place in the 18mm hole on
the top of the case.
This is done by unscrewing the large
plastic nut, and then passing the switch
and its splayed wires down into the
box via the 18mm hole. Then screw
34 Silicon Chip
the nut back on again inside the box,
to hold it in position.
But before you tighten the nut completely, make sure that the switch is
positioned so that the white dot on its
rocker actuator is positioned on the
right, directly in line with the “ON”
label of the dress front panel.
Next, cut the two 25mm untapped
spacers down to a length of 16.5mm,
using a jeweller’s saw and smoothe off
the cut ends using a small file.
Then fasten them temporarily to the
two mounting spacers moulded into
the inside of the top of the case (at the
output end), using the two 25mm long
countersink-head self tapping screws
with about five or six small flat washers under each screw head as packing,
so the screws don’t enter the moulded
spacers very far – just enough to hold
the 16.5mm spacers in place.
Then pass a 15mm long Nylon M3
screw (cut from a 25mm long screw)
down through the central hole near
the input end of the case front panel,
slip the 6mm untapped spacer up over
the end of the screw and fit an M3
nut – screwing it up to hold the 6mm
spacer firmly against the underside of
the front panel.
You should now be almost ready to
apply a fillet of epoxy cement around
the top end of each of the three spacers,
to hold them in place securely.
But there’s one more thing to do first:
fit the Pressboard isolation barrier into
the top half of the case. Its 26mm-high
“L section” should be over on the side
ready to slip into the cutout for battery
2, with the 20mm-high section with
its cutouts for S2 and OPTO1 passing “east-west” and aligned centrally
between the contacts at the rear of S2.
Once you’re happy that it’s in the
correct position, it can be secured
there using a few small dabs of epoxy
adhesive between the barrier and the
inside of the case top.
Then while you have the epoxy cement mixed up, cement the spacers to
the case top as well.
When the cement has had time to
cure, you can unscrew both of the
Resistor Colour Codes
p
p
p
p
p
p
p
p
p
p
p
p
No. Value
2 620k
1 560k
1 200k
1 180k
2 62k
2 56k
1 16k
4 10k
2 2.0k
1 330
2 150
1 100
4-Band Code(1%)
blue red yellow brown
green blue yellow brown
red black yellow brown
brown grey yellow brown
blue red orange brown
green blue orange brown
brown blue orange brown
brown black orange brown
red black red brown
orange orange brown brown
brown green brown brown
brown black brown brown
5-Band Code (1%)
blue red black orange brown
green blue black orange brown
red black black orange brown
brown grey black orange brown
blue red black red brown
green blue black red brown
brown blue black red brown
brown black black red brown
red black black brown brown
orange orange black black brown
brown green black black brown
brown black black black brown
siliconchip.com.au
Take note of the order of assembly in the text, especially the Presspahn isolation barrier (arrowed) which wraps around
the lower battery and sits across the middle of the PCB, as indicated by the red dotted line. This is all necessary to ensure
good isolation between the battery and PCB and between the two poles of the power switch.
The next step is to attach the 15mm
long M3 tapped spacer to the PCB (at
top centre), using a 6mm long M3 screw
passing up from underneath. It’s a good
idea to tighten this screw firmly (but
not TOO firmly) using a screwdriver,
with the spacer held by a small spanner
or nut driver.
After this, mount the two input
connectors CON1 and CON2 into the
input end panel of the case, with the
red one on the right as viewed from
behind the panel. Tighten their nuts to
secure them in place, and then solder
a short length of tinned copper wire to
the rear lug of each connector.
Capacitor Codes
Value
μF
value
100nF 0.1μF
4.7nF
NA
1.0nF
NA
220pF
NA
100pF
NA
10pF NA
4.7pF NA
siliconchip.com.au
IEC
code
100n
4n7
1n
220p
100p
10p
4.7p
EIA
code
104
472
102
221
101
10
4p7
threaded ferrule of rotary switch S1
passes up through its matching hole
in the top of the case.
When the assembly can’t be pushed
in any further, you should be able to
secure it all together by screwing the
two self-tapping screws back into
the matching holes of the mounting
spacers moulded into that end of the
case top, and also by passing the 15mm
long Nylon screw down through the
matching hole in the centre of the input
end of the case top, so it passes down
through the 6mm untapped spacer and
can then be screwed into the top of the
15mm long M3 tapped spacer.
If you found this description somewhat confusing, try looking at Fig.6.
This shows what you’ll be working
towards.
When the PCB assembly is secured
28
12
18
20
4.5
12
11
12
17.5
(FOLD UP BY 90°)
Final assembly
Then, with the centre axis of the
two connectors positioned about 6mm
above the top end of the PCB, solder
each wire to its matching pad on the
PCB. These pads are provided with
a centre hole, so you can pass each
wire down through the hole before
soldering.
Next, fit the output end panel of the
case over the shank of CON3, after
removing its nut. Then screw the nut
back on again, to complete the PCBand-end panels assembly.
By now you should be ready to fit
this completed board assembly up into
the top half of the case, by introducing
it so that each of the two end panels
slips into the matching slots in the ends
of the case half, the four wires from
S2 pass down through their matching
holes in the PCB and the shaft and
(FOLD DOWN BY 90°)
25mm long self-tappers and remove all
but two of the washers on each, ready
to secure the PCB shortly.
At the same time you can unscrew
the 15mm M3 screw and its nut holding
the 6mm spacer in place, and you’ll be
ready for final assembly.
30.5
26
17
100
MATERIAL: 0.8mm THICK PRESSBOARD/PRESSPAHN ELEPHANTIDE SHEET
ALL DIMENSIONS IN MILLIMETRES
Fig.7: here’s how to cut and
fold the sheet of insulation
material. It forms a physical
barrier between the input and
output sides.
January 2015 35
in place as shown in Fig.6, you’ll be able to fit switch S1’s
spindle with its control knob. Of course you’ll also need
to solder the wires from S2 to their pads on the PCB, after
which you can cut off their excess lengths.
All that remains now is to attach each 9V battery to its
snap connector, and then lower it into its waiting “slot” at
the side of the PCB.
The final assembly step is to fit the bottom of the case
and fasten it in place with the four 20mm long countersink
head M3 screws supplied with it. However just before you
do this, you’ll need to cut off the two PCB mounting spacers
moulded into the bottom of the case at the output end.
This is because if left in situ, they’ll interfere with the
heads of the mounting screws on the underside of the PCB.
It’s not hard to cut off these spacers with a pair of sharp
side cutters.
After these “minor trimming” jobs, you should find that
the bottom of the case will mesh nicely with the PCB-andtop assembly, allowing you to fit the four screws holding
it all together.
MAXIMUM INPUT VOLTAGES
FOR THE THREE INPUT RANGES
Set-up & calibration
/500
1414Vp-p (500V RMS)
/100
800Vp-p (280V RMS)
/10
80Vp-p (28V RMS)
There isn’t much involved in setting up and calibrating
the probe.
The first step is to connect a DMM (set to read DC volts,
on its 2V range) to the probe’s output connector CON3 using
a cable ending in a BNC plug. Now turn range switch S1
to the “/500” position, and also plug two input leads into
CON1 and CON2. Connect their far ends together to make
sure the probe definitely has “zero input”.
Next turn on the probe’s power switch S2, and you’ll
probably see the DMM reading move to a value slightly
above or below 0V. The idea now is to adjust trimpot VR2
(Offset Adjust) in one direction or the other with a small
screwdriver or alignment tool, to bring the reading as close
as possible to 0V.
This is the initial setting for VR2. However, it may have to
be readjusted by a small amount after you have performed
the second step – calibration.
To calibrate the probe, the simplest approach is as follows. First connect its output (at CON3) to an input of your
scope or DSO, using a reasonably short BNC-to-BNC cable.
You can adjust the scope’s input sensitivity to, say, 1V
per division and if it has a switch or option for setting its
calibration to allow for a probe’s division ratio, set this to
the 10:1 position. (This should change the effective input
sensitivity to 10V/division.)
Next turn the probe’s range switch S1 to the /10 position
(fully clockwise) and connect the probe’s input leads to a
source of moderately low voltage AC.
This can be from an audio generator set to provide a sinewave at about 1kHz with an output level of say 10V RMS
(= 28.8Vp-p) or a square wave or function generator set to
provide a square wave of again 1kHz at about 20 - 25Vp-p.
Or if you don’t have access to either kind of generator,
you could use a step-down transformer with a known (ie,
measured) secondary voltage of around 12-15V RMS (=
34 – 42.4Vp-p).
When you now turn on the probe’s on/off switch (S2),
you should see the waveform from your signal source on
the scope’s display. Its frequency and amplitude should
also be displayed if your scope has this facility built in, as
most do nowadays.
36 Silicon Chip
–
INPUTS
+
DIVISION FACTOR
/100
/500
/10
ON
OFF
POWER
ISOLATING HIGH
SILICON VOLTAGE
PROBE
CHIP
FOR OSCILLOSCOPES
OFFSET
ADJUST
OUTPUT
TO SCOPE
GAIN
CALIBRATE
Fig 8: same size front panel artwork – photocopy
this (or download it from siliconchip.com.au) and
glue it to your box before inserting S2.
Now the odds are that while the frequency reading will
be correct (either 1kHz or 50Hz as the case may be), the
amplitude reading will probably be a little higher or lower
than the known level of the signal being fed into the probe.
So what’s needed now is to adjust the probe’s “Gain
Calibrate” trimpot VR1 in one direction or the other using
a small screwdriver or alignment tool, to bring the reading
as close as possible to the correct value.
After doing this calibration step, it’s a good idea to go back
and repeat the first “Offset Adjust” step – especially if you
had to turn VR1 quite a few turns to achieve calibration.
This is done quite easily, simply by removing the probe’s
input leads from your source of AC and connecting them
together. Then after turning the range switch to “/500”, you
can reconnect the probe’s output to your DMM and check
what reading you get.
If it has moved slightly away from the “0V” mark, it’s
simply a matter of adjusting trimpot VR2 to bring it back
again. Then your probe will be set up, calibrated and ready
for use.
SC
siliconchip.com.au
High-Energy
Multi-Spark CDI For
Performance Cars
Pt.2: By JOHN CLARKE
Six Versions To
Suit Your Car’s
Trigger Source
In Pt.1 last month, we introduced our new High-Energy MultiSpark CDI and described its operation. In this article, we give the
assembly details for six different versions to suit your car’s trigger
source and describe the installation.
T
HE ASSEMBLY of the Multi-Spark
CDI is straightforward, with all
parts installed on a double-sided PCB
coded 05112141 (110.5 x 85mm). This
PCB can be obtained either as part of a
complete kit (ie, from parts retailers)
or can be purchased from the SILICON
CHIP Online Shop.
Fig.5 and Figs.6(a)-6(e) show the
38 Silicon Chip
parts layouts to suit different ignition
pick-up versions. It’s simply a matter
of building the version to suit the ignition pick-up in your car.
The first step is to install surface
mount chips IC1, IC2 & IC3. These are
in SOIC packages, so they are not that
difficult to solder in place due to their
relatively wide 0.05-inch pin spacing.
Each IC is mounted on the top of the
PCB and must be orientated as shown
on Fig.5.
Note that pin 1 is difficult to discern
on IC3. However, if you look at the end
profile of the IC, there will be a chamfer
down one edge. This side has pins 1-4.
To solder an IC in place, you will
need a soldering iron with a fine tip
siliconchip.com.au
+
10Ω
TC4427
1 µF MMC
(SEC.)
4007
4007
D2-D5
TO
CHASSIS
EYELET
680k
Low ESR
MULTISPARK CDI
Q4
1 µF X2
C1 = 470nF FOR 8 CYLINDERS; 150nF FOR 6 CYLINDERS; 120nF FOR 4 CYLINDERS
–
+ Coil -
C 2014
Q3
Chassis
100 µF
MOV1
180k
4148
*
100nF X2
680k
22Ω
IC3
4007
22Ω
33k 1W
L6571
100 µF
180k
D9
2.2k
D6
1
4.7nF
C1
4007
S1
4007
10Ω
100 µF
T1
13k
56k
BC337
33k 1W
33k
4148
Tacho
10k
S2
14121150
47k
5.1V
ZD3
10k
GND
BC337
S1
F1
Q7
Q5 D8
+12V
100nF X2
F1
BC337
10k
Q6
F2
100k 100k
2 .2 nF
FOR NO
MULTISPARK
= 15nF
*C1
out
270k
ZD2
10k
1k
470pF
+12V
10k
TP1
VR1
270k
VR2
IC2
1
75V
10k
150Ω
4148
+5V R,K H+,A TRIG.
10k
150Ω
D7
10k
TO
TACHO
47k
1nF
3x
100nF
TO
RELUCTOR
COIL
10 µF
10k
1 µF MMC
1
1M
4700 µF
Q2
ZD1
16V
IC1 TL494
1M
1M
47k
4.7k
4004
8.2k
Q1
10Ω
4.7k
D1
TO COIL
+
WARNING: COIL OUTPUT
OPERATES AT HIGH VOLTAGE
Fig.5: follow this PCB layout diagram if your car’s distributor has a reluctor pick-up. Be sure to install the three SMD
ICs (IC1-IC3) first and note that capacitor C1 must be chosen to suit the number of engine cylinders. Alternatively,
leave out C1 and change the adjacent 4.7nF capacitor to 15nF if you wish to disable the multi-spark feature.
and some “no-clean” flux paste. Begin
by carefully placing the IC on top of its
pads, ensuring that its orientation and
alignment are correct. That done, place
a dab of flux paste on one of the corner
pins, then put a little solder on the tip
of your soldering iron and touch the
pin gently, without disturbing the IC.
The flux paste should help “suck” the
solder onto that pin and pad.
Now check the IC’s alignment. If it’s
out, reheat the joint and gently nudge
it into place. Once the alignment is
good, use the same technique to solder
the diagonally-opposite pin.
It’s then just a matter of soldering
the remaining IC pins and cleaning up
any bridges using solder wick. Refresh
the joints on the first two pins you soldered, too. Adding no-clean flux paste
is recommended for both procedures;
when soldering the pins, it reduces
the chance of bad joints.
Finally, clean off any excess flux
using an appropriate solvent (metho
will do in a pinch) and check the
joints under magnification to ensure
that solder has flowed properly onto
every pin and pad.
Once the ICs are in place, the
through-hole parts can be installed,
starting with the resistors, diodes
and zener diodes. Table 1 shows the
resistor colour codes but you should
siliconchip.com.au
also check each one with a multimeter
before fitting it to the PCB.
Be sure to orientate the diodes and
zener diodes as shown on Figs.5 &
6. The zener diode type numbers are
shown in the parts list.
Mosfets Q1-Q4 are next on the list.
These must all be installed so that the
tops of their metal tabs are 20-25mm
above the PCB. The easiest way to do
that is to first loosely fit all the devices
in place, then rest the board upside
down on 20-25mm-high supports (one
at either end). The Mosfet devices can
then be pushed down so that their tabs
rest against the bench-top and their
leads soldered.
Once these parts are in, you can
install the capacitors. Note that the
electrolytic types must be orientated
with the correct polarity (ie, negative lead towards the top edge of the
PCB in each case). Note also that the
4700µF and 100µF capacitors must be
low-ESR types.
Multi-turn trimpot VR1 can now
go be fitted. It goes in with its screw
adjustment end towards the bottom
edge of the PCB (ie towards Q7).
Transformer winding
Fig.7 shows the transformer details.
It’s made up by first installing three
windings on an ETD29 13-pin bobbin:
a 240-turn secondary winding and
two primary windings. The bobbin is
then fitted to two N87 ferrite cores to
complete the assembly.
The secondary winding goes on
first and is wound using 240 turns of
0.25mm-diameter enamelled copper
wire (ECW), about 20m long. The first
step is to scrape away about 10mm of
the insulation from one end using a
sharp hobby knife. This end is then
soldered to pin 10 (S1) on the 7-pin
Warning – High Voltage!
This circuit produces an output voltage of up to 300V DC to drive the
coil primary and is capable of delivering a severe (or even fatal) electric
shock. DO NOT TOUCH any part of the circuit or the output leads to the
coil from CON2 while power is applied.
To ensure safety, the PCB assembly must be housed in the recommended
diecast case. This case also provides the necessary heatsinking for the
four Mosfets.
January 2015 39
75V
270k
ZD2
270k
1k
33k 1W
33k 1W
5.1V
180k
4148
4148
4148
D9
D7
ZD3
2.2k
10k
4148
270k
ZD2
270k
75V
TP1
D9
33k 1W
180k
4148
*
C1
D7
4148
4.7nF
4148
BC337
33k 1W
13k
(D) CRANE OPTICAL PICKUP TRIGGERING
75V
270k
ZD2
270k
13k
BC337
180k
4148
4148
*
C1
D9
10k
BC337
4.7nF
Q5 D8
Q6
33k 1W
33k
56k
33k 1W
10k
D7
Tacho
FOR NO
MULTISPARK
= 15nF
* C1
out
4148
GND
TACHO
TP1
100k
5.1V
PHOTODIODE
ANODE
150Ω
VR1
22k
LED
CATHODE
150Ω
+5V R,K H+,A TRIG.
+5V
Fig.6(a)-(e): here’s how to mount the parts on the
input section of the PCB to suit other ignition
trigger types. It’s just a matter of choosing the
layout to match your car’s ignition trigger and then
mounting the remainder of the parts as shown on
Fig.5. Note that the 100W 5W resistor used in the
points triggering version should be secured to the
PCB using neutral-cure silicone, to prevent it from
vibrating and fracturing its leads and/or solder
joints.
33k
56k
Q5 D8
BC337
(C) ENGINE MANAGEMENT TRIGGERING
5.1V
ZD3
10k
4148
180k
4148
*
C1
10k
ZD3
33k 1W
FOR NO
MULTISPARK
= 15nF
*C1
out
Q6
D9
BC337
TACHO
150Ω
100k
D7
4148
2.2k
10k
BC337
C1
VR1
4.7nF
Q5 D8
Q6
*
22k
75V
270k
ZD2
270k
13k
GND
Tacho
Tacho
56k
LED
ANODE
PHOTODIODE
CATHODE
GND
GND
33k
33k 1W
100k
10k
4.7nF
150Ω
+5V R,K H+,A TRIG.
+5V R,K H+,A TRIG.
TACHO
TP1
VR1
FOR NO
MULTISPARK
15nF
*C1= out
13k
(B) HALL EFFECT OR LUMINITION TRIGGERING
(A) POINTS TRIGGERING
ENGINE
MANAGEMENT
SYSTEM
33k
56k
BC337
BC337
120Ω
C1
180k
4148
*
D9
BC337
BC337
10k
Q5 D8
Q6
D7
4148
2.2k
10k
4.7nF
Q5 D8
Q6
FOR NO
MULTISPARK
= 15nF
*C1
out
2.2k
13k
TP1
100k
120Ω
56k
TACHO
150Ω
VR1
2.2k
33k
33k 1W
10k
Tacho
Tacho
FOR NO
MULTISPARK
= 15nF
*C1
out
33k 1W
SIG
GND
150Ω
100Ω
75V
270k
ZD2
270k
100 Ω 5W
(POSITIVE
SUPPLY)
H+
GND
GND
TACHO
100k
+5V R,K H+,A TRIG.
+5V R,K H+,A TRIG.
POINTS
TP1
VR1
(E) PIRANHA OPTICAL PICKUP TRIGGERING
side of the bobbin (see Fig.7).
The next step is to wind on four 60turn layers. Begin by winding the wire
clockwise, with the turns placed sideby-side, until the first 60-turn layer is
completed. The winding should end
up near the edge of the bobbin on the
opposite side to the S1 start pin.
Cover this winding with a single
layer of insulation tape, taking care
40 Silicon Chip
to also cover the start of the wire as it
comes down from the bobbin pin. The
next 60-turn layer can then be wound
on in the same clockwise direction,
again with the wires close-wound and
laid side-by side. Cover this winding
with another single layer of tape, then
complete the other two 60-turn layers
in exactly the same manner, finishing
with another layer of tape.
The end of the winding is now
trimmed, stripped of insulation and
soldered to pin 8 (F1), as shown. As
before, make sure that the wire end is
covered with a layer of insulation tape
as it exits from the bobbin to connect
to the pin. The idea is to make sure
that the secondary winding will be
electrically isolated from the primary
windings.
siliconchip.com.au
This inside view shows the completed High-Energy Multi-Spark CDI with the parts installed for a reluctor pick-up
trigger (see Fig.5). Be sure to use heavy-duty automotive cable for the external wiring connections.
1
6
60 TURNS
EACH LAYER
7
F1 8
FIRST WIND THE SECONDARY, 5
USING 0.25mm ENAMELLED
4
COPPER WIRE: FOUR 60 -TURN
LAYERS, STARTING FROM PIN 10
AND ENDING AT PIN 8 .
PLACE ONE LAYER OF PLASTIC
3
INSULATING TAPE OVER
2
EACH LAYER.
(SEC.) 9
S1 10
11
12
1
2
THEN WIND THE PRIMARIES,
USING EIGHT TURNS OF 1mm
ENAMELLED COPPER WIRE FOR
EACH (WOUND TOGETHER –
I.E., BIFILAR FASHION).
TERMINATE THE START WIRES
AT PINS 13 & 1 2 AND THE
FINISH WIRES AT PINS 2 & 1 .
13
ETD29 FORMER
UNDERSIDE (PIN SIDE) VIEW
7
6
5
F1 8
4
(SEC.) 9
S1 10
11
3
S2 12
2 F1
1 F2
(PRIMARY)
(8 TURNS EACH)
S1 13
ETD29 FORMER
UNDERSIDE (PIN SIDE) VIEW
Fig.7: the winding details for transformer T1. The secondary is wound first using four 60-turn layers of 0.25mmdiameter enamelled copper wire (ECW), starting and finishing at pins 10 & 8. The primary is then wound on using
eight bifilar turns of 1mm-diameter ECW, starting at pins 13 & 12 and finishing at pins 2 & 1 respectively.
The primary windings are wound
using two separate 600mm lengths
of 1mm ECW. Start by scraping about
10mm of insulation from one end of
each wire, then wrap and solder them
to pins 13 & 12 on the bobbin.
The two primary windings are now
wound on together (ie, bifilar wound).
It’s just a matter of winding on eight
turns and then connecting the wire
ends to pins 1 & 2. Note that the wire
that starts at S1 (pin 13) must connect
to F1 (pin 2), while the wire from S2
(pin 12) must connect to F2 (pin 1).
siliconchip.com.au
You can identify the windings using
a multimeter. There should be close to
0Ω between S1 & F1 and close to 0Ω
between S2 & F2. Conversely, there
should be high impedance (>1MΩ)
between S1 & S2 and between the two
primary windings and the secondary.
Once the primary has been completed, cover this winding with a single
layer of insulation tape cut to fit the
inside width of the bobbin. It’s then
just a matter of sliding the two ferrite
cores into the bobbin and securing
them in place using the supplied clips.
The transformer assembly can now
be installed on the PCB. It can only go
in one way, since one side of the bobbin has six pins while the other has
seven. Be sure to push the transformer
all the way down onto the board before
soldering its pins.
The PCB assembly can now be
completed by soldering long lengths
of heavy-duty automotive cable to the
PCB wiring points for the +12V supply,
trigger inputs, coil connections and
tacho connection. The chassis connection (near the coil connections) goes to
January 2015 41
SILICONE
WASHER
M3 x 10mm
SCREW
INSULATING
BUSH
M3 NUT
Q1-Q 4
PCB
CASE
Fig.8: the mounting details for
Mosfets Q1-Q4. The metal tab of
each device must be insulated
from the case using an insulating
bush and silicone washer. Do the
mounting screws up firmly, then
use a DMM to make sure each tab
is indeed insulated from the case.
a solder lug that’s secured to the case,
so this lead can be kept short.
Preparing the case
The completed PCB assembly is
housed in a diecast metal case measuring 119 x 94 x 57mm. This has to have
a number of holes drilled in order to
mount the PCB, secure the tabs of Q1Q4 and fit cable glands.
Start the case preparation by drilling
the PCB mounting holes. To do this,
first place the PCB assembly inside
the case and mark out the four corner
holes in the base. That done, remove
the PCB, drill these holes out to 3mm
diameter and remove any burrs using
an oversize drill. These holes should
then be countersunk on the outside
of the case, to accept M3 countersink
head screws.
Next, secure four M3 x 9mm tapped
spacers to the PCB mounting holes
using M3 x 6mm pan-head screws,
reposition the PCB inside the case and
mark out the tab mounting hole positions for Q1-Q4. Drill these out to 3mm
diameter and lightly countersink them
using an oversize drill to remove any
sharp edges on the holes. This step is
vital to prevent the insulating washers
that fit between the Mosfet tabs and the
case from being punctured.
While you are at it, drill a 3mm hole
in the side of the case so that the earth
solder lug can be attached. This lug can
then be installed using an M3 x 6mm
machine screw, nut and shakeproof
washer.
Holes are also required in the lefthand and righthand ends of the case to
accept the two specified cable glands.
These two 15mm-diameter holes
should be located 15mm down from
the top of the case and 50mm in from
the rear. You can drill the cable gland
holes in one step using a 15mm Irwin
Speedbor drill.
Alternatively, use a small pilot drill
to start the holes, then carefully enlarge
them to size using a tapered reamer.
Remove any sharp edges and metal
swarf using a rat-tail file.
Once all the holes have been drilled,
install the PCB in the case and secure
the spacers to the base using four M3 x
6mm countersink-head screws fed up
through the base. Mosfets Q1-Q4 can
then be fastened to the sides of the case
Table 1: Resistor Colour Codes
o
o
o
o
o
o
o
o
o
o
o
o
o
o
o
No.
3
2
2
2
1
2
3
1
7
1
2
1
2
3
42 Silicon Chip
Value
1MΩ
680kΩ
270kΩ
180kΩ
56kΩ
47kΩ
33kΩ
13kΩ
10kΩ
8.2kΩ
4.7kΩ
2.2kΩ
22Ω
10Ω
4-Band Code (1%)
brown black green brown
blue grey yellow brown
red violet yellow brown
brown grey yellow brown
green blue orange brown
yellow violet orange brown
orange orange orange brown
brown orange orange brown
brown black orange brown
grey red red brown
yellow violet red brown
red red red brown
red red black brown
brown black black brown
as shown in Fig.8. In each case, this
involves using a silicone washer and
insulating bush to electrically isolate
the device tabs from the case. Secure
each tab assembly to the case using an
M3 x 10mm machine screw and nut.
You can also fit a shakeproof washer
if you wish.
Now check that the tab of each
device is indeed electrically isolated
from the case. That’s done simply
by measuring the resistance between
the case and each Mosfet tab using a
multimeter. Each device should give
a very high ohms reading, although
the reading may initially be low and
then quickly increase as the capacitors
charge up via the multimeter’s leads.
A permanent low ohms reading
means there is a short between the tab
of that particular device and the case. If
that happens, undo the assembly, clear
the fault (eg, metal swarf or a sharp
edge on the mounting hole) and replace
the silicone washer with a new one.
Finally, trim and solder the chassis
wire to the earth lug and attach it to
the side of the case.
The +12V lead should be fed through
the left cable gland along with the trigger wires. The two ignition coil wires
should pass through the right hand
cable gland. Be sure to use heavy-duty
automotive cable for all these connections and lace the wiring securely to
ensure reliability.
Table 2: Capacitor Codes
Value
100nF
4.7nF
1nF
µF Value
0.1µF
.0047µF
0.001µF
IEC Code EIA Code
100n
104
4n7
472
1n
102
5-Band Code (1%)
brown black black yellow brown
blue grey black orange brown
red violet black orange brown
brown grey black orange brown
green blue black red brown
yellow violet black red brown
orange orange black red brown
brown orange black red brown
brown black black red brown
grey red black brown brown
yellow violet black brown brown
red red black brown brown
red red black gold brown
brown black black gold brown
siliconchip.com.au
Note that running the +12V lead
through the same clamp as the ignition
coil would induce high voltage spikes
into the +12V supply, so don’t do this.
Testing
Installation
Be sure to mount the CDI case in a
splash-proof location where air flows
over it and make sure that it is well
away from the exhaust side of the
engine. It can be secured inside the
engine bay using self-tapping screws
or you could use brackets. Make sure
that the case is well-earthed to the
vehicle chassis.
Once it’s in place, connect the
positive supply lead to the +12V ignition line and the trigger input to the
ignition pick-up. The coil leads go to
either side of the ignition coil primary.
Disconnect any other wires that are
siliconchip.com.au
This view shows how Mosfets Q3 & Q4 are secured to the case for heatsinking.
Make sure that their case mounting holes are free of any metal swarf before
installing the insulating washers and mounting screws. Mosfets Q1 & Q2 are
mounted in similar fashion (see Fig.8).
SILICON
CHIP
HIGH-ENERGY
MULTI-SPARK CDI
WARNING: HIGH VOLTAGE OUTPUT
If possible, use a current-regulated
power supply to initially test the DCDC converter in the Multi-Spark CDI
unit. And here a word of warning: this
inverter produces around 300V DC,
so don’t touch any part of the circuit
while it is operating. For the same
reason, it’s important not to touch the
output wires to the coil.
Before applying power, it’s a good
idea to fit the lid on the box. Electrolytic capacitors have a nasty habit of
exploding if they are installed with
reverse polarity, so this simple step
will protect your eyes. At the very
least, wear eye protection if you intend
operating this unit with the lid off.
If everything is OK when power
is applied, then power off again and
remove the lid. VR1 now has to be adjusted to set the converter’s output to
300V. To do this, connect a multimeter
between the chassis and test point TP1,
then reapply power and adjust VR1 for
a 300V DC reading (be careful not to
touch any part of the circuit).
For a reluctor pick-up, VR2 has to be
adjusted so that the pick-up sensitivity
is correct. That’s done as follows:
(1) Connect the reluctor to the CDI.
(2) Turn VR2’s adjustment screw anticlockwise by 10 turns, then adjust this
screw clockwise until Q7’s collector
drops to 0V.
(3) Turn VR2’s adjustment screw anticlockwise so that Q7’s collector just
goes to about 5V, then adjust VR2
anticlockwise by two more turns (this
ensures that Q7 is not prone to switching on and off with no reluctor signal).
Fig.9: the front panel artwork can be downloaded from the SILICON CHIP
website, printed out and sandwiched between the case lid and a Perspex
sheet. Use neutral cure silicone to secure the Perspex in place.
part of the original ignition system.
The tacho signal leads runs direct to
the tachometer (again, disconnect the
existing signal lead).
Note that a reluctor coil pick-up
must be connected with the correct
polarity in order to give the correct
spark timing. This is best determined
by testing the engine. If it doesn’t fire,
reverse the leads and try again.
You may find that with the MultiSpark CDI installed, the spark timing is
a little advanced, due to the CDI’s fast
rise time. If so, you may need to retard
the static timing slightly to prevent
pinging or a slightly rough idle.
Note that it’s always a good idea
to turn the ignition on for one or two
seconds before actually cranking the
engine. This will allow IC3’s 100µF
filter capacitor to fully charge and give
the inverter circuit sufficient time to
generate its 300V DC output.
Once it’s all working, use neutral
cure silicone to seal the lip of the case,
the cable glands and any mounting
screws. This will ensure that the case
is watertight and ensure reliability. SC
January 2015 43
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.
REG2 LM1117T
+3.3V
OUT
1000 µF
100nF
100nF
IN
GND
REG1 LM7805
+5V
100nF
OUT
3x
10k
13
IC1
SCL
PCF8563
2
4
5
6
3
9
Rx
Tx
4
4
NC
6
2
Vdd
RS
EN
5
16 x 2
LCD MODULE
6
3
10k
BC548
B
E
11
20
GND
OUT
DATA OUT
8
19
27
47 µF
TANT
Using a Micromite to control a
PCF8563 real-time clock
will find any number of suppliers
selling the boards for about $6.
The PCF8563 keeps accurate track
of the time and date and has two
separate alarm functions. The first is
the usual alarm based on the time of
day, just as in a normal alarm clock.
The second is a countdown timer
as you might use for time exposure
in a UV light-box. The countdown
timer can count down from times as
large as 255 minutes. Both alarms are
implemented in this project and both
can be operating simultaneously.
The circuit diagram shows how
simple it can be to use this timer
module with the Micromite. The
PCF8563 uses a serial I2C bus for
communication but fortunately the
Micromite makes using this protocol
relatively simple. The SDA and SCL
OUT
IN
C
7805
LM1117T
23
12
K
CONTRAST
R/W
5
22
21
The Micromite has inbuilt time
and date functions which are suitable for short-term time keeping. But
if used continuously over extended
periods, such as in a watering system
or pool pump control, the clock will
inexorably drift to such an extent that
the devices may well be switched on
when it is illegal to do so.
One solution is to hand over the
time-keeping duties to a real-time
clock chip such as the PCF8563.
This chip needs a few additional
components (including a 32.768kHz
crystal) to turn it into an accurate
time-keeper. The best way of doing
this is to buy a PCF8563 real-time
clock board. These boards have all
the components already installed,
44 S
hip this project. Just
ready ilicon
to slotCinto
Google “pcf8563 rtc board” and you
CONTRAST
24
14
GND
A
D7 D6 D5 D4 D3 D2 D1 D0 GND
1
14 13 12 11 10 9 8 7
15
TO SERIAL
TERMINAL
COM
1N4004
MICROMITE
16
DATA IN
NO
Q1
BC548
+5V
25
#
E
D1
1N4004
A
K
RLY1
26
0
C
B
ALARM TRIGGERED OUTPUT
3
*
2.2k
9
2
+
Q2
BC548
E
18
1
8
C
B
TIMER TRIGGERED OUTPUT
4 x 3 KEYPAD
7
2.2k
7
17
SDA
–
1000 µF
–
28
10
INT
+
12V BUZZER
1
Vdd
IN
GND
100nF 1000 µF
12V
DC IN
+12V
GND
IN
GND
OUT
pins on the module must connect to
pins 18 & 17 respectively – these being the Micromite pins specifically
devoted to I2C communications. The
timer interrupt pin is active low and
connects to Micromite pin 10. The
three associated 10kΩ resistors function as pull-ups.
The interrupt can result from
either the alarm or countdown
timer (or both), and is used by the
Micromite to switch either pin 9 or
pin 7 high. Flags in the timer chip
indicate which process(es) caused
the interrupt(s) so that the correct
pin(s) can be turned on.
A 4x3 keypad is used to enter timer
and alarm data and a 16x2 LCD is
used to display the time and date on
line 1 and the state of both alarms on
line 2. They are directly connected
to the Micromite pins as shown. The
circuit requires 12V, 5V and 3.3V DC
supply lines and these are derived
from a 12V plugpack feeding in series
a 5V and a 3.3V regulator. Use a small
heatsink on the 5V regulator.
When power issiliconchip.com.au
first applied, the
correct time and date need to be en-
STARTER SWITCH
RLY2
24V
K
+24V
IN
D2
RELAYS ON BATTERY BOX WALL
K
A
FUSE
D1
A
COLD START
PILOT
STARTER
AUX
RELAY
STOP
GLOW
PLUG
RELAY
C
Q2
BC337
E
LIMIT
SWITCH
24V DC
ZD1
8.2V
A
B
SCR1
C106Y
GLOW TEMP
SWITCH
ON ENGINE
220nF
+
STOP
MOTOR
10k
G
K
START
68k
C
100 µF
1k
B
Q1
2N6388
K
A
–
E
FUSE
+24V
IGNITION
BR1 W04
REG1 7805
+5V
KEY
LED14
A
λ
LEARN
LED1
560Ω
100 µF
λ
K
K
100nF
4
14
LED2
λ K
Vdd MCLR
18 A
RA1
7
RB1
17
RA0
LED4
RA7
LEARN
λ
16 A
6
RB0
RB5
RB4
+5V
RA2
10k
RA3
3
RA4
RB2
λ
~
S2
Vss
RB3
λ
A
λ
K
LED7
K
10
λ
A
1
A
ERROR
LED13
λ K
A
Q3
BC337
C
E
B
560Ω
K
A
560Ω
560Ω
A
DETECT
8
9
λ
A
10k
TO COLD
START PILOT
USER 8
LED11
2
A
USER 6
LED9
K
RLY1
24V
D3
USER 4
USER 7
K
LED10
λ
K
USER 5
LED8
11 A
USER 2
USER 3
K
LED5
K
NO GO
SELECT
λ
LED6
RB6
330Ω
1
K
LED3
A
IC1 RB7
PIC16F628A 12
28
26
1000 µF
3 5V
USER 1
λ
A
K
15
13 A
16
4
RA6
S1
RFID
MODULE
GND
100nF
–
10k
560Ω
27
+
IN
10k
560Ω
SENSING
COIL
15
OUT
A
~
SCR2
C106Y
10k
G
GO
K
λ LED12
K
560Ω
5
W04
BC 33 7
LEDS
ALL DIODES: 1N4004
A
K
Engine immobiliser
uses RFID tag
This circuit is based on the RFID
tag project featured in the November 2010 issue of SILICON CHIP. It is
available from Oatley Electronics,
Cat. K291.
tered. Pressing 1 on the keypad will
prompt for the time to be entered in
siliconchip.com.au
HHMMSS
format. The entered digits
are echoed on line 2 of the display.
K
A
B
E
C
G
A
A
B
K
The circuit has been modified
so that once the valid RFID tag
has been sensed, the relay latches
on permanently rather than being
energised only briefly, as it would
if it was being used to control a
door lock solenoid. This change
has been achieved by changing the
When all six digits have been entered
you will be prompted to enter the
date in DDMMYY format. After this,
continued next page
C
C
IN
E
+~~–
7805
2N6388
C106Y
GND
GND
OUT
relay switching transistor to a C106Y
SCR (SCR2) which latches on, once
triggered.
It was installed on a vehicle with
a 3.9L 4 cylinder diesel engine and
it simply prevents the motor being
started if a valid RFID tag is not
sensed. In this case, it prevents the
24V motor in the diesel shut-down
continued on page 48
January 2015 45
Circuit Notebook – Continued
RTC . . . continued from page 45
the display will show the time and
date and the alarm states similar to
that shown below (assuming the time
and date entered are those shown):
14:27:35 26/10
no alarm no timr
Note that the full date cannot be
displayed, through lack of space. You
are expected to be able to remember
what year it is!
To set the alarm, press 3 on the
keypad and you will be prompted
to enter the alarm time in HHMM
format. When all four digits have
been entered, the display might read:
14:29:47 26/10
07:30 no timr
The countdown timer is initiated
by pressing 2 on the keypad. You will
prompted to enter the countdown
4-digit
thermometer
This 4-digit thermometer is based
on an ICL7135 precision analog-todigital converter with multiplexed
BCD output, digit driver and blinking
outputs that give visual indication
of over-range and under-range. The
chip contains all the necessary active devices with the exception of
display drivers, reference and clock.
These are externally added to it in
this circuit.
A silicon diode-connected transistor is employed as a sensing element.
The full scale is set to 400mV (±199.9
counts) with the righthand-most
digit displaying fractions of 1°C.
In the analog section, Q1 serves
as a sensor with a temperature coefficient of -2mV/°C. The base-emitter
junction of this transistor, which is
forward-biased by a 4.7kΩ resistor, is
connected to the IN LO input of IC1
value which must be a number from
1-255. You will next be asked to
name the units. Enter “2” if seconds
or “3” if minutes; are the units to
employ. After entering the data, the
display might look something like:
14:29:47 26/10
07:30 150 sec
This assumes, of course, that you
entered 150 seconds for the countdown timer value.
While entering data at any of the
above stages, “*” will act as a back
space to erase an incorrect digit. “#”
will abort the process and also turn
off all alarms.
If the alarm is triggered, pin 9 goes
high and activates the relay. This
can be used to turn on a radio, for
example. If the countdown timer is
triggered, pin 7 goes high and in this
at pin 9. The voltage on this diode is
proportional to the temperature. At
0°C, the voltage is equal to 641mV.
Thus VR2 should be set to 641mV at
pin 10 (IN HI) for a display reading
of 000.0 reading at 0°C.
The REF voltage on pin 2 of the
chip is set to 200mV for 400mV
(±199.9 counts) full scale. This
means that the voltage on pin 9 of
the chip can be within the range of
+641mV (at 0°C) ±400mV. Beyond
this range, the display will blink.
The clock is built around LM311
single comparator IC3 which is
configured as an oscillator with its
frequency set to 100kHz. This arrangement is suitable for both 50Hz
and 60Hz mains power as it maintains good power supply rejection.
Each measurement cycle goes
through four phases. They are (1)
auto-zero, (2) signal-integrate, (3)
de-integrate and (4) zero-integrator.
Thus, the analog signal of the input
co nt ri bu ti on
MAY THE BEST MAN WIN!
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Each month the BEST contribution (at the sole discretion of the editor)
receives a $150 gift voucher from Hare&Forbes Machineryhouse.
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- buy some tools you’ve always wanted, or put it towards that big
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46 Silicon Chip
www.machineryhouse.com.au
Contribute NOW and WIN!
Email your contribution now to:
editor<at>siliconchip.com.au
or post to PO Box 139, Collaroy NSW
case the buzzer will sound. You can
substitute another relay in place of
the buzzer if that suits your purpose.
If the alarm has been triggered, “*”
will turn the alarm off (ie, set pin 9
low) but keep the alarm setting so
that it will come on again at the same
time the next day.
If the timer was triggered, it is
automatically cancelled and will not
count down again until new values
are set. “*” will turn the alarm off
(ie, set pin 7 low). Pressing “#” will
turn both the alarm and timer off and
cancel them.
The Micromite time and date are
synchronised with the PCF8563
time and date once every day. The
software, rtcalarm.bas, is available
for download from the SILICON CHIP
website.
Jack Holliday,
Nathan, Qld. ($60)
is converted to a digital format.
IC2 is a BCD to 7-segment decoder
that drives the common anode LED
display. The four transistors tied to
the anodes of the display serve as
anode drivers.
Transistor Q3 blanks the leading
digit when the reading is negative
but turns on its middle ‘g’ segment
to show a minus sign. When Q4 applies voltage to this digit’s anodes,
the D5 output of IC1 is high and if
the reading is negative, so is the POL
output at pin 23. Thus the base of
Q3 is pulled high which brings the
ripple blanking input (RBI) at pin 5
of IC2 low, disabling IC2’s outputs.
The ‘g’ segment is then driven directly by Q3.
Transistor Q8 drives the decimal
point when the third digit is active,
indicating that the right-most digit
represents increments of 0.1°C.
To calibrate the thermometer,
make sure that VR1 is set for 200mV
at pin 2 of IC5. Place the sensor in ice
water and adjust zeroing trimpot VR2
for a display reading of 000.0. This
will happen when the voltage on pin
10 of IC5 is adjusted to 641mV - or
perhaps a slightly different value,
depending on the properties of Q1.
Finally, place the sensor in boiling
water and adjust scale-factor trimpot
VR1 for a reading of 100.0 at sea
level.
Mahmood Alimohammadi,
Tehran, Iran. ($50)
siliconchip.com.au
siliconchip.com.au
January 2015 47
230V
AC
10k
220nF
10k
A
K
A
D4
D2
470pF
IC3
LM311
3
1
8
ADJ
4
47k
7
220 µF
220 µF
+1.2V
A
K
D9 1N4148
100Ω
4.7k
A
K
A
K
47k
100k
OUT
2
IN
REG3 LM317LZ
D3
+5V
+5V
9V
0V
9V
D1
K
B
4.7k
OUT
GND
GND
OUT
E
C
470nF
ZERO
ADJ
Q1
10k
27Ω
4
5
6
2
1
–REF CAP
+REF CAP
B2
B4
(MSB) B8
POL
(MSD) D5
D4
D3
D2
(LSD) D1
RUN/HLD
STROBE
O vrRNG
K
D1 – D8: 1N4004
24
(LSB) B1
DigGnd
COMMON
A
11
13
14
15
16
23
12
17
18
19
20
25
26
27
V+
28
UndRNG
IC1
ICL71 35
CLOCK IN
IN LO
IN HI
INT OUT
AZ IN
BUFF OUT
REF IN
V–
3 ANALOG
7
8
22
9
10
1 µF
1 µF
1 µF
VR2
20k
–5V
100 µF
100 µF
+5V
100k
+641mV
+200mV
REG1 79L05
IN
VR1
10k
100nF
100nF
IN
REG1 78L05
A
K
D9: 1N4148
47k
B
E
C
7
1
2
6
4
5
3
E
A0
A1
A2
A3
16
Vcc
330Ω
C
BC547
GND
8
IC2
7447
B
BI/RB0
RBI
LT
+5V
B
Q2
Q3
E
C
47k
Ya
Yb
Yc
Yd
Ye
Yg
Yf
14
15
IN
13
12
11
10
9
Q4
A1
12
E
C
A2
9
E
Q5
A3
8
E
C
Q6
A4
6
E
C
Q7
47k
g
5
ADJ
LM317LZ
10
OUT
f
1
e
OUT
2
d
4
IN
GND
7
b
LM79L0 5
c
IN
OUT
78L05
GND
E
B
8x
220Ω
3
DP
C
Q8
11
a
8.8.8.8.
B
B
C
B
B
+5V
Don Amos
is this mon
th’s winner
of a $150 g
ift voucher
from
Hare & Forb
es
Circuit Notebook – Continued
The big problem is that the micro
USB is also the charging port, so
you can either charge the tablet or
use the USB port but not both at the
same time. I spent a lot of time experimenting with cables and I found
that while the tablet is in USB OTG
mode it will not accept charge, so the
tablet’s battery will gradually run flat.
The solution is simple – don’t use
the OTG cable! It turns out that the
tablets are quite happy to behave
as a host when you use a non-OTG
device cable and they will then accept a charge at the same time. This
is done by making up a cable using
the arrangement shown above.
You need to sacrifice two cables:
a USB Type A male to USB micro-B
(eg, Jaycar WC-7708) and a USB Type
A male to USB Type A female (eg,
Jaycar WC-7708). You should have
the first cable already, as it came with
the tablet. The
second cable is
just a USB Type
A extension cable.
Cut both cables in
half and put the extra USB Type A
male cable aside – it is not required.
Connect the white and green wires
between the USB micro B connector
and the USB Type A female connector, matching the colours as you
go. Now connect all three red wires
and all three black wires between
the USB Type A male, USB Type A
female and USB micro-B connectors.
Insulate all your connections and
you are ready to go.
Plug the USB Type A male connector into your existing charger,
the USB micro B into the tablet and
the USB Type A female connector
into a powered USB hub (it does not
need to be powered but this allows
higher power devices). You can then
plug keyboards, mice, USB sticks,
hard disks and any other devices
into the USB hub, and use them all
at once. I found my tablet initially
said “plugged in – not charging”
but after a minute or so it changed
to “plugging in – charging”.
I also found that I can use any
spare 5V regulated plugpack (1A and
above) to charge the tablet instead
of using the USB type A plug. Just
connect the four wires from the USB
Type A female to the USB micro-B
and connect the 5V regulator to the
red and black wires. This saves the
original cable and charger so they
can be used when you want to use
the tablet as a tablet.
Don Amos,
Ingleburn, NSW.
tag is suspended on a piece of chain
60mm long.
The top section of the circuit is
more or less incidental and is associated with the glow plug switching
for a diesel engine where the plugs
are energised for a brief period
(3.5s) before the engine is cranked
to start it.
Transistor Q1 controls a timer
circuit to hold the start circuit off
until the shut-down unit is in the
start position. The 24V motor in
the shut down unit goes in the one
direction only, one half turn at a
time, being controlled by the limit
switches operated by a cam on the
output shaft. The power has to be
available to the relay contacts all the
time, so as to be able to power the
motor to the stop position when the
ignition is turned off.
Note that since the circuit is being
used in a 24V vehicle, relay RLY1
must have a 24V coil. Altronics Cat.
S-4162 will fit into the RFID PCB
from Oatley Electronics. In 12V vehicles, this change is not necessary.
Ron Groves,
Cooloola Cove, Qld. ($45)
ALL FOUR WIRES
OF BOTH THESE
LEADS JOINED
TOGETHER
USB TYPE A MALE
PLUG (CONNECTS
TO CHARGER)
USB TYPE A FEMALE
SOCKET (CONNECTS TO
USB HUB UPSTREAM PORT)
USB OTG
charging cable
You can now purchase 8-inch
Windows tablets at a very low price.
Typically, you get a quad core tablet
with Windows 8 and Microsoft Office
for less than $300. These are quite
powerful and are capable of being
used as desktop computers as they
have HDMI ports that can drive 1920
x 1080 displays and they also have
USB ports, allowing for expansion.
You can use a USB OTG (on the
go) cable to convert the tablet’s micro
USB to a USB female connector and
then use a range of USB devices. The
USB OTG cable tells the tablet to stop
behaving like a USB device and start
behaving like a USB host. It does this
by using the fifth pin on the micro-B
connector to tell the tablet to use the
USB OTG mode.
Engine immobiliser –
continued from page 48
unit from rotating to the start position. On other vehicles, it could disable the ignition or stop the fuel flow
with a solenoid valve. This would
be done via the switch contacts of
relay RLY1.
The RFID sensing coil was concealed inside the steering column
of the vehicle and the tag is on the
ignition key ring so that it can be
read by the sensing coil once the
ignition has been turned on. The
48 Silicon Chip
1
3
2
4
1
3
2
4
WHITE (D –) &
GREEN (D+) WIRES OF
THIS LEAD CUT SHORT; ONLY
RED (Vbus) & BLACK (GND)
WIRES JOINED TO THOSE
OF THE OTHER LEADS
USB MICRO-B PLUG
(CONNECTS
TO TABLET)
siliconchip.com.au
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ICD 2, for example, is not compatible with MPLAB X IDE.
This offer also covers older versions
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Until 28th February you can trade
in your old programmers and debuggers too, for a PICkit 3, ICD 3 or PM 3
at 50% off the retail price!
Upgrading is easy: simply download
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Spirit’s Melbourne 200MB/s SDSL – Faster than NBN!
Melbourne’s premier Multi-Dwelling-Units are about to receive ultrafast symmetric upload and download
speeds of up to 200Mbps from Spirit.
Spirit Telecom has launched its
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competition, including NBN, with
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UFi (meaning Ultra-Fast Internet),
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Spirit UFi uses its own in-building
network, rather than old copper and
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Carlton. Using a sizable sample of
customers, the result was a 61%
increase in data uploads, compared
to the same period in 2013.
Contact:
Spirit Telecom
PO Box 377, Prahran, Vic 3181
Tel: 1300 007 001 Fax: 1300 887 813
Website: www.spirit.com.au
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Despite checks made by SILICON CHIP
prior to publication, we have since been
advised that the advertisement for “Network Communications” on page 9 of our
December 2014 issue is bogus. There
is no connection with Network Communications in Queensland. Readers are
advised NOT to have any dealings with
this advertiser.
This warning also appears on our
website, siliconchip.com.au
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January 2015 57
SERVICEMAN'S LOG
DIY printer repairs can easily go wrong
There are lots of traps for the unwary when
it comes to fixing printers, especially if you
download “printer reset” software from the
internet. Want to get the back seat of your
car covered in printer ink? It happened to a
customer of mine.
One of the first peripherals purchased by most computer owners is a
printer. Printers really haven’t changed
a lot in the past decade, although there
have been refinements to the print
heads in inkjet type devices and to the
drum technology used in laser printers.
What we have seen is the price of
printers falling through the floor, usually because printer manufacturers
have cottoned on to the fact they can
sell the printer almost at cost and make
their real money by gouging the user
with shockingly expensive consumables. In fact, it has reached the stage
where inkjet owners will simply buy
another printer rather than replace
empty cartridges, while laser printer
users will chuck the device away and
buy a new one rather than shell out
58 Silicon Chip
for a new drum and/or toner assembly.
The resulting e-waste is almost
criminal and it is with good reason that
many countries now force manufacturers to run their own recycling schemes.
In reality, this sometimes involves
sending containers full of dead printers to China or India where the locals
use crude methods to strip anything
valuable from them. This would be
fine except that these processes often
Dave Thompson*
result in ecological damage such as
contaminated water supplies and
poisoned soil, something that doesn’t
sit easily with many of us.
My brother runs a printer repair outfit and has a literal mountain of these
dead devices. Some he keeps for parts
and some he keeps because it seems
criminal to throw them away. One
problem he faces is that sourcing new
spare parts for printers can be a lesson
in abject frustration, so it’s not only the
prohibitive cost of consumables that
causes these devices to be discarded.
For example, one particular multifunction model has a propensity to
break a Mylar ribbon cable that’s used
to connect a couple of moving parts.
This ribbon cannot be purchased as
a spare part, meaning that this $200
printer is rendered useless for the
sake of a part that would cost no more
than a few dollars and could be easily
replaced.
That’s why my brother keeps dead
machines; by scrounging parts from
these old carcasses, he can often get
a customer up and running again,
thereby saving them the hassle of
buying a new machine and disposing
of the old one.
Of course, the main flaw in this
scheme is that many dead machines
of a particular model are junked for
the same reason. This means that they
are often useless for parts unless it is
something else that has failed in the
client’s machine. All in all, it’s a difficult situation and if I had the answer,
I’d share it.
Against that background, it’s no
wonder that many people with malfunctioning printers just toss them
and buy a new one. All we can do is
hope that when someone says they
will correctly dispose of an item, they
actually do break it down and dispose
of it sensibly.
However, some people do choose
the repair option. Whether it’s because
they are like me and think that keeping a good printer going is better than
chucking it out or they just deem it
siliconchip.com.au
more sensible to repair rather than replace, we still get printers in for repair.
Faulty inkjet printer
Problems with ink are among the
most common faults reported by end
users. In one recent case, a customer
brought in an inkjet printer that wasn’t
very old but had done a fair amount
of work. Unfortunately, it had covered
portions of the back seat of his car in
printer ink and from experience that
stuff doesn’t come off very easily.
In some ways, it was poetic justice
because this guy had been using
information gleaned from so-called
experts on the Internet in an effort to
fix it himself. In the process, he had
bypassed some built-in safeguards,
resulting in the soiled back seat.
As you know, I’m all for people having a go at doing things themselves in
many cases but there is a right way
and a wrong way of going about it.
Exercising due diligence and finding
out all there is to know about the device before jumping in and trying all
manner of repairs is one of the most
important steps in the DIY process.
Extracting the correct information
out of all the misinformation posted
on the web by so-called “experts” is
critical and simply chucking every
“fix” you find at a problem can easily
end up making things worse. Or make
a mess of the back seat of your car!
In this case, the customer’s problems
began after his printer had output a
certain number of pages and had then
begun indicating an error. And by that
I don’t mean that it indicated what was
wrong on the tiny LCD panel. Instead,
the error was indicated by a flashing red LED and the printer simply
stopped printing.
Since the flashing LED is a “catchall” error indicator, it is up to the user
or technician to deduce what the real
problem is. While some printers will
keep working in an error state, it depends on the problem and most will
remain inoperable until something
has been done to resolve and clear
the fault.
Waste ink pads
That’s where Google came in. In
an effort to fix the problem himself,
this guy had done a quick search and
downloaded a small software tool
that’s used by printer technicians to
reset errors and manipulate the various sensors and counters most printers
use. What he didn’t realise was that, in
this case, the error condition had been
tripped because the waste ink pads
in his printer were full, meaning that
they required cleaning or replacement.
Most people, including my client,
don’t realise that the majority of inkjet
printers have these waste ink pads
tucked away inside the printer. They
vary in shape and size but are typically made of dense felt-type material,
ideal for soaking up any excess ink
produced by the print-head.
This excess ink is usually produced
by the head cleaning process but can
also occur if the wrong ink has been
used in self-fillable or non-factory
refill cartridges. It may only be a tiny
drop at a time but the waste ink pads
eventually become saturated and if
they are not cleaned or replaced, the
Items Covered This Month
• DIY printer repairs can easily
go wrong
• Faulty Sunna 1500TL solar
inverter
• Road-kill resuscitation
• Fender guitar amplifier
• Faulty heatpump
*Dave Thompson runs PC Anytime
in Christchurch, NZ.
Website: www.pcanytime.co.nz
Email: dave<at>pcanytime.co.nz
ink ends up spilling into the body of
the printer and then out through any
gap or hole it finds in the case.
To prevent this from happening,
printers with waste ink pads often
have a sensor mounted in the wasteink reservoir to detect when the level
gets too high. Alternatively, in lessexpensive models, a simple page count
method is used to trigger the error LED
to indicate that the ink pads should be
checked and/or replaced.
In this particular case, the software
tool that my client downloaded is
used to reset the page counters and to
modify other parameters. However,
this tool should only be used once the
problem(s) that caused the error state
in the first place have been resolved.
Resetting the page count without
cleaning the waste ink pads will get the
printer up and running again but the
waste ink system will soon overflow
and that’s exactly what happened in
this case.
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January 2015 59
Serviceman’s Log – continued
A little bit of luck coupled with
determination to “give it a go” can
often get an expensive bit of gear running again. It certainly paid off for L.
W. of Rochedale South, Qld when he
tackled a faulty solar inverter. Here’s
what happened . . .
After returning home from a
3-month caravanning holiday, I noticed that my Sunna 1500TL solar
grid-tied inverter didn’t appear to
be working. The LCD was blank and
there were no LEDs lit to indicate that
it was providing power to the grid.
In fact, it looked like it had gone into
sleep mode which is what it does
when the Sun goes down. The only
trouble was that it was mid-afternoon
in sunny Queensland.
I first tried to reset the unit by
turning off the AC Solar Supply main
switch, followed by the PV Array
circuit breaker. After a short delay,
I then turned the PV Array circuit
breaker on again which should have
started the inverter, lighting up all
the LEDs and the LCD in the process.
Unfortunately, nothing happened!
The next thing to do was to make
sure that the voltage from the PV
(photovoltaic) array was not only
present but greater than 120V. A
check with a multimeter soon confirmed that the open circuit voltage
coming from the array was indeed
well over 270V DC. So that meant
that the problem was somewhere in
the inverter.
This particular inverter came with
a 10-year warranty but as I soon
discovered, both the company that
provided this warranty and the firm
that installed the system just over
two years ago were no longer in business. So there was nothing for it but
to see if I could fix it myself.
Not feeling very confident, I placed
the inverter on the workbench,
removed the front covers and took
a look inside to see if there were
any obvious signs of distress. To my
surprise, the whole unit looked to be
very well made. The metal cabinet
was very soundly constructed and
the circuit boards all looked neat
and tidy.
I began with a quick visual inspection and a “smell test” but there
was nothing obvious, so I turned
my attention to a fuse on the main
circuit board. It tested OK so I turned
to the Internet to see what I could
find out about this model inverter.
There were a few tales of woe but
not much more.
It was beginning to look like I
would have to buy a new inverter
but first I thought that I would take
another look at it. After all, I had
nothing to lose.
It was then that I noticed a small
circuit board sitting vertically along
the lefthand side of the case. This
was plugged into the main circuit
board and was easy to remove, so I
extracted it and set it on the workbench for further investigation.
It appeared to be a power supply of
some sort. There were a few labels on
the pins that plugged into the main
board and from these I was able to
determine where the external supply
voltage entered the smaller board.
In addition, I was able to determine
where the derived voltage rails left
to go back to the main board.
At this stage, I decided to test the
diodes, starting with D54. This was
tested in-circuit and it appeared to
be a partial short circuit. Removing it
from the board proved that this was
indeed the case.
Next, I checked D25 but this tested
OK. D28, D29 & D30 all tested shortcircuit however but removing them
In case you’re wondering, the pads
are usually inexpensive and relatively
easy to replace. What’s more, any
printer repair agent worth his salt
will give the printer a good clean and
service while doing the pads, thereby
extending the usable life of the printer.
In this case, I disassembled the
printer on a workbench protected by
a sheet of plastic cut from a bin liner.
I then used lots of paper towels to
sop up any surplus ink that was still
sloshing around the inside. It was
a real mess, although it cleaned up
relatively easily with some methylated
spirits and isopropyl alcohol. After
that, it was just a matter of replacing
the pads, cleaning the print heads with
an ultrasonic cleaner, and resetting
the counters.
vast majority of their revenue comes
from. Actual printer sales account for
very little revenue because the profit
margins on printers are almost nothing. However, the vendors recognise
that, over the life of a printer, the end
user may spend thousands of dollars
on cartridges and so this is where the
real money is.
Someone once claimed that printer
ink had to be the most expensive liquid in the world and they might well
be right, as least from the consumer’s
point of view. The reality is that printer
ink cartridges cost mere cents to produce but in some cases sell for nearly
$100, an amazingly high mark-up.
It’s no wonder then that third-party
cartridge suppliers and ink-filling companies flourished in the early 2000s as
end-users sought to lessen the financial
impact of feeding their inkjet printers.
This in turn created a huge problem
for printer manufacturers, as they saw
revenues flowing instead into the cof-
fers of those other companies.
As a result, they started getting
clever with the inks they used and by
manipulating the specific gravity and
consistency, could tailor a specific
ink for a given cartridge and printer.
This meant that using cartridges with
standard refill ink from third-party
companies could result in the print
head either blocking up due to the ink
being too thick or the ink simply pouring through because it was too thin.
The refill companies soon took
notice of this and began sourcing
and using the different inks required
to maintain their competitive edge.
The printer manufacturers then went
one step further and changed their
warranty agreements to include the
use of only original, factory-supplied
cartridges.
Of course, printer repair outfits can
easily recognise the symptoms of nonstandard cartridges being used and
customers using these cartridges have
Faulty Sunna 1500TL Solar Inverter
Liquid gold
Printer manufacturers are quite
insistent about the proper use of consumables because this is where the
60 Silicon Chip
siliconchip.com.au
one at a time proved D30 to be the
real culprit.
I now turned my attention to the
other semiconductors. The voltage
regulators all checked out OK as
did various other parts but when I
came to Q27, the main switching
device, it too appeared to be faulty. It
turned out to be a Mosfet and it was
short circuit between the drain and
source.
It was then that I noticed what initially looked like a resistor mounted
on its end but it was labelled as ‘F1’.
Closer inspection showed that it was
a 2A fuse and it was open circuit.
All the diodes were 2A fast-recovery types, while the Mosfet was a 7A
N-channel device. A quick search on
the Internet revealed that they could
all be purchased in Sydney.
The fuse posed a bit of a problem
because I was unable to source a
direct replacement. In the end, I decided to try to remove the pig-tails
from the blown fuse and resolder
them to the smallest 2A fuse I had,
even though this was twice the size
of the original.
During this process, both the endcaps came away from the fuse body,
leaving me with everything I needed
to make a good new fuse except for
some 2A fuse wire. This I was able
to salvage from a 3AG 2A fuse I had
on hand. After a bit of fiddling, I was
able to solder this fuse wire in place
and I then had a 2A fuse that looked
just like the original.
Everything else seemed to check
out OK, so I soldered the repaired
fuse in place and waited for the other
parts to arrive. They turned up a
couple of days later and I wasted no
time fitting them to the circuit board.
Once everything was in place, it
was time to refit the circuit board
to the inverter. I then reconnected
the inverter to the solar panels and
turned on the DC circuit breaker to
see what happened. After a short
delay, all the LEDs lit up and the LCD
displayed the test cycle before eventually indicating that all was well.
The yellow LED was lit, indicating
that no utility was connected, and
the green LED was flashing.
Finally, after reconnecting the AC
wiring, I threw the main AC switch.
The yellow LED immediately went
out (indicating that the utility was
present), while the green LED now
remained on to indicate that the
DC input was greater than the sleep
power.
And that was it; the inverter has
now been running happily for several months. I was lucky with this
one but you never know what can
be achieved unless you “have a go”.
discovered that their printers were
no longer covered under warranty,
all because they wanted to save a few
bucks on ink.
prisingly hard when dry and minute
particles of wet ink or toner are created
when the printer is operating (and also
in inkjets when the heads are being
cleaned). These tiny droplets or particles dry to form a large-grained dust
and if this dust is allowed to build up
on sensors and feed rollers, it can cause
all manner of problems.
This means that cleaning up and
removing this dust should be part of
any printer maintenance or service
schedule.
Another common problem is paper
jams. This frustrating issue can have a
number of causes, from the aforementioned dusty and/or dirty feed rollers
to damp paper.
Other printer problems
Aside from any potential ink issues
(easily avoided by using the correct
consumables), printers are usually
very reliable devices. Like any mechanical device though, they do need
servicing and most printer repair
companies will offer a general service
for a reasonable fee.
Ink waste pads should be part of
any regular check-up, while rollers
need to be cleaned and various sensors
checked for correct operation. These
are all important elements in any
printer. In addition, both inkjet and
laser types are notorious for producing
a fine dust that’s quite abrasive and
this can cause damage if it gets into
the inner workings
Both printer ink and toner are sursiliconchip.com.au
Be careful with paper jams
One of the worst things a printer
owner can do when a page jams in
the printer is to pull the paper out the
wrong way. If the page hasn’t yet appeared on the outside of the printer but
is accessible from the inside, it’s all too
tempting to grab what can be seen of
it and pull it back through. However,
some of the rollers may be applying a
lot of pressure to the paper (ie, to feed
it through), which means that gears
can be forced to rotate the wrong way
(and thus damaged) or sensors can be
knocked out of line.
If you get a paper jam in your printer
and you can see the page from the output side (and can get hold of it) then by
all means try to gently pull it through
but avoid jerking the page or making
any other sudden movements. Bear
in mind that if it is still under tension
from the feed rollers, the paper may
tear and leave bits and pieces behind,
so take it easy when pulling a jammed
page through.
I’ve seen many printers in my workshop where the owner has pulled the
page backwards through the rollers and
damaged the printer’s internal workings, so this should be avoided at all
costs. If you are handy with a screwdriver, by all means strip the printer
down to the level required to remove
the page safely; Google and YouTube
are handy tools for discovering how
to properly tear down a printer but be
warned it isn’t all gravy.
Indeed, printers are just the type
of device that can catch an unwary
DIYer out. You only have to upset the
gear meshing of a feed roller or the
position of a sensor to render a printer
completely unserviceable.
Of course, if your printer is one
of those ultra-cheap models and you
really have nothing to lose by diving
in and having a go, then by all means
crack on. Just be sure to take photos
and keep a good record of what you
take off and where it came from, so that
you can later put it all back together
again. If necessary, mark rollers and
gears so that they go back into exactly
the same position, as they are critical
to the operation of the device.
Colour laser printers
With the advent of cheap colour laser
printers, it’s possible that inkjet-style
printers will soon be a thing of the
past. Lasers tend to be less “fussy” than
inkjets but unless it’s a really low-cost
unit, you should use factory toner cartridges and other genuine replacement
parts such as drums.
Plenty of companies also offer reconditioned drums and toner cartridges for
laser printers and most will work withJanuary 2015 61
Serviceman’s Log – continued
Road-kill resuscitation
Road-kill usually has a bad smell
but K. D., of Chermside, Qld was
able to breathe new life into a couple
of no-so-smelly recent casualties.
Here’s what happened . . .
I was recently handed a bag that
a friend had found on a busy main
road. By the look of it, the bag had
fallen from a vehicle moving at a fair
speed or had been run over. When I
took a look inside, I found a CABAC
power point tester (TEL1TLV2) and
a Fluke insulation meter (1577)
complete with its test leads and accessories.
The power point tester appeared
to have suffered the worst damage.
The prongs on the 3-pin plug were
bent at right angles, the case was split
at the seams, the knob was bent at
an angle and it rattled badly when
shaken. I was about to toss it into the
bin when I decided to at least have a
look inside to see how it was made.
I began by removing the knob and
the nut securing the switch. The
welded seams of the plastic case
were already mostly split and the
unit cracked fully apart with some
gentle levering. Once inside, I found
that the rotary switch had been
squashed almost flat, while the PCB
was in three pieces. The neons and
resistors all appeared intact.
On a whim (and ever the optimist), I decided to see if I could fix
it. First, I de-soldered the remains of
the switch and glued the PCB back
together with Loctite 401 adhesive.
A fibreglass pencil was then used to
remove the solder mask at the breaks
in the PCB tracks and these breaks
were then bridged with wire links.
A rotary switch with the correct
pin orientation was found on eBay
for $5, while a replacement pushbutton switch came from my junkbox. These were fitted to the repaired
PCB and a new 3-pin plug was fitted
to the cord. The plastic case was then
out problems but again warranties can
be voided by using the wrong spares.
In short, check on your printer’s
warranty before buying consumables.
As mentioned earlier, it often appears
to be cheaper to buy a new printer
than to replace toner cartridges and/
or drums. However, keep in mind that
many new printers ship with “starter”
cartridges that only contain 10% or
15% of the actual capacity of a full
cartridge. These are intended to get
you up and running but will run out
pretty quickly so you’ll soon need a
proper replacement.
Inkjet manufacturers also commonly
do this, shipping their printers with
low-volume cartridges that will print
a couple of dozen pages (depending on
actual coverage) but not much more. In
both cases, you need to weigh up the
benefits of buying a new printer over
replacement consumables.
Finally, here’s a tip to keep your
inkjet printer printing nicely; at least
once a week, try to print a small image using all possible colours to keep
the print heads in good condition. If
ink dries in the tiny matrix of holes
in a print head, it’s almost impossible
to clear, even using the inbuilt headcleaning system. Instead, an ultrasonic
cleaner must generally be used to clear
this type of blockage.
Printing an image that uses all the
print heads will prevent them from
drying out and causing this problem
in the first place.
62 Silicon Chip
Faulty heat pump
A. F of Kingscliff, NSW was recently
faced with a choice: fork out around
$3000 for a new solar hot-water system or have a go at fixing his existing
heat pump system. He chose the latter
course . . .
When I moved into a new house
recently, it had a heat pump system
to provide hot water. As soon as I saw
the heat pump unit, I took an instant
dislike to it. It consisted of a large compressor box with copper pipes leading
from it to a 400-litre hot-water cylinder
located around the corner of the house.
The compressor unit itself had been
installed at the end of the car port, exactly where I could see myself sitting
in the shade in a comfy chair, with a
nice cup of tea, reading a book. This big
metal box stuck out into my entertain-
softened in boiling water and pushed
back into shape.
Next, I scanned the original damaged label and created a new one
with a graphics program. Once reassembled the unit worked as expected
and so the case was glued together. It
certainly doesn’t look “as new” but
it is both functional and safe.
By contrast, The Fluke insulation
meter had suffered little visible damage. There were, however, a couple
of tiny cracks in the case and some
chipping on the edge of the clear
plastic covering the display. In addition, the battery cover had been
forcibly dislodged.
When switched on, the unit powered up but the display showed only
a series of dashes. I downloaded the
user and service manuals but the display I was seeing wasn’t mentioned.
I could, however, access the various
power-on options, so I assumed that
a lot of the circuitry was functional.
Removing the back cover immediately revealed one obvious problem.
One of the heaviest components,
surface-mount transformer T1, had
broken away from the PCB and its
ing area, darn it!
The unit had obviously been installed many years earlier and judging
by the large copper pipes that came
out of it and disappeared around the
corner, it would not be easy to move.
In the end, I decided that it could stay
but I secretly hoped that it would soon
break down. When it did, I could then
replace it with a nice solar hot water
system, which would be cheap to run.
My house is only about 200km south
of the Sunshine Coast area, in an area
of abundant sunshine, so why hadn’t
a solar system been installed? A few
of my neighbours also had these heat
pump systems and when I quizzed
them, they told me the reason they had
them installed was because they were
so cheap to run.
Apparently, when the village was
being built some years earlier, there
had been several public meetings and
the sales people had explained these
units were very cheap to operate. And
because of this sales pitch, many people had agreed to have them installed.
However, I’m always sceptical about
the claims of sales people, so I started
doing some research of my own.
siliconchip.com.au
fine leads had also broken away from
their mounting points on the former.
I began the repair by securing the
transformer back in place with Dow
Corning 314 conformal silicone.
Next, with the aid of a microscope,
some tinned copper wire and a very
small soldering tip, I reconnected
the stubs of the fine enamelled wires
from the windings to the pads. I then
reassembled the meter but it still
displayed only dashes and wouldn’t
measure anything.
I disassembled the meter again
and went over the entire PCB using
a microscope, even removing the
shielding and rotary switch contact
assembly to check for cracks underneath. I couldn’t find any more damage but when I put it back together
again, it worked!
I can only assume that the rotary
switch assembly had popped apart
slightly on the road and that I’d completely re-seated it when I put it back
together the second time.
So, with no real expenditure apart
from my time and $5 for a switch, I’d
resuscitated two useful pieces of test
gear. Both items will come in handy.
One of my neighbours had an
original installation manual, which I
borrowed. The manual explained that
this was a low-cost way of obtaining
hot water because it heated the water
by taking the “free heat energy” from
the surrounding air. This explained
why the salesman’s pitch had been so
successful. I guess that “Rated Power:
700 to 1400 W” on the information
panel on the side of the heat pump
means little to most people.
I recently had to repair one neighbour’s solar hot water system which
had a storage tank in the laundry. It
had a water circulating pump about
the size of a coffee mug and a small,
simple control board. It was powered
from a GPO in the laundry and it drew
14W when the pump was running. It
runs for about two minutes every 20
minutes (or 2.4 hours a day), whereas
my system runs every second night for
about two hours. The difference is that
my neighbour’s solar system draws just
14W while it’s running whereas mine
uses 700-1400W.
I was glad when one day I found that
I had no hot water. At last I could replace my heat pump system! However,
siliconchip.com.au
when I looked at the price of a suitable
solar hot water system, I found that I
would have to pay over $3000. At that
price, my joy quickly faded.
So I went outside and stared at the
heat pump box. Of course, nothing
was working because it was daytime
and the supply to it was off-peak. This
first came on at 1am, so I set my alarm
clock to that time before going to bed
that night.
At 1am, I staggered out into the car
port with a torch, trying to convince my
brain that a new day had begun. There
was the loud sound of an electric motor
and rushing air from the compressor
box. So my unit had power to it and it
wasn’t dead.
The next morning, I found an ABS
plastic box mounted on the side of the
compressor box, along with a large
isolation switch. There was no power
to the circuit due to the off-peak state
but to be safe, I turned off the isolation
switch just to make sure. I then took the
cover off the ABS box and discovered
a circuit board with a PIC16F microcontroller chip and several large relays.
I now needed to have power applied
to the system in order to make further
checks. One possibility was that power
wasn’t being supplied to my system for
long enough to heat the water properly.
But applying power to a circuit which
has been disconnected by the Energy
Supply Company via the off-peak relay
(Ripple Tone Control Relay) is a very
unwise and illegal action.
In the end, I decided to ask my
electricity provider how many hours
of off-peak power were supplied each
night. I phoned the company and it
took me awhile to find someone who
was knowledgeable on this subject.
They asked me if I had received a letter from them stating that my ripple
control relay had been upgraded. I said
I didn’t know, as I had only lived in the
house for a few months.
After a brief discussion, they said
that they would send an engineer out
to check for the upgrade. And in less
than 30 minutes an employee appeared
at my door, said that my relay was OK
and to prove it, he had switched on
the supply.
That was great; I could now do some
checking as the system had power. The
fan was making a lot of noise again so
I quickly dug out my multimeter and
found that there was power to the circuit board and to the compressor terminals. However, the copper refrigerant
pipes stayed at ambient temperature.
Could there be a gas leak somewhere
or was the compressor seized?
I turned off the power at the isolation switch and decided to check the
large “Motor Run” 47µF 230V capacitor
for the compressor motor. This was
mounted next to the control board and
if it was faulty, the compressor would
fail to start.
Unfortunately, my capacitance meter was still buried in a cardboard removals box somewhere but I did have
an old trick up my sleeve. Many years
ago, I learnt that I could do a rough
check on a capacitor using nothing
more that the high ohms range on a
multimeter and a stopwatch.
First, I completely discharged the
47µF start capacitor and disconnected
both terminals. I then set my meter to
the 200kΩ range, connected it to the
capacitor and kept an eye on both the
meter and my watch. The meter started
at 0Ω and rapidly increased until it read
“Out of Range”. The time taken for this
was just two seconds.
Next, I retrieved a spare 20µF 230V
motor start capacitor from my junk
box and repeated the test. This junk
box 20µF capacitor took 40 seconds to
charge – 20 times longer than the 47µF
capacitor from the heat pump!
So the 40µF compressor capacitor
from my heat pump wasn’t much of a
capacitor. I replaced it with the 20µF
unit from my junk box and switched
on the isolation switch. I then had to
wait for the system timer to count up
its obligatory 10 minutes (in case the
Freon gas pressures have to equalise).
At the end of this 10-minute period, the
relays clicked and the system sprang
into life.
I still couldn’t tell if the compressor
motor was working, due to the roaring
noise from the fan motor. However,
after a few minutes I detected that one
of the copper refrigerant pipes was becoming warm to the touch, which was a
good sign. It took a full 10 minutes before the pipe became hot, as the Freon
gas liquefied on the high-pressure side
of the system.
The system eventually ran for about
six hours, during which time the water
became increasingly hotter. It continued to work well with the 20µF motor
start capacitor, so I left it in place until
a replacement 47µF capacitor arrived.
Oh, the joy of being able to have hot
showers again – not to mention saving
SC
around $3000!
January 2015 63
By Nicholas Vinen
The Currawong Stereo
10W Valve Amplifier, Pt.3
In the last two instalments, we introduced the Currawong valve
amplifier, described its circuit and gave the PCB assembly and
wiring details. This final article describes the optional remote
volume control, the acrylic cover and the setting-up procedure.
Y
OU DON’T HAVE to build the
remote volume control board but
we think most constructors will want
to. It’s just so convenient when it comes
to setting the volume and is far easier
than having to wander over to to wind
the volume control up or down.
If you intend building the remote
control into the Currawong, you should
have already fitted the motorised pot to
the main board. The 50 x 50mm remote
board hangs from the front-right corner
of the main PCB via a tapped spacer
and is connected via a 4-pin header.
There is also a connection from the
remote control board to the pot motor.
64 Silicon Chip
If you aren’t fitting the remote control option to your Currawong amplifier, skip down to the “Initial power up
& testing” cross-heading below.
IR remote control circuit
The remote control circuit is shown
in Fig.12. It’s based on the low-noise
remote-controlled preamplifier used
in the Ultra-LD Mk.3 Stereo Amplifier
described in the November 2011 issue.
Basically, we took the remote control
parts used in that project and put them
on a separate PCB, without the preamplifier circuitry (which is already present on the Currawong’s main board).
It works as follows. The remote
control is set to generate Philips RC5
protocol codes which are picked up
by infrared receiver module IRD1.
Its output goes to pin RB0/INT on
PIC16F88 microcontroller IC2. IC2
decodes the remote commands and if
it detects a relevant code (volume up/
down/mute), it then uses its RB1-RB4
output pins to drive transistors Q10Q13 which are arranged in an H-bridge
configuration, to drive the pot motor
in the appropriate direction.
A 1µF capacitor is connected across
the motor terminals on the PCB to
reduce hash from the motor brushes
siliconchip.com.au
CON11
22Ω
+ 1 5V
REG 2 7805
LED1
GND
100 µF
25V
LED2
+5V
OUT
IN
10k
1 0 0 µF
100nF
GND
4
100Ω
1 µF
MMC
IRD1
3
1
λ
3 x 10k
2
3
4
5
6
7
8
9
10
(INPUT
BOARD
NOT USED)
17
3
LK7
LK7
5V:
MUTE RETURN
0V: NO MUTE RETURN
CON13
1
+5V
1 0 0 µF
2
14
MCLR
Vdd
RA0
RB3
RA4
RB4
1k
9
'1'
12
'2'
13
'3'
11
IC2
PIC16F88-I/P
RB6
RB1
RB7
RA1
RB5
RB2
X1 4MHz
22pF
22pF
16
OSC2
AN3
OSC1
RA2
K
MOTOR
–
1k
7
1k
8
Q11
BC337
10k
B
C
E
Vss
5
Q14
BC547
1 µF
MMC
C
B
2
Q13
BC337
E
ENDSTOP
ADJUST
VR3
1k
18k
B
C
E
10Ω
100nF
A
SC
CON12
K
1N4148
20 1 5
E
C
1 µF
MMC
D8
1N4148
18
1
B
C
+5V
15
Q12
BC327
E
A
D7
1N4148
RB0
B
1k
10
A
6
Q10
BC327
+
FROM MAIN
PCB (CON10)
K
CURRAWONG REMOTE VOLUME CONTROL
B
E
1
C
7805
IRD1
BC327, BC337,
BC 54 7
2
3
GND
IN
GND
OUT
Fig.12: the circuit for the add-on remote volume control is based on the one used in the Ultra-LD Mk.3 Stereo Amplifier
(November 2011). The infrared signal is received by infrared receiver IRD1 and passes to microcontroller IC2 which
decodes it and uses Q10-Q13 to drive the pot motor in the required direction. Power comes from the main board.
while there is also a capacitor soldered
directly across the motor terminals,
at the other end of the figure-8 wire
from CON12.
IC2 monitors the motor current
across a 10Ω shunt resistor. The feedback voltage is adjusted using pot
VR3 and goes through a low-pass RC
filter (18kΩ/100nF) before being fed to
analog input AN3 on IC2. IC2 can thus
detect the increase in current when the
pot hits one of its end-stops.
This feedback is used for the mute
function. When mute is pressed, the
motor is driven anti-clockwise until
the pot hits its minimum end-stop.
IC2 detects the increase in current and
shuts the motor off once minimum
volume has been reached. If mute is
then pressed again and LK7 is in the
high position, the motor is driven
clockwise for the same time as it took
to reach the end-stop, thus returning
the pot to the original volume level.
For this to work, VR3 must be adjustsiliconchip.com.au
ed correctly. If it’s set too high, the motor may stop prematurely while if set
too low, the motor may not stop once
minimum volume has been reached.
In the November 2011 design, IC2
flashed an acknowledge LED to indicate when a valid remote control
command was received. We have
used the same output (RA2) to drive
NPN transistor Q14 which pulls the
cathodes of small signal diodes D7 &
D8 low in acknowledgement. These go
to either end of red/green LED1 on the
main board via pin header CON11. As
a result, when a command is received,
LED1 is shorted out and so it flashes
off briefly. This avoids the need for an
extra LED to be fitted for the remote
control function.
The only change in the microcontroller software compared to the UltraLD Mk.3 remote preamp is to increase
the time that pin RA2 is driven high
upon receipt of a valid remote command. That’s done in order to make
the LED flashing more visible.
PIC microcontroller IC2 uses 4MHz
crystal X1 for time-keeping. This is required as the remote control commands
are sent at a particular frequency and
the micro needs to be able to “lock on”
to these commands to properly decode
them.
Multiple input option
We’ve kept the original design’s
Transformer Bolt
Earthing – Warning!
Note that the mounting bolts for
mains transformers T1 & T2 must not
be separately earthed (ie, via earth
leads) if the amplifier is mounted in a
metal chassis.That’s because running
earth leads to them would result in a
shorted turn on each transformer and
this would immediately blow the fuse
in the IEC socket.
January 2015 65
sistors here, since they fit more easily.
Solder the IC socket in place next,
with its notched end to the left, followed by REG2. Prepare the regulator
by first bending its leads down through
90° about 6mm from the tab, then attach the tab to the PCB using an M3
x 6mm machine screw and nut. Make
sure the screw is done up tightly before
soldering and trimming the leads.
The ceramic capacitors can go in
next; their polarity does not matter.
You will be left with a 1µF type to be
soldered across the motor terminals
later.
Follow with the small signal transistors, taking care to avoid getting the
three types mixed up. Crank their leads
out to fit the PCB pads using small pliers.
If you have a low-profile 4MHz crystal, this can be fitted to the top of the
board as shown in Fig.13. Otherwise,
you will need to cover the metal can
with a short length of 10mm diameter
heatshrink tubing, shrink it down,
bend the leads through 90° and fit it to
the underside of the board so that it’s
laying horizontally under PIC micro
IC2. In this case, solder its leads on the
top side of the board.
Note that in our photos, X1 is shown
bent over to the left but this was found
to interfere with the mains power
switch when the board was in place,
so we later moved it to the underside
and bent it in the other direction as
described above.
The right-angle polarised header
for the motor is also mounted on the
underside of the board, with its pins
facing the righthand edge, for the same
reason (again, shown differently in the
photo). Solder its pins on the top side.
X1* 22pF
LK7 SILICON
REG2
REG2
CHIP
1µF 7805
Motor
10k
CON12*
Q11
1k
1k
1k
100Ω
1µF
+
SEE TEXT
Q10
100µF 1µF Q12 Q13
+
44111110+
01111144
18k
100nF
22Ω
10Ω
D8 4148
Q14 4148
D7
VR3
1k
*
*
IRD1
CON11
4MHz
22pF
10k
1k
IC 2 PIC16F88-I/P
100µF
CON13*
100µF Remote Volume
10k
10k
10k
ADD RESISTORS SEE FIG.13
C 2014
MOUNT ON
BACK OF PCB
SEE TEXT
ON BACK OF PCB
Fig.13: follow this parts layout diagram to build the remote volume control PCB.
This sits just below the main board, so the available component height is limited. As
a result, motor header CON12 and crystal X1 (if full height) must be fitted at right
angles on the underside of the PCB (not on top as shown in the photo). In addition,
the electrolytic capacitors should be pushed all the way down to the board before
soldering or else bent over so that they will later clear the main board assembly.
10-pin header CON13, which was
used to connect to two other PCBs
for input switching. This enables the
possibility of fitting multiple inputs
to the Currawong and having remotecontrolled switching. This would
require the main Currawong board to
be built into a larger case with enough
room for the extra inputs and the relay
board required.
In the standard Currawong design,
(ie, no input switching), we just connect 10kΩ pull-up resistors from pins
7 & 8 (+5V) to pin pairs 1/2, 3/4 and
5/6 as shown so that the unit will
function without the input switching
board connected.
Power for the remote control unit
is derived from the Currawong’s unfiltered low-voltage DC rail of around
15V via pins 1 & 4 of CON11. This
supply goes through a low-pass RC
filter (22Ω/100µF) before being fed to
a standard 5V regulator, REG2.
The 5V output from REG2 is used to
power the micro and the motor but is
further filtered using a 100Ω resistor
and 100µF capacitor for infrared receiver IRD1 (plus an extra 1µF ceramic
bypass capacitor) in order to prevent
motor hash from interfering with infrared command reception.
Remote PCB assembly
The remote control PCB is coded
01111144 and the parts layout is
shown in Fig.13. Start by fitting the
two diodes, cathode stripe to the left,
then follow with the resistors. You
can check their striped bands against
the resistor colour code table (Table 3)
however it’s also a good idea to measure them with a DMM as the colours
can be hard to read clearly.
Note that while most of the resistors
are laid flat in the traditional manner,
the three 10kΩ resistors soldered to the
pads for CON13 will need to be fitted
vertically, with two leads sharing one
of the holes. We used mini 0.25W re-
Table 4: Capacitor Codes
Value
1µF
100nF
22pF
µF Value
1µF
0.1µF
NA
IEC Code EIA Code
1u0
105
100n
104
22p
22
Table 3: Resistor Colour Codes
o
o
o
o
o
o
o
No.
1
5
4
1
1
1
66 Silicon Chip
Value
18kΩ
10kΩ
1kΩ
100Ω
22Ω
10Ω
4-Band Code (1%)
brown grey orange brown
brown black orange brown
brown black red brown
brown black brown brown
red red black brown
brown black black brown
5-Band Code (1%)
brown grey black red brown
brown black black red brown
brown black black brown brown
brown black black black brown
red red black gold brown
brown black black gold brown
siliconchip.com.au
The 3-pin header for LK7 and 4-pin
header socket CON11 are fitted as
usual, to the top side of the board.
Put the shorting block over LK7 in the
position shown for mute return or fit
it in the alternative position to disable
mute return.
Trimpot VR1 is a vertical type, so
that it can be accessed once the remote
control board has been plugged into the
main board. You will need to bend its
rear pin out slightly to fit the mounting
pads. The three electrolytic capacitors
can then go in, with their longer (positive) leads orientated as shown.
The infrared receiver is fitted with
its leads bent so that the bottom of the
receiver is level with the PCB but it is
spaced about 6.5mm away from the
bottom of the board – see photo. You
will need to bend its leads backwards
close to the body of the receiver, then
crank them up, then bend them back
down again about 8mm behind the
body of the receiver to fit through the
holes on the PCB.
The final adjustment to make the
infrared receiver “look” through its
front panel hole will be done later,
when the board is fitted.
You can now finish the remote PCB
assembly by plugging microcontroller
IC2 into its socket, with pin 1 at left.
Installing the remote PCB
Solder a 4-pin male header to the
underside of the main PCB, at bottomright, to match up with the female
header socket (CON11) on the remote
board. While you’re at it, feed the leads
of the remaining 1µF ceramic capacitor
through the holes in the two terminals
on the back of the pot motor and solder
them in place. Trim off any excess lead.
Now you will need to make up the
lead for the pot motor. Start by cutting
a length of light-duty figure-8 cable so
that it will reach from the rear of the
pot over to the right-angle pin header
on the remote board. Be a little generous, keeping in mind the orientation
of the plug and the fact that you will
need some slack in order to plug it in.
Strip and separate the wires at both
ends of this cable and crimp both wires
at one end into two polarised header
pins. We like to solder the wires after
crimping (being careful not to get any
solder outside of the crimp section) so
that they can’t pull out.
Next, push the pins into the polarised block using a small jeweller’s
screwdriver. They should click into
siliconchip.com.au
The remote volume control PCB is
attached to a single mounting point
under the main PCB (see text).
place. If they won’t go in, don’t force
them; you may need to pull them out
and straighten the “springy” section
before they will go in properly.
Now solder the other ends of the
lead to the pot motor terminals (or to
the capacitor leads which are already
soldered to them). Unfortunately,
there’s no good way to figure out the
polarity so you’ll just have to pick one
and then reverse the connection if it’s
wrong but we’ll get to that later.
Next, insert an M3 x 6mm machine
screw through the sole mounting hole
on the remote control board, head
on the underside, with a shakeproof
washer under the screw head. Place a
Nylon washer on top and then screw
it into an M3 x 9mm tapped spacer.
Do it up nice and tight.
Plug the remote board into the
4-pin header on the main board, then
use another M3 machine screw and a
flat washer to hold it in place via the
provided mounting hole on the main
board. Finally, plug the polarised
header from the motorised pot into
CON11 on the bottom of the remote
board and you are ready to test it.
Note that the pot motor lead should
not be able to reach the mains switch
which, in any case, should be completely covered in heatshrink tubing.
The next step is to drill a 4mmdiameter hole in the front panel for
the IR receiver. This 4mm hole should
be positioned exactly 27mm to the
left of the power LED (LED1). Having
done that, leave the front panel off for
the moment, so that you can set VR1
correctly and if necessary, swap the
motor polarity.
Initial power up & testing
When we left off last month, we had
built the PCB and plinth, wired up the
WARNING! HIGH VOLTAGES
High AC and DC voltages are present in this amplifier. In particular, mains
voltages (230VAC) are present on the IEC socket and the primary side of the
mains transformers (including the wiring to the power switch). In addition, the
transformer secondaries together provide a 114VAC output and the power
supply produces an HT voltage in excess of 300V DC which is present on
various parts of the amplifier circuit (including the output transformers).
Do not touch any part of the amplifier or power supply circuitry when
power is applied otherwise you could get a severe or even fatal electric
shock.
The blue LEDs in the circuit indicate when high voltages are present. If they
are lit, the power supply and various parts on amplifier board are potentially
dangerous. The completed amplifier must be fitted with Perspex covers
as described in Pt.3 this month, to ensure safety.
January 2015 67
Parts List: Currawong Remote Control
1 double-sided PCB, code
01111144, 50 x 50mm
1 4-pin header, 2.54mm pitch
(CON10)
1 4-pin female header, 2.54mm
pitch (CON11)
1 1kΩ mini vertical trimpot (VR1)
1 4MHz crystal, HC-49 (low-profile
if possible*) (X1)
1 3-pin header, 2.54mm pitch, with
shorting block (LK7)
1 18-pin DIL IC socket
1 2-pin right-angle polarised header
1 2-pin polarised header plug with
crimp pins
1 200mm length light-duty figure-8
cable
1 9mm tapped Nylon spacer
3 M3 x 6mm machine screws
1 M3 nut
1 3mm ID shakeproof washer
1 3mm ID flat washer
1 3mm ID Nylon flat washer
1 universal remote control (eg, Altronics A1012, Jaycar AR1719)
power supply and mounted the PCB
in place. Now it’s time to power it up
without the valves in place and check
that the power supply is working.
Start by popping the fuseholder
out of the mains input socket using
a flat-bladed screwdriver, then fit the
fuse (plus a spare) and re-install it.
Leave LK4 & LK5 off the board for now.
From this point on until the top cover
is fitted, be careful to avoid putting
either of your hands near any of the
components on the top of the board
– touch the assembly using insulated
probes only.
Now set your DMM to DC volts (with
a range that goes up to at least 300V),
plug in the mains cord, switch on and
observe the LEDs. The four blue LEDs
adjacent to output transformers T3
& T4 (LEDs3-6) should immediately
light. Blue LED2, next to the headphone socket should remain off while
LED1 (power) should be red.
If your amplifier doesn’t display this
behaviour, switch off immediately and
wait for the HT voltage to drop to a safe
level before troubleshooting. This can
be monitored by connecting the negative probe of your DMM to one of the
valve socket mounting screws and the
positive to the cathode (striped end)
of D1. Wait for it to drop below 40V
68 Silicon Chip
Semiconductors
1 PIC16F88-I/P programmed with
0111114A.HEX (IC2)
1 infrared receiver (IRD1)
1 7805 5V linear regulator (REG2)
2 BC327 PNP transistors (Q10,Q12)
2 BC337 NPN transistors (Q11,Q13)
1 BC547 NPN transistor (Q14)
2 1N4148 signal diodes (D7,D8)
Capacitors
3 100µF 16V electrolytic
2 1µF monolithic multi-layer ceramic
3 100nF monolithic multi-layer
ceramic
2 22pF disc ceramic
Resistors (all 0.25W, 1%)
1 18kΩ
1 100Ω
5 10kΩ
1 22Ω
4 1kΩ
1 10Ω
* If using a full-height can crystal,
add 1 x 20mm length of 10mmdiameter heatshrink tubing
before touching the board and to 10V
before doing any soldering or other
work on the board.
Assuming blue LEDs3-6 are working properly, these indicate the state of
the HT rail. They will be glow brightly
when dangerous voltages are present
and dim significantly once the HT
capacitors have discharged to a safe
level. Note that they will continue to
produce a small amount of light for a
long time after switch-off but will be
quite dim by the time the HT rail drops
below 10V or so.
If these LEDs do not light up, one or
more could be installed with the wrong
polarity or might be faulty. Once the
HT has discharged, you can connect a
current-limited voltage source across
each LED to check them. Some (but not
all) multimeters can light blue LEDs
when set on diode test mode.
If LEDs3-6 are working but LED1
does not come on, this points to a
possible fault in the low-voltage AC
wiring, the regulator section or a problem with IC1 or Q5-Q8 and associated
components. Check these areas, starting by measuring the voltage between
pins 4 & 5 (the two topmost pins) of
one of the 9-pin valve sockets, which
should be stable at just above 12V and
proceed from there.
On the other hand, if LED2 is on,
that suggests a fault in Q9 or its base
resistor or a short circuit in that section
of the board.
Assuming that you get the correct
LEDs lighting, LED1 should turn green
about 20 seconds after switch-on. During this time, you can check that the
various voltage rails are correct.
First, measure the DC voltage between pins 4 & 5 of the 9-pin valve
sockets as mentioned above and check
that you get close to 12.3V. You can
also confirm that there isn’t too much
ripple on the regulated supply by
measuring the AC voltage between
these pins; it should be below 100mV.
Now check the unfiltered HT supply
voltage, between the cathode of D1
and one of the valve socket mounting
screws. You should get a reading close
to 320V.
The filtered HT voltage can be measured between pin 3 of any 8-pin valve
socket and one of the earthed mounting screws. Pin 3 is the pin closest to
you, on the right – see Fig.6 in Pt.2
last month. This should give a low
reading (a few volts) initially while
LED1 is red and then it should shoot
up to 318V or so (ie, a couple of volts
below the unfiltered HT rail) as soon
as LED1 turns green.
The other filtered HT rails can also
be checked, at pins 1 & 6 of each 9-pin
valve socket (lower-right and upperleft respectively). With the valves not
yet fitted, these should all be pretty
close to the main filtered HT rail at
around 318V although they will rise
more slowly after LED1 turns green.
Testing the remote board
If you have fitted the remote control
board, this is a good time to test it
now that you have determined that
the power supply is working properly.
First, set your remote control to one of
the supported codes. For the Altronics
A1012, this is either 023 or 089. For
the Jaycar AR1719, use 97948 (Philips
02 CJ 412 TV).
Now aim the remote control at the
receiver and hold down the volume up
or volume down button. You should
see the acknowledge LED (LED1) flash
and the pot shaft rotate.
If nothing happens and you have
definitely programmed the remote
for the correct code then that suggests
either a fault on the remote control
board or an improperly programmed
PIC micro. Check that the board’s 4-pin
siliconchip.com.au
header (CON11) is plugged in correctly
to the main board and that there is
around 15V between pins 1 & 4.
If the pot rotates in the wrong direction, you will need to switch off
and reverse the motor connections
(once the HT rail has discharged sufficiently). This can be done by using
a fine flat-bladed screwdriver to press
in the retention tabs on the polarised
header pins, then sliding the pins out
of the housing (while holding the tabs
down) and refitting them so that they
are swapped around.
Once you have the pot motor rotating correctly, press the mute button
and check that the pot rotates to the
fully anti-clockwise position and
stops. If it doesn’t stop, turn VR1 clockwise until it does. If it only rotates part
of the way, turn VR1 anticlockwise
until it mutes properly.
Ideally, VR1 should be set about
mid-way between the too-low and
too-high positions, to avoid later malfunctions if the pot shaft’s mechanical
resistance increases slightly.
Note that you may need to manually
rotate VR1 clockwise to about half-way
(or use the volume up button) before
the mute function can be tested. Once
it has been set up, you can refit the
front panel and if necessary, bend the
leads of IRD1 and LEDs1&2 so that they
line up with their respective holes.
Fitting the valves
Assuming that the voltages check
out, switch off the power and wait for
the HT capacitors to discharge, then
plug in all the valves. The sockets
will probably be very stiff the first
time they are fitted; a small amount of
contact cleaner on the pins can help
ease them in.
Don’t push them too hard; you will
need to wiggle them in and it’s better to push down on the octal valves
by holding the base rather than the
envelope. The 12AX7s have no base
but they should require less insertion
force anyway.
The glass envelopes are pretty strong
but they can be broken with enough
force and there’s also the possibility
of the glue holding the envelope to
the base giving way. So slowly wiggle
the valves in. After the first couple of
insertions, the sockets will loosen up
and fitting/removing the valves will
be a lot easier.
This may seem obvious but we
should point out that V5-V8 will get
siliconchip.com.au
This is the laser-cut clear acrylic top cover for the main PCB assembly (the
white colour is a reflection). Not shown are the front cover and the four pieces
that are attached as shield plates to guard the output transformer connections.
Acknowledgements: we’d like to thank Ada Lim and the people at Sydney
hackerspace “Robots & Dinosaurs” for their help with the laser cutter.
very hot during operation and you
should not touch them! Even brief
contact can result in a painful burn.
Consider that with the glass envelopes
and about 25W dissipation, they are
similar to an incandescent light bulb
– ie, they get very hot!
Now, while we have provided a minimal output load on the PCB (~470Ω
per channel), it’s still a good idea
to hook up a “proper” dummy load
until you’re ready to connect some
speakers, to prevent flash-over due to
excessive voltage when the amplifier
is lightly loaded. A couple of 10Ω 5W
resistors connected across the speaker
terminals will do, although any value
in the range of 3.9-100Ω is acceptable.
Turn the volume control right down
initially. If you have an oscilloscope
and signal generator, you can feed sinewave signals into the inputs, power the
unit up, advance the volume control
and check the shape of the output
waveforms on each channel. Otherwise, all you can really do is hook up
a signal source (eg, a CD player) and
some speakers and listen to it.
Note that there won’t be much
output (if any) until several seconds
after HT has been applied (ie, LED1
has turned green), as it takes time for
the various bias voltages in the circuit
to stabilise. And it takes several more
seconds until the amplifier can deliver
a significant portion of its rated power.
The warm-up is complete and the full
~10W/channel is available around 10
minutes after switch-on.
Before that, you’ll probably run into
clipping at 8-9W per channel. It simply
takes that long for the valves to reach
operating temperature.
Assuming it appears to be working
normally, switch off, turn the volume
control back down and fit shorting
blocks to LK4 and LK5 to enable global
feedback. This dramatically lowers
distortion, from around 0.5-1% down
to 0.05-0.1% (ie, by at least an order
of magnitude) so we definitely recommend operating the amplifier with
these links in.
Now switch the amplifier back on,
slowly turn the volume back up and
check that it’s still working properly.
If you get a high-pitched squeal, you
may have wired the output transformers improperly, turning the negative
feedback into positive feedback and
causing oscillation. You’ll have to
switch off and check the transformer
wiring and feedback components (resistors/capacitors).
Making the top cover
The top cover is vital since contact
with some of the components during
operation could be lethal. We’ve designed a clear acrylic top cover to suit
the plinth as described last month, so
you can still see all the circuitry while
keeping it safe. It also helps to keep
dust and dirt off the board (although
January 2015 69
ACRYLIC SHIELD
PLATES
INSULATE ALL TRANSFORMER
TERMINALS WITH A DOUBLE
LAYER OF HEATSHRINK TUBING
NEUTRAL-CURE SILICONE
The two shield plates for each output transformer are glued together at right
angles and then glued at right angles to the main cover. Some neutral-cure
silicone is also used to provide further protection and to help hold the acrylic
shield plates in place.
Another close-up view of the output
transformer shield. Don’t leave
this shield out – the transformer
terminals operate at 308V DC so it’s
an important safety feature.
not entirely, since there are cooling
slots cut into it).
Technically, acrylic plastic is polymethyl methacrylate and is sold (with
some variations in the formulation)
under several brand names, including
Plexiglas, Perspex and Lucite.
The cover panel likely won’t be
included in any kits but you can purchase it direct from SILICON CHIP (eg,
via our online shop). Alternatively, if
you have access to a laser cutter with
a bed of at least 300 x 300mm, you
could cut it yourself. The cutting file
is available on our website in various
formats including DXF, SVG and PDF
(as a free download for subscribers).
70 Silicon Chip
We used a laser cutter with a 50W
CO2 laser and found that we got good
results cutting the 3mm acrylic using
two passes at 50% power.
Once you have your cover, check
which way around it goes (the cutouts are not symmetrical), then slip it
over the top of the assembly to make
sure that it fits in place and that the
plinth mounting holes are not too far
out of their expected positions. Leave
the protective film on for the time being. If you’re using valves with large
envelopes (eg, KT66s) then you may
have to remove them in order to fit
the cover. 6L6s can be left in place.
Push it down until it sits on top of the
low-profile 39µF capacitors.
If it won’t go all the way down,
chances are you haven’t positioned
transformers T3 & T4 in the middle
of their mounting locations. It’s possible to carefully loosen their mounting screws, just enough to move the
transformers, then tighten them again
without having to remove the board.
Now remove the cover and peel the
protective film off the five pieces to be
glued. These all have crenellated edges
(like a castle rampart, with a series of
square protrusions). While super glue
(cyanoacrylate) is suitable for gluing
acrylic, we strongly recommend that
you use a proper, solvent-based adhesive as this will give a much stronger
bond.
We used SciGrip Weld-On 16, fastsetting “clear, medium-bodied solvent
cement”. This states on the label that
it’s suited for Butyrate, Polycarbonate,
Styrene and Acrylics. You are unlikely to find this type of adhesive in
a hardware store but should be able
to get it from a plastics supplier. Ours
came from Plastix [Sydney (02) 9567
4261; Sydney Northern Beaches (02)
9939 0555].
This forms a strong bond quickly
so you only have about 30 seconds
to mate the pieces and ensure that
they are square before it’s too stiff to
manipulate. Full strength is achieved
after about 24 hours. The bond is clear
but you don’t want to get excess adhesive on the material as it will affect the
surface finish and you definitely don’t
want to drip it on the cover. It tends to
get a bit “stringy” (sort of like melted
mozzarella) after coming in contact
with the acrylic.
In fact, to give yourself the best
chance of getting a clean-looking bond,
we’d recommend squeezing some of
the adhesive out onto a smooth piece
of timber or metal (not plastic!) and
using a small paintbrush (hair, not
Nylon) to apply it to the acrylic. This
makes it easier to control how much
you are applying compared to using
the tube directly. You’ll also need a
clean rag on hand.
Start by gluing the two pairs of
transformer shield plates together.
Before applying any adhesive, figure
out which surfaces will be in contact
(they are on two faces). That done,
apply a thin layer of adhesive to all
those surfaces, then press the two
pieces together. Make sure that they
are at a 90° angle and that the tabs are
fully inserted into the slots. Wipe off
any excess adhesive and be careful not
to get it on areas of the acrylic away
from the join.
You can then lay the part on its
side to cure. Do the same for the other
identical piece. Note that while there
are two different orientations in which
these pieces can be glued together, it
doesn’t matter which way you do it as
they are symmetrical.
Once you’ve done those, you can
move onto gluing the front and top
sections together. This is a much larger
join but the technique is basically the
same. However, the orientation does
matter in this case – be sure to glue
the front section on such that when
the cover is in place, it hangs down
rather than sticks up. Acrylic adhesive
is very strong so if you get it wrong, you
probably won’t be to get them apart
siliconchip.com.au
This view shows the amplifier
with the acrylic cover in
place. It provides an attractive
finish while protecting against
dangerous voltages. Note that
the output valves get hot so
be sure to place the amplifier
away from young children
and where there is plenty of
ventilation.
Before Switching On
• Check that the IEC socket’s
Earth pin is connected to all
exposed metalwork.
• Check the isolation between the
Active & Earth pins and Neutral
& Earth pins of the IEC socket.
• Check the output transformer
and mains switch insulation. The
output transformer terminals
must be fully insulated with a
double layer of heatshrink.
• Don’t touch any parts if the unit
is being tested without the cover.
• Be sure to fit the cover when
testing is complete.
again without breaking something.
Again, it’s important to make sure
that the sections are at right angles
and pushed fully together to get a neat
result. You will need to peel away the
protective film from the top cover near
the front but it’s a good idea to leave
it in place on the rest of the panel
to protect it during gluing. The best
way to do this is to peel back the film
around the area to be joined and then
use a pair of scissors to cut a strip of
it away, so the rest can be laid back
down on the surface.
Once you’ve joined those parts,
leave it for a few minutes and it should
then be strong enough to allow you to
glue the two transformer cover pieces
prepared earlier into the crenellated
siliconchip.com.au
sections at the front of the transformer
cut-outs. Glue the pieces in so that the
horizontal pieces at the top project out
over the cut-out areas in the top cover
below (ie, not pointing towards the
front of the panel).
Fitting the top cover
While full strength won’t be achieved
for 24 hours, the joins should be strong
enough after about 10 minutes to allow you to (carefully) fit the cover to
the amplifier. Again, if using KT66s
or other valves with envelopes larger
than the 6L6s, remove them first.
Lower the cover until it’s resting
on top of the five low-profile capacitors. Take care to avoid touching the
underside as this may leave visible
fingerprints. If you do get fingerprints,
polish them off with a soft cloth.
You may need to push down on it
gently but firmly to get it to go all the
way down. If it won’t go, re-check the
positioning of T3 and T4 and move
them slightly if necessary.
You can then mark out the seven
mounting hole positions around the
perimeter of the cover and drill 2mm
pilot holes a few millimetres deep in
each location. You can remove the
cover to do this if you want to (which
makes it easier to remove the resulting wood particles), however it isn’t
strictly necessary.
Next, peel the protective film off
seven of the small doughnut-shaped
laser-cut pieces. Once you’ve cleared
the area around each hole, slip these
“doughnut” spacers under the cover
and push them into place (eg, using a
screwdriver). You can then feed a 4G
x 12mm self-tapping screw in from the
top and do it up until the top panel is
resting on the spacer. You may want
to do up all seven screws loosely and
then slightly adjust the top cover position before making them all tight to
hold it in place.
All that’s left now is to squeeze a
small bead of neutral-cure silicone
sealant into the gap at the upper-left
corner of each output transformer.
This helps hold the acrylic covers in
place and also prevents small fingers
or other objects from being pushed
into this gap (see photo). The easiest
way to do this is to cut a thin strip of
plastic from a take-away container lid
or similar, place a bead of silicone on
the end and use it like a trowel to push
it into the gap and wipe off any excess.
Once it has all dried you can plug
the valves back into their sockets and
the amplifier is ready to go! Note that
the output valves get hot in operation
so be sure to place the amplifier where
SC
there is plenty of ventilation.
January 2015 71
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Issue:
January
2015
PRITCHARD RD
285
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T 2000
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X 0202
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include shoulder strap.
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T 2630 Iron & Cartridge.
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119
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22.50
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D 0505
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T 4704
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T 4632A
Never lose a screw again when working!
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22
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Combo Wire
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Hard wearing 4m plastic coil makes
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January 2015 73
BUILD IT YOURSELF ELECTRONICS CENTRE
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74 Silicon Chip
BUILD IT YOURSELF ELECTRONICS CENTRE
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anuary
2015 75
Christchurch JShirley
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PC +64 3 3543333
Your first project: a
Pico
Mini
Cube
One of our neighbours at last
September’s Electronex show in
Sydney was a company called PicoKit,
which had a range of educational
projects especially for beginners.
It’s been a while since we featured a
real beginner’s project in SILICON CHIP so with
PicoKit’s assistance, we’re going to publish one now
– and it’s ideal for school holiday fun!
WANT
SEE A MOVTO
THE PICOM IE OF
INIC
IN ACTION UBE
?
Go to
siliconchip
video/pico .com.au/
minicube
Design by Philip Tallents* Article by Ross Tester
W
hen we say a beginner’s project, the PicoMiniCube
is just that, with about 20 components (mainly
resistors) to solder onto a small PCB and 27 LEDs
to solder together into a 3-wide x 3-deep x 3-high matrix,
forming the display.
It’s powered by three AA batteries and driven by a preprogrammed microcontroller, a PIC16F1503.
When finished, the PicoMiniCube gives an eye-catching
display, perfect for school projects and electronics/radio
club demonstrations.
Best of all, it sells for less than $30.00!
Because of the way the LEDs are soldered together, you’ll
gain some valuable soldering experience, not to mention
component identification.
If it’s not 100% perfect, it will either not work properly
or not work at all!
What you’ll need
First up, you’ll need the PicoMiniCube kit. It’s available
via the PicoKit website (www.picokit.com.au) and sells for
$26.05 (inc GST) with a pre-programmed PIC chip. If you
want to (or can!) program your own PIC, the kit with an un76 Silicon Chip
programmed PIC sells for $24.95 – hardly worth the hassle!
You can order it with blue LEDs, green LEDs or red LEDs.
While you might be tempted to used different colour LEDs
for different levels of the matrix, remember different colour
LEDs have different apparent brightnesses, so the display
might not look as eye-catching.
As far as tools are concerned, the requirements are pretty
basic: a 30W soldering iron (with a reasonably fine tip), some
electronics solder (0.7mm, rosin-cored), a pair of needlenose pliers (fine), a pair of small side cutters and finally, a
wet sponge to clean your soldering iron tip.
First of all . . .
When you open a kit, you should always check to see
if all the components (parts) are there. It’s most unusual
to find anything missing in a kit but it’s better to find out
now than at 8pm on Saturday night when you can’t finish
the project!
Perhaps you need some help in identifying the components – we’ve put some illustrations in the parts list to
help you there.
Next, divide the components into the various types –
siliconchip.com.au
resistors, capacitors, transistors, ICs (integrated circuits
– there is only one in this project), and the “hardware”–
sockets, connectors, the PCB, Nylon standoffs and nuts, etc.
The LEDs are normally supplied in their own bag which
keeps them separate – for now, you might as well leave
them in there.
Many hobbyists like to use small containers to hold the
separate “bits” for projects – tiny plastic food containers,
emptied(!) and cleaned, are ideal.
Or if you can get your hands on some, a scrap of polystyrene foam makes a great storage area because you can
push the component leads into it!
Where a component (especially an IC) is supplied in
black foam plastic, leave it in that until ready for use: the
foam is actually conductive and is designed to stop static
electricity damaging sensitive components.
The next step is to identify the resistor values. With
young eyes, it’s not too difficult to read the colour bands
and so work out the values but as many colours are easy
to mistake (orange and red, for example), nothing beats
using a digital multimeter (on Ohms scales, of course) to
get a definite reading.
Tolerance
You will almost certainly discover that a resistor is not
exactly the value its colour code suggests. The band at the
end of the resistor gives its “tolerance”, or how close it is
to its marked value. These days, it’s most unlikely to be
worse than 5% and more than likely better.
If its colour bands are brown, black, green and gold,
that means it is 1.0 megohms (1M), with the gold band
meaning it is plus or minus 5% of that value – so the actual
value could be anywhere between 950,000 ohms (950k)
and 1,050,000 ohms (1.05M).
That’s fine – the circuit is designed to take that variation
into account. If the circuit actually needs a closer tolerance,
it will say so. A 1M, 1% resistor could be anywhere from
990,000 ohms (990k) to 1,010,000 ohms (1.01M). Even
closer tolerance resistors are available but the closer they
are, the more expensive they are – and, as we said before,
most circuits don’t need them.
Incidentally, the same comments apply to virtually ALL
“passive” components – capacitors, inductors, and so on.
You’ll find that some components have much wider tolerances – electrolytic capacitors being a case in point with
10% and even 20% not uncommon.
Fortunately, there are only three types of resistors in
this circuit – ignoring the last (tolerance) band, 100
(brown-black-brown), 330 (orange-orange-brown) and
1M (brown-black-green).
In many cases, up to 1000 ohms value, the symbol
(or decimal point) is replaced with the letter “R” – so a
100R would mean 100; 2R2 would mean 2.2 and so
on. Above 1k, the letter k serves the same purpose –
100k would mean 100,000 ohms, 4k7 would mean 4.7k
or 4,700. Above 1M, the M symbol does the same: 1M
means 1M, 3M3 means 3.3M, etc. In this project, the
white PCB overlay is marked using this standard.
There’s only one capacitor used here, a tiny 1000nF (or
1F) ceramic type. It will probably be marked “105” – that
means it is 10pF followed by five zeros or 1000000pF. Converting from pF to F means we move the decimal point
six places to the left and end up with 1.000000F.
siliconchip.com.au
Most of the components solder to the top side of the PCB
which becomes the underside with the LED display on top.
Confused? Just remember that all components except the
LEDs and on/off switch are on the side with the component
overlay printed on it.
There’s also only one type of transistor – a BC327 PNP
switching transistor in a “TO92” case. Don’t worry too much
about what those numbers mean – it will all come in time!
Of all the above-board components, only the transistors
and integrated circuit are polarised (ie, orientation matters
on the PCB) – and we’ll look at them in more detail shortly.
The “display” components, which mount under the board
are the 27 LEDs, (light-emitting-diodes) which could be
red, green or blue, depending on what you have ordered.
Like all diodes, LEDs are also polarised. You will note that
the two legs of the LED have different lengths – the longer
leg is its anode (A), while the shorter leg is its cathode (K).
Why is it K, not C? To avoid mixing it up with the “Collector” of a transistor, which has the abbreviation “C”. (K
stands for Kathode, the German word for . . . you guessed it!).
About the only other component, as such, is the microcontroller, a PIC16F1503 (it could be a PIC16F1505 – in
this circuit, they are functionally identical).
There are loads and loads of PIC types; the 16F1503 is
large enough to contain the code stored within it and has
enough outputs to drive the 27 LEDs.
The code, also called the “program”, can be changed by
erasing it and writing new code into its memory; however,
you need to know how to write programs to do so. Otherwise, once erased, it will sit there like a dumb, black,
plastic thing with lots of legs!
As we mentioned earlier, the PicoKit normally comes
with the PIC already programmed – and there’s not much
you can do which will erase it unless you specifically go
about doing so – so rest easy!
The PCB (Printed Circuit Board)
The PicoMiniCube uses a double-sided board (ie, there
January 2015 77
Q1
BC327
A
l LED
19
K
A
l LED
10
K
A
l LED
1
K
A
A
l LED
20
K
A
l LED
21
K
A
K
A
K
K
A
l LED
4
K
l LED
15
K
A
l LED
3
A
l LED
14
K
A
l LED
2
K
A
l LED
13
K
l LED
24
K
A
l LED
12
A
l LED
23
K
A
l LED
11
A
l LED
22
A
l LED
5
K
l LED
6
K
K
A
A
l LED
25
l LED
26
K
K
A
A
l LED
16
l LED
17
K
K
A
A
l LED
7
l LED
8
K
K
E
B
C
330W
A
l LED
27
K
Q2
BC327
E
B
C
330W
A
l LED
18
K
Q3
BC327
E
B
C
A
l LED
9
330W
K
5x 100W
4x 100W
1
13
5
6
12
Vdd
RA0/AN0
AN5/RC1
RC5/PWM1
AN7/RC3
RC4/C2OUT
AN4/RC0
S2
(ON
PCB)
9
1mF
7
MMC
10
11
RA1/AN1
AN2/RA2
IC1
PIC16F1503
8
Q4
BC327
AN6/RC2
LEDS
K
A
BC327
RA3
AN3/RA4
E B C
RA5
4
B
C
3
4.5V
2
Vss
14
PICOMINICUBE
S1
E
1M
Ó2014
Fig.1: the LEDs are arranged in three layers of nine and are powered by the four transistors switching on and off according
to the outputs of the PIC microcontrollers, which in turn are controlled by the code, or program, previously stored in the
PIC. Our LEDs are shown here as red but they could be equally be green or blue, depending on what you order.
are tracks on both the top and bottom) though in this case
they’re quite hard to see. All the tracks are covered with a
black “solder mask” which makes soldering a bit easier. But
there is a downside – to see the tracks under the mask you
have to hold the board so the light reflects in a certain way.
It’s easy to identify the top and bottom of the board – the
top side has the component positions and other information
printed on it – what is known as a “component overlay” or
“silk-screen overlay”. (It’s called that because a technique
called silk-screen printing is traditionally used to print the
overlay onto the PCB. It’s a process that’s commonly used
for printing a vast array of items, probably including the
T-shirt that you have on right now!)
In this particular PCB, there are also components marked
on the bottom side but they are only the bottom layer of
LEDs in the display and the on/off switch.
The holes in the board, into which you place the components and solder them in place, are “plated through”
78 Silicon Chip
(where required) so that when you solder one side, the
opposite side also solders.
Soldering
We’ve almost glossed over one of the most important
parts of building this, or any other, project – soldering. Kit
suppliers tell us that incorrect component placement or
orientation accounts for only about one third of errors in
construction. The other 90% is poor soldering!
Not only do you need to solder the LEDs together, you
also need to solder components to the PCB. And some of
them have pins that are pretty close together. Good soldering
is a skill that all hobbyists need to develop – you need the
right equipment and as mentioned earlier, the right solder.
Beginners often ask why they need to use solder especially made for electronics work and not “ordinary” solder
sticks with a tin of flux, such as that used by plumbers and
sheet metal workers.
siliconchip.com.au
How it works
The PicoMiniCube consists of two main sections: the 3 x 3
x 3 LED matrix forming the display and the circuitry to drive
it, consisting mainly of a PIC microcontroller. First of all, we’ll
look at the 27 identical LEDs.
A light-emitting-diode, or LED, behaves in a very similar way
to other diodes – that is, it conducts, or turns on, only when its
anode (A) is made sufficiently positive with respect to its cathode
(K). However, it has one major difference to other diodes – when
it conducts, it emits light.
The colour of the light depends on the materials from which
the LED is made – and you can get a wide range of colours,
ranging from infrared (ie, you can’t see it glow) right through
all the colours of the rainbow, to ultraviolet (again, you can’t
see it glow but it does make many things glow themselves!).
The various colour LEDs require different voltages across
them – red LEDs, for example, require a much lower voltage
to make them glow than do blue. The 4.5V supply (3x AA cells)
is sufficient to light any colour LED. In most cases, a resistor
is necessary to limit the current through the LED, otherwise it
can burn out. That’s the purpose of the 100resistors in series
with each of the groups of LEDs in this circuit.
The LEDs are switched on and off by the microcontroller, IC1.
This has been programmed with code specifically designed to
power the LEDs in certain patterns. The program tells each of
the output pins (pins 1-12) when to go “high” or “low” when
appropriate.
On its own, the microcontroller can’t supply enough current
to make the LEDs glow brightly, so connected to pins 1, 2 and
3 are small PNP transistors. These act as switches, turning on
and therefore supplying power from the battery to the layers
of LEDs when the microcontroller sends pins 1, 2 and 3 low.
A fourth transistor, Q4, is used to supply extra power to Q3
because pin 4 cannot even handle the current necessary by itself.
If the cathodes of the LEDs were connected to the negative
supply, they would light up whenever the transistors turned on.
But they aren’t: each LED group is connected (again via that current limiting resistor) to yet more outputs of the microcontroller.
Again, these outputs go high and low as the microcontroller
program tells them to. To make the LEDs glow, the pins 5-13
microcontroller outputs need to go low at the appropriate time,
so current can flow through the LEDs, through the microcontroller to the negative supply.
So to light up, the group of LEDs need one of the transistors
to turn on AND the associated microcontroller output to go
low – for example, when Q1 turns on because pin 2 goes low
and when pin 12 goes low, LED 19 will light. If at the same time
pin 13 goes low, LED 22 will light. When the transistor turns
off or either microcontroller output goes high again, it/they will
go dark. If pin 12 stays low but Q2 turns on, LED 10 will light.
The result of the continual switching on and off is the pattern of LEDs lighting in the PicoMiniCube whenever it is turned
on. You can’t control either the LEDs or the pattern – these
are determined by the program. Your choices are power on
or power off!
use an iron that is either too hot or too cold – either
The reason is twofold: (1) plumber’s solder
runs the risk of making a “dry joint”, which often
has a much higher melting point than electronics
results in the solder not properly “taking” to one
solder. This heat could damage components
part or the other.
and (2) ordinary soldering flux is usually quite
This can mean that there is no electrical conneccorrosive. That doesn’t matter so much with thick
tion
between them from the start, or it can mean
copper pipes, etc but in quite a short time would
that it’s a fault waiting to bite you later on when
play havoc with the very thin copper tracks on a
it inevitably fails.
PCB and/or component leads.
Another common mistake, made even by those
Just as importantly, electronics solder is norSolder for
with
many years experience, is to attempt to solelectronics use is
mally supplied as a relatively fine “wire” and
der oxidised wires and leads. Copper (especially)
is much easier to handle than a stick of solder, normally supplied
in 500g or even
but also tin and most other metals oxidise over
particularly in fine work. It also usually has the
time and solder simply will not take to them
flux, or rosin, running through its core – and that 1kg rolls – various
gauges
(thicknesses)
properly. If in doubt, scrape clean the lead or
flux is specifically designed (it’s non-corrosive)
are available but
part to be soldered beforehand with some fine
for use in electronics.
0.7mm to 1mm are
emery cloth or even a sharp hobby knife.
A common mistake that beginners make is to
popular.
FLAT EDGE
ON LED BODY
ANODE
CATHODE
(K)
CATHODE
ANODE (A)
An old block of styrene
foam (eg, from appliance
packaging) makes
component storing easy . . .
siliconchip.com.au
Identify the LED leads – the
anode is the longer lead
and there’s a flat on the LED
body against the cathode.
On 18 of the 27 LEDs, bend
the cathode down 90° with
needle-nose pliers and bend
it straight 90° again.
Now bend the anodes of 12
of them 90° out in the “9
o’clock” direction. Notice
the “crank” in the cathode.
January 2015 79
CATHODES
(LED17,
LED26)
ON
LED7
LED7
CATHODES
(LED16,
LED25)
LED8
LED9
“LED” SIDE OF PCB
(BECOMES THE UPPER SIDE)
330W
100W
100W
PicoKit
–
+
CATHODES
(LED18,
LED27)
Q3
Q2
Q1
www.picokit.com
There are three layers of nine LEDs, two of
which are made up as shown here. The top
row cathodes solder to the cathodes of the
middle row (below), The middle row cathodes
and both leads of the bottom layer solder to
the PCB. However, to get the spacings right,
you can temporarily place the LEDs in their
respective spots in the PCB – but be very
careful not to solder them in (yet!). The crossconnections (shown in grey) can be made up
from excess component lead clippings.
LED6
Q4
330W
100W
S1
LED5
100W
1M
LED4
OFF
PROG1
K
= NO CONNECTION
CATHODES
(LED15,
LED24)
IC1
PIC16F1503
CATHODES
(LED14,
LED23)
CATHODES
(LED13,
LED22)
© 2013
FLAT
SIDE
100W
100W
1m F
A
A
K
LED2
PicoMiniCube
A
= SOLDER
K
A
A
LED3 CATHODES
(LED12,
LED21)
–
K
K
A
100W
100W
K
LED1
K
CATHODES
(LED11, LAYER2 LAYER3
LED20)
+
FLAT
SIDE
A
A
K
A
K
CATHODES
(LED10,
LED19)
330W
100W
“SCREENED OVERLAY” SIDE OF PCB
(BECOMES THE LOWER SIDE)
We call these diagrams “component overlays” because they show precisely
where all the components go on the PCB. On a single-sided PCB, its as if
you are looking through the board like an X-ray, with the copper tracks
underneath. The photo at right shows the same board from the component
side – that is, the side which has the component positions marked on it.
Good soldering is a subject which could take many pages
to explain and even then, possibly not be enough.
By far the best idea is to start with some scraps of wire
and try your soldering techniques out before going anywhere
near a component or PCB.
For a beginner, it’s always easiest to solder the component
to the PCB before cutting the excess leads off. Experienced
constructors often do it the other way around, claiming a
better and neater solder joint.
If you want more information, there are many, many
websites which will take you through the rudiments of
soldering (and even some to help make you an expert!).
Ready to start?
OK, here’s the order of construction in ten easy steps:
(1) Bend the legs of the LEDs
(2) Solder 18 of the LEDs together into two layers of nine.
(3) Solder the two layers together
(4) Test that all the LEDs light using the battery pack with
a 100 resistor temporarily connected in series.
(5) Place and solder the components (except LEDs) on the
PCB, including the PIC socket (but not the PIC!).
(6) Place and solder the bottom layer of LEDs on the PCB
(7) Solder the two layers of LEDs to the bottom layer.
(8) Connect the battery box wires to the PCB.
(9) Fit the threaded standoffs to the PCB to act as feet
(10) Fit the PIC chip in its socket
The LED matrix
Before we solder any components onto the PCB, we’re
going to make up the two thirds of the LED “matrix” which
forms the display. The matrix eventually mounts on the
underside of the PCB (ie, the non-component side) and
needs to be connected as shown and described, otherwise
the display won’t – display, that is!
The rows are labeled Layer 2 and Layer 3 on the PCB –
that’s a bit confusing, so we’ll refer to them as the top (layer
3), the middle (layer 2) and the bottom (layer 1).
The top layer of LEDs have their cathodes soldered to
the cathodes of the layer below; later, the middle layer of
LEDs will have their cathodes soldered to the PCB. The
bottom layer of LEDs have both leads soldered to the PCB.
The anodes of the middle layer all connect to the point
on the PCB marked “layer 2”; similarly the anodes of the
top layer all connect to the point marked “layer 1”.
Making it!
First you’ll need to bend the cathode leg of 12 of the LEDs
sharply out 90° away from the LED body, nice and close
to the body. Then as close as your needle-nose pliers will
allow, bend it back down 90° again, so that it has a little
“crank” in it – this allows the leg to pass by the body of
CATHODE
ANODE
The other six LED anodes are
bent out in the opposite (3
o’clock) direction. The other
nine LED leads are not bent.
80 Silicon Chip
Keep those different types
of LEDs separate! It won’t
work properly if they’re
mixed up.
Assemble each layer of
LEDs by using the PCB as
a template. Make sure you
don’t solder them in!
Connect the anodes in
the top and middle layers
with some component lead
offcuts or hookup wire.
siliconchip.com.au
the LED underneath (ie, on the next layer down), where it
will solder to its cathode (eg, LED 25 K connects to LED
16 K which connects to LED 7 K).
However, the anodes (A) of the LEDs aren’t all the same.
12 of the LEDs are bent 90° one way while six have their
anodes bent 90° in the opposite direction (see photos).
These bends are to allow each LED to connect to the anode
of the next LED. See how all three LEDs in the one group
(ie, one row of one layer) have their anodes connected
together on the circuit diagram?
It’s probably easiest to follow the diagram opposite to
work out where the LEDs go and which way around. See
how six of the LEDs on each layer have their anode lead
bent out one way while three go in opposite direction
You can use the PCB to properly space the LEDs while
soldering but be careful not to solder the leads to the PCB.
The flat side of the LEDs on the PCB indicate the nine
CATHODES. They can be held in place by using the same
block of styrene foam mentioned earlier. Solder three LEDs
together, anode to anode, remove and repeat for the next
three LEDs, and so on, until you’ve soldered all nine for
the first layer.
The sets of LEDs are “cross-braced” by a pair of wires
soldered anode to anode to anode. These wires can be the
offcuts of component leads. Repeat for the middle layer.
Now you can carefully solder the upper two layers of the
cube together (see photo).
Another connection is required between the anodes on
the top two layers and the PCB (the points marked “layer
2” and “layer 3”). It’s probably a bit long to use component
offcuts for the top layer so use the supplied short length
of hookup wire. If you use uninsulated wire, make sure it
touches nothing else!
Parts List – PicoMiniCube
1 PicoMiniCube PCB, 50 x 50mm
1 3x AA battery holder* with switch and connecting wires
1 2.5mm stereo socket (optional – for programing if required)
1 mini PCB mounting SPDT switch
4 5mm nylon PCB standoffs (with M3 nylon nuts) – [for “feet”]
Semiconductors
1 PIC16F1503 (or PIC16F1505)
programmed microcontroller
NOTCH
PIN
14
PIN
7
PIN
1
FLAT
SIDE
27 5mm LEDs (all same colour)
K
LONGER
LEAD
4 BC327 PNP Transistors
FLAT
SIDE
Capacitors
1 1F ceramic (code: 105 or 1.0)
E B C
A
105
Resistors (0.25W, 5% supplied in kit)
9 100 (code: brown black brown gold)
3 330 (code: orange orange brown gold)
1 1M (code: brown black green gold)
Where to get the kit:
All the components above are available exclusively in a kit from
PicoKit, who hold the copyright on the design, code and PCB. It sells
for $23.68 complete with programmed PIC (ref no is kit #119).
Visit www.picokit.com.au for full details of this and many other
Picokits to keep you busy these holidays!
* You’ll also need 3 x AA batteries (not supplied in kit)
Once the two upper layers of the LED cube is completed,
before you go any further, use the battery pack (3xAA cells)
with one of the 100 resistors temporarily wired in series
and check each of the LEDs in your cube. It might be a bit
tedious but you really need to ensure that all the LEDs are
soldered together correctly. Connected one way, (positive
to anodes) the LED should glow. Reverse the connection
and it should not.
Having satisfied yourself that the cube is all OK, you can
start soldering the components onto the PCB. Remember
that the components are placed onto the opposite side of
the PCB compared to the LED cube but are soldered from
the LED cube side. You’ve had plenty of practice soldering
the LEDs together so soldering to the PCB should be easy!
It is usual practice to leave semiconductors until last (to
minimise the chance of damaging them) and to start with
the lowest-profile components, the resistors.
As mentioned earlier, there are only three values – 9 x
100, 3 x 330 and 1 x 1M. Resistors are not polarised –
they can mount either direction. However, it is considered
good practice to align them so they all read the same way
in either the horizontal or vertical direction.
Note that while the resistors supplied in the kit were all
5% tolerance, with a gold band at the end, it is possible
that 1% tolerance resistors (with a brown band) could be
supplied. The easiest way to identify these is to separate
the 330types (first two bands are orange) then look for the
single 1Mtype – it will have brown, black, black, yellow
Check all of the LEDs in
the layers work with the
battery pack in series with
a 100 resistor.
Complete soldering the top
side of the PCB and, once
again, check that everything
is in the right place.
Testing the cube
siliconchip.com.au
Start placing the components – resistors first. Check
twice that they’re in the
right places!
Solder the bottom layer of
LEDs onto the underside of
the PCB. The square on the
overlay marks the anode.
January 2015 81
and brown bands. The remaining nine resistors would of
course be the 100types: brown black black black brown.
Next, solder in the single capacitor – it too is not polarised
so can go into the PCB either way.
Follow the capacitor with the PIC socket (but without
the PIC itself). While the socket itself is not polarised, the
PIC chip which plugs into it certainly is! The socket has
a notch in one end which matches the notch on the PCB.
Be careful soldering the pins of the socket – they’re quite
close together and it’s easy to bridge across adjacent pins.
This will either prevent the PIC working properly or, at
worst, could destroy it.
The PIC programming port can go in next, although if you
don’t know how to program a PIC, this can be left out – it
plays no part in the operation of the circuit.
Next come the four PNP transistors. Their orientation
is clearly shown on the PCB – one side is curved and the
other flat. They must go in this way or they could be damaged – at best, they certainly won’t work! Once again, take
care soldering: their pins are very close together.
We said earlier that all components apart from the LEDs
solder on what is normally the top side of the PCB – but
there is an exception. That’s the tiny on-off switch which
can now be placed on the opposite side (it doesn’t matter
which way around) but soldered from the top sides.
Finally, you need to connect the red and black power
supply wires from the battery holder onto the board. First,
pass both these wires down through one of the two larger
holes alongside their solder pads then back up again through
the other hole, from underneath the board – this take the
strain of the flexible wires so they will have less tendency
to break off at the solder joints. The red wire then solders
down through the “V+” pad and the black down through
the “GND” pad.
You may be wondering why this is called “GND” or
ground – in battery circuits, it is generally assumed that the
negative terminal from the battery is at ground potential,
or 0V. Often you’ll see this referred to as “Earth”, perhaps
with an earth symbol ( ). Often, the terms are interchangeable (but not always – there are exceptions sometimes!).
Plug in the PIC
All that remains now is to plug the PIC16F1503 chip into
its socket. If you look carefully at the chip, you see it has a
notch at one end which matches the notch on the socket.
Align the chip over the socket so the notches match and
very carefully push the chip in, taking a lot of care that you
Connect all the middle
layer cathodes to the PCB
– both of the arrowed holes
in the PCB are for cathodes.
82 Silicon Chip
Join the top and middle
layer anodes to the PCB middle to position “layer 2”
and top to “layer 3”.
get all the pins into the socket and not bent underneath or
splayed outside.
The battery box
It’s easy to damage the battery box getting the lid off.
There are two clips at one end which must be VERY gently
prised out to clear the locating lugs underneath. This can
be done with a very small screwdriver or a hobby knife
(careful!). Don’t bend them too far or they will break off.
Put three AA batteries in the box in the polarity shown
and place the lid back on, snapping it in place.
Turn the power switch on the battery box to the ON position and similarly turn the power switch on the PCB to
ON. (It’s a bit of a trap having two switches – it’s probably
better to leave the one on the PCB on all the time).
You should now be rewarded with all the LEDs lighting
in sequence, then repeating. Congratulations!
Uh-oh . . . It’s not working!
If it either doesn’t work at all, or if only some of the LEDs
light up, there is obviously a problem somewhere.
First thing to check is the batteries – if you measure
across the V+ and GND terminals on the PCB, you should
get very close to 4.5V (assuming standard AA batteries). If
you get zero, make sure the switch on the battery box is on
and the batteries are all seated properly. If this still gets you
nowhere, check that each battery is delivering about 1.5V.
If you did get 4.5V, make sure the switch on the PCB is
on. If it is and the LEDs aren’t flashing, there is obviously
an error somewhere. Check your soldering and the placement and orientation of polarised components.
Make sure the PIC16F1503 is inserted in its socket correctly (ie, the right way around) and no pins have missed
their correct positions.
If you get some LEDs flashing and others not, the chances
are that one or more LEDs is the wrong way around or
there’s a bad solder joint on the PCB – probably one of the
transistors or one of the resistors. You can troubleshoot
which component(s) might be suspect by tracing back from
the unlit LEDs to the PCB.
Because there are so few components, there’s not much
that can be wrong. If all the components are soldered in
properly, are in the right place and where necessary oriented
correctly, it works. If not, it doesn’t!
SC
*Philip Tallents is Manager and Product Designer at
PicoKit (www.picokit.com.au)
Run the battery wires down
and back up again through
the strain relief holes and
solder to the correct pads.
Plug in the PIC chip,
making sure it goes in the
right way around (align the
notch on the chip & socket).
siliconchip.com.au
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2015 83
Tektronix RSA306 USB
Real Time Spectrum Analyser
Review by JIM ROWE
We have reviewed a number of USB spectrum analysers and now
Tektronix has entered the market. Its RSA306 spectrum analyser
hooks up to a late-model PC, laptop or tablet via a “SuperSpeed”
USB 3.0 cable. Together with Tek’s SignalVu-PC software, it offers
virtually all the features of a real-time spectrum analyser at a
fraction of the cost.
I
T WAS ONLY a matter of time before
Tektronix decided to take advantage
of the computing power of today’s PCs.
Enter Tektronix’ new RSA306 which
basically consists of similar signal
acquisition front-end hardware as in
one of their high-end RSAs (real-time
spectrum analyser), housed in a small
(190 x 127 x 33mm, 590g) ruggedised
84 Silicon Chip
box. It’s designed to be controlled by
Tek’s powerful SignalVu-PC software
running on a fast PC, linked via a SuperSpeed USB 3.0 cable.
It seems that the SignalVu-PC software is almost identical to the data
processing firmware used in Tek’s
high-end RSAs – simply ported over
to run under Windows 7 or 8. As a
result, the RSA306-plus-SignalVu-PC
combination running on a modern
PC can provide a very high order
of performance but at a fraction of
the cost.
Recently, I had the opportunity to
spend a couple of days with an RSA
306 and the Tektronix “self guided
demo kit”. Here’s a quick run-down
siliconchip.com.au
Fig.1: this screen grab shows how a standard swept spectrum display (on the
right) can easily miss a brief transient about 12MHz higher than a 2.445GHz
carrier, while the transient is easily detected by the real-time DPX spectrum and
spectrogram on the left.
measurement using user-defined limit
lines and masks, across the instrument’s entire spectrum range
(8) The availability of applicationspecific option add-on modules for the
SignalVu-PC software, covering areas
such as digital modulation analysis
(27 modulation types including 16/
32/64/256 QAM, QPSK, O-QPSK,
GMSK, FSK and APSK); WLAN analysis of 802.11a/b/g/j/p, 802.11n, and
802.11ac; mapping and signal strength;
pulse analysis; and AM/FM/PM/direct
audio measurements including SINAD
and THD.
The demo kit consists of a 194 x
132mm PCB which can be switched
to generate a wide range of different
RF and baseband signals, with many
different kinds of analog and digital
modulation. It comes with cables to
hook it up to the PC and to the input
of the RSA306, plus a 104-page A5
guide book to get you going.
What makes an RSA?
Fig.2: taken from Tek’s Demo8, this screen grab shows how the RSA306 and its
software can easily analyse a QPSX signal and display its DPX spectrum (lower
right), its constellation diagram (upper right), its symbol table (upper left) and
signal quality data.
of the main specifications for the
RSA306 itself:
(1) Frequency range: 9kHz to 6.2GHz.
(2) Measurement range: from +20dBm
down to -160dBm.
(3) Frequency span range: from 100Hz
to 6.2GHz in swept spectrum analysis
mode; up to 40MHz span in real-time
DPX spectrum/spectrogram mode
(both modes can be used at the same
time).
And these are the main functions of
the SignalVu-PC software:
(1) For standard spectrum analysis:
three traces (+Peak, -Peak and average),
plus a maths and spectrogram trace.
(2) Five measurement markers with
power, relative power, integrated power,
power density and dBc/Hz functions.
siliconchip.com.au
(3) For real-time spectrum and spectro
gram displays: 100% POI (probability
of intercept) of transient signals lasting for 100μs or more in spans up to
40MHz.
(4) Basic vector analysis functions
including amplitude, frequency and
phase vs time; also RF I and Q com
ponents vs time.
(5) For real-time spectrogram displays:
the ability to analyse and re-analyse
signals with either a 2D or 3D waterfall
display.
(6) Analysis and measurement of key
modulation parameters for AM, FM
and PM signals, plus the ability to hear
and record FM or AM demodulated
audio signals to a file.
(7) Spurious signal detection and
Before going any further, we should
note the difference between a conventional “swept” spectrum analyser or
SA/SpecAn and a real-time spectrum
analyser or RSA.
Basically, a conventional spectrum
analyser sweeps over a range of fre
quencies being examined (the “span”)
in sequence, taking a finite time for
each sweep. This has two significant
drawbacks in today’s rapidly digitising world, one being that any specific
frequency in the span is only examined
briefly once per sweep and, of course,
none of the individual frequencies is
examined at exactly the same time as
the others.
These drawbacks were of little
consequence a few decades ago, when
most of the signals were controlled and
relatively static. But nowadays there
are many situations where the signals
you may want to examine are changing
very rapidly in terms of amplitude,
frequency or phase.
With a swept spectrum analyser, it
can be surprisingly difficult to even
find a briefly appearing signal, let
alone capture and measure it. You
may have to sweep over the frequency
range concerned many hundreds of
times, until it happens to show up at
the exact instant that your analyser is
examining that particular frequency.
An RSA gets around these problems
by taking advantage of high-speed
digital sampling (via an ADC) and
January 2015 85
that at least some of the phosphors
could be made to persist – ie, the
emitted light faded relatively slowly,
allowing you to see events which
lasted for a very brief time.
DPX can provide this function digitally, with added advantages like easily
variable persistence time, statistical
persistence functions and selectable
colour schemes. So all Tektronix RSAs,
including the RSA306 (or strictly
speaking the SignalVu-PC software
running with it) incorporate DPX, or
digital persistence.
What sort of PC is needed?
Tek’s RSA306 Self-Guided Demo Kit comprises a digital signal generator PCB
module with a wide range of selectable outputs and is powered from two ports
on your PC. There’s also a well-written 104-page guide book.
Because it’s fully controlled by the SignalVu-PC software, the RSA306 has only
four sockets on its front panel. These are (L to R): the main RF input, an input
for an optional external 10MHz frequency reference, an external trigger input
and the USB 3.0 socket used to connect it to the PC. Also shown here is the
helical whip antenna and N-type/BNC adaptor.
digital signal processing (DSP). This
allows it to sample all the signals in
the frequency band being examined
– simultaneously. It does this continuously, with the resulting timecontiguous stream of samples being
stored in memory as well. They can
be processed and analysed both during capture in real time and afterwards
(from memory).
Because every signal frequency in
the span range is being sampled every
time, this means that an RSA can
capture even very brief signals which
appear anywhere in that range.
Nyquist’s sampling theorem applies
here just as it does anywhere else – in
order to capture all frequencies in a
certain frequency band, an RSA must
use a sampling frequency of more than
twice that bandwidth. That is why the
86 Silicon Chip
RSA306 needs to be linked to your PC
using a USB 3.0 cable, to handle the
very fast stream of samples (USB 3.0
can pass data at up to 625MB/s).
What is DPX?
DPX is an acronym used by Tektronix in describing the RSA306’s
real-time spectrum and spectrogram
display capabilities. It stands for “Digital Phosphor Analysis”, a Tektronix
patented technology which is built into
their SignalVu firmware and software.
It allows modern flat-screen displays
to imitate the display persistence of
CRTs which relied on a phosphor coating on the rear of the screen.
Each particle of phosphor emitted
light or fluoresced when the electron
beam scanned across them. And one
of the advantages of CRT displays was
The SignalVu-PC software that con
trols the RSA306 is pretty demanding
in terms of computing power. This
is the minimum PC specification required to achieve full performance:
• A PC using an Intel Core i7 4th
generation processor, running either
the Windows 8 or Windows 7 (SP1)
64-bit operating systems;
• At least one USB 3.0 SuperSpeed
port;
• 8GB of RAM;
• At least 20GB of free space on the
C: drive;
• A drive capable of streaming storage
rates of 300MB/s to support the stream
ing data feature; and
• An internet connection for software
activation.
So you do need a fairly “hot” desktop or laptop to get the best out of the
RSA306. By the way, the SignalVu-PC
software and all the documentation
comes not on an optical disc but on a
4GB USB memory stick.
Putting it through its paces
While I’ve never actually driven an
RSA previously and although SignalVu-PC is a complex software package, it wasn’t as difficult as might be
expected. This is thanks to the many
kinds of continuous and semi-random
signals that can be generated by the
Demo Board and the clarity of the
explanations of each graded demo in
the guide book.
Most impressive was Demo5, where
you learn how the DPX spectrum
display can be used to detect and
measure brief spurious signals that
simply don’t show up on the normal
swept spectrum display – or only
very occasionally. This is an excellent demonstration of the benefits of
real-time spectrum analysis coupled
with DPX processing.
siliconchip.com.au
Another very impressive demo is
Demo8. This uses SignalVu’s DPX
spectrum function to look at a QPSK
signal at 2.445GHz (from the Demo
Board) and you lets you use its constellation display, symbol table and
signal quality measurement displays
to examine the signal in depth.
After a session with the demo
board, I started using the RSA306 to
examine signals from the helical whip
antenna supplied with it and then
with my wideband VHF-UHF discone
antenna outside, the output from my
GA1484B signal generator, and also
the 10.000000MHz output from a GPSdisciplined PRS10 Rubidium Frequency Standard.
Before I did those tests, I screwed a
50Ω shielded wideband termination
directly to the N-type input connector of the RSA306, and used this to
carry out DANL/noise floor tests at
100MHz, 1.0GHz, 2.0GHz, 2.45GHz,
3.0GHz, 4.0GHz, 5.0GHz, 6.0GHz and
6.195GHz. All of these tests were done
with a span of 10MHz and a resolution
bandwidth (RBW) of 10Hz, a reference
level of -50dBm, and averaging over
10 traces.
The DANL figures achieved were impressive, varying from -137.10dBm at
100MHz and 1.0GHz up to -136.76dBm
at 5.0GHz and then down again to
-138.36dBm at the very top of the range
(6.195GHz, nudging the RSA306’s upper limit of 6.20GHz).
There were a few tiny spurious response “spurs” visible here and there,
mainly at ±4MHz points on either side
of 100MHz, 1GHz, 4GHz and 5GHz.
However, these were very small, varying between +0.5dB and +4.56dB in
amplitude (the worst case). So the peak
value of the highest spur (at 5.004GHz)
was still only -132.2dBm.
When I tried using the RSA306
with its small helical whip antenna
to look at the WiFi signals near my
ADSL modem/wireless router, there
was no trouble finding the router’s
“anybody there?” interrogating signal,
even though there were no WiFi-linked
PCs powered up at the time.
Next, I hooked the RSA306 up to
the wideband discone antenna outside and tuned its centre frequency
to 92.9MHz with a span of 500kHz.
This showed the Sydney ABC-FM
signal with a peak value of -36.8dBm.
When I enabled SignalVu-PC’s FM
demodulation function, I could not
only see the station’s audio in the leftsiliconchip.com.au
Fig.3: a screen grab taken in the vicinity of a WiFi router, using the RSA306 and
its helical whip antenna. Although the “anyone there?” signal was not detected
on the swept spectrum display on the right, it’s clearly visible in the real-time
DPX spectrum at lower left.
Fig.4: a screen grab showing the 4.0GHz -90dBm signal from a GA1484B signal
generator. The swept spectrum display is at right, with the DPX spectrum and
spectrogram at left.
Fig.5: this screen grab shows the 1.0GHz -90dBm signal from the GA1484B
signal generator on an expanded swept spectrum. The amplitude is now shown
as -97.14dBm, suggesting lower cable losses at this frequency. A small spur is
also visible in the centre.
hand window but also hear it via the
laptop’s speakers.
Next I checked the DAB+ signals
received from Sydney’s Digital Radio
Multiplex Transmitter (DRMT). The
multiplexed DAB+ signals are in
January 2015 87
could well have significant losses.
Trying the same test at 1.0GHz, I
obtained a much closer reading of
-97.14dBm (about 3.15µV). However,
SignalVu-PC now gave the signal
frequency as 1.000001787GHz, or
1.787kHz high.
I’m pretty sure that the GA1484B’s
accuracy is somewhat closer than
this, so I tried checking the 10MHz
output from my GPS-disciplined rubidium frequency standard. This time
SignalVU-PC told me that the signal
frequency was 10.000014MHz. Since
the rubidium standard is much closer
than this, I concluded that at least part
of the error was due to the accuracy
of the RSA306’s internal frequency
reference – specified as ±25ppm +
ageing (±3ppm in the first year), after
a 30-minute warm-up.
By the way, the RSA306 does have
provision for connecting an external
10MHz frequency reference. It also
provides an external trigger input.
Both of these inputs are via SMA
sockets.
Taken from the Tektronix media website, this picture shows an RSA306 (centre
foreground) being used with the Demo Kit and a laptop running the SignalVu-PC
software, in a typical workshop.
three 1.536MHz blocks, centred at
202.928MHz (Ch9A), 204.640MHz
(Ch9B) and 206.352MHz (Ch9C). I had
no trouble finding the three blocks
and displaying their peak and average values.
I wasn’t very successful in displaying the multiplex constellation diagram for any of the three but this may
have been because I wasn’t driving the
OFDM constellation function correctly.
An unmodulated 4.0GHz signal from
the GA1484B signal generator, set to
give an output of -90dBm (7.1µV), was
very easy to see on both of SignalVuPC’s spectrum displays, although the
measured signal level was at -114dBm
(446nV). This may be because I was using a 5m-long RG213 cable to connect
the two, using SMA connectors and
SMA-N series adaptors. At 4GHz, this
cable plus the connectors and adaptors
Conclusion
Overall, I was most impressed with
the Tektronix RSA306 and SignalVuPC combination. They certainly seem
to offer a level of performance approaching that of high-end real-time
spectrum analysers but at a much
lower price. The SignalVu-PC software
is also very easy to use once you get
the hang of it.
Finally, the RSA306 Self Guided
Demo Kit really helps in becoming
familiar with “driving” and using
the RSA306 and the SignalVu-PC
software. I’m sure that many buyers
would appreciate a loan of the Demo
Kit, or perhaps rental of one, for a
week or two.
The introductory Australian price
of the RSA306 is $4770 plus GST.
This includes a USB3.0 cable and the
SignalVU software.
Call Vicom for information on
Tektronix products on 1300 360 251
or visit www.vicom.com.au or email
info<at>vicom.com.au
Handy links:
Fig.6: this screen grab was taken while using the RSA306 to examine the
channel 9A DAB+ signal block from the Sydney DRMT (Digital Radio Multiplex
Transmitter). The spectrum at right is clear but I couldn’t get a clear constellation
display. I can’t blame the RSA306 or its software – just my poor driving!
88 Silicon Chip
(1) Vicom Australia: www.vicom.
com.au
(2) Tektronix Spectrum Analysers:
www.tek.com/spectrum-analyzer A
free primer titled “Fundamentals of
Real-Time Spectrum Analysis” can also
SC
be downloaded from this link.
siliconchip.com.au
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CHIP
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PCBs and other hard-to-get components now available direct from the SILICON CHIP ONLINESHOP
NOTE: PCBs from past ~12 months projects only shown here but the SILICON CHIP ONLINESHOP has boards going back to 2001 and beyond.
For a complete list of available PCBs, back issues, etc, go to siliconchip.com.au/shop Prices are PCBs only, NOT COMPLETE KITS!
TINY TIM POWER SUPPLY
DEC 2013 18110131 $10.00
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DEC 2013 08112131 $10.00
PORTAPAL-D MAIN BOARDS
DEC 2013 01111131-3 $35.00/set
(for CLASSiC-D Amp board and CLASSiC-D DC/DC Converter board see Nov 2012/May 2013)
LED PARTY STROBE (also suits Hot Wire Cutter [Dec 2010]) JAN 2014 16101141 $7.50
BASS EXTENDER Mk2
JAN 2014 01112131 $15.00
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JAN 2014 09107134 $15.00
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FEB 2014 10102141 $12.50
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MAR 2014 14103141 $15.00
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APR 2014 04105141 $10.00
USB/RS232C ADAPTOR
APR 2014 07103141 $5.00
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MAY 2014 10104141 $10.00
RGB LED STRIP DRIVER
MAY 2014 16105141 $10.00
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MAY 2014 18104141 $20.00
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JUN 2014 01205141 $20.00
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JUL 2014 99106141 $10.00
MICROMITE ASCII VIDEO TERMINAL
JUL 2014 24107141 $7.50
FREQUENCY COUNTER ADD-ON
JUL 2014 04105141a/b $15.00
VALVE SOUND SIMULATOR PCB
AUG 2014 01106141 $15.00
VALVE SOUND SIMULATOR FRONT PANEL (BLUE)
AUG 2014 01106142 $10.00
TEMPMASTER MK3
AUG 2014 21108141 $15.00
44-PIN MICROMITE
OPTO-THEREMIN MAIN BOARD
OPTO-THEREMIN PROXIMITY SENSOR BOARD
ACTIVE DIFFERENTIAL PROBE BOARDS
MINI-D AMPLIFIER
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DIGITAL EFFECTS UNIT
DUAL PHANTOM POWER SUPPLY
REMOTE MAINS TIMER
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ONE-CHIP AMPLIFIER
TDR DONGLE
MULTISPARK CDI FOR PERFORMANCE VEHICLES
CURRAWONG STEREO VALVE AMPLIFIER MAIN BOARD
CURRAWONG REMOTE CONTROL BOARD
CURRAWONG FRONT & REAR PANELS
AUG 2014
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SEP 2014
SEP 2014
OCT 2014
OCT 2014
OCT 2014
NOV 2014
NOV 2014
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DEC 2014
DEC 2014
DEC 2014
DEC 2014
DEC 2014
24108141
23108141
23108142
04107141/2
01110141
05109141
23109141
01110131
18112141
19112141
19112142
01109141
04112141
05112141
01111141
01111144
01111142/3
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JAN 2015
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$5.00
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$5.00
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PIC16F877A-I/P
PIC18F2550-I/SP
PIC18F45K80
PIC18F4550-I/P
PIC18F14K50
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IR-to-UHF Converter (Jul13), UHF-to-IR Converter (Jul13)
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Receiver (Jun13), Revised 10-Channel Remote Control Receiver (Jul13),
Nicad/NiMH Burp Charger (Mar14) Remote Mains Timer (Nov14)
Garbage Reminder (Jan13), Bellbird (Dec13)
LED Ladybird (Apr13)
6-Digit GPS Clock (May-Jun09), Lab Digital Pot (Jul10)
Semtest (Feb-May12)
Batt Capacity Meter (Jun09), Intelligent Fan Controller (Jul10)
USB Power Monitor (Dec12)
GPS Car Computer (Jan10), GPS Boat Computer (Oct10)
USB MIDIMate (Oct11)
PIC18F27J53-I/SP
USB Data Logger (Dec10-Feb11)
PIC18LF14K22
Digital Spirit Level (Aug11), G-Force Meter (Nov11)
PIC18F1320-I/SO
Intelligent Dimmer (Apr09)
PIC32MX795F512H-80I/PT Maximite (Mar11), miniMaximite (Nov11), Colour Maximite (Sept/Oct12),
Touchscreen Audio Recorder (Jun/Jul 14)
PIC32MX170F256B-50I/SP Micromite Mk2 (Jan15) – also includes FREE 47F tantalum capacitor
PIC32MX170F256D-501P/T 44-pin Micromite Mk2 (Now with Mk2 Firmware at no extra cost)
PIC32MX250F128B-I/SP GPS Tracker (Nov13) Micromite ASCII Video Terminal (Jul14)
PIC32MX470F512H-I/PT Stereo Audio Delay/DSP (Nov13), Stereo Echo/Reverb (Feb 14),
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(Oct-Dec10), SportSync (May11), Digital Audio Delay (Dec11) Level (Sep11)
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dsPIC33FJ64MC802-E/P Induction Motor Speed Controller (revised) (Aug13)
dsPIC33FJ128GP306-I/PT CLASSiC DAC (Feb-May 13)
ATTiny861
VVA Thermometer/Thermostat (Mar10), Rudder Position Indicator (Jul11)
ATTiny2313
Remote-Controlled Timer (Aug10)
ATMega48-20AU
Stereo DAC (Sep-Nov09), RGB LED Strip Driver [-20AU chip] (May14)
When ordering, be sure to nominate BOTH the micro required AND the project for which it must be programmed.
SPECIALISED COMPONENTS, SHORT-FORM KITS, ETC
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NEW:
ISOLATED HIGH VOLTAGE PROBE - Hard-to-get parts pack:
all ICs, 1N5711 diodes, LED, high-voltage capacitors & resistors:
(Jan15) $40.00
10A 230V AC MOTOR SPEED CONTROLLER
(Feb14)
CDI - Hard-to-get parts pack: Transformer components (excluding wire),
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GPS Tracker MCP16301 SMD regulator IC and 15H inductor
SMD parts for SiDRADIO
RF Probe All SMD parts
(Nov13)
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(Oct13)
$20.00
all ICs, Mosfets, UF4007 diodes, 1F X2 capacitor:
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CURRAWONG AMPLIFIER Hard-to-get parts pack:
(Dec 14)
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(Nov 14)
DIGITAL EFFECTS UNIT WM8371 DAC IC & SMD Capacitors [Same components
also suit Stereo Echo & Reverb, Feb14 & Dual Channel Audio Delay Nov 14]
AD8038ARZ Video Amplifier ICs (SMD)
(Oct14)
$15.00
$25.00
For Active Differential Probe (Pack of 3)
(Sept 14) $12.50
44-PIN MICROMITE Complete kit inc PCB, micro etc
MAINS FAN SPEED CONTROLLER - AOT11N60L 600V Mosfet
RGB LED STRIP DRIVER - all SMD parts and BSO150N03 Mosfets,
(Aug14)
$35.00
(May14)
$5.00
does not include micro (see above) nor parts listed as “optional”
(May14)
$20.00
HYBRID BENCH SUPPLY- all SMD parts, 3 x BCM856DS & L2/L3
(May 14)
$45.00
USB/RS232C ADAPTOR MCP2200 USB/Serial converter IC
NICAD/NIMH BURP CHARGER
(Apr14)
$7.50
(Mar14)
$7.50
1 SPD15P10 P-channel logic Mosfet & 1 IPP230N06L3 N-channel logic Mosfet
40A IGBT, 30A Fast Recovery Diode, IR2125 Driver and NTC Thermistor
$45.00
(Aug13) $5.00
Same as LF-UF Upconverter parts but includes 5V relay and BF998 dual-gate Mosfet.
LF-HF Up-converter Omron G5V-1 5V SPDT 5V relay
(Jun13)
$2.00
“LUMP IN COAX” MINI MIXER SMD parts kit:
(Jun13)
$20.00
Includes: 2 x OPA4348AID, 1 x BQ2057CSN, 2 x DMP2215L, 1 x BAT54S, 1 x 0.22Ω shunt
LF-HF UP-CONVERTER SMD parts kit:
(Jun13)
$15.00
Includes: FXO-HC536R-125 and SA602AD and all SMD passive components
CLASSiC DAC Semi kit – Includes three hard-to-get SMD ICs:
(Feb-May13) $45.00
CS8416-CZZ, CS4398-CZZ and PLL1708DBQ plus an accurate 27MHz crystal and ten 3mm blue LEDs
with diffused lenses
ISL9V5036P3 IGBT Used in high energy ignition and Jacob’s Ladder (Nov/Dec12, Feb13) $10.00
2.5GHz Frequency Counter
(Dec12/Jan13)
LED Kit: 3 x 4-digit blue LED displays
$15.00
MMC & Choke Kit: ERA-2SM+ Wideband MMC and ADCH-80+ Wideband Choke
$15.00
ZXCT1009 Current Shunt Monitor IC
(Oct12)
As used in DCC Reverse Loop Controller/Block Switch (Pack of 2)
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January 2015 89
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Salvage It!
By KEN KRANZ
This is a rather different
Salvage It: We’re not trying
to recycle a complete device
but instead, just one part of it.
We’re looking at Switch-Mode Power
Supplies . . . and specifically, the CommonMode Choke at the mains input. There’s a lot you
can do with one of these handy components.
T
hese days, most electronic equipment has a switchmode (or switching) power supply. They’re cheaper
than transformer-based (linear) supplies and you can
obtain more “grunt” from a given space.
And while they’re pretty reliable, they do occasionally
fail (sometimes spectacularly!).
There’s not much worth safely salvaging in a dead switchmode supply – the chances are at least some of the semis (if
not most/all) have failed and, given the supply’s relatively
high temperature operation, you wouldn’t
want to place too much faith in any electrolytics (check them out – we’d bet London to a
brick that many would show signs of distress
– especially swelling on top).
50kHz
Apart from the smoke which escaped from
DRIVE
(1) 200W Mains Inverter, Februaryl 1994*
(2) Courtesy Light Delay, October 2014
* some components may now be difficult to obtain
SPICE simulations may be downloaded from
siliconchip.com.au
90 Silicon Chip
FLOATING DRIVE
SECTION
K
D2
BAT54
Q1
IRF1405
A
D1
BAT54
10nF
D
150W
K
C1
20nF
SILICON CHIP Floating Gate
Drive circuits
Two projects spring to mind which had floating gate drives, employing the type of circuitry in
this feature. They provide good background and
reinforce the theory explained here:
the supply above (and there was a lot of it!) at least some
of the electrolytics are showing they’ve failed the battle of
the bulge.
But there is one component which is worth saving, if only
because it is so useful in other ways. That component is the
common-mode choke (CMC).
It’s rare that the CMC will have failed (and that is easily
checked) so it’s well worthwhile to remove it before junking
the rest of the SMS.
G
S
A
V1
L1
30mH
R1
22W
L2
30mH
K
10nF
D3
BAT54
A
K
22k
10pF
10nF
D4
BAT54
A
Fig.1: An LTSPICE simulation of the CMC used to provide a floating gate
drive for a MOSFET. In this simulation, the voltage source (V1) at the left
simulates a PIC micro with a 4.9V supply.
siliconchip.com.au
What’s a CMC?
The attraction of CMCs is the fact that two windings are
on a closed ferrite core, often with very good high-voltage
insulation between the windings and low capacitance between the windings.
The chokes are not designed to be used as transformers
but if the choke and application are selected carefully the
results can be very good indeed.
First some recommendations: keep the core flux density
below 1500 Gauss and limit the frequency to <75kHz. Below
20kHz most cores seem to be OK at around 2000 Gauss. To
calculate the flux density use the following simple formula:
Bmax = 108 E
KANf
Bmax = maximum flux density in Gauss.
E = voltage across coil.
N = number of turns of the coil.
A = effective area of the coil in cm2.
f = frequency in Hz.
K = 4.44 for sinewave (RMS).
K = 4 for squarewave (peak).
Often the number of turns can be counted or estimated
(without destroying the coil). The small black 30mH CMC
tested had 93 turns on each winding (one winding was un-
Actual volage drop across the 22 resistor.
wound for this information, it was worth the sacrifice as it
cost less than $1.50 on ebay).
Leakage inductance is normally higher than for a customwound transformer but often it is more than satisfactory for
the task. The low capacitance between windings is often a
big win.
It was decided to test the circuit at high power; as I do
not own a 300W 10resistor a simulation was carried out,
again using SPICE.
A 10 250W resistor and a 50V, 5A power supply were
simulated, with the input signal to the CMC a 20ms burst
of 50kHz (FET-on) followed by 20ms of no drive (FET-off).
The FET turn-on switching loss was <3mJ, the FET turn-off
switching loss was <10mJ, the power FET’s loss when ON
(static) was <200mW.
MISS THIS ONE?
This simulation is of a 3ms on-pulse, actually a 3
millisecond burst of 50kHz from the PIC, the waveform
measurement was taken at the gate-drive test point.
Published in Dec 2012
2.5GHz 12-digit
Frequency Counter
with add-on GPS accuracy
And here’s a scope trace of the actual waveform. It has
more ripple than the simulation; this could be removed,
at the expense of a longer turn-off time, by increasing the
value of C2 (10pF). In the simulation, it effectively does
nothing, the gate capacitance of the FET does the job – it
is on the schematic to show where to add capacitance if
desired. The ripple is well above the FET’s gate turn on
voltage so it’s not actually a problem.
siliconchip.com.au
Wow! 10Hz – >2.5GHz in two ranges; 1ms - 999,999s
with a 12-digit LED display. It’s a world beater and it’s
the perfect addition to any serious hobbyist’s bench –
or the professional engineer, technician, in fact anyone
who is into electronics!
You’ll find it one of the handiest pieces of test gear you
could ever own and you can build it yourself.
All the hard-to-get bits (PCBs, micros, LEDs, panels, etc)
are available from the SILICON CHIP Online Shop.
You’ll find the construction details at
http://siliconchip.com.au/project/2.5ghz
PCBs, micro etc available from On-Line Shop
January 2015 91
RL
TP1
R2: 50W*
OUTPUT
CMC
R3
1W
L1
30mH
*SIGNAL GENERATOR
OUTPUT RESISTANCE
L2
30mH
R1
1k
Fig.2: using a 30mH CMC as a
transformer.
USING A COMMON MODE CHOKE AS A TRANSFORMER
INPUT
37.3kHz
SQ WAVE
L3
7.5mH
R2 0.031W
L4 34mH
OUTPUT
R1
7.2W
L5
7.5mH
R3 0.031W
R2, R3 = WINDING RESISTANCE
L4
= LEAKAGE INDUCTANCE
R1
= 20W LOAD AT 12 VOLTS
Fig.3: this time the input is a square wave at 37.7kHz but
SIMULATION OF THE SAME CIRCUIT
the CMC is much smaller.
The slow speed of the switching is fine for many applications – it actually keeps the RFI down.
How much drive current does this require ?
For the following test C1 was changed to 100nF to increase
the gate voltage and the drive was a continuous 50.25kHz
square wave from the PIC. The voltage drop was measured
across the current sense resistor R1 in Fig.1.
The peak voltage was 104mV, peak current 4.7mA
(0.104/22) and RMS voltage 52.2mV, so the current required
to hold the high-side switch on is very reasonable.
Common mode chokes are a good choice for pulse triggering of SCRs, quite high trigger currents can be obtained
with suitable chokes.
The actual measurements above were taken using a square
wave drive from a PIC 16F1783. This has a super-cool PSMC
(Programmable Switch Mode Controller Module) with no
less than 10 modes of operation:
• Single phase
• Complementary single phase
• Push-pull
• Push-pull H-bridge
• Complementary push-pull H-bridge
• Pulse skipping
• Variable frequency fixed duty cycle
• Complementary variable frequency fixed duty cycle
• ECCP compatible modes
- Full bridge
- Full bridge reverse
• 3-phase 6-step PWM
The chip looked so interesting I made up some test boards.
Other uses for CMCs
If the rules regarding flux density are followed and the
source impedance is low enough, CMC’s can be used at
low frequencies with a reasonable bandwidth, normally
obtained at millivolt levels.
The primary inductance combined with the signal source
impedance forms a high-pass filter. Making the source impedance low reduces this effect. The leakage inductance
combined with the load on the secondary forms a low
pass-filter. A higher value load resistor can be an advantage.
As a rule of thumb when using a CMC as a signal transformer, I keep the source impedance under 1/10th of the
primary inductive reactance Xl, calculated for the minimum
frequency that is expected to be used.
Most cores at low frequency seem to be OK with a maximum flux density of 2000 Gauss.
Using the 30mH CMC a circuit was set up as shown below.
At 50Hz sine wave, the maximum input voltage would be
53mV (1974 Gauss). The 50resistor was used as it is built
into my signal generator. With the 50:1voltage divider
the maximum input
(AC in) is 2.55VRMS.
Some tests were
carried out with the
signal generator set
such that the input
into the transformer
was a 68.8mV square
You can get enough
power out to run a
10W halogen globe,
as seen here.
The input into the transformer was a 68.8mV square wave at 1.0kHz from the signal generator. The scope screen at left
shows the 1kHz output, with a very respectable rise time (right). A gain recovery amplifier would normally be required.
92 Silicon Chip
siliconchip.com.au
Sine Wave Tests
My signal generator started to clip when driven to
53.3mV RMS, so testing was carried out at 56mV peak
into the transformer (across the 1 resistor).
wave at 1000Hz, with the results shown opposite.
What about higher power?
A CMC was removed from the mains input filter of a large
switched mode power supply (the one shown overleaf) that
had destroyed itself, along with many major components.
The core details measured were:
Core OD .......................................................... 22.4mm
Core ID............................................................... 14mm
Core Height ...................................................... 8.3mm
Core cross sectional area .................................35 cm2
Measured Inductance ........................................7.5mH
Measured Leakage inductance ............................35H
Number of turns ....................................................... 29
DC resistance.................................................... .031
50 Hz output into 1000.
A 20W halogen lamp was set up as a secondary load and
a 37.3kHz square wave used as an input to the primary.
After running for half an hour the CMC was warm to touch.
The calculated flux density was 2116 Gauss.
It can be seen that common mode chokes can be very
handy when used for applications other than their intended
purpose. The construction used for the mains input types
gives superb high voltage isolation.
Note: I adjusted the simulation for a 10W halogen lamp;
the reduced effect of the leakage inductance allowed the
input voltage to be reduced to 15.1V peak input for 12VRMS
out. The output was a nicely rounded square wave. The
flux density was just over 1500 gauss.
I re-ran at 25kHz, 13.9V peak input for 12VRMS at the
load, with the calculated flux density 2090 gauss.
SC
Radio, Television & Hobbies:
ONLY 0
the COMPLETE
0
$ 2
6 0 P&P archive on DVD
+ $1
1kHz output into 1000.
100kHz output into 1000.
It can be seen apart from the low level and low-Z input
the results are very handy for less than $1.50. It should
be possible to run some low frequency Manchester code
through these devices when low capacitance galvanic
isolation is required. Even audio could be worth a try –
some opamps can deliver the current required. 1k input
impedance can be very low noise for many opamps.
siliconchip.com.au
• Every issue individually archived, by month and year
• Complete with index for each year
• A must-have for everyone interested in electronics
This remarkable collection of PDFs covers every
issue of R & H, as it was known from the
beginning (April 1939 – price sixpence!)
right through to the final edition of R, TV
& H in March 1965, before it disappeared
forever with the change of name to
Electronics Australia.
For the first time ever, complete and in one
handy DVD, every article and every issue is covered.
If you're an old timer (or even young timer!) into vintage radio, it
doesn't get much more vintage than this. If you're a student of
history, this archive gives an extraordinary insight into the amazing
breakthroughs made in radio and electronics technology following
the war years. And speaking of the war years, R & H had some of the
best propaganda imaginable!
Even if you're just an electronics dabbler, there's something here to
interest you.
NB: Requires a computer with DVD reader to view
– will not work on a standard audio/video DVD player
Use the handy order form
included in this issue
January 2015 93
Vintage Radio
By Associate Professor Graham Parslow
The Stromberg-Carlson 1946 model 5A26 radio
Released in 1946, the Stromberg-Carlson
model 5A26 was a good-performing 5-valve
superhet radio in an attractive Bakelite
cabinet. The set featured here was acquired
in relatively good condition and was easy to
restore.
I
N 1894, ALFRED STROMBERG and
Androv Carlson took advantage of
the fact that Alexander Graham Bell’s
patent for the telephone had expired.
They established a firm in Chicago to
manufacture telephone equipment
and eight years later re-incorporated
as a New York state corporation. They
then diversified into other electronic
products, while retaining a focus on
telephone equipment.
The first US radio from Stromberg
Carlson was manufactured in 1924 and
it used a neutrodyne circuit designed
by L. A. Hazeltine. In 1926, Stromberg94 Silicon Chip
Carlson became the first manufacturer
to merge phonograph and radio technology by incorporating a phonograph
jack into its radio chassis.
Australian operation
Stromberg-Carlson Australia was
an autonomous operation and ran
its business largely independent of
its American parent. The Australian
company began by importing receivers
from the USA in 1927. It then began
local manufacture of both receivers
and most of the components used in
them a year later.
By 1936, production levels justified the construction of a new factory
at Bourke Road, Alexandria NSW.
Stromberg-Carlson subsequently made
receivers and components under both
their own brand name and for other
brands, including Audiola and Crosley.
The 1930s represented boom years
for Stromberg-Carlson’s radios. During
that time, the company introduced
new technology such as automatic
volume control, improved amplifying methods and an early pushbutton
tuning mechanism. They also developed an acoustic labyrinth that was
a complex baffle which improved
sound quality by guiding audio waves
through a series of interlocking chambers.
During the war years from 19391945, Stromberg Carlson produced telephones and telephone switchboards
for the Australian Army. Advertisements during the 1940s proclaimed
that “there is nothing finer than a
Stromberg Carlson”. Throughout their
history, the company aimed for the
high end of the market as illustrated
by the 1953 advertisement reproduced
with this article.
Stromberg-Carlson radios continued to sell well through the 1950s.
The company then switched from
valve to transistor technology and
their last sets were a line of distinctive portable transistor radios clad in
patterned leather. Stromberg-Carlson
subsequently attempted to participate
in the Australian television market but
they were not competitive and all local
manufacture ceased in 1961.
The 1946 model 5A26
The model 5A26 set featured here
was a popular mantel radio in its time.
Many have survived and the author
has three examples. Unfortunately, it
took all three radios to get a complete
set of genuine knobs.
Basically, the knobs are unique
siliconchip.com.au
Fig.1: the circuit of the Stromberg-Carlson model
5A26. V1 (6J8) serves as a mixer-oscillator while V2
(6G8) is an IF amplifier, detector & AGC source. V3
(6B6) functions as an audio preamplifier and this
drives V4 (a 6V6 output tetrode). V5 (5Y3G) is the
rectifier.
to this radio because the shafts they
connect to are inset within the radio
and the knobs have a long moulding
behind them to reach the shafts. The
side knob has a longer moulding than
the others to reach the top-cut tone
control. The matching front knobs are
for tuning and volume.
As an aside, radios with missing
knobs can be a real problem for radio
collectors, as genuine replacements
can be difficult (if not impossible) to
obtain. It was not uncommon for an
owner to remove the knobs from a
radio at the end of its service life (because they could be handy to keep in
a junkbox), before either disposing of
the set or storing it in a shed.
The radio featured here was also the
only one of three to retain its frontpanel badge. This badge is glued on
and is often “souvenired” at the same
time as the knobs. The heraldic knight
featured on the badge was doubtless
intended to give the impression of
tradition and high class. This motif
on the badge continued into the early
1950s and then disappeared when
the cabinets changed from Bakelite
to PVC.
The cabinet used for the set featured
here is a classic brown Bakelite type.
A cabinet with a rainbow of mottled
colours could be purchased at slightly
siliconchip.com.au
greater cost (see p212-213 of the book
“Radio Days”, by Peter Sheridan and
Ritchie Singer).
Although fairly sturdy, the cabinet
used for the 5A26 can also be rather
brittle (especially with age) and the
other two examples in my collections
have cracks in them. The design is
slightly different to other radios sold
at the time, being somewhat longer
and lower than competitive offerings. However, insetting the dial into
a rounded profile at the top of the
cabinet was common to many other
radios of the 1940s.
The grille has the appearance of
perforated metal behind the moulded
bars. In reality, it’s not metal but is
printed cardboard with perforations
to let the sound through. A thicker
laminated inset of cardboard forms
a baffle for the speaker and improves
the bass response by acting as a seal
around the speaker’s frame
to audio preamplifier stage V3 (6B6G)
via volume control R7A and this then
drives audio output stage V4 (6V6G).
V4 in turn drives the loudspeaker via
an output transformer.
Valve V5 (5Y3G) is the rectifier and
this provides full-wave rectification
of the centre-tapped HT secondary
winding on the power transformer.
The 5Y5G was a common pre-war
rectifier and has a directly heated
cathode which required a separate 5V
transformer winding.
With an input of 240VAC, the first
filter electrolytic capacitor (C13A)
settles at 267V. Further HT filtering is
Circuit details
Fig.1 shows the circuit details of
the Stromberg-Carlson model 5A26.
It’s a conventional 5-valve superhet
configuration with valve V1 (6J8G)
functioning as a self-oscillating mixer
and V2 (6G8G) as an IF amplifier/
detector/AGC stage.
The detected audio from V2 is fed
This is the badge used by StrombergCarlson on the 1946 model 5A26.
January 2015 95
then provided by inductor L6A and
electrolytic capacitor C15A.
Note that three of the valves (V1, V2
& V3) have top-cap grid terminations,
as indicated by the pin-out diagrams
in Fig.2 (reproduced from the data
published in the Australian Official
Radio Service Manual, 1946). The
loudspeaker is a Rola 5-inch permanent magnet type, so filter inductor
L6A is a discrete component rather
than a field coil.
In short, the set’s performance is
excellent, making the 5A26 a worthy
addition to any radio collection.
Above: the inside of the old radio looked like it had been
splattered with fat but this “grease” probably came from
the wax impregnation used in the power transformer and
other components.
The chassis was given a thorough clean up with mineral turpentine to remove
the wax and dust, while abrasive paper was used to restore the appearance of
the aluminium IF-coil cans and the transformer covers.
Restoration
The chassis is easy to remove from
the case. Once the three knobs have
been removed (by pulling them off), it’s
just a matter of removing two screws
at the rear and then sliding the chassis (complete with speaker and dial
assembly) out.
The two metal brackets over the
top of the chassis are mainly there to
support the glass dial and other dial
assembly parts. As a bonus, they also
provide a stable platform when the
chassis is turned upside down for
servicing.
As acquired, the old StrombergCarlson radio was dusty and soiled
and it was tempting to clean it before
testing it. However, I have found by
experience that this can inadvertently create problems by disturbing
pin connections and/or breaking fine
wires, etc. In my opinion, it’s always
Below: the under-chassis view before restoration. Most of the electrolytic and paper capacitors had already been replaced,
while the mains cord had been restrained by a knot (which is now illegal) and did not have its Earth wire connected to
chassis.
96 Silicon Chip
siliconchip.com.au
helpful to know whether or not a radio
worked before cleaning it and whether
any subsequent failure may be due to
the cleaning process used.
This particular radio worked from
first plug-in and drew a reasonable
46W, indicating that there were no
disastrous failures in the filter electrolytics. The radio could be tuned
using the front tuning knob but the
dial pointer didn’t move.
This can occur because the tuning
mechanism has two driven sections:
(1) a friction-geared coupling from the
front panel knob that turns the tuning
gang; and (2) a dial-cord arrangement
driven by a drum on the tuning gang
shaft and threaded around pulleys that
guide the dial pointer along its path.
The dial cord hadn’t broken but had
come away from its track, so I had to
figure out the correct path in order to
rethread it. This was more challenging
than on most radios I’ve tackled but I
eventually got it working. The trick
is to make two loops around a stringclamp to get just the right amount of
spring tension.
All components on the top of the
chassis looked like they had spent
years next to a fry pan in a kitchen and
had been splattered with fat. However,
there are two pieces of evidence against
this explanation: (1) the soiling was
not spread across the components in a
pattern consistent with splatter; and (2)
another 5A26 showed identical soiling,
indicating a characteristic inherent to
these Stromberg-Carlson radios.
Something had apparently deteriorated into an aerosol over the years
and had covered the upper chassis
components. I have no idea what the
source was and it was a mystery that I
was happy to move on from. (Editor’s
comment: this grease may have come
from the wax impregnation in the
power transformer and other components. In the early days, wax was used
for impregnating transformers while
later production models would have
used varnish impregnation. In fact,
wax impregnation was still being used
for high-voltage paper capacitors [in
tin-plate cans] in the 1960s and 1970s).
A thorough clean-up of the chassis
with mineral turpentine removed the
grease and dust. Some 180 grit abrasive paper was then used to shine the
aluminium IF-coil cans and clean the
steel chassis. Note that although steel
wool does a good job when it comes
to bringing back a shining metal sursiliconchip.com.au
This advertisement for Stromberg-Carlson appeared in 1953 and illustrates the
range of high-end radios and radiograms offered by the company at that time.
This view shows the chassis of the Stromberg-Carlson 5A26 after restoration.
The dial cord had come away from its track and figuring out the correct path
in order to restring it was one of the challenges faced in restoring this radio.
January 2015 97
Stromberg-Carlson pioneered gramophone playback via a radio’s audio
amplifier stage. This photo shows the
box-top of a 1928 add-on “Magnetic
Pick-Up Outfit”.
A new fabric-covered mains cord was fitted to the restored chassis. This was
anchored using a cable clamp and its Earth wire secured to the chassis.
face, it should not be used to clean
old radios. That’s because conductive
fragments can end up in odd places,
particularly in the tuning gang and the
speaker magnet.
For really badly-soiled low-value
radios, I occasionally use a waterbased degreaser. This does an excellent job in cutting away the grime but
a great deal of care must be taken to
protect the power transformer. It’s also
necessary to give the chassis sufficient
time to completely dry out.
Loose grid cap
The 6G8 valve’s grid cap came off
while I was removing the valves, prior
to cleaning the chassis. This was repaired by first tinning the small wire
left protruding from the valve’s glass
envelope, then drilling through the
top of the cap before carefully gluing
it to the glass envelope with Araldite.
The cap was then filled with solder via
the drill hole, in order to electricallyconnect it to the grid wire.
As stated above, three of the valves
have top-cap grid connections. In the
case of V1 & V2, these go to the tuning
gang and the secondary winding of the
first IF coil respectively, while V3’s grid
connects to the wiper of the volume
control via a capacitor. These top-cap
connections allow the leads to be kept
short, to minimise stray capacitance.
In radios of this vintage, it’s usually
fair to assume that electrocution is
unlikely due to accidental contact with
a top connector to a valve in the RF
stages because the grid voltage is low.
Fig.2: the pin-outs for
the valves used in the
5A26. Note that three
of the valves (V1-V3)
have top-cap grid
connections.
98 Silicon Chip
By contrast, contact with a an audio
power output valve with a top-cap
could well prove fatal. That’s because
the cap is feeding the full HT voltage
to the valve’s anode, as a means of
avoiding arcing between its pins at
the base. So err on the safe side and
avoid contact with top caps – at least
until you’re sure that dangerous HT
voltages aren’t present!
Capacitor surprise
My biggest surprise with this radio
came when I looked under the chassis and discovered that someone had
previously replaced many of the capacitors and had done a thorough job.
So despite external appearances, the
radio was in remarkably good condition overall.
That was in marked contrast to another 5A26 I recently worked on where
it had taken some time to establish that
the 6J8 and 6V6 valves had failed, along
with capacitors C7C, C11A, C13A
& C17A, resistor R4A (in the cathode
circuit of V4) and the speaker transformer. It’s worth noting that C7C
(between V3 & V4) failed only after
I replaced the filter electrolytics and
the HT increased. This illustrates the
value of replacing all paper capacitors,
particularly in high-voltage sections, to
avoid progressive failures.
Finally, a replacement 3-core mains
lead had been installed by the previous restorer but the earth had been
left floating. The olive-green colour
of that replacement cable didn’t suit
the set, so I substituted a black-flecked
cloth-covered cable and connected
the Earth lead securely to the chassis.
This new cable was also clamped to
the chassis, rather than using a knot
inside the chassis (now illegal), as used
SC
to “restrain” the old cable.
siliconchip.com.au
ASK SILICON CHIP
Got a technical problem? Can’t understand a piece of jargon or some technical principle? Drop us a line
and we’ll answer your question. Send your email to silicon<at>siliconchip.com.au
Can the Currawong be
used in bridge mode?
I hope the new Currawong valve
amplifier takes off. I think it will be in
many constructor’s budget – this is an
important fact. My question is could it
be run in bridge mode with a bridging
adapter? (B. H., via email).
• We certainly hope the Currawong
does not “take off”, as in oscillate
supersonically! We have tested it for
stability and can state that it is unconditionally stable. Note that some
old valve amplifiers could not make
that claim.
As far as bridge mode is concerned,
you could do that but it is not very
good at driving low impedances. This
means that you will get less power
than you might expect in bridge mode.
Problem with links
to on-line videos
I buy your magazine every month. I
tried to download the video at http://
youtube/AHrZgS-Gvi4 in the feature
article on Argus in the December 2014
issue. “Video not available” was the
the response. Please send me the current URL or send me the video. (M.
K., via email).
• The link does work but you have
to type it exactly as it is printed. You
have made a mistake in the typing of
“youtu.be”. Try again at http://youtu.be/
AHrZgS-Gvi4 You will find it then
transfers you to a secure Youtube
video.
Other readers have found difficulty
with a link to an oscilloscope competition on page 99 of the same issue. In
that case, the problem is more subtle
because the underscores in the web
address have been hidden by the blue
underline. The only clue is the spaces
between some letters in the address.
If you frequently like to look at the
websites in the magazine, you will find
that all links in the on-line edition at
www.siliconchip.com.au are “live”.
There is no need to laboriously transcribe them – you just need to click
your mouse on them to make the jump
to the web page.
Similarly, you will find that a lot of
our advertisers have live links on their
advertising in the magazine. Some
even have live links embedded in
photos and illustrations. If you hover
the mouse over the illustration and
the arrow cursor changes to a “hand”
symbol, then you can click on it to go
to another web page.
Multiple questions
& answers
I have a number of questions which
I would like to ask. I hope there are not
too many for the system.
Firstly, I understand that volume
control pots have a logarithmic taper
and the reason for this is that it mimics the human ear’s response to sound.
What I don’t understand is why different projects use different values for
their volume control pots?
Over the years I have seen pot values
of 10kΩ, 25kΩ, 50kΩ and others. What
is the reason for using different values?
Is it for impedance matching or is it
related to the amount of current that
the source signal can supply?
Secondly, I have a question about
“Flaring” or “Spillover” in CRT TVs.
When I studied TV theory and was repairing TVs over 20 years ago, I worked
on TVs with cathode-ray tubes. Some-
Driving One Set Of Speakers With Two Amplifiers
Can you please tell me if it is safe
to connect two stereo amplifiers to
the same set of speakers? The amplifiers are both solid-state and will of
course not be used simultaneously.
(I. P., via email).
• It is definitely not safe to do
this. Depending on the signal level,
it could damage both the driving
amplifier and the amplifier that is
turned off. It is difficult to analyse
exactly what would happen but
perhaps the amplifier that is turned
off is the one that is at greatest risk
of damage.
Consider that even though it is
turned off, its output transistors and
the junctions of the driver transistors will definitely be affected by
the presence of a large amplitude
siliconchip.com.au
audio signal across them and heavy
currents could flow. At the very least,
the fuses in the driving amplifier
may blow.
Of course, if both amplifiers have
loudspeaker protection relays which
disconnect the speakers when they
are turned off, no damage may result.
However, we would want to make
sure that the protection relays do not
short the speakers when the amplifiers are turned off.
SILICON CHIP loudspeaker protectors do, in fact, short the speakers
when the amplifiers are turned off
and the idea behind that is to short
any heavy DC arc current which may
flow if you have a catastrophic fault
in the amplifier.
So in this case, protection relays
in the off amplifier could damage
the driving amplifier. If you tried it,
the shorted outputs of the off amplifier might mean that you could be
tempted to turn up the wick because
no sound would emanate from the
loudspeakers. That could be the
coup de grace for at least one of the
amplifiers.
Really, the only safe way to connect two stereo amplifiers to one set
of loudspeakers would be to use a
pair of changeover (ie, DPDT) relays,
together with suitable switching of
the relay coils using a “break before
make” switch. This would ensure
that only one relay could be energised at one time and would provide
complete isolation between the two
amplifiers.
January 2015 99
Model Train Controller With Inertia
I have bought two 10/20A motor
speed control kits (SILICON CHIP, June
1997) for use as PWM model railway
controllers from the Jaycar agents
in Tauranga, NZ. I was wondering
about modifications to allow simulated inertia and braking by applying
capacitance to the wiper of VR1.
Also, I am curious as to the effect
of a dead short across the tracks
(output). Is there a way to incorporate an automatically reset overload
protection (say with a transistor and
LED) which will protect the Mosfet
and the chip? (P. O., via email).
• We published a Li’l Pulser train
Controller in July 2013 with revision
in January 2014. This incorporated
back-EMF feedback for extra smooth
running and compensation for load
and incline, inertia and braking plus
over current protection, forward
and reverse. It is the best solution
for your application. The June 1997
Motor Speed Controller is far from
ideal for use as a model train controltimes I would encounter an old picture
tube. If the colour control pot and/or
the contrast control was turned up
too high, and sometimes even when it
wasn’t, I would often observe smeary
colour effects.
This could present itself on a human
face, for example, where instead of the
edges being sharp and well defined,
the colours would smear and spread
out. I’ve always wondered what caused
this fault. Is it because the phosphor
dots on the inside of the picture tube
have aged and are no longer sharp but
respond to the electron bombardment
by smearing instead?
Thirdly, I was very pleased to read
about “Little Jim” (SILICON CHIP, January 2006), an AM transmitter for use
with AM radios. As a member of the
Historical Radio Society of Australia
(HRSA), I can see the value of being
able to generate AM transmissions
containing old radio programs or music that can add “life” to an old radio
on display or perhaps even in a workshop. Unfortunately, with the demise
of RCS Radio, a PCB for this project is
no longer available and therefore, this
project can no longer be built.
The circuit is not particularly complex so that even if a kit wasn’t releas
100 Silicon Chip
ler, due to its lack of features and no
overload protection which is vital in
a train controller.
For the Motor Speed Controller,
adding capacitance to the speed pot
wiper will give a variable inertia that
depends on speed pot position. Also
to get realistic inertia, the capacitor
would need to be 4700µF assuming
a mid-position potentiometer and
that is for 20s inertia. At lower speed
settings, this would be considerably
less.
Over-current protection could be
incorporated by adding a currentsensing resistor between the Mosfet
source and 0V. Then add a BC337
NPN transistor with emitter to 0V,
base to the source of the Mosfet and
the collector to the gate. A 0.47Ω 5W
resistor would give about a 1A limit
and 0.1Ω, around 4A. The 4.7Ω gate
resistor would need increasing to,
say, 100Ω to prevent high current in
the BC337 transistor when it shunts
the gate to 0V.
ed by Jaycar or Altronics, I could foresee, with access to a PCB via the SILICON CHIP Online Shop, that it could be
constructed relatively easily. Are you
going to produce a “Little Jim” Mk.2?
Fourth, I want to build a communications speaker that would be suitable
for ham radio use. My plan would be
to use an 8-ohm speaker out of a TV.
I could use the 8-ohm speaker without a filter but then it would pass all
frequencies which I figure would be
undesirable.
As I understand it, voice frequencies
cover the frequency range from 200Hz
to 3kHz. Ignoring the 200Hz part, that
means I need to use a low-pass filter
which will only pass frequencies below 3kHz. I went to the Jaycar website
and located their excellent document
on the subject: crossovr.pdf. From that
document, it appears that I should
be using a 0.4 millihenry inductor in
series with an 8-ohm speaker.
The inductive reactance at 3kHz is
8Ω so I figure half the signal will appear across the inductor and half will
be across the speaker. Is the frequency
range I quoted and my method correct?
(R. F., via email).
• We will answer your questions in
the order that you asked them.
Values of volume controls are
typically selected with an eye to the
impedance of the source but another
parameter which can affect the choice
is to provide a low source impedance
for the following circuitry, in order to
minimise residual noise.
Typically, picture tubes used to flare
because the cathode emission was
low or the EHT supply was defective.
Either way, the electron beam current
was insufficient to enable an increase
in brightness.
The PCB for the Little Jim AM transmitter is available from our website at
www.siliconchip.com.au/Shop/8/864
Note that you also get the front panel
artwork for free when you order the
PCB.
Simply inserting an inductor in series with a loudspeaker, which itself
has inductance, will have little apparent effect on the high frequencies. In
practice, you need to use an LC filter
so as well as the inductor, you also
need to shunt the loudspeaker with a
capacitor. Try a value of 6.8µF.
Mini-D Class-D as a
headphone amplifier
The thought occurred to me that this
amplifier could be used as a headphone
amplifier. It is efficient and has reasonable specifications.
To do as I propose would require that
the negative sides of both the left and
right channel outputs are connected
together to allow the usual “three terminal” connection required for normal
headphones and to allow the correct
phasing of the audio.
Can this be done safely without
causing damage to the TPA3113D2?
(R. G., via email).
• It would not be practical to do that.
You can’t tie the negative outputs together, as they are actively driven and
the chip would detect this as a short
circuit or DC fault and just shut down.
There are some rare headphones
with separate wiring for both drivers or
with the wires joined right at the plug.
In those cases it would be practical to
replace the normal headphone plug
and jack socket with a 4-core shielded
cable and with a 4-pin mini-DIN connector on the end.
But there is little point in doing this
since the Mini-D’s efficiency will be
lower than normal at the low operating
power required for headphones anyway. Its performance isn’t particularly
siliconchip.com.au
good at very low power levels either. So
you would be better off using a standard class-A or class-B amplifier circuit.
You could also look at the Portable
Headphone Amplifier design from
April 2011. That has good sound
quality and low power consumption
although it can suffer from RF pickup.
This could be reduced by building it
into a metal case to provide shielding.
While larger and more complex,
our Hifi Stereo Headphone Amplifier
project from the September & October
2011 issues has been very popular and
is hard to go past in terms of performance. It’s also somewhat easier to
build, using all through-hole components and can even be used to power
a small set of speakers. Its quiescent
current could be adjusted down so it
uses less power while still providing
better sound quality than the Mini-D.
PIC EMI filtering
in a Landcruiser
I realise that this may be an out of
the ordinary enquiry but thought that
I might write to you with a problem I
have. After a few hints from my wife
after she had been driving her Mazda 3
for a while and got used to having an
external temperature display, I designed a reasonably simple circuit to
display both the internal and external
temperatures for our 2005 Series 100
Landcruiser.
The circuit is currently working OK
on the bench and uses a Microchip
PIC18F2520 running at 4MHz, two
Maxim DS18B20 temperature sensors
and a Fordata 8 x 2 LCD (from RS
Components). I thought that I may later
How Do Impact Drivers Develop Such High Torque?
Perhaps you can clear up a mystery for me. I was reading a Bosch
power tool catalog and I was amazed
by the torque which they claim that
impact drivers can develop.
For example, they describe a
battery-powered impact driver, Cat.
GDS V-LiHT, that is an 18V 3Ah unit
capable of 650Nm of torque. If you
calculate what the power input is,
let’s say 18V x 20A, since it is only
short-term, that is only 360W or only
about 0.5HP.
I was further amazed by a mainspowered impact wrench, Model
GDS 30, with a 1-inch (2.54mm)
square drive, that develops hard/
update it to a PIC18F4520 running at
10MHz as I could add the capability
to read and display the charge currents for both the house battery in my
caravan and the auxiliary battery in
the car when travelling.
If I proceed with this, I intend to
use Allegro ACS714 Hall effect current sensors and 433MHz transmitter/
receiver modules to get the data from
the caravan to the car.
My problems arose when I came to
take into account the noise generated
on the 12V supply leads to the PIC and
the coupling into the other car wiring
when the PIC communicates with the
DS18B20s and the LCD – the possible
effect on the other electronic parts of
the car, such as computers, radio etc.
I intended to use screened cable
between the sensors and display and
soft torques of 1000/500Nm and
from “only” a 920W power rating.
My car has a 120kW 2.1-litre turbo/
diesel engine than “only” develops
400Nm of torque. How does this
work? (I. S., via email).
• High gearing is the answer. Consider that these motors can typically
run at 10,000 RPM or more and are
geared down to maybe only 300 RPM
for an impact driver. Furthermore, a
permanent magnet motor has a very
high stall torque, especially when
powered by a lithium battery. Multiply this stall torque by the gearing
and you have something that really
does “torque”!
a well-grounded diecast box housing
the PIC PCB, as well as Murata chip
ferrite beads and chip EMIFIL capacitor type filters on the supply and I/O
lines. Unfortunately, my consideration
of the use of the Murata components
was short-lived when I read the Murata data sheets which stated that
these components should be reflow
soldered (and with special expensive
alloy solders), a little more than my
capabilities at home.
A possible solution could be ferrite
suppression sleeves for the data lines
and winding ferrite toroid cores for the
supply wiring but my strength (if you
could call it that) is with the micros
and programming.
Now to my questions: have you ever
published any articles on this subject
that may be able to help me or could
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January 2015 101
Frequency Compensation In Differential Probe
I was surprised by the circuit for
the Wideband Active Differential
Probe in the September 2014 issue
of SILICON CHIP. The surprise was
that when it is switched to x10 mode
and the 9MΩ resistance is added,
it maintains its high-frequency
response. Usually it’s necessary to
have a small compensation capacitor in parallel with that resistor or
the high-frequency response falls off
dramatically.
Usually too, it needs adjusting to
an exact value on a fast-rise squarewave test to get it bang on.
I think what must have happened
there, if it really does maintain a
flat high-frequency response in x10
mode, is that it turned out that the
you suggest any other articles that
may help me with my design? Alternatively, could you suggest a possible
solution? (K. D., Kareela, NSW).
• We haven’t published any articles
on this topic. The 12V supply to the
PIC regulator will need to be passed
through a voltage clamp such as a
zener diode via a low-value resistance
to prevent damage to the 3V or 5V
regulator for the PIC, or you can use
the LM3940 type which is rated for
automotive use.
As for EMI, this is not likely to be
generated by the PIC or by communication to the sensors or data lines to
the LCD to any extent as the current is
low, ie, in the mA range. Suppression
is generally only required when higher
currents are switched such as with
switchmode power supplies.
You can house the circuitry in a
shielded box as you mention to pre-
capacitance of the switch was just
the right value to compensate it. (H.
H., via email).
• You are quite right about the
switch capacitance (by sheer good
fortune) providing very close to the
correct shunt capacitance to provide
compensation for the 10:1 range.
However that’s not to say that it
wouldn’t be possible to “tweak up”
the response on this range by fitting
a small two-insulated-wires-twistedtogether gimmick capacitor across
each side of the switch. This could
probably be done, although ideally
the two gimmick compensation capacitors should really be matched
to maintain the probe’s differential
balance.
vent the PIC from being affected by
ignition lead interference. The use
of shielded leads for the temperature
sensors is a good idea.
The vehicle ECU will be fully protected from EMI and should not be
affected by your circuit. The radio also
will not be affected. You can use ferrite
beads on the signal lines. This will
round off fast switching edges and so
suppress high-frequency signals sent
down the wiring.
Interference from
ignition system output
I work on a variety of outboard motors and one common problem that I
encounter on Johnson and Evinrude
outboards is that they have an overrev mode, usually 6100RPM, built
into their ignition modules. These go
bad now and then and the module
starts reading wrongly and will start
to miss at around 4500RPM instead of
6100RPM. Therefore you have to buy
a complete new CDI system.
My question is why can’t there be
some kind of a blocker made that
could be put in line to stop or fool the
module from reading the RPM? It gets
its reading from the stator that charges
the module. Older models never had
this over-rev mode and did not have
this kind of problem.
On most outboards that have this
type of ignition, they recommend the
use of a Champion QL prefix type spark
plug which, if I am right, has to do
with radio-frequency suppression and
I have often wondered if this problem
could occur if just standard plugs are
installed.
Could the standard type of plug be
sending out this radio frequency interference? (V. C., via email).
• It seems that an internal breakdown
in the ignition module allows radio
frequency interference (RFI) to upset
the module so as to limit at the earlier
4500RPM instead of 6100RPM. If you
can reduce the source of the radio signal with the RFI-reduced spark plugs
then that is a good solution. Also, using
radio suppressed ignition leads could
also work.
Have a look at this website from
which we have lifted the following salient text about RFI suppression: www.
maxrules.com/fixomcoisignition.html
It states: “There are a couple of critical
items you need to be aware of on these
engines. First, the spark-plug wires
need to be the gray inductive resistor
wires – these are not automotive wires.
Secondly, the spark plugs should be the
factory recommended QL78YC. Use of
other spark plugs or wires can cause
problems inside the power pack from
RFI and MFI noise.”
WARNING!
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 out according to the instructions in the articles. When working on these projects use extreme care to ensure that you do not accidentally come into contact with mains AC voltages or
high voltage DC. If you are not confident about working with projects employing mains voltages or other high voltages, you
are advised not to attempt work on them. Silicon Chip Publications Pty Ltd disclaims any liability for damages should anyone
be killed or injured while working on a project or circuit described in any issue of SILICON CHIP magazine.
Devices or circuits described in SILICON CHIP may be covered by patents. SILICON CHIP disclaims any liability for the infringement of such patents by the manufacturing or selling of any such equipment. SILICON CHIP also disclaims any liability
for projects which are used in such a way as to infringe relevant government regulations and by-laws.
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102 Silicon Chip
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. . . continued from page 102
You could also try adding RFI suppression on the stator lead. There are
clamp-on suppression ferrite sleeves
(eg, Jaycar Cat LF-1294) that may work
or try adding an earthed metal shield
around the ignition module. Otherwise
a high-frequency inductor in line with
the lead may solve the problem, eg,
Jaycar LF-1400, along with a capacitor
on the module side to ground. A 100nF
630V ceramic should be suitable.
Fix for relay chatter
in Tempmaster
I built your temperature controller
to make home brew less hit and miss
in the brewing stage. It controls a small
siliconchip.com.au
fridge and is set to 21°C and I have had
a case of relay chatter which was a bit
disconcerting.
I read during the year that someone
else had the same problem which you
cured but the writer did not elaborate
on the fix. Help please as with summer
coming on I do not need a bad brew.
(P. G., via email).
• We are not sure which project you
are referring to. It doesn’t appear to
be Precision Temperature Logger and
Controller from the January & February
2010 issues or the High Temperature
Thermometer/Thermostat from the
May 2012 issue.
We think you might be referring to
the Tempmaster, the latest iteration of
which was in the August 2014 issue.
The previous version was in February
2009. The latest version is a different
circuit and it does appear to have com-
pletely solved relay chatter problems.
You can see a 2-page preview of
the article at siliconchip.com.au/
Issue/2014/August/The+Tempmaster
+Thermostat+Mk.3
Ceramic jug
element switching
I have a question about the MEN
system that has been discussed in the
magazine lately. Back in the 1950s,
1960s and 1970s, everyone had a china
electric jug. I remember way back when
I was a kid in the 1950s, I first noticed
that in everyone’s kitchen, the power
point Active pin was always brown
and in some cases even black, with
bits crumbling away.
I figured back then it had to be something to do with the jug. They had a
continued page 104
January 2015 103
Majestic Loudspeakers & A Suitable Amplifier
I have been reading SILICON CHIP
magazine and came across some kits
that interested me with regards to
the “man cave” that I have. I have
a shed where I tinker and relax and
have made some additions to it but
I am looking to make some more,
especially with regards to the entertainment set-up.
The Majestic loudspeakers described in the June & September
2014 issues would be good in my
paradise. However, I have some questions about them. I have small and
large children who like to poke their
fingers into everything, God bless
them but they have a habit of destroying things in the process. Are there
speaker grilles, corner protectors or
some devices available to protect
them besides placing them up high?
Then there is the question of the
amplifier that would drive these
speakers. I found the Ultra-LD Mk3
200W Amplifier module (SILICON
CHIP, July to September 2011). Would
this unit do the job to drive the speakers above or is there another unit
more suitable? I live away from my
neighbours so noise complaints are
not on my list of priorities.
As well, I have a big screen TV,
for the big matches, which has many
HDMI ports and a digital audio output port. I would like to connect it to
the amplifier. Do you have a preamp
or a method to connect the audio
from the TV to the amplifier?
Also, I have assorted iPod, DVD &
CD players that have RCA plugs and
Apple connectors that I would like to
interconnect into the system. Is there
a method to connect these devices as
well? (B. D., via email).
• We agree that the Majestic loud-
Ask SILICON CHIP
. . . continued from page 103
wirewound element to heat the water.
You could also get replacements that
just had two metal plates and if you
used these with rain water you had
to add a pinch of salt or they would
not work.
Over the years I have thought about
it but cannot figure out why this should
happen as there were only two wires to
104 Silicon Chip
speakers would need protective
grilles if you have children or pets,
otherwise they will be damaged
quite quickly. There are various 15inch speaker grilles available which
could work. For example, Jaycar has
a clip-on type, Cat. AX3598.
The tweeter could potentially
require protection too. It’s mounted
higher up and back in the horn but
it might still be possible to poke a
finger in and damage it. The simplest
solution in that case might be to tell
them not to do that!
The Ultra-LD Mk3 would be ideal
for driving these speakers and there
is an Altronics kit, Cat.K5125. If
you don’t want to spend that much
money, the smaller Tiny Tim amplifier also works well. That project
was published in the October 2013,
December 2013 and January 2014
issues.
Our CLASSiC DAC design (February-May 2013) will convert stereo
digital audio to high-quality analog
signals that can then be fed to the
amplifier. However you should first
check if your TV has a “stereo downmix” or similar option for the digital
output as this DAC can’t handle compressed audio such as Dolby Digital.
It can also play music and switch
between multiple digital inputs. The
Ultra-LD Mk3 has three inputs but if
you have more audio sources than
that then you would need an external
switching device.
A commercial home-theatre receiver might be a good choice too.
It can do all the switching and
digital-to-analog conversion and you
can feed its left and right channel
pre-outs (assuming it has them) to a
better quality stereo amplifier.
the jug and the jug was insulated, being
china, so there was no way for extra
leakage current to flow back through
the Earth. So what is the explanation
as to why the Neutral terminal did not
also turn brown?
Maybe there is a very wise electrician out there who could explain why
this occurred. (D.F., via email).
• We think you will find that the
blackening of power points in those
days was because people often pulled
the plug straight out of the socket rather
Advertising Index
4D Systems Pty Ltd........................ 9
Altronics.................................. 72-75
Element14...................................... 5
Emona Instruments........................ 3
Hare & Forbes.......................... OBC
Icom Australia.............................. 11
Jaycar .............................. IFC,49-56
KCS Trade Pty Ltd........................ 37
Keith Rippon .............................. 103
KitStop............................................ 9
LD Electronics............................ 103
LEDsales.................................... 103
Microchip Technology..................... 7
Mikroelektronika......................... IBC
Ocean Controls.............................. 6
Quest Electronics....................... 103
Radio, TV & Hobbies DVD............ 93
Sesame Electronics................... 103
Silicon Chip Binders................... 101
Silicon Chip Online Shop............. 83
Silicon Chip PCBs...................... 103
Silicon Chip Subscriptions........... 89
Silvertone Electronics.................... 8
Trio Test & Measurement................ 4
Tronixlabs................................... 103
Wabeco Australia......................... 10
Wiltronics...................................... 59
Worldwide Elect. Components... 103
than switching off first. And if they did
switch off first, the resulting arc across
the switch contacts (in the Active)
circuit eventually led to carbonisation
around the Active terminal.
Note that if the jug boiled over (a
frequent occurence), there was the possibility of leakage to Earth, particularly
if the jug was close to a stainless steel
kitchen sink. In fact, a boiled-over jug
could give a “tingle” if it was not first
turned off before being unplugged.
Also, as these jugs became older, the
Bakelite lids could become partially
conductive and again lead to a “tingle”
from time to time. That was generally
an indication that the jug needed a
new lid or that it should be replaced
SC
altogether.
siliconchip.com.au
siliconchip.com.au
January 2015 105
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