This is only a preview of the March 2018 issue of Silicon Chip. You can view 37 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 "Arduino-based Earthquake Early Warning Alarm":
Items relevant to "Full Wave, 230V Universal Motor Speed Controller":
Items relevant to "An AM Radio Transmitter to build":
Articles in this series:
Items relevant to "Analog Audio/Video Modulator for Vintage TV sets":
Purchase a printed copy of this issue for $10.00. |
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Contents
Vol.31, No.3; March 2018
Features & Reviews
22 Generation IV Nuclear Power – making their own fuel
The new generation of Nuclear Reactors promise many advantages over
existing designs, including safety – and even today’s power plants are orders
of magnitude safer than any other form of power generation. And the new
generation don’t have a waste problem: they use it all – by David Maddison
73 El Cheapo Modules 14: Logarithmic RF Detector
Another one from Banggood, this gives a DC output voltage which varies
linearly with the RF input power level, over a super-wide bandwidth of 1MHz to
8GHz, and a range of 60dB. It’s suitable for a wide variety of RF measurement
equipment – by Jim Rowe
Constructional Projects
14 Arduino-based Earthquake Early Warning Alarm
Everyone knows the first warning you get of an earthquake is when the building
shakes, right? Not quite – there are certain waves which arrive first and can
give you quite a bit of warning. This Arduino-based detector can detect these
early waves – by Allan Linton-Smith and Nicholas Vinen
34 Full Wave, 230V Universal Motor Speed Controller
You’ll be amazed at the performance of this controller. Because it’s full wave
(Triac-based) you get excellent speed control from near zero to maximum while
maintaining torque. Perfect for drills and small hand tools with “universal” motors
– by John Clarke
64 An AM Radio Transmitter to build
Every kid’s dream: become a DJ, transmitting music around the home. But this
also has other uses too – vintage radio enthusiasts can transmit programming
to their restored (AM) radio receivers. And you can re-transmit DAB+ programs
so other AM receivers are in sync! – by Nicholas Vinen & Jim Rowe
SILICON
CHIP
www.siliconchip.com.au
Using a simple 3-axis
accelerometer, this
Arduinobased
detector
could give
you precious minutes early warning
of an impeding earthquake – Page 14
Gen IV Nuclear
Power Stations
are now being
built all around
the world . . .
except for
a notable
exception. Why?
– Page 22
Triac-based so it
gives full-wave
control, our
new motor
speed control
is just what every
workshop needs! – Page 34
1MHz to 8GHz RF
measurement was
never so easy, nor
so inexpensive! –
Page 73
80 Analog Audio/Video Modulator for Vintage TV sets
Restoring old/vintage TV sets is becoming quite popular. But now that analog
TV has gone, what can you display on them? This modulator cleans up virtually
any analog TV signal (eg, from a tape, a DVD/Blu-Ray disc and even off-air
programs from a digital STB!) to suit old TV sets – by Ian Robertson
Your Favourite Columns
58 Serviceman’s Log
Squeezing an elephant through the eye of a needle – by Dave Thompson
45 Circuit Notebook
(1) Drift-free induction balance metal detector
(2) Colour slideshow with alarm clock using an ESP32
91 Vintage Radio
Philips 1953 portable 5-valve model 148C radio – by Graham Parslow
Everything Else!
4 Editorial Viewpoint
6 Mailbag – Your Feedback
57 Product Showcase
96 SILICON CHIP Online Shop
98 Ask SILICON CHIP
103 Market Centre
104 Advertising Index
104 Notes and Errata
Our new AM Radio Transmitter will
take input from
a variety of
sources and
transmit to
any AM radio
set. And best
of all, it’s
completely legal! – Page 64
Into vintage TV restoration? What
do you display on them? This audio/
video modulator lets you use any
modern source
and feeds the
required
signal to
any analog
TV receiver
– Page 80
www.facebook.com/siliconchipmagazine
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SILICON
SILIC
CHIP
www.siliconchip.com.au
Publisher
Leo Simpson, B.Bus., FAICD
Editor
Nicholas Vinen
Got a project idea? There’ll be a
badly designed app for that!
Derby Street, Silverwater, NSW 2148.
In thinking up ideas for projects to publish in Silicon
Chip, we have a lot of hurdles to overcome and they
seem to be multiplying.
Increasingly, we face the challenge of coming up with
designs that aren’t already available commercially (eg,
from China) for less than the retail cost of the parts. We
also have to consider the availability of smart phone
apps which purport to do a similar job.
But while there is often an “app for that”, it usually turns out to be a bit of
a joke. For example, while working on the Earthquake Early Warning project
published this month, we decided to try out a few earthquake alert apps first.
One claimed to provide “earthquake early warning” but seems to rely mostly on alerts from the USGS Earthquake Notification Service which states: “Information for earthquakes in the U.S. is generally available within 5 minutes;
information for earthquakes elsewhere in the World is generally available
within 30 minutes”.
Hmm. Getting a message 30 minutes after a quake does seem a little pointless!
Now, the app does claim that it uses your phone and others running the
same app in the general area to directly detect and warn of earthquakes but
since there haven’t been any earthquakes in our area in the last couple of
months, we have no way of evaluating its true effectiveness. What if nobody
nearby is running the app? How do we know their earthquake detection software really works?
And this is not an isolated case. For example, we’ve long thought that pretty much all “sound meter” apps are generally useless since the microphone
in your phone doesn’t have enough dynamic range and isn’t calibrated. And
audio oscillator apps cannot be guaranteed to generate the frequencies you
might select. You might hear a tone but it might be far removed from the frequency it purports to be.
This was driven home for me while watching an episode of the TV show
“Top Gear” a few years ago where the host as the time, Jeremy Clarkson, attempted to measure the noise levels of three different cars using his iPhone.
He got pretty much the same reading in each case (within 1dB); possibly because the microphone was being overloaded by the noise. And the app “sort
of” works, while the microphone sensitivity is an unknown and therefore any
measurements may have very doubtful accuracy.
Maybe this was a stunt; surely a TV show with a multi-million dollar budget could afford a proper sound level meter? But I wonder how many users of
this sort of app realise its limitations?
Light meter apps also must be suspect. While seemingly useful, we have to
wonder just how accurate they are; presumably they sample the light using
the phone’s camera and its accuracy will vary from model to model. And the
apps rarely provide any information as to the reliability or precision of their
readings. They could be spot on or way off. Unless you compare them directly
to a calibrated instrument, how would you know?
Having said all that, some apps definitely are handy. For example, we’ve
published circuits in the past to generate white noise, water sounds and so on
but now there are free “white noise” apps which make such projects obsolete.
And that’s just one example that comes to mind.
So when you see a project in the magazine, know that we’ve considered all
the above. And before you rely on any app, make sure you check to ensure
that it can deliver what it promises.
ISSN 1030-2662
Recommended & maximum price only.
Nicholas Vinen
Technical Editor
John Clarke, B.E.(Elec.)
Technical Staff
Ross Tester
Jim Rowe, B.A., B.Sc
Bao Smith, B.Sc
Art Director & Production Manager
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Reader Services
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Glyn Smith
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glyn<at>siliconchip.com.au
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Editorial Viewpoint
Silicon Chip
Celebrating 30 Years
siliconchip.com.au
siliconchip.com.au
Celebrating 30 Years
March 2018 5
MAILBAG – your feedback
Letters and emails should contain complete name, address and daytime phone number. Letters
to the Editor are submitted on the condition that Silicon Chip Publications Pty Ltd may edit and
has the right to reproduce in electronic form and communicate these letters. This also applies to
submissions to “Ask SILICON CHIP”, “Circuit Notebook” and “Serviceman”.
Lath-E-Boy wiring is dangerous
as presented
I just received the January issue and
as usual it was a great read! But looking at the schematic on page 39 for the
Lath-E-boy, there is a very problematic
scenario in the bottom right-hand corner. The wiring for the induction motor is the big concern.
As per AS3000, under no circumstances are you allowed to use the yellow/green wire for power. It is only to
be used for earthing. On page 41, in the
picture of the junction box, you can
see the yellow/green wire connected
to the blue wire.
Even if the motor is mounted to the
machine which is usually metal you
still have to earth the motor separately,
in case the bolts come loose.
I know some electricians are using
the yellow/green wire for switching.
In doing so, the wire must be covered
by heat shrink so everyone is aware
that this is not Earth.
It is just easier (and safer) to use a
5-core cable (red, white, blue, black
and yellow/green) with adequate wire
size as you need the yellow/green wire
to earth the motor anyway.
Please make your readers aware of
this and publish a correction!
Thomas Siegmeth,
Camira, Qld.
Comment: Thanks for bringing this to
our attention. It is a big No-No and we
should have spotted it.
We are publishing errata on this in
the current issue and we will change
the motor wiring in the bottom righthand corner of the above circuit:
green/yellow to dark blue and motor
earth to green/yellow. The online edition will have this issue fixed.
Lath-e-Boy reversal
not suitable for all lathes
I have a warning regarding the
Lathe-E-Boy Lathe Controller from the
January 2018 issue (siliconchip.com.
au/Article/10933).
Reversing a lathe such as a Tida
which has a camlock chuck is fine but
if an unwary person sets up a lathe
6
Silicon Chip
with a screw-on chuck to be reversible, the chuck can easily wind off the
spindle nose. Otherwise, I found it to
be a very interesting article. Keep up
the good work.
Ian Stewart,
Camberwell, Vic.
Some vehicles charge their batteries
sporadically
Your recent project for a variable
speed fan controller (January 2018;
siliconchip.com.au/Article/10938) is
a superb piece of simple electronics.
However, recent trends in vehicle
electronic design have now caused
a huge problem, namely that battery
voltage regulation as we have known
it over the past one hundred years is
no more.
The latest Mazda 2 models do have
an upper charge voltage of 14.6V. The
actual voltage with the engine running
varies between 12.0 and 14.6V. I once
travelled 70km with a battery voltage
of 12V, and had to garage the car with
near flat battery! It can continuously
vary around the 12-13V.
This means that designs such as the
fan controller will not work as the low-
Bug fixes for Micromite Mk2
I have produced a new version
of the Micromite Mk2 firmware, for
both Micromite and Micromite Plus
devices: V5.04.07.
This fixes a fairly serious bug reported by Silicon Chip staff, which
results in memory corruption when
a function modifies the contents of
an array of strings passed to it.
The new version can be downloaded from http://geoffg.net/
micromite.html (scroll to the bottom
of the page). You will need a PICkit
3 or Microbridge to upload it to the
PIC32 chip.
I also received a report of LCD
corruption when using the Explore
100 to drive the specified 5-inch
touchscreen at higher CPU speeds
(100MHz+).
Celebrating 30 Years
voltage cut-out may never be exceeded
for long periods. The dealer service division state that it is not a fault, just
normal operation.
I contacted Mazda Australia but
they will not answer any questions of
any nature about this charging scheme
and are very secretive about the whole
matter.
Some auto repair technicians I know
have struck the same problem and
they are baffled and confused. I can’t
find any mention of this in the owner manual, nor do they mention it in
their brochures. Would you consider
doing a feature about this matter in
your magazine?
H. Wrangell,
Elimbah, Qld.
Nicholas responds: we have noticed
this in other vehicles too. Leo Simpson
owns a Honda which sometimes does
not charge the battery unless you turn
on the headlights. Then it will always
charge it. On the other hand, my car
always charges the battery while it’s
It turns out that some LCDs don’t
like the pulse width of some of the
drive signals while other seemingly
identical screens will handle it just
fine.
So I have produced a beta version,
V5.04.08, also available at the above
download link. This increases the
width of the drive pulses and it appears to now work consistently on
all 5-inch LCDs at all CPU speeds
supported by the Micromite Plus
(ie, up to 120MHz).
Geoff Graham,
Perth, WA.
Comment: thanks for these bug fixes. We have updated the downloads
on our website and will program future batches of PIC32 chips that we
supply with the latest (non-beta)
firmware.
siliconchip.com.au
running, so the fan controller works
fine.
We probably should have mentioned this behaviour in the article
and stated that if your vehicle does
not always charge the battery with
the engine running, you will need to
run the Fan Speed Controller from an
ignition-switched supply line and set
its low-battery cut-out threshold below
the minimum expected battery voltage
while driving.
While we do not like this scheme,
it won’t necessarily harm the battery.
But as you say, having to park a vehicle with a near-flat battery is not great.
What if you’re about to go away for a
couple of weeks? What if the weather
is going to get a lot colder during that
period? They must have designed the
battery with enough capacity to still
start the engine under these conditions... you hope.
Possibly it’s a fuel-saving measure
since constantly keeping the battery
on charge will load the engine slightly.
But we’d be surprised if the savings
come to more than a few dollars a
year and the savings would be negative if you had to replace your battery
prematurely.
WiFi model railway control
is already available
I agree with Martyn Davison’s assessment, on page 13 of the January
2018 issue, that Digital Command Control (DCC) is “aged” technology. It is 40
years this year since it was first used to
control model locomotives. DCC has
not only aged, it has become cumbersome and increasingly expensive as it
tries valiantly to meet increasing expectations of modellers.
As a former member of the NMRA’s
DCC Working group, I remember the
pain endured attempting bidirectional
communication with several ineffective solutions battling it out. The fact
is that DCC runs at a bit rate between
4.5 and 9kHz – it’s slow!
Leo Simpson’s reply expresses
doubt as to the ability of Bluetooth or
WiFi to replace DCC despite Martyn
pointing out that Bluetooth model railway control is already being marketed.
Martyn and Leo are both apparently
unaware of recent developments in
WiFi control of model railroads.
Silicon Chip had an article in the
December 2013 issue on the ESP8266
WiFi server (siliconchip.com.au/
Article/8194). These are small and
siliconchip.com.au
cheap; a complete WiFi server the size
of a postage stamp! As soon as I read
it, I realised my dream had come true.
With the help of my son (doing the
programming), I built a prototype that
fitted into an HO diesel locomotive.
It was ugly, comprising an ESP WiFi
module, H-bridge module and a driver
IC. The same circuit built on one board
by a machine would be similar in size
to a DCC decoder.
It worked. Fellow Victorian NMRA
members with little instruction could
select the Loco’s WiFi identity on their
phone, open a browser and view a web
page stored in the WiFi server within the loco itself. Pressing buttons on
the page controlled direction, speed,
lights, horn(s) and uncoupling.
With WiFi, many things are possible
and most are already in use – bidirectional communications is standard,
sound and video achievable.
The same machine that makes DCC
decoders in China could make WiFi
controllers at the same price. It should
be half the price though, as the controller module could be used for many
Internet of Things projects outside the
model railroading hobby.
Having worked towards standards
all my life, I felt a simple standard was
required to ensure universal control between manufacturers. I contacted the
technical department of the NMRA.
They weren’t interested, being currently bogged down with another cumbersome technology – the Layout Control
Bus, DCC-compatible of course.
Manufacturers had invested in LCB
and had a vested interest in keeping
DCC. It was this manufacturer control
of the NMRA that caused me to leave
the DCC working Group in about 2001.
I started my own working group,
find it at: siliconchip.com.au/link/aaj0
A number of modellers joined the
working group. Unfortunately, about
half of them were there to destroy the
project. Vested interests in the US saw
Direct WiFi Control (DWiC) as a direct
threat to their business. It is.
All you need is a $20 controller for
your loco and a phone, tablet or PC.
The loco will run on DCC track, DC,
AC or battery. There’s no need for expensive command stations, boosters
or a plethora of other accessories – the
source of a DCC manufacturer’s profit.
Meanwhile, my son and I had completed the prototype, proved the technology, and sat back and waited for a
manufacturer to seize the opportunity.
Celebrating 30 Years
March 2018 7
Well, one has, and his business is in
Australia; see www.wifitrax.com
DCC took 10 years from its introduction to the NMRA in 1990 till its general acceptance in about 2000. Hopefully, DWiC will not take as long to
be accepted.
Bob Backway,
Belgrave Heights, Vic.
Comment: charging a supercapacitor
bank at each station is an interesting
idea. One hopes that the tram doesn’t
encounter any unexpected obstacle
which causes its bank to become discharged before reaching the next station! Perhaps an onboard emergency
backup power source would be a good
idea.
Error introduced in editing letter
Speaker for the Super-7 AM radio
is sold as a 5-inch unit
I note that you have edited my letter, titled “Instantaneous electric
water heaters technology of the 1940s”,
on pages 10-11 of the January 2018 issue.
Where I stated that the heater was
connected “across phases”, this was
changed to read “across the three
phases”.
I should have said that they were
connected between two of the three
phases of the supply, as the only connection points were (1) to the body of
the heater and (2) to the carbon electrode. There was no place to connect
a third phase.
These heaters did not suffer from
the “slow flow dropout” problem
common to the three-phase models,
as they would continue to draw current as long as any water was present
to provide a path between the carbon
electrode and the body.
Indeed it was possible – although
unwise – to reduce the flow until the
water boiled, resulting in jets of steam
from the outlet.
G. D. Mayman,
Sturt, SA.
Comment: thank you for clarifying this.
Proposed NZ trams use
supercapacitors
I have just finished reading the January 2018 issue of Silicon Chip. There
are once again very interesting articles
about electric and autonomous vehicles. You may be interested in a story
published in the New Zealand Herald
on December 20, 2017 regarding the
proposal for trams in Auckland. See:
siliconchip.com.au/link/aaiv
At the moment, there’s a lot of debate about introducing trams between
the Auckland CBD and Auckland International Airport. We have traffic
congestion just like Sydney. With the
population increase in Auckland, it
is adding an extra 800 cars per week
to our roads.
Keep up the good work.
Graham Street,
Auckland, NZ.
8
Silicon Chip
In the January 2018 issue, P. C. of
Woodcroft, SA complains about not
being able to source a suitable 4-inch
speaker for the Super-7 AM Radio
(Ask Silicon Chip, page 94). I had the
same trouble until I considered the
Jaycar 5-inch round speaker, catalog
code AS3007.
This unit must be the one intended
by the design because it fits onto the
PCB perfectly and looks identical to
the speaker in the prototype photograph. The difficulty has arisen because a 4-inch speaker is specified in
the parts list whereas Jaycar regard the
AS3007 as a 5-inch unit.
Russell Howson,
Bronte, NSW.
Motor start capacitors
degrade over time
Based on recent experience, I wonder how many whitegoods finish up
in landfill for the sake of a $5-10 part.
I recently had the impression our
freezer was “hard-starting”. Measuring
with SC’s Energy Meter (upgraded using Geoff Graham’s firmware) showed
a starting power of 1500W averaged
over the one second update period –
this for a device that draws only 100W
when running!
Further investigation showed the
compressor was driven by a permanent
split-capacitor motor and the run capacitor, labelled as 4µF, had dropped
to a measured value of only 0.5µF.
A replacement capacitor, purchased
from either element14 or RS components, measured 4µF and dropped the
start power to 600W. That’s still a lot
but at least more reasonable.
So, went on to check (then fix)
the fridge, where the capacitor had
dropped from 4µF to 2µF and this had
halved the starting current.
Ian Thompson,
Duncraig, WA.
Leo comments: We suspect that faulty
motor-run capacitors are the reason
many appliances with induction moCelebrating 30 Years
tors are discarded. Just recently I found
that my pool pump motor was reluctant to start and it occurred to me that
the bearings might be dry and needing
lubrication.
However, at around the same time, a
reader I was trying to assist (with problems with our Induction Motor Speed
Controller) found that his problem was
caused by a faulty motor run capacitor; down from 25µF to 17µF.
I duly checked my pump (as part
of a sand filter re-install) and found
that its run capacitor had dropped
from 20µF to 13µF. I replaced it with
a capacitor from Jaycar (Cat RU-6606
<at> $16.95) and that fixed it.
Incidentally, both Jaycar and Altronics have a small range of suitable
motor-run capacitors but they erroneously list them as “motor-start”. The
good thing is that Jaycar and Altronics stores are open seven days, which
is great for “weekend warriors” – that
probably applies to most DIYers.
Sewer Pump Sentry design proposal
I’m writing to you today to present a
project article idea for a “Sewer Pump
Sentry”.
Years back I was having trouble with
my sewer system; in particular the
pump. On one occasion, the pump impeller got jammed by a foreign object
and the motor burned out. On another
occasion, when the septic field froze,
the pump couldn’t empty the tank and
never stopped running until it burned
out. This kind of event often causes a
sewer backup which is no fun and often expensive to deal with.
As a solution to these issues, I designed and built a microprocessorbased system to monitor the sewer
pump motor current and runtime.
Should the current be excessive or the
pump runs too long, my monitor produces an alarm.
Initially I had to measure the pump
current outside the house, at the sewer
pump electrical outlet, since the pump
was not on a circuit by itself. This introduced additional problems in that
the enclosure for the monitor had to
be weather proof and the circuitry had
to operate at potentially -40°C.
In addition, when an alarm condition exists, how is it announced and
noticed when it’s out of the house?
The solution I found for this was kind
of clever (I think). A 60Hz intercom
was modified so that the call function
could be activated by the micro. This
siliconchip.com.au
meant that the alarm could be heard in the house and in
more than one room.
This project has been running for about 10 years now
and has been (for me anyway) one of the most useful things
I have built. Just last week it warned me of a toilet that
hadn’t stopped flushing. So, that’s my project and proposal.
Do you think you folks would like to publish my project?
Gordon Dick,
Alberta, Canada.
Comment: thanks for sending us your circuit. It seems fine
but we already published something quite similar. That
project is the 230VAC Cyclic Pump Timer from the September 2016 issue, by John Clarke. It also monitors the
mains current drawn by a pump and switches it off if it
runs for too long.
While it doesn’t have provision to switch the pump off if
the current is too high, it does include a mains fuse which
should blow in this case (if sized correctly), preventing the
pump from burning out.
That just leaves the issue of how to sound the alarm in
either case. The Cyclic Pump Timer has a fault LED but
this will not switch on if the fuse blows. We will consider
updating that project to include an alarm which will sound
either when fault LED3 lights or fuse F1 blows. Your idea
of using an intercom to make it audible inside your house
is a good one. A wireless doorbell could also be used.
Custom case for Equaliser and VU Meter looks great
I wanted to share with you my realisation of putting the
10-Octave Graphic Equaliser (June-July 2017; siliconchip.
com.au/Series/313) together with the Stereo LED Audio
Level/VU Meter (June-July 2016; siliconchip.com.au/
Series/301).
You published a photo of the custom case I used to
build my Ultra-LD Mk.3 amplifier and CLASSiC DAC on
page 16 of the June 2016 issue. So I decided the equaliser/
VU Meter combination should go into a similar case that
would stack with those.
My top criterion was the look of the enclosure. It had to
be neat. I used the same construction as before – a 10mm
aluminium faceplate, 2U enclosure. I used your two PCB
layouts to design the front panel drawings with Adobe Illustrator and provide .dxf files to the manufacturer.
The equaliser part was the most straightforward with
only the holes for the linear pots and the power LED. For
the Stereo VU Meter, I had several choices of design:
• a rectangle hole to encompass the area with 80 LEDs,
with a Plexiglas sheet between the PCB and the enclosure faceplate, or
• two rectangles, corresponding to each channel with
the same Plexiglas sheet behind, or
• replacing the SMD LEDs with 3mm through-hole LEDs
and drilling 80 holes. This solution had my favour
initially, although desoldering the LEDs would have
been tedious, or
• milling one rectangle and inserting a piece of Plexiglas inside (since the faceplate is 10mm thick). That
would have been nice, but I was afraid the light conveyed from the LEDs would not be seen as individual
light spots, or
• milling individual holes for each LED with an individual Plexiglas insert to “bring” the light from the LED to
the faceplate. I thought this would be the best solution.
10
Silicon Chip
So I looked for Plexiglas cutting services and specified 2 x 6mm rectangular pieces (pretty much the size of
the LEDs).
I needed around 12mm between the faceplate and the
PCB. But they cannot cut a 12mm thick sheet. So they
cut a 2.54mm thick sheet to 6 x 12mm instead and I used
these pieces side-on.
But one important point had to be taken into consideration: the milling bit cannot make perfectly square holes
in the aluminium plate. There was a radius for each cut
in the aluminium. So I asked the cutting guy to round the
corners of each Plexiglas piece.
When the enclosure came back, I was pleased as the
two PCBs fitted exactly right. Indeed, space is very tight
behind the faceplate! Everything was perfectly aligned.
One challenge for the enclosure manufacturer was that
each hole was specified as 2.54 x 6mm: rather small to mill
in 10mm thick aluminium. So they had to mill the back
of the faceplate by 8mm to facilitate the usage of a small
drill bit – making the holes actually 2mm deep.
When the Plexiglas pieces came back, their corners were
rounded but not as I expected! I should have thought about
it harder before. Since the sheet was 2.54mm thick, the
rounded corners were those around the 6 x 12mm face
and not the 2.54 x 6mm face.
So I had to file the corners of each piece with my Dremel.
Eventually, I inserted the 88 pieces into their respective
holes. Friction held them in place quite nicely.
One more criterion on top of the look was that I wanted
the unit to be powered on and off together with the amplifier (my wife would have complained about one more
button to push!). So I ran the power supply from the AC
plugpack to the amplifier switch then back to the enclosure. It works well.
As I said in my previous letter, I no longer have any
noise from the shared power supply, as the units are independently powered after the mains switch.
I’m including a photo of my set-up now. I am very
happy with the final result. The light of each LED is well
separated from its immediate neighbour. The VU Meter
is connected directly to the amplifier speaker outputs at
the back.
Thanks and keep up the good work in the magazine!
Olivier Aubertin,
Singapore.
Comment: we think this is an outstanding result, well done!
Celebrating 30 Years
siliconchip.com.au
Hot Water Systems article criticism
I have been waiting for someone else to advise you that
your recent article on adjusting hot water system thermostats (October 2017; siliconchip.com.au/Article/10834)
should either be retracted or, at least, heavily qualified;
it looks like it’s up to me.
There is a reason why such thermostats must work at
70°C or higher. It’s to prevent Legionella bacteria (of legionnaire’s disease fame) from growing in the hot water
tank. A quick internet search will support this.
There is also a requirement to reduce the temperature
of the water to less than 55°C at the outlet. This being to
reduce the risk of scalding. This requirement is usually
met with the use of a “tempering valve” that mixes cold
water with hot water at the system outlet.
In summary, that water is heated up then cooled down
as required. I haven’t researched it but I’m pretty sure that
this situation is legislated and that anyone messing with
it is open to action from on high.
By the way, I consider Silicon Chip to be one of the finest magazines there is.
Peter McAulay,
via email.
Leo responds: no-one else has sought to comment on the
veracity of the article and I believe that I adequately covered both the dangers of Legionella and tempering valves
in the article. I read a number of current health and safety
papers and regulations while I was writing the article, so
I think it is technically correct.
You can argue about whether the minimum temperature in a hot water tank should be 60°C or 65°C but 70°C
is far too hot and it wastes energy.
While I did not specifically mention it, many hot water
systems are close to or actually in home laundries. That
can mean there is a significant risk of scalding from the
hot water tap over laundry tubs. Arguably, a tempering
valve could be fitted in these circumstances.
One of the main reasons I wrote the article is that many
hot systems are simply set far too high, with the attendant dangers of scalding of infants and older people. In
only takes two seconds exposure to hot water at 60°C to
cause scalding.
I have grandchildren and I have seen first hand how
they can turn on the hot water tap while they are cavorting in the bath. In almost the blink of an eye, they could
have been scalded if the temperature was at 60°C.
Instances of scalding are quite common while Legionella
in hot water systems is fairly rare, although it is fairly common in air conditioner cooling towers in large installations.
100
95
75
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EL_Aus_Resins_87x120mm_012018_prepress
23 January 2018 16:56:22
Article on inverter generators wanted
Firstly, thanks for a great publication that I look forward
to receiving each month. Could you please do an article
on inverter generators?
I have been looking at buying a small generator and have
been overwhelmed by the range available and the claims
made. I like many others do not trust the power grid and
want some personal backup power at home. Some of the
factors I have been presented with include.
• inverter generators will carbon up the cylinder if run
too long on a light load because the revs vary with the
load (including Honda generators, which are regarded
as the benchmark).
siliconchip.com.au
Celebrating 30 Years
March 2018 11
• cheap inverter generators are not
suitable for powering electronic
loads – only the more expensive
inverter units are suitable.
• all inverter generators claim to
have a “pure sine wave” output –
is it a better sinewave than a standard generator?
• does the output of an inverter generator have lower harmonic content than a standard generator?
• inverter generators have an advantage in weight and portability.
• the small profile of inverter generators might become a problem
with heat dissipation at high load
(high revs).
• how is protection earthing
achieved with an inverter type?
Standard generators have the earth
conductor bonded to the neutral
conductor inside the generator in
order to complete the fault circuit
path to trip the protection during
a fault.
• motor starting ability – most inverters are rated for peak and continuous watts. Their motor starting
ability is vague at best. It would appear that standard generators have
better motor starting ability due to
rotational inertia.
• some inverter generators have
paralleling kits available (which I
think is not much use to a homeowner wanting small loads during
a blackout).
It would probably be good to include
something on the danger of powering
the house through a male/male extension cord powering the house back
through a power point. A common
practice as I understand it.
I look forward to any future article
on generators.
John Lean,
Orange, NSW.
Comment: we will consider publishing an article on inverter generators
but this would be a big undertaking.
Carbon build-up is definitely an issue for internal combustion engines
that never run near red-line or at full
load. This can usually be fixed by purposefully loading the engine for a few
minutes (eg, by plugging in a radiator) which will burn off or blow out
the carbon build-up. When done with
a motor vehicle, this is known as an
“Italian tune-up”!
Most electronic loads don’t need
a sinewave to operate properly. Even
a square wave with the appropriate
12
Silicon Chip
voltage is fine. That’s why most UPS
devices, designed to power computers
and such, do not produce a sinewave
output.
The main reason why electronic
loads would challenge an inverter
would be the high inrush current but
this can be mitigated with a soft starter (as published in our April and July
2012 issues).
You may also be able to use a Soft
Starter to improve motor starting, depending on the type of motor. The
speed controller on page 34 of this
issue would definitely help if you’re
running power tools from an inverter
(assuming they aren’t powered by an
induction motor).
The earthing arrangement for an inverter generator should be similar to
any other generator.
A non-inverter generator likely
would have a fairly pure output offload but the sinewave will distort under heavy load. That’s less of an issue
with inverter-based generators.
So we would guess that the waveform from an inverter generator under load would have lower overall
harmonics.
But most loads are not terribly sensitive to this. Consider that the mains
already has fairly high distortion (up
to a few percent).
Problems loading Arduino sketches
Thanks for the interesting article
on barometric pressure sensors in the
December 2017 issue. I purchased the
code for the Arduino and installed the
SFE_BMP180 Library. I renamed the library folder to match the library name
in the sketch.
However, the sketch would not compile and I have sent a couple of pictures to show the error (SFE_BMP180
does not have a name type). I am using
Arduino 1.0.5 r2 which I have never
had any trouble with
I got the same error on sketches
downloaded from the Elecrow site
as well.
I eventually managed to solve the
problem, as follows. I’m not sure
why but the zip file I got was called
“BMP180_Breakout_Arduino_Library-master.” The Arduino IDE didn’t
like that so I changed the folder name
to “SFE_BMP180”.
The IDE liked this and allowed the
library to be installed but the sketch
still would not compile. Upon opening the library folder I found another
Celebrating 30 Years
folder named “src”. The header and
.cpp files were in that folder instead
of the main folder.
I copied them into the main library
folder “SFE_BMP180” as above and
Bingo! Maybe I downloaded the library
from somewhere else other than your
recommended link.
It is worth passing this onto other
readers as I have experienced other
library folder names not matching the
include statement in the sketch.
It is also worth checking that the .h
and .cpp files are visible in the first
folder when you open the library.
This causes a fair bit of frustration
but is great once you finally solve the
mystery.
On another Arduino-related subject,
I had trouble some time ago with the
Arduino sketch for the GSM Remote
Monitoring Station from the March
2014 issue. See www.siliconchip.com.
au/Article/6743
The sketch refused to compile on
IDE 1.8.1 and I found that when I tried
it again on 1.0.5 r2, it worked. Hopefully, these pointers may stop someone
else going mad.
Geoff Coppa,
Alstonville, NSW.
Comment: unfortunately, the link given in the article for the SFE_BMP180
library no longer takes you to a page
with a direct download link for the library. We think this is the source of
the confusion.
You are right that the .h and .cpp
files should be in the main directory
of the Arduino library or it will not
work. A forked version of the original
library that will install directly can be
found at github.com/LowPowerLab/
SFE_BMP180
Clicking on the “Clone or download” on this page and then “Download ZIP” links yields a library with
the files in the right places.
The original library can be found
at github.com/sparkfun/BMP180_
Breakout and github.com/sparkfun/
BMP180_Breakout_Arduino_Library
Comments on past issues
In regards to the January 2018 editorial by Nicholas Vinen on autonomous
vehicle security: driverless cars will
be far safer if their driving computer
is fully air-gapped.
CPUs are so cheap that any ancillary
service(s) should have their own system and not potentially compromise
the driving computer.
siliconchip.com.au
Secondly, the driving computer
must not be proprietary/closed so a
user can be assured that there are no
“back-doors” nor outside control.
The business models of the likes of
Apple, Microsoft etc cannot be trusted
to implement this. A recent example
is Apple deliberately interfering with
the iPhone’s speed.
Then there is the issue of governments’ control/interference! The most
dangerous component of a car is the
nut that holds the steering wheel. The
fact is that 99% of accidents are due
to human (driver) error.
Regarding the November 2017 Dipole Loudspeaker System (siliconchip.
com.au/Article/10865); I love the concept and innovation (and the potential
to reuse old speakers). But looking at
it makes me wonder if it could be rationalised further. How about using
power line networking?
The signal generator then does not
need to be near anything and you can
put the rest in the speaker. The speakers still require both signal and amplification/power which can then be done
from one plug anywhere in the house.
Woofers which have different/bigger amplifier requirements could be
easily separated out and extras added
as desired.
Raspberry Pis are so cheap that they
can easily be used in each speaker
to digitally manipulate/filter the audio frequencies before converting to
analog. Are there any non-proprietary
power line networking “El Cheapo
Modules” for such a project?
Regarding the October 2017 article on setting hot water thermostats
(siliconchip.com.au/Article/10834);
the nuisance I’ve noticed with tempering valves is a reduced flow rate
where they’ve been installed and the
complete loss of really hot water in
situations where it is wanted (eg. dishwashers, laundry etc).
Regarding the September-October
2017 Fully Adjustable, 3-way Active Loudspeaker Crossover project
(siliconchip.com.au/Series/318); this
project seems to be half a step away
from being a simple surround sound
decoder. Perhaps a revised project implementing this improvement would
be worthwhile.
J. Williams,
Elanora, Qld.
Comment: we agree that air gap security for autonomous vehicles would
vastly reduce the chance that they
siliconchip.com.au
could be compromised but it would
also severely limit their usefulness.
They would not be able to download updated maps or software. These
could only be updated during a service and even then, the update process
could potentially be compromised and
malware could be installed without
your knowledge.
Tesla already sell semi-autonomous
vehicles and they are definitely not
air-gapped. In fact, the autonomous
capabilities were added to vehicles
that were already in customers’ hands
and they didn’t have any say in the
matter.
We’re not sure that adding an audioover-power-line interface to an active
loudspeaker system could be considered rationalisation.
It surely is technically possible but
would require some fairly complex
hardware and software.
Ethernet-over-power adaptors are
not terribly expensive and could certainly be teamed up with Raspberry
Pis, or any other single-board computer with an Ethernet port. WiFi seems
like it would be easier and cheaper,
though.
Tempering valves are not normally
installed in kitchens or laundries. They
are primarily for use in bathrooms,
mainly in showers and baths.
These types of valves can also result
in some feedback problems with instantaneous hot water systems, where
the tempering valve lowers the hot
water flow rate over time such that the
hot water system starts to flow cold
water and the tempering valve then
increases the flow rate again and the
cycle repeats.
Can satellites help locate
missing aeroplane?
I enjoy reading your magazine
through the library. I especially liked
the article on Tiny Satellites in the
January 2018 issue (siliconchip.com.
au/Article/10930).
In view of the phenomenal numbers
of satellites generally and their amazing capabilities, has anyone asked the
question of the owners as to whether
there were MH370 sightings when and
where the plane was flying?
Is it naive to think that the answers
lie within some multi-billion terabits
of storage held somewhere?
Thanks for a great magazine.
John Cooper,
via email.
SC
Celebrating 30 Years
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March 2018 13
•Arduino based • Low Cost • Easy to build • Little or no experience needed!
Earthquake
Early Warning Alarm
Concept by Allan Linton-Smith • Circuit and software by Nicholas Vinen
Earthquakes can strike anywhere . . . and usually with very little
warning. But these days there are ways that you can get an early
warning, that may be the difference between getting to safety (eg,
an open area) and possible injury or death. So how do you go about
getting early warnings of impending earthquakes? Read on...
P
robably the easiest way to get
earthquake warnings is to install
an early warning app on your
smartphone.
The idea is that a network of seismographic sensors based around the
world will pick up an earthquake soon
after it occurs and determine its location (based on triangulation), depth
A P Wave
and magnitude.
The app receives this data within
seconds and compares it to your location.
Depending on your proximity to
the earthquake and its magnitude, it
can generate an alert, seconds or even
minutes before the destructive waves
of the earthquake arrive.
Ground is shaking this way
But this does rely on a few things
working properly: you have to have a
smartphone, it has to be charged and
switched on, it has to have a working
internet connection, the app needs
to be installed and running properly.
And there’s also the fact that, depending on where the seismic sensors are located geographically, signifi-
B S Wave
Waves are travelling this way
Fig.1: the four different waves caused by an earthquake. In order of fastest to slowest, (a) the P-wave is a compression
wave, (b) S-wave is up-and-down and/or side-to-side motion.
14
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Celebrating 30 Years
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A commercial earthquake early warning alarm, the
FREQL (Fast Response Equipment against Quake Load),
used by rescue teams in earthquake areas. Ours is very
much simpler . . . and cheaper!
cant time could pass before the alert
is even raised.
We installed some popular earthquake early warning apps and set
them up to warn us about earthquakes
around the world. (There are, literally, hundreds of earthquakes occuring
every day – only the largest make the
six o’clock news . . .)
Timing!
We found that we sometimes got
alerts many minutes after an earthquake had occurred – somewhat pointless, you’d agree!
Of course, even if the warning is
timely, you might not hear the alert
or you may not look at the screen
straight away.
But there’s another option and it
may be much more useful, because it
doesn’t rely on remote seismic sensors,
an internet connection or any software.
And you don’t even need to own a
smartphone.
Early warning using P-waves
Earthquakes cause a disturbance
C Love Wave
Here’s another commercial detector – the Chinese-made
XYB01A. It’s not intended for first-responder use; in fact,
it’s designed for home use, mounting on a wall as shown.
We found it tricky to set up and use.
in the Earth’s crust that you can feel.
They are generally caused by a sudden rock fracture where the pressure
has built up at the junction of two tectonic plates, due to continental drift.
When this energy is suddenly released, it causes waves to travel
through the Earth’s crust away from
the location of the fracture.
You may not realise it but a single
seismic event can cause at least four
different waves to travel through the
Earth and shake the ground beneath
your feet.
Unless you are very close to the epicentre, these waves will arrive at different times and they will have different strengths and effects.
The first wave to arrive is the pressure wave or P-wave. This travels in a
similar manner to the way sound travels through air – see Fig.1(a).
Part of the reason why it arrives
first is that it can travel through solids and liquids, so it can take a direct
path through the Earth to your location (ie, it doesn’t have to follow the
curvature of the Earth, despite the fact
that there are liquid layers under the
Earth’s crust).
The P-wave is usually not terribly
strong nor destructive but it certainly
can be detected using seismic monitoring equipment and this will give
you the most warning before the destructive waves arrive at your location.
The secondary wave is known as
the S-wave and this is caused by rock
particles moving side-to-side or up
and down, similarly to the way that a
wave travels through deep water – see
Fig.1(b). Because the S-wave cannot
travel through liquid, it can not pass
through the Earth’s outer core and so
generally arrives after the P-wave. It is
usually strong enough to be felt but is
not the most destructive wave.
The third wave to arrive is the Love
wave (named after A.E.H. Love) – see
Fig.1(c). This is the fastest surface
wave and is caused by the surface of
the Earth moving side-to-side.
Because it has to travel along the
surface, it takes the longest path and
therefore arrives after the S-wave and
P-wave.
D Rayleigh Wave
(c) the Love wave is side-to-side and (d) the Rayleigh wave has
a vertical, rolling action (and tends to be the most damaging). Source: US Geological Survey.
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March 2018 15
SURFACE WAVES
S-WAVES
AMPLITUDE
P-WAVES
TIME
Fig.2: a seismograph plot taken some distance from an earthquake, showing that the P-waves arrive first, then the
S-waves, then the surface (Love and Rayleigh) waves.Typically, the surface waves have the greatest amplitude and will
be the most destructive. Source: US Geological Survey.
Shortly after the Love wave comes
the Rayleigh wave, which also travels
along the surface. It causes vertical motion as the ground “rolls”, much like
waves in shallow water – see Fig.1(d).
This is the wave which is normally
felt the most and causes the most destruction.
The relative speeds of the P-waves,
S-waves and surface waves can be
seen in the seismograph plot of Fig.2.
Fig.3 gives more detailed information
on the relative speeds of P-waves and
S-waves while Fig.4 shows how the
P-waves and S-waves travel at different speeds through different parts of
the Earth’s crust.
Notice though that the P-wave velocity is always higher than the S-wave
velocity, so in most cases it will arrive
much earlier.
Fig.3 shows how long a typical Pwave and S-wave take to reach a certain distance from the epicentre. As
you can see, the S-wave takes around
twice as long to reach a given point
compared to the P-wave.
If we can detect the passage of the Pwave, then the interval between these
two lines is the amount of warning we
get before the larger S-wave arrives.
For example, if you are 200km from
the epicentre, you would get around
Detecting the P-wave
Commercial P-wave detector devices do exist. One example is the portVELOCITY (km/s)
P & S WAVE TRAVEL TIMES
30
30 seconds’ warning while if you are
2000km away, you will get around five
minutes’ warning.
Unfortunately, the closer you are,
the less warning you will get and the
more destruction the earthquake will
cause (as the waves drop in power as
they travel away from the epicentre
and expand).
For the most damaging ‘quakes, you
probably won’t get more than one minute of warning.
2
4
6
8
10
410
660
12
14
TRANSITIONS
25
SHEAR
WAVE
15
DEPTH (km)
TRAVEL TIME (minutes)
MANTLE
20
10
COMPRESSION
WAVE
5
0
0
2000
4000
6000
DISTANCE (km)
4000
8000
10000
based on Press & Siever, 3rd ed.
Fig.3: a graph of approximately how long it takes
for the P-wave and S-wave to reach a point a certain
distance from the epicentre. The P-waves travel about
twice as fast as the S-waves so they reach the same
distance in about half the time. The lines are curved
due to the curvature of the Earth.
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S-WAVE
P-WAVE
D”-LAYER
OUTER
CORE
INNER
CORE
6000
Fig.4: this shows how fast the P-wave and S-wave
typically travel at various depths in the Earth’s crust.
The P-wave travels faster so it will arrive first.
Celebrating 30 Years
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able FREQL (Fast Response Equipment
against Quake Load). This is used by
rescue teams and fire departments in
Japan and is especially useful for early
warning of dangerous aftershocks during difficult rescue phases. It’s shown
overleaf.
You can also get consumer-grade devices such as the Chinese-made XYB01A detector. This is a wall-mounted unit which runs from a 9V battery
and uses a pendulum to make contact
when a P-wave is experienced, sounding the alarm.
It is mechanically adjustable but is
a little tricky to set up.
The P-wave normally has a frequency of between one and five hertz (15Hz) and could consist of just a short
jolt, a series of tremors or a continuous wave, depending on the nature of
the earthquake.
So to give you the best chance, the
device needs to be as sensitive as possible to signals in that frequency range
and with the correct orientation, without being so sensitive that it could be
set off by other vibrations.
The tiny MPU-6050 3axis accelerometer
which is the “heart” of
the project, detecting
distant P-waves.
erometer/gyroscope, MOD2.
MOD2 uses the MPU-6050 IC and
we’ve chosen this one in particular because it has an on-board 16-bit digitalto-analog converter (DAC). Note that
we aren’t using the gyroscope feature,
just the accelerometer.
At maximum sensitivity, the fullscale reading of this device is ±2g on
each of the three axes and the 16-bit
DAC means this has a resolution of
0.0006g [(2 ÷ 32768].
That’s what we need to detect the
very small vibrations of a P-wave from
a distant source.
P-waves are often so faint that you
can’t feel them with your sense of
touch but this device can potentially
detect such small tremors.
One of the handy things about the
MPU-6050 is that it has configurable
digital low-pass and high-pass filters.
The low-pass filter can be configured with a -3dB point of 5Hz, 10Hz,
21Hz, 44Hz, 94Hz, 184Hz or 260Hz.
We have chosen 5Hz as this suits our
application.
Similarly, you can configure it for a
high-pass filter of 5Hz, 2.5Hz, 1.25Hz
or 0.625Hz.
We have used the last option, giving
a response of 0.625-5Hz. We provide
an additional 1Hz high-pass filter in
the software (which also helps to remove any residual gravity from the
readings, eg, if the unit is not mounted
perfectly horizontally).
The Arduino makes a couple of
dozen readings of the X, Y and Z axis
acceleration figures each second and
after processing them, it uses an RMS
Our detector
The electronic device we describe
here uses a relatively inexpensive but
very sensitive accelerometer combined with a regular Arduino board.
Depending on where you live, it
may give you enough warning to find
a safe place if it detects an oncoming
earthquake or aftershock. And it may
be useful if you live near an active volcano; volcanoes can generate P-waves
prior to eruption.
No promises, of course: but it’s
much better to have a detector which
could give you warning than have no
detector and have no chance!
Besides, it’s cheap, easy to build and
requires very little soldering. You can
put it together in about an hour or so,
even if you aren’t very experienced.
We considered designing the device
around analog circuitry but P-waves
can come from any direction and thus
some fairly intense signal processing
is required.
This is much easier to do with software and it doesn’t require a customdesigned PCB.
Circuit details
Our circuit is shown in Fig.5. The
two main components are the Arduino Uno (or equivalent) board, MOD1,
and the Altronics Z6324 digital accelsiliconchip.com.au
Fig.5: full circuit of the Earthquake Early Warning Alarm, including the
components for the optional battery-backed supply, at bottom. The Arduino
(MOD1) constantly reads the three acceleration values from MOD2, performs
digital filtering and amplification, then decides whether to light up LED1 and
sound the loud piezo siren.
Celebrating 30 Years
March 2018 17
The two sides of the Arduino Uno board, shown here close to life size (in this case the duinotech UNO from Jaycar – there
are several compatible boards). The protoboard (opposite) simply plugs into the sockets on the edges of the board.
formula to compute the magnitude
of the resulting X/Y low-frequency
vector.
This is multiplied by a sensitivity
factor, set using trimpot VR1, and if
it exceeds an arbitrary threshold for
more than about 200ms, the alarm is
triggered.
To sound the alarm, output pin D12
is pulsed high and low at about 1Hz.
When high, bright blue LED1 lights up
and NPN transistor Q1 is switched on.
This triggers the very loud piezo siren.
Its volume and pitch are similar to a
smoke alarm.
If an S-wave or surface wave is detected (by a similarly large excursion
in the magnitude of the Z-axis measurement), LED1 and the piezo siren
also light but they are on continuously,
rather than pulsed.
This should alert you to the fact
that you are currently experiencing
an earthquake, in case the other signs
(shaking, falling objects etc) are not
obvious enough!
The unit can be mains-powered, via
a USB port on a PC, from DC plugpack
or the optional battery-backed supply (shown as MOD3 at the bottom of
Fig.5) can be used.
This consists simply of a single Liion/LiPo cell combined with a small
charger/power supply board. The battery is kept charged by the USB power
supply when mains is present.
The battery can power the rest of
the circuit for a few hours if there is
a blackout.
While we haven't shown a solar panel connected there is provision for one
– this could make the whole project
fully self contained with solar-backed
18
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power if you wished to remotely use it.
Virtually any 6V-12V solar panel could
be pressed into service – the circuit
only draws significant power from the
battery when the alarm is going off . . .
at which time a flattening battery is
likely to be the least of your concerns!
To make construction easy, we wired
trimpot VR1 directly to pins A0, A1
and A2. A1 is used as an input while
A0 and A2 are programmed as digital outputs.
So we simply pull A2 high (to +5V)
and A0 low (to 0V) just before measuring A1.
Therefore we read the position of the
trimpot as a digital value and use that
to determine the sensitivity.
This is computed exponentially so
that the full range of rotation of VR1
gives about a 100:1 ratio between the
level of vibrations needed to trigger
the alarm at its two extremes.
We’ve set up the sensitivity so that
at maximum, the unit will trigger on
the tiniest tremor, while at the minimum setting, you’d probably have to
hit it with a hammer to set it off.
Also note that to save power and
simplify the circuit, we wired the
warning LED in series with the base
current limiting resistor for Q1.
The LED current is around 11mA
[(5V-3.3V-0.7V)÷91Ω]. If you use a different colour LED, it will be driven at a
slightly higher current, due to its lower forward voltage but it shouldn’t be
necessary to change the resistor value.
(If you don’t have a 91Ω resistor, 100Ω
should be fine).
Construction
While you could build the device
Celebrating 30 Years
by wiring up the various components
with flying leads, we used a protoboard
to give a neater result, as you can see
from the photos.
No component overlay is shown
for the protoboard as there are so few
components involved – all of the interconnection details are clearly shown
in the photograph.
By soldering connected components
close together, we only needed to run
five wires, all of which you can see
on the top of the board (two 0Ω resistors and three lengths of hookup wire;
blue, green and red).
Wire links can be used in place of
the 0Ω resistors if you prefer. (Wire
links are also a tad cheaper!)
Start by soldering an 8-pin header to
the MPU-6050 accelerometer module,
then solder it to the prototyping shield.
You will need to make four connections between this module and the
shield headers: VCC to +5V, GND to
GND, SDA to SDA and SCL to SCL.
Having done that, solder the 91Ω resistor from pin D12 to a pad near the
edge of the board, then connect it to the
LED anode. Connect the LED cathode
to the base (middle pin) of Q1.
The collector of Q1 is the right-most
pin when looking at its labelled face
and this is connected to 5V. The remaining pin of Q1 goes to the negative
pin of the piezo siren via CON1, with
the positive pin wired to VIN.
We connected the piezo siren via a
2-pin polarised header. This is handy
for testing since the siren is very loud,
If it's too loud while you're setting
up, it can be temporarily muted by having something placed over its opening
(a piece of sticky tape or insulation
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Parts list –
Earthquake Early
Warning Alarm
The two PCBs simply plug into each other via the header pins on the top board
and the matching sockets on the Arduino board, as shown here.
tape, for example) or placing it upsidedown on your bench top.
If you don’t want to solder the wires
to a plug and the header to the PCB,
you can directly solder the piezo wires
to the board.
Finally, solder trimpot VR1 to pins
A0, A1 and A2, as shown in the photo.
That’s it – those are all the connections
you need. Solder the headers to the
shield board, then put it aside while
you program the unit.
Programming it
Download the Arduino sketch,
named EarthquakeEarlyWarning.ino,
from the SILICON CHIP website.
You will also need to have the Arduino IDE installed on your computer.
The latest version can be downloaded
for Windows, macOS and Linux from
www.arduino.cc/en/Main/Software
Once it’s installed, load it up and
open the sketch.
There is one additional library that
needs to be installed. It’s called “Filters” and a zip file is included in the
download package. Use the Sketch ->
Include Library -> Add .ZIP Library
menu option to install this file on
your system.
Now plug the Arduino into your
computer using a USB cable (without
the shield, for now) and then go to the
Tools menu and make sure the correct
Port has been selected.
You can then use the Sketch -> Upload command to upload the code to
the Arduino module.
Check the output at the bottom of the
screen to make sure it has been compiled and uploaded without errors.
You can now unplug the Arduino
module from your PC and plug the
completed shield into it.
Then plug it back into your PC and
open the Serial Monitor in the Arduino IDE. It’s available under the Tools
menu. Pretty soon, you should see an
output like this:
1 Arduino Uno or compatible board
(MOD1)
1 MPU-6050 based accelerometer/
gyroscope module with 8-pin header
(MOD2; Altronics Z6324)
1 1-13V loud piezo siren (Altronics
S6115)
1 Arduino prototyping shield PCB and
header set
1 high-brightness 5mm LED (LED1)
1 BC337 NPN transistor (Q1)
1 100kΩ mini horizontal trimpot (VR1)
1 91Ω 0.25W resistor
1 2-pin polarised header and matching
plug (CON1)
a few short lengths of light-duty
hookup wire
1 small plastic box (eg, UB5 Jiffy box)
1 USB charger or other USB power
source
Optional parts for battery backup
1 solar charger module (eg, SILICON
CHIP Online Shop Cat SC4308)
1 small single-cell Li-ion/LiPO cell
1 short USB cable to suit solar charger
module
1 6-12V mini solar panel, if required
|XY| = 0.05, |Z| = 0.11
|XY| = 0.37, |Z| = 0.05
|XY| = 0.17, |Z| = 0.04
|XY| = 0.22, |Z| = 0.29
|XY| = 0.20, |Z| = 0.08
|XY| = 0.27, |Z| = 0.20
|XY| = 0.16, |Z| = 0.21
|XY| = 0.02, |Z| = 0.25
|XY| = 0.42, |Z| = 0.04
Here’s the protoboard with
the LED, transistor, resistor
and trimpot plus the MPU6050 accelerometer board all
mounted, as per the circuit
overleaf. This assembly plugs
into the Arduino Uno. The
two light blue “resistors”
(bottom of PCB) are actually
0Ω links.
The piezo “siren” is rather
loud, as you would want it
to be if it is to warn you of
impending doom!
Not shown here is the
optional battery and
recharger – see full details of
this in the article in SILICON
CHIP, August 2017.
siliconchip.com.au
Celebrating 30 Years
March 2018 19
These are the readings from the accelerometer. |XY| is the dimensionless magnitude of the horizontal AC
vector while |Z| is the magnitude
of the AC component of the vertical
vector.
If you shake the unit, you should
see these values temporarily increase,
then settle back towards zero. Rotating
VR1 clockwise should cause them to
increase and with VR1 fully clockwise,
even the slightest nudge should cause
LED1 to light up and flash.
Assuming it’s working, turn VR1
clockwise as far as you can go while
ensuring that LED1 remains off when
the unit is sitting untouched on a
steady surface.
Note that the alarm condition persists for several seconds after any
shock so you will need to make small
adjustments and leave the unit alone
for a few seconds to see whether the
sensitivity is correct.
A cheap 6V-12V solar panel, as shown here, a surplus mobile phone battery
(both commonly available on ebay) plus one of the small
"Elecrow" Li-Ion battery charger modules
(available from the SILICON CHIP Online
Shop, Cat 4308) will make a fine power
supply for your Arduino-based
Earthquake Early Warning Alarm, with
the added advantage of making it
completely self-contained: no external
power supply is required!
You can then plug the siren in and
check that it sounds when you bump
the unit.
Setting it up
Mount the unit inside a box so that
it’s held firmly in place within that
box. The ‘‘noise hole‘‘ of the piezo siren (ie, where the sound comes out!)
should line up with a similar hole in
the box.
The orientation of the electronics
don’t matter, as long as when the device is mounted on a wall (the preferred location), the accelerometer
PCB is horizontal.
The device should be firmly fixed
to a solid wall and if set correctly, it
will sound the alarm when it experiences significant horizontal movement in any direction. Since the wall
should be solidly fixed to the ground,
that normally will only occur if the
ground moves.
We can’t rule out the occasional
false alarm due to heavy vehicles,
trains, nearby hammer blows or similar but you can turn VR1 anti-clockwise slightly if you are experiencing
false alarms, reducing its sensitivity
SC
until they stop.
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Celebrating
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Years
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Latest generation
. . . and what’s to come
Nuclear power stations generate about 11% of the world’s base load
electricity but many older nuclear plants are near the end of their service
life. What are their likely replacements? This article examines present
day reactors and the new Gen IV designs.
F
irst, let’s look at the most common current design,
the pressurised water reactor (PWR) and then we will
describe the six Gen IV designs, all selected by the international Gen IV Forum (GIF) committee:
•
•
•
•
•
•
Sodium Fast Reactor (SFR),
Lead Fast Reactor (LFR),
Gas Fast Reactor (GFR),
Supercritical Water Reactor (SCWR),
Very High Temperature Reactor (VHTR) and
Molten Salt Reactor (MSR).
The pressurised water reactor accounts for 65% of the
world’s ~450 nuclear power plants (NPPs). This wasn’t always the case and in the 1950s many countries developed
their own designs.
Thus, the Canadians developed the CANDU heavy water moderated reactor that used natural uranium (99.27%
U-238, 0.73% U-235). The UK developed the gas-cooled reactors (eg, Magnox and AGRs) which also used natural ura22
Silicon Chip
nium and are very safe on account of their low power density (with lots of graphite in the core and not a lot of fuel).
For their part, the Americans developed a compact pressurised water reactor (PWR) that used highly enriched uranium (>20%) to power their naval vessels. From there, they
developed land-based PWRs up to 1350MWe (megawatts of
electrical power) using low enriched uranium (5%). These
have been found to be very economical to operate.
Subsequently, PWRs have been widely deployed in Russia, China, Japan, UK, France and other European Countries,
displacing these countries’ own designs.
PWRs are very safe on account of their negative thermal
reactivity feedback – meaning that the hotter the core gets,
the less nuclear reaction takes place in the core. The materials and heat transfer characteristics of PWRs are well known.
Water under pressure is well understood, as are the properties of steel which makes up the reactor pressure vessel
(RPV) and the zirconium alloy ‘fuel pins’ (ie, hollow tubes)
that contain the sintered uranium-dioxide fuel pellets.
Celebrating 30 Years
siliconchip.com.au
nuclear reactors
By Dr Mark Ho* & Dr David Maddison
The Russian BN-800 Sodium-cooled Fast Reactor now in
commercial operation. It is a direct forerunner and technology
demonstrator for other Generation IV reactor designs such
as the BN-1200. It produces 880MW of electrical power. It is
one of only two Sodium-cooled Fast Reactors commercially
operating in the world out of a total of 447 power reactors.
So nuclear regulators have confidence in these designs and
PWRs have become the mainstay of the global nuclear fleet.
After some 50 + years of operations, these Generation II
PWRs are nearing the end of their service life and are being
slowly replaced by Gen III PWRs and BWRs (Boiling Water
Reactors which generate steam directly in the reactor core).
Gen III reactors have active and passive safety systems
which ensure heat can be removed from the reactor core
after shutdown.
Why is this necessary?
In a nuclear reaction, a typical uranium-235 nucleus with
92 protons and 143 neutrons can split after absorbing a neutron, producing two elements of lower mass numbers (fission products), 2-3 neutrons and some energy in the form
of gamma radiation.
The fission products continue to radioactively decay after
shutdown, generating roughly 1.2% of the reactor heat at
full power one hour after the control rods are dropped. So
siliconchip.com.au
for a 3000MW-thermal / 1000MW-electric reactor, the core
continues to generate 36MWth (megawatts of thermal output) one hour after shutdown.
This ‘decay heat’ is removed either by pumps to drive water through the core or as in the case of some Gen III reactors, by natural circulation which does not require pumps
or off-site power. New PWRs and BWRs are often built with
large water reservoirs that act as a “thermal-sink” for decay
heat removal.
By eliminating the need for off-site power, Fukushimatype accidents would be eliminated.
Apart from needing improved safety features, there are
other other features which one might have for a nuclear reactor. These include:
(1) to breed nuclear fuel without creating nuclear weapons
materials (ie, non-proliferation)
(2) to burn radioactive waste
(3) to burn nuclear fuel more completely
(4) to supply high temperature heat for industrial processes
Celebrating 30 Years
March 2018 23
Timeline showing development of various generations of reactors. Generation IV reactors are intended to be deployable
no later than 2030. Image credit: US Nuclear Engineering Division
(5) to operate more economically.
Not surprisingly, these attributes are the expressed goals
of the Gen IV forum (GIF) which is a group of 14 nations
(now including Australia) working together on the next generation of power reactors.
So let us discuss these desired points.
Fuel breeding and non-proliferation
Currently, PWRs cannot breed enough fuel to be self-sustaining. In fact, readers might be surprised to know PWRs and
BWRs do create fuel by exposing the ‘fertile’ uranium-238
content (95% of the uranium-dioxide) to neutron bombard-
CONTROL RODS
PRESSURISER
STEAM
STEAM
GENERATOR
STEEL
PRESSURE
VESSEL
ment. This results in neutron absorption and transmutation
into the fuel plutonium-239.
What is more interesting is that about half of the power
that comes from a usual 18 month burn-cycle (the duration
a fuel bundle is in the core) actually comes from burning
plutonium created in the core when exposed to neutrons!
Thus the bred plutonium is beneficial as it’s essentially
‘free power’.
Some people may ask whether “bomb-grade material” is
being made in the reactor. The short answer is no, because
plutonium 240 is also made along with Pu-239 in the core
and the mixture of both makes it unusable as a bomb material.
There is also no easy way to separate Pu-240 from Pu-239
without a dedicated isotopic-separation facility which is difficult to engineer, requires large amounts of power to operate and thus is difficult to hide from satellite surveillance.
Despite progress made to maximise fuel breeding in PWRs,
the maximum PWR conversion ratio (ie, total fuel produced/
total fuel burnt) is about 0.6 or 60%.
A self-sustaining fuel cycle would require a conversion
ratio above 1.0. To do so would also require a very different type of reactor, one that operates in the ‘hard neutron
spectrum’.
WATER
FUEL ELEMENTS
REINFORCED CONCRETE
CONTAINMENT AND SHIELD
Pressurised Water Reactor
Fuel:............................................ uranium dioxide (4 - 5% enriched)
Fuel Cladding: ...................... Zircaloy (98% zirconium, 2% tin)
Moderator:..................................................................................... light water
Loops :............................................................ 2 – primary & secondary
Coolant:.............................................................light water – light water
Core temperature:.................................................................. 300 – 330°
Operating pressure:..................................................................... 150 atm
Rankine (steam) cycle:............................................... 33% efficiency
24
Silicon Chip
Nuclear fuel inside a reactor.
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ELECTRICAL
POWER
GENERATOR
CONTROL
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ELECTRICAL
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HELIUM
HEADER
TURBINE
TURBINE
U-TUBE HEAT
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MODULES (4)
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COMPRESSOR
REACTOR MODULE/
FUEL CARTRIDGE
(REMOVABLE)
COOLANT
MODULE
COOLANT
HEATSINK
INTER
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PRE
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INTERCOOLER
COMPRESSOR
HEATSINK
INLET
DISTRIBUTOR
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The Gas-cooled Fast
Reactor. Source: Idaho
National Laboratory.
HEATSINK
HEATSINK
REACTOR
CORE
REACTOR
PRE
COOLER
REACTOR
COMPRESSOR
Lead-cooled Fast reactor. Note the natural convective
pathway for cooling. Source: Idaho National Laboratory.
PWRs operate in the thermal neutron spectrum, when
neutrons are slowed to the speed of gas molecules at room
temperature, about 0.25eV (electron volts). Fast neutron reactors operate in the hard neutron spectrum with neutrons
zipping around at 5% the speed of light at ~1MeV.
An example of a much-studied fast reactor is the SFR, the
Sodium Fast Reactor.
The conversion ratio for the SFR is theoretically limited
to 1.3. Since the conversion value is > 1.0, it’s called the
“breeding ratio”.
The probability of neutron capture for all nuclear fuels are
two to three orders of magnitude less in the fast spectrum
than in the thermal spectrum. Thus a fast neutron reactor
requires a lot more fissile material than a ‘thermal reactor’
like the PWR. Hence, one can see why thermal-neutron reactors have been in wide usage, as they require less fissile
material per reactor to achieve criticality.
For a reactor to be stable, the amount of neutrons produced is balanced by an equal amount of neutrons lost. It
is known as achieving criticality in the core when the core
reactivity is equal to 1. Less than 1 is sub-critical and more
than 1 is super-critical
Burning radioactive waste
Radioactive waste created in PWRs and BWRs can be
loosely separated into two categories: long-lived and shortlived waste. Short-lived waste comprises fission products
with a half-life of about 30 years.
Long-lived waste comprises high mass-number elements
created from uranium-238 capturing several neutrons and
transmutating into elements such as neptunium, plutonium,
americium and curium. These trace elements are known
as ‘minor actinides’ as they are actinides created in small
quantities.
What is important to note is that short-lived wastes pretty much fully decay after about 300 years or about 10 successive half-lives, whereas long-lived wastes could last for
RADIOACTIVITY
(GBq)
GBq = 109 becquerel
107
TOTAL
FISSION PRODUCTS
106
ACTINADES
105
104
ORIGINAL ORE
103
102
10
Russian hexagonal PWR fuel bundle.
siliconchip.com.au
102
103
104
105
106
107
YEARS AFTER SEPARATION
Decay in radioactivity of high-level waste from
reprocessing one tonne of spent PWR fuel. The straight line
shows the radioactivity of the corresponding amount of
uranium ore. Source: OECD NEA 1996, Radioactive Waste
Management in Perspective.
Celebrating 30 Years
March 2018 25
Neutron Cross Sections of various nuclear fuels over a range of energies.
100,000+ years.
But it is the short-lived waste that is the most radioactive
as it’s decaying at a much faster rate than the long-lived
waste. In reality, radioactive waste is not an insurmountable issue as it is possible to engineer containing structures that are very good at shielding radiation and resistant to corrosion.
When spent fuel is reprocessed and the useful uranium
and plutonium content is extracted, the remaining fission
products are usually immobilised as glass (vitrified) and
this is known as high-level waste which is radioactive for
10,000 years.
For unprocessed fuel assemblies held in hardened,
shielded casks, the time it takes for the waste to reach a
level of radioactivity no more than in uranium ore is about
120,000 years.
Still, there are some who wish for minor actinides to
be destroyed and this can be achieved by “burning” them
in a fast neutron reactor. In fact, the Russian BN-600 SFR
has been burning excess weapons-grade plutonium since
2012 as per their arms-reduction agreement with the USA.
Similarly reprocessed actinide waste can be burnt in the
form of mixed-oxide (MOX) fuel.
Better burn-up of nuclear fuels
As stated earlier, PWRs and BWRs use uranium dioxide pellet fuels enclosed in thin-walled zircalloy cladding.
These long fuel pins are injected with helium gas and sealed
to improve heat conduction. Uranium dioxide is a ceramic
with a very high melting point (2865˚C!) but is relatively
low in thermal conductivity at 2.0 – 2.5W/(m.K) between
900 and 2200˚C.
In comparison, stainless steel has a conductivity of 1518W/(m.K) and Zircalloy 21.5W/(m.K). More important to
note is the thermal conductivity in uranium dioxide degrades as fission gasses build up, causing cracks to occur.
Naturally, we want thermal conductivity in the fuel to
be as high as possible for effective heat transfer, so fuel
must be removed from the reactor before the structure of
the pellets starts to degrade substantially. Another factor to consider is fission product (FP) build-up which
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accumulates as the fuel is burnt.
Fission products parasitically absorb neutrons, affecting
the core’s neutron economy and thus they restrict the fuel’s residence time in the core. For these reasons, fuel bundles usually stay in the core for no longer than two years.
The maximum burn-up of reactor fuel is measured as the
power created divided by the tons of heavy metal ‘burnt’.
For uranium dioxide at 5% enrichment, the burn-up
tops out at around 60GW-days/ton of heavy metal (where
‘heavy metal’ (HM) is a mix of uranium, plutonium and
minor actinides). Fast neutron reactors which do not suffer as much for the effect of fission-product build up have
been shown to achieve a burn up of up to 200GWd/tHM.
Readers might be surprised to know that PWR-spent fuel
Safety of nuclear power
Despite the claims made often in the popular press, nuclear
power is by far the safest form of energy production, from mining right through to waste disposal.
In three significant nuclear incidents, Three Mile Island, Chernobyl and Fukishima, no one died in the first one, 38 died (four in
a helicopter accident) in the second one and nobody died in the
last one despite 20,000 people dying in the associated tsunami.
The Chernobyl reactor was a simple and cheap design whose
purpose, apart from producing electricity, was to generate as a
by-product plutonium for nuclear weapons with no regard to safety. Even so, the area around Chernobyl is now a wildlife paradise
with many once-endangered species now thriving.
COAL
OIL
BIOFUEL
GAS
HYDRO
SOLAR
WIND
NUCLEAR
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36
12
4
1.4
0.4
0.15
0.04
Deaths per terrawatt-hour of electricity produced
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CONTROL ROD
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CLOSURE HEAD
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NOZZLE (1 OF 8)
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SODIUM
(HOT)
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VESSEL
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HEAD
SSTAR reactor concept. It is a compact design that has
an electrical output of 20MW and when fuel needs to
be changed it is removed as a “cassette” by the reactor
supplier and replaced with a fresh one. This design is
scalable up to an electrical output of 180MW however
development seems to have ceased at the moment. A
100MW version would be around 15 metres high and 3
metres in diameter and weigh 500 tonnes.
The GE Hitachi PRISM (Power Reactor Innovative Small
Module) reactor is another type of Sodium-cooled Fast
Reactor under development. It is a breeder reactor and
closes the fuel cycle. It will be produced as 311MW units
that are factory assembled. The UK has analysed some
scenarios to burn the country’s reprocessed spent-fuel
using this reactor which could supply the UK’s current
electrical demand for the next 500 years.
still contains 95% U-238 which can be reprocessed and
reused as Mixed Oxide (MOX) fuel in a PWR or any of the
other Gen IV reactors.
The limitation for PWRs and BWRs is of water which
must remain pressurised to prevent boiling, dry-out and
core meltdown. With the exception of the Supercritical Water Reactor, all Gen IV designs circumvent this problem by
using more exotic coolants that remain liquid at very high
temperatures and without pressurisation.
Some of these liquids include sodium (boiling point
892˚C), molten salt (bp ~1400˚C) and lead (bp 1737˚C)
which are used in three of the six Gen IV designs. And
Very High Temperature Reactors use helium gas instead
of a liquid coolant.
High temperature reactors to supply heat for
industrial processes
Today’s PWRs and BWRs operate at about 300˚C which is
sufficient to drive a steam turbine at a thermal efficiency of
33% but they are unable to supply the very high temperature heat required for direct-thermal minerals refinement,
hydrogen production or synthetic fuel manufacturing.
6.27mm
Pressurised Water
Reactor and 17 x 17 Fuel Bundle.
4.177mm
4.75mm
SPACER
GRIDS
FUEL UO2
GAP: He
NUCLEAR
FUEL
PELLET
CLAD: Zr
MODERATOR: H20
CLADDING
4.095mm
FUEL ROD
PRESSURISER
GUIDE TUBE
STEAM GENERATOR
CONDENSOR
INSTRUMENT TUBE
GENERATOR
RPV
REACTOR
CORE
COOLANT
PUMP
PREHEATER
CONDENSOR
PUMP
PRIMARY SYSTEM
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POWER
TRANSFORMER
PUMP
SECONDARY SYSTEM
COOLING WATER –
RIVER OR SEA WATER
COOLING TOWER
March 2018 27
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COOLANT SALT
ELECTRICAL
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PURIFIED
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TURBINE
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SALT
CHEMICAL
PROCESSING PLANT
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RECUPERATOR
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PLUG
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EMERGENCY
DUMP TANKS
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HEAT
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HEAT
SINK
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COOLER
The US company
EXCHANGER
TerraPower is developing
a molten salt reactor using chloride salts rather than the
more conventional flouride salts, the Molten Chloride
Fast Reactor. It is doing this research alongside its other
development project, the Travelling Wave Reactor.
TerraPower’s Molten Chloride Fast Reactor.
Economic construction and operation
Reactor safety
The Levelised Cost of Electricity (LCOE) is often used
to assess the overall cost of a generation system averaged
over its lifetime. This takes into account the Capital Cost
(build cost), Operating Cost (eg, fuel and maintenance),
Grid Connection Cost (eg, grid build-out, stand-by supply)
and Financing Cost.
Established nuclear power plants have very low operating costs (as low as 3 US cents/kWh) because the build and
financing which currently accounts for 80% of the lifetime
costs have usually been paid off.
On the other hand, the LCOE of new nuclear reactors is
highly sensitive to the cost of financing (ie, the discount
rate usually set at 7%) because nuclear is capital-intensive
and much of the investment happens initially during the
5-7 years build phase. Experience in building nuclear reactors also contributes greatly to cost reductions. South Korea
has built PWRs continually over the last 30 years and has a
LCOE nearly half that of the UK and the United States who
are only just restarting their new-build programs.
To counter rising costs, some reactor designers, such as
NuScale, are simplifying and miniaturising PWRs in the
form of small modular reactors (SMR) that generate 50MWe
instead of 1000MWe. (See SILICON CHIP, June 2016: “Small
Nuclear Reactors” [siliconchip.com.au/Article/9957]).
The intention is to install then in banks of 12 inside a
common pool to provide passive heat removal after shutdown. With a bank of 12 50MWe modules, the plant could
produce 600MWe, well suited to replace coal plants, for
small grid systems or for remote deployment.
The aims are to reduce the build time to three years, improve costs and quality control by building each reactor
in a controlled factory environment (instead of an external
environment) and to accumulate experience more quickly
by building many reactors on an assembly-line, similar to
aircraft manufacturing.
To ensure Gen IV designs remain cost-competitive, it will
be important to combine the lessons of continual build, design simplification and modular construction with clever
design work that incorporates new materials, fuels and
exotic coolants.
Reactor safety involves four main concerns:
(1) ensuring the reactor has a negative thermal reactivity characteristic so that an increase in core temperature
decreases fission activity;
(2) maintaining structural integrity in the fuel, cladding
and primary loop containing the coolant that circulates
through the core;
(3) avoiding total coolant phase-change (and thus loss
of flow) in the core in the event of a reactor power excursion or reactivity spike and
(4) the ability to remove decay heat after shut-down.
PWRs have by-and-large demonstrated these characteristics. Only when there is insufficient decay heat removal
does the question of boiling, structural integrity and fission product release come into play.
To improve the intrinsic safety of future reactors, three
Gen IV designs: the Sodium Fast Reactor, Lead Fast Reactor and Molten Salt Reactor (SFR, LFR, MSR) use unpressurised, high boiling-point liquid coolants that can ensure
uninterrupted passive decay heat removal.
Liquid metal coolants such as sodium and lead are also
very good conductors of heat, so the task of decay heat removal is easily achieved. The Very High Temperature Reactor and Gas Fast Reactor (VHTR, GFR) circumvent the
coolant phase change problem entirely by using helium
gas as the coolant.
For high temperature reactors such as SFRs, LFRs, VHTRs
and MSRs, passive decay heat removal using air instead of
water is achievable because of the large temperature difference between the core and the ambient air temperature.
Now let us take a look at the Gen IV designs, focusing on
the sodium fast reactor and molten salt reactor.
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Sodium Fast Reactors
The end of the Second World War ushered in the Atomic Age which promised a seemingly inexhaustible energy supply. But there was concern amongst scientists that
the world’s uranium resources were limited and could be
quickly exhausted. Thus, work started on “breeder reactors” which could create more fuel than was burnt.
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In the course of testing the neutron cross-section of different materials, it was found that sodium was one of the
most neutron-transparent, being six times less neutron
absorbing than lead. This made sodium an excellent candidate as a reactor coolant to maximise the reactor core’s
neutron flux.
More neutrons in the core meant the possibility of using
excess neutrons to transmute fertile uranium-238 into plutonium-239 fuel or burning neutron-parasitic actinide-waste.
Another feature of sodium is that it is only lightly moderating which means a sodium-cooled reactor could operate in
a fast spectrum and directly burn uranium-238, something
that thermal-neutron spectrum reactors cannot do.
By calculations, a sodium fast reactor could theoretically
attain a breeding ratio of 1.3, meaning that 30% more fuel
could be produced than is used. In comparison, a lead fast
reactor has a theoretical breeding ratio of 1.0 (making it
an “iso-breeder”) and a PWR has a conversion ratio of 0.6
(making it a “converter” as noted earlier).
By utilising SFRs, it has been calculated that uranium
resources can extend the life of economically recoverable
reserves by at least 60 times. Before the Gen IV forum started, there was already much co-operation between the US,
Russia, France and the UK on SFRs.
Sharing SFR research in the interest of reactor safety
was deemed more important than the possibility of future
commercial conflicts of interest. So information on materials neutron cross-section measurements, zero-power
critical assembly studies, SRF core layouts optimisation
studies and safety analysis research were shared. As a result, the SFR core layouts of most countries ended up being quite similar.
SFR fuel
SFRs are similar to PWRs in their use of uranium dioxide and plutonium dioxide fuels. In the future uranium nitride, which can carry a higher uranium loading per unit
volume and metallic fuels, which have better heat conductivity, could become a possibility.
Plutonium has a larger neutron cross section than uranium for neutrons above 1MeV. Thus, a Fast Neutron Reactors is actually optimised to burn plutonium.
Also, the number of neutrons produced per plutonium-239 fission is 25% more than from uranium-235 and
neutrons produced from Pu-239 are more energetic, thus
are better at maintaining the fission process. As mentioned
earlier, U-238 under neutron bombardment transmutes
into Pu-239 and Pu-241 that can be burnt as fuel and some
U-238 can be directly burnt by 1MeV neutrons.
Specific advantages of Generation IV reactors
• Greater fuel efficiency than current Generation III+ reactors
with 100 to 300 times more energy output for a given amount
of fuel. There will be less useful fuel left over in waste.
• In some reactor designs, existing nuclear waste can be consumed, extending the effective nuclear fuel supply by orders of magnitude. For example, it has been estimated that
if the existing nuclear waste of the United States was dug
up and used in new reactor designs it could keep the entire
US supplied with nuclear electricity for 70 years. This concept also closes the nuclear fuel cycle, meaning the waste
is reprocessed as opposed to the “once through” or “open
fuel cycle” in which waste is buried rather than reprocessed.
• Waste products that are hazardous for only centuries instead
of thousands of years. From current engineering experience we know that structures such as buildings can easily
last hundreds of years, even those built with centuries old
technology so underground containment structures should
pose no problem.
• Many different types of nuclear fuels can be used with different encapsulation methods such as in ceramics or no
encapsulation.
• Reactor designs are designed to be intrinsically safe with no
external emergency shut down systems or power required
in the event of an emergency and (depending on design)
low pressure reactor operation. A Fukushima type event
where external power failed would not lead to reactor failure.
a high neutron flux, SFR cores are typically smaller than
PWRs (eg, The Dourneay FR 65MWth was the size of a rubbish bin) but because of the smaller neutron cross sections
of 1MeV neutrons, the fissile loading of SFRs are typically
three times that of PWRs.
A higher core power density necessitates a superior form
of coolant which is why liquid metal is used. Passive reactor control is maintained by a strong negative temperature
coefficient which for fast reactors is dependent on the Doppler Broadening phenomenon. When nuclear fuel is heated, the resonance energies for capturing neutrons broaden,
resulting in neutron absorption instead of fission. (ie, the
fuel becomes self-shielding from neutrons).
Since sodium is very reactive to water, most SFRs use
an ‘integral design’ to prevent coolant leakage. In an in-
SFR design
A typical SFR fuel bundle is shown opposite. The fuel
pins which contain uranium dioxide pellets are packed
into a tight hexagonal arrangement to maximise the core’s
neutron flux. Stainless steel instead of Zircalloy is used for
the fuel rods as stainless steel is transparent to fast neutrons, not-corroded by sodium and relatively inexpensive
to fabricate.
The fuel rod wires that curl around the fuel pin promote
flow, mixing and prevent flow dead-spots from forming. Finally the hexagonal fuel bundle is surrounded by a hexagonal shroud to prevent the possibility of large cross flows
which would result in fuel bundle vibrations. To maintain
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Typical Hexagonal SFR fuel bundle cross section.
Celebrating 30 Years
March 2018 29
Integral Molten Salt Reactor (IMSR).
tegral configuration, the core sits in a large pool of liquid
sodium with a cover gas – typically argon.
Having the total primary sodium coolant held inside
the thick walled reactor vessel minimises the risk of sodium leakage. For the BN-800 reactor heat removal is accomplished by three independent coolant loops supplying
power to a common turbine.
Each loop is comprised of a primary, secondary and tertiary circuit which transfers power to the turbines but also
isolates the very radioactive primary sodium coolant from
the water-based tertiary coolant. The SFR core operates at
a higher temperature than PWRs with an exit temperature
of 547˚C which allows it to drive a superheated steam cycle at ~40% efficiency.
Future of SFRs
In total, 20 SFRs have operated since the 1950s, accumulating a total of 400+ SFR reactor years of experience.
The list of past SFR prototypes includes:
(1) Experimental Breeder Reactors 1 & 2 (USA)
(2) BOR / BN series (Russia)
(3) Phénix and Superphénix (France)
(4) Dounreay FR and PFR (UK)
(5) Monju (Japan) and
(6) CEFR (China).
After a flurry of initial research, most SFR prototypes
BN-800 fuel flow diagram. Three consecutive coolant
circuits prevent radioactivity from penetrating into the
steam generators.
30
Silicon Chip
have permanently shut down after uranium reserves were
found to be much more plentiful than initially thought
and PWRs & BWRs were optimised to run economically.
The exception is in Russia who has operated the BN-600
(600MWe) SFR since the 1980s and have recently commissioned their BN-800 reactor.
There are plans to build an even larger BN-1200 reactor
which will further simplify the core design and test new
fuels and materials in the quest to close the nuclear fuel
cycle (ie, fully consume all radioactive waste generated).
In terms of cost, SFRs are currently more expensive to
run than PWRs. It was reported that BN-800 capital costs
were 20% more than a Russian VVER-1200 (Russian PWR)
and BN-800 operational costs were 15% more than a VVER.
Still, work continues on SFRs in some countries such as
France who are planning to build the next generation SFR
called “Astrid” and have studied scenarios to replace half
of the current PWR fleet with SFRs.
The UK Department of Energy and Climate Change had
also studied scenarios of eventually phasing out PWRs
with SFRs but has opted to focus on PWRs and BWRs in
its new-build program. China, which is currently building
most of the world’s PWRs, plans to build its own BN-800
reactor with Russian assistance.
In the West, multiple SFR designs are on the drawing
board such as the GE Hitachi PRISM reactor and the TerraPower Travelling Wave reactor (TWR). TerraPower recently
entered into partnership with China National Nuclear Corporation (CNNC) to further develop the Travelling Wave
reactor. The intended purpose of the TWR is to burn spent
fuel generated in PWRs using less nuclear fuel and producing less nuclear waste than today’s PWRs.
Molten Salt Reactors
Molten salt reactors use fluoride or chloride salts as coolant and can be designed to burn either solid fuels (SF) or
liquid fuels (LF).
The salt is not dissolved in water; the salt in molten form
is the coolant. The choice between a chloride or fluoride salt
depends on the desired neutron spectrum. Lithium-beryllium fluoride (FLiBe) works as a thermal spectrum salt on
account of the low mass numbers of lithium and beryllium.
Chloride salts paired with heavier elements are much
less moderating and good at maintaining a fast neutronspectrum. All salts have excellent heat transfer characteristics. For example FLiBe salt has the same volumetric
heat capacity as water but remains a liquid up to 1400°C
without pressurisation.
This is due to the FLiBe salts having a very low vapour
pressure (ie, rate of evaporation). Other attractive aspects
of the salt include a low neutron absorption cross section, resistance to radiation damage on account of their
ionic bonds, being non-reactive to air or water and visually transparent.
MSRs possess a substantial safety margin between the
reactor’s operational temperature and the salt’s much higher boiling point, as boiling could lead to a loss-of-flow accident in the core. Added to this, since pressurisation is
not required, the reactor pressure vessel (RPV) can be designed to have a thinner wall compared to the 20cm thickness of a PWR RPV.
Due to the MSR’s high core temperature, a Brayton-cycle
gas turbine operating at a high thermal efficiency of 45%
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Very high temperature gas reactor.
CONTROL RODS
GRAPHITE
REACTOR
CORE
PUMP
GRAPHITE
REFLECTOR
WATER
BLOWER
OXYGEN
REACTOR
HELIUM
COOLANT
HEAT
EXCHANGER
can be used.
HEATSINK
HYDROGEN
HYDROGEN
PRODUCTION PLANT
Solid Fuel MSRs
Current SF-MSR designs are salt-cooled, graphite-moderated reactors that use TRISO (Tri-structural-isotropic) fuel
that was developed during earlier research into High Temperature Gas Reactors (HTGRs). TRISO fuel is composed
of thousands of 0.5 mm diameter uranium dioxide kernels
wrapped in layers of carbon and silicon carbide that trap
solid and gaseous fission products without degrading the
fuel’s thermal conductivity.
A sphere of ten thousand TRISO particles is surrounded
by layer of graphite, making a 6cm diameter ball (known
as pebble fuel). Alternatively, TRISO fuel can be made into
large prismatic blocks of graphite with TRISO particles dispersed on the surfaces that interface with the salt coolant.
TRISO fuel is more accident-tolerant than standard PWR
fuel and has been tested to withstand temperatures up to
1800˚C without fission product release but the layers of
silicon carbide and carbon also make the fuel difficult to
reprocess and reuse so this is counter to the goal of closing the fuel cycle.
One may think of the SF-MSR design as being very similar to a HTGR. Both use TRISO pebble fuel and operate
in a thermal neutron spectrum but the helium coolant in
a HTGR is swapped out for the FLiBe salt. The operation
of SF-MSRs is similar to PWRs as both need periodic refuelling but fuel burn-up is enhanced due to TRISO fuel’s
superior thermal-performance.
One advantage of the SF-MSR is that it is more compact
than a HTGR due to the salt’s higher volumetric heat capacity. On the other hand, FLiBe coolant is more expensive to manufacture than helium. Currently, the Shanghai
Institute of Applied Physics (SINAP), Oak Ridge National
Laboratory (ORNL) and Kairos Energy based in California
are continuing research on SF-MSR designs.
Liquid Fuel Thermal MSRs
Liquid fuel, molten salt reactors use fuel (233UF4,
235UF4 or 239PuF4) that is directly dissolved into the
primary coolant itself. Having the fuel dissolved provides
some advantages for thermal-spectrum LF MSRs: 135Xenon – a highly neutron parasitic fission product – can be
removed as a gas during operation and refuelling can occur while the reactor is running.
The ability to constantly remove fission products means
a much higher rate of burn-up can be achieved (>50%) and
also means less decay heat to contend with after the reactor is shut down. The fact that both the fuel and the berylsiliconchip.com.au
lium moderator are in a liquid form results in them readily
expanding at high temperatures, giving the MSR a highly
negative reactivity thermal coefficient that prevents a runaway chain reaction.
However, having a fuel in solution also means the primary coolant salt becomes highly radioactive, complicating maintenance procedures and the chemistry of the salt
must be monitored closely to minimise corrosion. Another
advantage of the liquid fuel molten salt design is that it allows the breeding of 233U from 232Th in the thermal/epithermal neutron spectrum instead of using a fast-spectrum.
Neutron capture by thorium-232 results in beta decay
(one of the neutrons in the thorium nucleus expels an electron to become a proton) thus transmutating into rotactinium-233 which further beta decays into uranium-233. The
U-233 could then be used as an MSR fuel. The thorium
fuel cycle holds promise and studies have shown that a
breeding ratio of 1.06 to 1.14 is possible for thermal and
epithermal spectrum MSRs.
Despite the potential for breeding fuel, current efforts are
focused on simply bringing the LF-MSR to the commercial
market – one which satisfies the nuclear regulator’s stringent demands for safety. Various LF-MSR start-up companies are approaching the problem from different angles.
Terrestrial Energy’s (Canada) “Integral Molten Salt Reactor” (IMSR) uses low enriched (5%) uranium (ie, denatured uranium) dissolved in the salt coolant. The reactor
vessel is designed to be swapped out every seven years to
address possible issues with salt corrosion.
Another company, ThorCon, has a similar design, using
a FLiBe salt and graphite moderator but fitted on a ship.
Transatomic has a design using lithium-fluoride salt instead of FLiBe and zirconium hydroxide instead of graphite as the moderator with a view to burn radioactive waste.
The Shanghai Institute of Applied Physics is also pursuing a LF-MSR design and has worked with Oak Ridge
National Labs and with ANSTO on corrosion resistant
materials development. SINAP has secured $3.3 billion
USD to build a 10MWth thermal-spectrum LF-MSR prototype by 2020.
Fast spectrum, chloride-salt designs are being pursued
by the European SAMOFAR (Safety Assessment of the
Molten Salt Fast Reactor) consortium, Elysium Inc. (USA)
and Terrapower’s MCFR (Molten Chloride Fast Reactor)
which aims to burn the 700,000 tonnes of uranium held
in spent fuel from PWR and BWR operations in the USA.
VHTRs, GFRs, SCWRs & LFRs
Very High Temperature Reactors (VHTR), like their predeEQUIPMENT HATCH
CONTAINMENT
DOME
SECONDARY SODIUM
PIPES AND GUARD PIPES
LARGE AND SMALL
ROTATING PLUGS
REACTOR HEAD
INTERMEDIATE HEAT
EXCHANGERS (4)
THERMAL SHIELD
IN-VESSEL FUEL
HANDLING MACHINE
REACTOR &
GUARD VESSEL
UPPER INTERNAL
STRUCTURE
REACTOR CORE & CORE
SUPPORT SCTRUCTURE
PRIMARY SODIUM
PUMP (2)
The travelling wave reactor (TerraPower).
Celebrating 30 Years
March 2018 31
Fuel pellets for Terrapower Molten Chloride Fast Reactor
cessor the HTGRs, are graphite-moderated, helium-cooled
reactors with a once-through fuel cycle (ie, the fuel is not
reprocessed) using TRISO fuel. VHTRs have a target operational temperature of 900°C whereas HTGRs’ core outlet
temperature is about 700°C.
The higher temperature of 900°C would enable hydrogen
production or the delivery of heat for industrial processes.
Difficulties in realising a VHTR design are mainly due to the
limitations of material performance as the rate of material
corrosion increases linearly with temperature. Thus materials research is continuing to enable the VHTR concept.
The USA, Russia, South Africa, Japan and the UK have
all built experimental HTGRs. China is close to completing
two HTR-PM (High-Temperature Reactor – Pebble Module)
prototypes which will deliver superheated steam to a common turbine generating 210MWe.
Limiting the thermal output of each HTR-PM unit to
below 300MWth ensures the maximum fuel temperature
limit of 1600°C will not be compromised after reactor shutdown, thus guaranteeing the reactor’s inherent safety. It
is envisaged new HTR-PM units will replace current coal
plants which drive the same superheated steam cycle and
so quickly reduce China’s pollution problems.
Gas Fast Reactors (GFRs) can be thought of as an extension of VHTR technology but with a higher fissile loading
(on account of the fast spectrum) and without the presence
of moderating graphite. It is a challenging design as the removal of the graphite severely reduces the core’s thermal
inertia (ie, the ability of the core material to ‘suck up’ the
decay heat).
Progress on this design has been slow and depends on
the outcome of VHTR research.
The Supercritical Water Reactor (SCWR) could be thought
of as a Boiling Water Reactor with the primary loop directly
driving a steam turbine.
The water coolant is heated beyond 375°C and 22.1MPa
in a super-critical state whereby the total liquid inventory
behaves like steam and the transitional dynamics of boiling can be avoided.
This design is focused mainly on improving the efficiency
of the thermal cycle but faces the challenges of increased
thermal stress on reactor components, accelerated corrosion rates at elevated temperatures and a reduced water
inventory in the primary loop which normally serves as a
buffer for sharp changes in reactor power.
32
Silicon Chip
(For more on supercritical steam see SILICON C HIP , December
2015 – siliconchip.com.
au/Article/9634).
The last Gen IV reactor design is the Lead
Fast Reactor. Both the
US and Russia have
studied reactor concepts
using a lead coolant but
only Russia has fielded
the LFR in its naval vessel, most notably in the
Alfa-class attack-submarine (see below).
Since fast reactors
operate with a compact
core to maximise the
neutron flux, the leadbismuth cooled OK-550 Chinese HTR-PM
fast reactor with an out- (High Temperature
put of 60MWe could fit Reactor – Pebble
inside a small cross-sec- Module).
tional hull and propel
the submarine up to 41
knots (76km/h!)
These submarines
have all been decommissioned but plans for the new
BREST-300 LFR was recently granted approval for construction in Seversk, Russia and will serve as the demonstrator
unit before the larger BREST-1200 unit is built.
This concludes our brief run-down of all the six Gen
IV designs. All nuclear power reactors must extract large
amounts of power from the small volume of the core. This
necessitates both the fuel and the coolant to be in close
contact with one another to maximise reactor heat transfer.
Added to this, neutrons must be used sparingly via the
careful selection of component material so that excess
neutrons can be used to either bred fuel or burn radioactive waste.
In the end, the whole reactor system must be contained
by a durable and inexpensive material, resistant to corroSC
sion and radiation damage.
*Dr Mark Ho is the current president of the Australian
Nuclear Association. www.nuclearaustralia.org.au/
The Russian Alfa-class submarine which used a leadbismuth fast reactor. It could run at up to 41 knots.
Celebrating 30 Years
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Triac-based for ultra-smooth control!
BY JOHN CLARKE
Full-Wave, 10A Universal
This relatively simple but highly effective Triac-based circuit gives
smooth, full range speed control for electric drills, lawn edgers, circular
saws, routers or any other appliance with universal motors (ie, brushtype), rated up to 10A.
M
versal Motor Speed Controller provides much improved
ost SCR or Triac-based speed controllers ususpeed control because it not only uses a microcontroller to
ally have very poor low-speed control and won’t
provide more precise phase control of the Triac but it also
let the motor reach full speed. This speed limitaemploys current feedback.
tion comes about because these circuits can only switch on
This is not our first full range speed control for universal
every second half-wave of the 230VAC mains voltage. This
motors. Our last design was featured in the February and
means that they can only feed a maximum voltage of about
March 2014 issues. See www.siliconchip.com.au/Series/195
160VAC to the motor.
This had a complex circuit that rectified the 230VAC mains
These limitations are demonstrated in the waveforms
and used a rugged IGBT (insulated gate bipolar transistor) to
shown in Scope1 and Scope2, which come from the Halfrapidly switch the pulsating DC waveform at 980Hz.
Wave Speed Controller published in February 2009.
At low speeds, very narrow
Up till now it has been very
pulses are applied to the motor
difficult to design a Triacwhile at full speed the IGBT is
based circuit which would give
continually on. This technique is
smooth control over a wide • Full wave motor control
referred to as pulse width modurange of speeds.
• Full speed range
lation (PWM).
Nor was it is easy to provide
• 220VAC to 250VAC 50Hz/60Hz
That design is still valid but due
good speed regulation which
to its complexity, it also meant
means that the motor speed is • For “universal” motors (ie, series motors
that it was (and still is), large and
less likely to vary if the loadwith brushes)
expensive.
ing changes.
• 10A 230VAC or similar nameplate rating
Our new Triac-based design
But our new Full Wave Uni-
Features
• Soft start
34
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Motor Speed Controller
also offers impressive performance but it is less complex and
less costly. The Triac is phase-controlled and works similarly
to a leading edge light dimmer (more on phase control later).
The 600V 40A Triac is also arguably more rugged than the
IGBT used in the 2014 design. For an explanation of leading and trailing edge dimmer operation, see our article in
the July 2017 issue (www.siliconchip.com.au/Article/10712)
By the way, our new circuit offers much better speed
control than our Mk2 phase controller from February 2009
which used the same BTA41 Triac. See www.siliconchip.
com.au/Article/1339
Soft start
A particularly attractive feature of this new design is “soft
start”. This means that regardless of speed setting, the motor speed will smoothly build up to the setting and thereby
avoid any sudden kicks – an all-too-common reason for users presenting at hospital casualty rooms!
The new Speed Controller can be used with a 220 to
250VAC mains supply, at 50Hz or 60Hz. This means that
it can be used in any country that has a 220VAC or above.
However, it is not directly suitable for use with a 110VAC
mains supply; that would required some component changes.
Why do you need speed control?
Most power tools will do a better job if they have a speed
control. For example, electric drills should be slowed down
when using larger drill bits. This is particularly the case
siliconchip.com.au
when drilling sheet metal; using too fast a speed will result
in a triangular hole.
Similarly, it is useful to be able to slow down routers, jigsaws and even circular saws when cutting some materials,
particularly plastics, as many plastics will melt rather than
be cut if the speed is too high.
The same comments apply to sanding and polishing tools
and even electric lawn trimmers, where they are less likely
to snap their lines when slowed down.
Even if you do not want a reduced motor speed, the soft
start feature of this Speed Control is handy when using
large power tools such as circular saws and routers which
can otherwise give a substantial kick if started at full voltage. (Some modern power tools, such as electric chainsaws,
have this feature built-in).
Phase control
Before we continue, we should explain what we mean by
phase control that is used in this new design.
As you know, the mains AC voltage is a sinewave. It
starts at zero, rises to a peak, falls back to zero, then does
the same thing with the opposite polarity. This repeats 50
times each second for 50Hz mains and 60 times per second
for 60Hz mains.
We vary the speed of a motor by varying the time during
each half cycle when power is applied: feed power very early in the cycle and it runs fast; delay applying power until
much later in the cycle and it runs slowly.
Celebrating 30 Years
March 2018 35
These half-wave control waveforms are taken from our February 2009 Drill Speed Controller, for comparison with the new one . . .
Scope1: the controller is set for maximum output with resistive load. The yellow waveform is essentially a half-wave
rectified sinewave with a value of 161V RMS (70% of the
blue 230V mains waveform) and a peak value of 341V.
Phase control employs either an
SCR (silicon controlled rectifier) for
half-wave control or a Triac to provide
full wave control, as used in “leading
edge” dimmers.
Scope2: the Speed Controller set for maximum output
when driving an electric drill. There is considerable hash
at the beginning of each positive half-cycle, caused by
interaction between the drill’s commutator and the Triac.
Half wave control means that only
one side of the mains waveform (the
positive or the negative) is applied to
the motor.
These devices are turned on by a
trigger pulse applied to their gate electrodes and the term “phase control”
comes about because the timing of the
trigger pulses is varied with respect to
the phase of the mains sinewave.
Fig.1: The key components of the new controller circuit are the Triac and the PIC12F675 microcontroller, IC1.
IC1 monitors the speed potentiometer, VR1 at pin 6. It also monitors feedback gain potentiometer VR2, at pin 3, the
current feedback via current transformer T1, at pin 7 and the mains waveform via a 330kΩ resistor at pin 5.
36
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Celebrating 30 Years
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in fact, there is no comparison in performance!
Scope3: now set for a lower speed from the electric drill,
the Triac is on for a shorter time and the RMS value of the
waveform is considerably reduced to 45V. Note the
frequency error caused by hash on the waveform.
Speed regulation
For a motor to have good low speed performance, the
speed control circuit should compensate for any drop in
motor speed as the load increases, by increasing power to
the motor. Many simple SCR speed controllers rely upon
the fact that a motor produces a backEMF (electromoWARNING!
tive force) which is
(1) This Speed Controller circuit operates
proportional to its
directly from the 230VAC mains supply and
contact with live components is potentially
speed.
lethal.
The circuit com(2) This circuit is not suitable for use with
pensates for a drop
induction motors.
in back-EMF by
(3) Power tools with inbuilt fans must not
triggering the SCR
be operated at low speeds for long periods,
earlier in the mains
otherwise they may overheat.
half-cycle and so
applying more voltage to the motor.
In practice
though, the backEMF generated by
most appliance motors is quite weak
while the SCR is
not conducting.
This is partly because there is no
field current and
the generation of
voltage is only due
to remnant magnetism in the motor core.
Furthermore,
any back-EMF that
is produced tends
to be too late after
siliconchip.com.au
the end of each half-cycle to have a worthwhile effect on
the circuit triggering in the next half-cycle.
Our new Speed Control uses a different method to provide good speed regulation. It monitors the motor current
to sense motor speed. If it senses a drop in speed, it increases the effective voltage to the motor.
From the general discussion above you can assume that
our new design is significantly different to the February
2009 controller and although both use the same Triac.
The 2009 design uses the Triac as an SCR and the control to the motor is only half-wave.
Our new design uses the Triac to apply AC to the motor
and it is triggered in both half-cycles of the mains waveform.
Unfortunately, the triggering requirements for correct
operation with an inductive load such as a motor cannot
be provided by a simple circuit.
In fact, the Triac must have multiple triggering pulses in
each half-cycle and their timing is very critical. The only
solution is to use a microcontroller.
So let’s have a look at the full circuit in Fig.1.
Circuit description
The key components are the Triac and the PIC12F675
microcontroller, IC1. IC1 monitors the speed potentiometer, VR1 at pin 6. It also monitors feedback gain potentiometer VR2, at pin 3, the current feedback via current transformer T1, at pin 7 and the mains waveform via a 330kΩ
resistor at pin 5.
In response to all those parameters, IC1 produces a series of pulses and these drive the NPN transistor Q1 and
thence the gate of the Triac.
The Triac gate current flows via the 47Ω resistor connected between the 5.1V supply and the Triac’s A1 terminal, then out through the gate and to circuit ground via
Q1 (ie, the gate current is negative).
This method of connection places the 47Ω resistor between the 230VAC mains supply and the 5.1V supply
which runs the PIC microcontroller. This arrangement
has been used to avoid Triac switching noise getting into
the 5.1V supply which can cause latch-up of the microcontroller.
Snubber network
A snubber network comprising two 220Ω 1W resistors
in series and a 220nF 275VAC X2-rated capacitor connected between the A1 and A2 terminals of the Triac. This
network is there avoid rapid changes in voltage being applied to the Triac which would otherwiseit turn on (dV/
dt switching) when it is supposed to be off.
These rapid changes in voltage can occur then power is
first applied or can come from voltage transients generated
by the inductance of the motor being controlled, each time
the Triac turns off. In effect, the snubber network acts to
damp transients and reduce their amplitude.
The DC supply for the microcontroller is derived directly
from the 230VAC mains supply via a 470nF 275VAC X2
rated capacitor in series with a 1kΩ 1W resistor. The capacitor’s impedance limits the average current drawn from
the mains while the 1kΩ resistor limits the surge current
when power is first applied.
It works in the following way. When the Neutral line is
positive with respect to the Active line, current flows via
the 470nF capacitor and diode D1 to the 470µF capacitor to
Celebrating 30 Years
March 2018 37
DRILL SPEED CONTROLLER PERFORMANCE WAVEFORMS
Scope4: this shows the waveform at maximum output.
There is only a very short period (<0.4ms) at the
beginning of each half-cycle when the Triac is off.
charge it up. On negative half-cycles, the current through
the 470nF capacitor is reversed via diode D2.
Zener diode ZD1 limits the voltage across the 470µF capacitor to 12V and that supply then feeds a second 470µF
capacitor via a 47Ω resistor and its voltage is limited to
5.1V by zener diode ZD2. This is the supply for the microcontroller, IC1.
IC1 has its MCLR input (pin 4) tied to the 5.1V supply
via a 10kΩ resistor and this provides a master clear (reset)
for IC1 when power is applied. The main 5.1V supply for
IC1 is decoupled with a 100nF capacitor.
VR1 is the speed potentiometer and it is connected
across the 5.1V supply with the wiper connected to the
pin 6, AN1 input. IC1 converts the voltage set by VR1 into
a digital value using its internal analog to digital converter. The 100kΩ resistor from the wiper to ground holds the
AN1 input at 0V, setting motor speed to zero should VR1’s
Scope5: here the output is set to about half, corresponding to
an RMS voltage about 180V.
Scope 4, 5 and 6 are all with an incandescent lamp load.
wiper go open-circuit.
Trimpot VR2 is also connected across the 5.1V supply
and has its wiper monitored by the AN3 input of IC1 at
pin 3. This voltage sets the gain of the feedback to maintain motor speed load. It is also converted to a digital value within IC1.
The 100nF capacitors at the wiper of VR1 and VR2 are
there to provide a low source impedance for the analog to
digital converter sample and hold input.
Mains synchronisation
Since the timing of the Triac’s trigger pulses are so critical to its correct operation, IC1 needs to monitor the mains
voltage. This is done by the GP2 input of IC1, at pin 5. This
monitors the mains Neutral via a 330kΩ resistor and the
signal is filtered with a 4.7nF capacitor.
An interrupt in IC1 occurs whenever the voltage chang-
What motors can be controlled?
We’ve noted elsewhere in this article that this controller suits
the vast majority of power tools and appliances. These generally
use universal motors and are series-wound motors with brushes.
Incidentally, they’re called universal motors because they can operate on both AC and DC.
You cannot use this Speed Control with any appliance which
has an electronic speed control built in, whether part of the trigger mechanism or with a separate speed dial.
This does not apply to tools such as electric drills which provide
a choice of two speeds via inbuilt reduction gears.
What about induction motors?
We have strongly warned against using any of our previous AC
speed controls with induction motors, for two reasons.
First, the output of our previous designs is variable unfiltered
DC – and that will not run an induction motor, which requires a
variable supply frequency for its speed to be varied.
38
Silicon Chip
Second, connecting an induction motor to any of our previous
speed controls usually resulted in serious circuit damage as well
possibly burning out the induction motor itself.
That won’t happen with this new Speed Control but since it does
not vary the mains frequency it cannot vary the motor speed.
You are unlikely to do any damage to the Speed Control though.
So how do you identify an induction motor?
Most induction motors used in domestic appliances will be
2-pole or 4-pole and always operate at a fixed speed, which is
typically 2850 rpm for a 2-pole or 1440 rpm for a 4-pole unit.
The speed will be on the nameplate. Bench grinders typically use
2-pole induction motors.
If you do need to control this type of motor, use the 1.5kW Induction Motor Controller published in April and May 2012. (www.
siliconchip.com.au/Series/25).
Note that there are important modifications for that project,
published in December 2012.
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This series of scope grabs (and those overleaf) shows the Triac Speed controller working with a 150 watt incandescent lamp load
and a Bosch 500W 2-speed drill. In each case, the connection to the output of the speed controller is made via a 100:1 probe. The
waveforms are identical to those taken with a fully isolated differential probe.
Scope6: the output is set to the minimum whereby the
Triac is still firing. The RMS voltage is 7.36V and the
lamp filament is not even glowing.
Scope7: here the output is set to maximum but the load is
the 500W drill. The hash on the waveform is due to the
motor’s commutator.
es from a high (around 4V) to a low level (around 1V) and
also from a low to a high.
That interrupt level occurs when the mains voltage
swings through zero volts in either direction. The interrupt tells IC1 that the voltage of the mains has just passed
through 0V.
That allows IC1 to synchronise gate triggering with the
mains waveform. Note that the 4.7nF capacitor at pin 5
introduces a phase lag (delay), but this is compensated for
within IC1’s software.
Construction
Current feedback
By now, you are probably wondering about the function
of transformer T1 and the associated bridge rectifier. This
is used to monitor the load current through the Triac. T1
is a current transformer comprising a ferrite toroid with
a 2-turn primary winding in series with the Triac. The
secondary winding has 1000 turns and it is loaded with
a 510Ω resistor.
With this loading, the transformer produces a voltage
of 800mV per amp of load current which is the current
through the motor being controlled.
This voltage is fed to the bridge rectifier consisting of
four schottky diodes and the resulting DC is filtered with
a 10µF capacitor.
The 1kΩ series resistor provides the attack time for the
resulting current feedback signal while the 10kΩ resistor
provides the decay, discharging the capacitor over time.
The current feedback signal is monitored at the AN0 input at pin 7 and the associated 10kΩ resistor and 100nF
capacitor provide extra filtering, as well as limiting any
current into the internal protection diodes at pin 7.
So transformer T1 provides the current feedback signal
for IC1 which gives motor speed regulation and trimpot
VR2 is gain control for that function. You set VR2 to give
the optimum speed regulation for the power tool you are
controlling.
siliconchip.com.au
With the exception of VR1 (the speed control potentiometer), the Full Wave Universal Motor Speed Controller
is constructed entirely on a double-sided, plated-through
PCB (printed circuit board) coded 10102181 and measuring 103 x 81mm.
This is mounted inside a diecast box measuring 119 x
94 x 34mm.
Follow the overlay diagram shown in Fig.2.
Assembly can begin by installing the resistors. The resistor colour codes are shown in a table but you should
also double-check each resistor using a digital multimeter.
Following this, fit the diodes, which must be orientated as shown. Be careful: there are several different diode
types – 1N4004 for D1 and D2 and BAT46 for D3 to D6;
zener diodes are a 12V 1W type (1N4742) for ZD1 and a
5.1V 1W type (1N4733) for ZD2.
If you get any of these mixed up, the circuit will not
operate.
IC1 is mounted on an 8-pin DIL socket so install this
socket now, taking care to orientate it correctly, with the
notch facing towards the top of the PCB.
Leave IC1 out for the time being though – we’ll fit it later
on. Q1 can be installed now.
Capacitors are placed next. The MKT capacitors and
the polypropylene types usually use a code for the value.
These are all shown in the capacitor code table. By contrast, electrolytic capacitors are almost always marked
with their value (in µF) along with their polarity (usually
the negative lead is marked with a stripe). They must be
inserted with the polarity shown.
The screw terminals are next. The 3-way terminal block
for CON2 is installed with the lead entries toward the lower edge of the PCB.
Finally (for now), install the current transformer, T1.
It does not matter which way it is oriented. The Triac is
fitted later.
Celebrating 30 Years
March 2018 39
Scope8: the output is set to about half with the 500W drill
as a load. The RMS voltage is just less than 180V, the
maximum you could expect with a conventional half-wave
SCR speed control.
Scope9: here the output is set to the minimum that will
give useful smooth low speed running from the drill.
Again, the severe hash on the waveform is due to the
motor’s commutator.
Fig.2: this combined component
overlay and wiring diagram
shows where everything goes and
the inter-connections required.
The Triac is secured to the
bottom of the case (ie, underneath
the PCB) with a 3mm screw and
nut – the oversize hole in the PCB
helps with tightening the nut. Its
leads are bent up 90° and then
soldered to the top side of the
PCB once fitted (the holes in the
PCB are all plated-through) – see
the inset diagram above. Ensure
all screws/nuts/etc are tightened
really well and all soldered joints
are exemplary!
40
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Parts list – Full Wave Universal
Motor Speed Controller
Scope10: the ramp-up of the Triac triggering angle during
soft startup. The full ramp-up takes more than one
second.
Drilling the case
Further construction requires drilling holes in the diecast enclosure. A template is shown in Fig.4 for the end
and side panel drilling details. The lid requires a 9.5mm
diameter hole for potentiometer VR1 and a 4mm hole for
the earth screw hole.
The PCB is mounted on the base of the case using M3
tapped spacers that are 6.3mm (or 8mm) long. Holes are
required for these mounting holes on the base of the case.
The CON1 screw terminal end of the PCB sits further
away from the end of the box compared to the other end.
This allows space for the cable gland nuts. Position the
PCB in the case to use as a template and mark out the hole
positions and drill out to 3mm.
Attach the 8 or 6.3mm long spacers to the PCB. Then
bend the triac leads up at 90° 4mm from the body of the
triac. Insert the leads into the PCB from the underside. If
you are using 6.3mm spacers, the underside pigtail leads
from the components must be cut short to prevent close
contact with the base of the case. They should be trimmed
anyway regardless of the spacer length.
The PCB can be secured to the case with screws from
the underside into the tapped spacers. Mark out the triac
mounting hole position on the base of the case.
Remove the PCB again and drill out to 4mm. Clean away
any metal swarf and slightly chamfer the hole edges. Reattach the PCB and adjust the Triac lead height so the metal
tab sits flush onto the flat surface.
Secure the Triac with the M3 screw and nut. The metal
tab is internally isolated from the leads and so does not
require any further insulation between its tab and case.
Solder the Triac leads on the top of the PCB and trim the
leads close to the PCB.
Now remove the screws to gain access to the underside
of the PCB and solder the triac leads from the underside of
the PCB. The four rubber feet can be attached to the base
of the case now.
Two holes are required in the lid – one for the speed control pot (9.5mm) and the other for the earth screw (4mm).
If you use a countersunk-head earth screw and countersiliconchip.com.au
1 PCB coded 10102181, measuring 103 x 81mm
1 diecast box 119 x 94 x 34mm [Jaycar HB-5067]
1 Talema AX-1000 10A current transformer (T1) [RS
Components 775-4928]
1 M205 10A safety panel mount fuse holder (F1) [Altronics
S5992]
1 M205 10A fuse
1 4-way PCB mount terminal barrier (CON1) [Jaycar HM3162]
1 3-way PCB mount screw terminals with 5.08mm spacings
(CON2)
2 cable glands for 5-10mm cable
1 DIL-8 IC socket
1 2m 250V 10A mains extension lead (cut in half to form
mains input and output leads)
4 4mm eyelet lugs
4 8mm or 6.3mm M3 tapped Nylon standoffs
1 M3 x 10mm screw (for triac mounting)
1 M3 nut and washer
2 M4 x 10mm screws (CSK head preferred)
2 4mm ID star washers
2 M4 nuts
8 M3 x 5mm screws
4 stick-on rubber feet
1 20mm length of 12mm diameter heatshrink tubing
1 80mm length of 3mm diameter heatshrink tubing
1 25mm length of 6mm diameter green heatshrink tubing if
required for chassis lugs
3 150mm lengths of 7.5A mains-rated wire for VR1
3 100mm long cable ties
Semiconductors
1 PIC12F675 programmed with 1010218A.hex (IC1)
1 BTA41-600B insulated tab 40A 600V Triac (Triac1)
[element14 1057288 or RS 687-1007]
1 BC337 NPN transistor (Q1)
1 12V 1W (1N4742) zener diode (ZD1)
1 5.1V 1W (1N4733) zener diode (ZD2)
2 1N4004 1A diodes (D1,D2)
4 BAT46 schottky diodes (D3-D6)
Capacitors
2 470µF 16V PC electrolytic
1 10µF 16V PC electrolytic
1 470nF 275VAC X2 class
1 220nF 275VAC X2 class
4 100nF 63V or 100V MKT polyester
1 4.7nF 63V or 100V MKT polyester
Resistors (0.25W, 1% unless specified)
1 330kΩ 1W carbon film 1 100kΩ
3 10kΩ
1 1kΩ 1 1kΩ 1W carbon film
1 510Ω
1 470Ω 2 220Ω 1W carbon film
2 47Ω
1 linear 10kΩ 24mm potentiometer (VR1)
1 10kΩ mini, top adjust trimpot (3386F style) (VR2)
Miscellaneous
1 knob to suit VR1
Super glue, heatsink compound, solder
Celebrating 30 Years
March 2018 41
Scope11&12: these show how the Triac triggering varies, depending on the speed setting. At low speed settings, there is
only one trigger pulse during each mains half-cycle. At higher power levels, there are multiple trigger pulses during each
half-cycle to ensure that the Triac stays turned on, in spite of the lagging load current (due to the inductive motor load).
sink the earth screw hole appropriately, it can be mounted under the panel label (looks neater!). Otherwise, you’ll
need to cut holes in the panel label (with a sharp hobby
knife) when the label is stuck on.
The panel label file can be downloaded (free for subscribers) from our website (www.siliconchip.com.au).
To produce a front panel label, you have several options.
For a more robust label, print as a mirror image onto clear
overhead projector film (using film suitable for your type
of printer). Attach the label printed side down to the lid
with a light coloured or clear silicone sealant.
Alternatively, you can print onto a synthetic “Dataflex”
sticky label that is suitable for inkjet printers or a “Datapol” sticky label for laser printers. Then affix the label using the sticky back adhesive.
(There’s more information on Dataflex at siliconchip.com.
au/link/aabw and Datapol at siliconchip.com.
au/link/aabx And there’s a few more hints on
making labels for projects – see siliconchip.
com.au/Help/FrontPanels).
Wiring
Cut the 10A extension lead into two to
provide one lead with a plug on the end and
another with a socket. Where the lead is cut
depends on how long you prefer each lead.
You may prefer a long plug cord and short
socket lead so the motor appliance is located
near to the controller, or the lead can be cut
into two equal lengths.
Before cutting make sure you have sufficient
length to strip back the insulation as detailed
in the next two paragraphs.
Make sure the plug lead and socket lead
are placed in the correct gland and wired as
shown.
First the socket (output) lead: you need a
100mm length of earth wire (green/yellow
stripe) for the connection between the chassis and lid, so strip back the outside sheath
insulation by about 200mm. Then cut the blue
The lid, with front panel affixed, “opens
out” from the box as shown in this photo,
reproduced about three-quarter size. Make
sure the wires to the speed pot are all
250VAC mains-rated (don’t use rainbow
cable!) and use cable ties and heatshrink
where shown above and in Fig.2.
42
Silicon Chip
Celebrating 30 Years
siliconchip.com.au
Three holes are required in the end of the case – the two
on the right are 15mm to suit the cable glands, while the
hole on the left is nominally 12.5mm but is “D” shaped
to hold the fuseholder in place. On the lid, a 9.5mm hole
to house the speed control pot sits slightly off-centre with
a 4mm hole (on the left in this photo) for the lid earthing
screw. As mentioned in the text, if this hole is shaped to
accept a countersunk-head screw, it can go underneath
the label and so not be visible.
neutral wire and brown active wires to 50mm and connect
them to their respective terminals on the terminal block.
You should be left with 100mm of earth wire (green/
yellow stripe) which is routed around the edge of the PCB
and twists with the earth wire from the plug (input) lead
to be crimped into one of the earth lugs.
The spare 150mm brown wire can be used later to con- Fig.3: the same-size front panel artwork which is designed to
nect from the fuse to the CON1 terminal via the trans- be glued to the case lid. It can be copied, or downloaded (free
former, T1. This has two turns of the active wire looped for subscribers) from siliconchip.com.au
through the transformer hole.
The plug lead outside sheath insulation should be stripe) wire and the output earth wire together and crimp
stripped back to expose 100mm of wire. This leaves suf- into one of the eyelet earth lugs.
Cut VR1’s shaft to 12mm long and file the edges smooth.
ficient lead length. All three wires are passed through the
Then attach the three 100mm lengths of 7.5A mains rated
cable glands and connect as shown in Fig.2. Cut the neutral
wire to 50mm and strip back the insulation before connect- wire to the three VR1 terminals and cover with the 3mm
heatshrink tubing. The other ends connect to CON2.
ing the neutral (blue) wire to the terminal block
These wires are secured using a cable tie that feeds
The active (brown) wire solders direct to the fuseholder.
10mm diameter heatshrink tubing should first be placed through holes in the PCB. Attach VR1 to the lid of the case
over active (brown) wire which slides up and over the fuse- – note that the potentiometer must be located as shown (ie,
holder after soldering to cover the side fuseholder terminal. leads emerging from the right) so it fits between the two
Similarly, 3mm diameter heatshrink tubing 3mm in di- mains rated capacitors on the PCB.
Fit the knob – you may need to lift out the knob cap with
ameter is used to cover the fuseholder end terminal. Once
both connections are soldered, pass the heatshrink over a hobby knife and re-orient the cap so its pointer position
matches the rotation marks on the panel.
the join and shrink.
That 100mm length of earth wire you cut off from the
Now twist the ends of the input earth (green/yellow
output lead can now be crimped into
two eyelet lugs, which are screwed to
Resistor Colour Codes
the underside of the box lid and the
Qty Value
4-Band Code (1%)
5-Band Code (1%)
earth screw on the side of the case using
1^ 330kΩ orange orange yellow brown orange orange black orange brown
1 100kΩ brown black yellow brown
brown black black orange brown
Small Capacitor Codes
3
10kΩ brown black orange brown
brown black black red brown
1+1^ 1kΩ brown black red brown
brown black black brown brown
Qty Value/Type
EIA
IEC
1 510Ω green brown brown brown
green brown black black brown
1 470nF X2
474 470n
1 470Ω yellow purple brown brown
yellow purple black black brown
1 220nF X2
224 220n
2^ 220Ω red red brown brown
red red black black brown
4 100nF MKT
104 100n
2
47Ω yellow purple black brown
yellow purple black gold brown
1 4.7nF MKT
472 4n7
^ = 1W, carbon film type
siliconchip.com.au
Celebrating 30 Years
March 2018 43
Fig.4: drilling detail of the specified
diecast box, reproduced same size.
Note that the hole for the fuseholder
is not circular – the D-shape keeps
the fuseholder from turning when
a fuse is being inserted or removed.
The 3mm diameter hole for the Triac
in the bottom of the box is not shown
–use the PCB to locate it.
M4 screws, star washers and nuts. Ensure that the nuts are
fully tightened.
Final assembly
Apply a smear of heatsink compound to the underside of
the Triac before installing the PCB inside the case. Again,
the tab of the Triac is insulated, so it can contact the case
with safety.
The last components to inserted are IC1 (taking care it
is oriented correctly), the 10A fuse into its holder and the
cover for the barrier terminals (CON1) – it is simply pressed
on to cover the screw terminals. Finally, rotate VR2 fully
anticlockwise to initially disable feedback.
Check your construction carefully and especially check
that the earth wires (green/yellow striped) actually connect together the case, the lid and the earth pins on both
the mains plug and socket. Check this with a multimeter
set to read low ohms.
The cable glands need to be tightened to hold the mains
cords in place. Because these are easily undone, the thread
of the glands should have a drop of super glue applied to
44
Silicon Chip
the threads before tightening. This way the glands cannot
be undone. Attach the lid to the case using the four screws
supplied with the case (don’t be tempted to run the speed
controller without the lid in place!).
Testing
Connect up a universal motor appliance (eg, an electric
drill) to the controller, apply power and check the motor
can be controlled when adjusting the speed potentiometer.
Once you have verified that it works, switch off power
and unplug the mains plug from the mains outlet. Then
remove the lid and adjust VR2 half way. Re-attach the lid
and apply power again and check the speed regulation of
the motor under load.
Trimpot VR2 may need further adjustment; anticlockwise if the motor speeds up under load and clockwise if
the speed drops off too markedly under load.
Note that any adjustment of VR2 must only be done with
the power off and mains plug disconnected. This means
that adjustment is a trial and error process. Power should
only re-applied after the lid is re-attached.
SC
Celebrating 30 Years
siliconchip.com.au
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.
Drift-free Induction Balance Metal Detector
Induction Balance (IB) metal detectors with concentric search heads are
very popular as they have a high sensitivity and allow you to pinpoint the
detected object. The simplest such instruments are based on a low-frequency RF oscillator tied to transmit coil(s),
a pickup coil feeding the RF pre-amplifier, a peak detector, DC amplifier
and an audio amplifier.
The problem with this approach is
that the RF oscillator must be very stable or the instrument must be continuously adjusted. Also, thermal drift of
the signal diodes used in the peak detector can affect their operation.
This design overcomes both problems by using a ceramic resonator to stabilise the RF oscillator and by employing pulsating DC current in the transmit
coils, eliminating the need for a peak
detector to rectify the received signal.
It can sense a coin at a distance of
around 200mm and a larger object
(400mm in diameter) 700mm away in
free air. It is equipped with a discriminator section that can be set to nonferrous (Mode 1) or ferrous (Mode 2)
detection with a momentary press of
the mode selector pushbutton.
The detector is built around a 4060B
oscillator and a frequency divider
(IC1), a TL064 quad op amp (IC2) and
two gates of a 4066B quad bilateral
switch (IC3). An ATmega8 microcontroller with a 16x2 alphanumeric LCD
module and a series of LEDs is used to
indicate the detector status.
IC1 forms the primary oscillator. Its
frequency is set to 455kHz by ceramic
resonator X1, which is accompanied
by two 220pF load capacitors. Output
pin 4 of IC1 (O5) provides a frequency
which is 1/64th of the oscillator, which
in this case is 7.1kHz.
This signal is then fed to control
pin 13 of bilateral analog switch IC3a,
causing it to dump the 5V charge
across the 100nF capacitor at pin 1
through transmit coils L1 and L2 about
7,100 times per second.
These DC pulses cause a pulsating
magnetic field around transmit coil L1
and bucking coil L2, which are wound
in opposite directions and connected
in series.
Under no-target conditions, their
induced magnetic fields cancel each
other out and so nothing is picked up
by receive coil L3. But when a metallic object is inside the magnetic field,
the balance of these magnetic fields is
affected, resulting in a voltage appearing across L3. This is fed to a differential amplifier based around op amp
IC2c and appears as an output signal
at its pin 8.
The two 330nF capacitors in series
across L3 (effectively, a single 165nF
capacitor) cause it to be resonant at
the expected signal frequency, rejecting external interference and maximising signal pick-up. The differential
amplifier has a gain of around 94 times
(220kW ÷ 4.7kW × 2).
The signal from IC1 which controls
when the pulses are applied to the
transmit coils is also fed to both inputs
(pins 5 & 6) of op amp IC2b. However,
the signal to non-inverting input pin
5 is delayed by an RC low-pass filter
with a time constant of 2.2kW x 4.7nF
= 10µs.
That causes output pin 7 of IC2b to
go high a short time after output O5
of IC1 goes high (ie, when the pulse
is applied to the transmit coils) and it
stays high for a short time after output
O5 goes low again.
This signal is used to control another
analog switch, IC3b, which gates the
output of differential amplifier IC2c so
that it’s only fed to the following amplifier stage, IC2d, during this window
period. This preserves the polarity of
the received DC voltage pulses and is
necessary for the micro to provide the
ferrous/non-ferrous metal discrimination function.
IC2d further amplifies the resulting
signal by a factor of 48 and also provides some low-pass filtering due to
the 33nF capacitor across its feedback
resistor. The signal then passes to sensitivity adjustment potentiometer VR1
and another low-pass filter. The resulting DC signal then goes to analog input
ADC5 (pin 28) of micro IC4.
IC4 converts this analog signal into
a number, then displays the received
voltage at right-hand side of the top
line on the LCD, reading 0-5V DC.
When a metal object is detected, the
micro also uses the change in DC voltage to light up one of ten LEDs, LED1LED10, giving an indication of the size
and closeness of the metal object with
LED1 indicating the weakest signal
and LED10 the strongest.
The micro also drives its PWM output at PB1 (pin 15) to produce an AC
waveform which is fed to an RC lowpass filter and thence to a 4046 voltage-controlled oscillator, IC5. Depending on the PWM duty cycle and thus
the voltage at pin 9 of IC6, it produces
a tone which is then fed to the piezo
sounder, to be heard by the operator.
The sounder is silent when nothing
has been detected. If the search head
detects an object, LED1 lights up and
the piezo audio frequency is set to
700Hz. It rises in steps of 120Hz, up to
2500Hz, as the voltage from the metal
detection circuitry increases.
Circuit Ideas Wanted
Got an interesting original circuit that you have cleverly devised? We will pay good money to feature it in Circuit Notebook. We can pay you by electronic funds transfer, cheque or direct to your PayPal account. Or you can use the funds
to purchase anything from the SILICON CHIP on-line shop, including PCBs and components, back issues, subscriptions
or whatever. Email your circuit and descriptive text to editor<at>siliconchip.com.au
siliconchip.com.au
Celebrating 30 Years
March 2018 45
Thus, the VCO generates 16 distinct
tones for objects producing weaker or
stronger magnetic fields or buried at
different depths.
When the LEDs light up, a corresponding 16-step bargraph is also displayed on the second line of the LCD.
Power is from a 9V battery, switched
by S1, with reverse polarity protection
diode D1. A 78L05 regulator reduces
the battery voltage to a steady 5V for
the rest of the circuit.
The search head includes transmit
coil L1, receive coil L3 (half the diameter of the transmit coil) and bucking
coil L2 which is wound on top of the
receive coil. All three coils are wound
using 0.315mm diameter (30SWG)
enamelled copper wire.
L1 consists of 80 turns wound anti-
46
Silicon Chip
clockwise on a 140mm diameter former (eg, a piece of plastic conduit).
Once complete, remove the completed
coil from the former and wrap it with
insulating tape.
Receive coil L3 is made using 160
turns wound anti-clockwise (just like
L1) on a 70mm diameter former. Bucking coil L2 consists of 27 turns wound
clockwise directly on top of the receive coil.
Remove the double coil L2/L3 from
the former, then secure them together
using strips of insulating tape. Leave a
moveable loop of about one half-turn
of wire from L3. This will be moved
around later, to get a good null when
the coils are being balanced.
Once the three coils have been
made, cut a 160mm diameter circle
Celebrating 30 Years
from 3mm plywood or similar. Mount
L1 and then the double coil L2/L3 at
its centre. All the three coils are positioned coplanar and concentric with
one another so that they are all centred on a common axis. Connect the
coils to the circuit according to the
schematic.
Notice that the bucking coil L2 is
connected in series with the transmit
coil L1 but with its phase reversed.
The most sensitive part of the search
head is the area under the receive coil.
For more details on the construction
of coplanar concentric coils, refer to
US patent 4293816 or visit this site:
siliconchip.com.au/link/aait
Having built the unit, you will need
to program microcontroller IC4. The
software is written in BASIC and a
siliconchip.com.au
HEX file is supplied along with it.
This was generated from the BASIC
code using BASCOM for Atmel AVR.
A free trial of this compiler is available at siliconchip.com.au/link/aacw
Upload the HEX file to the ATmega
chip using a compatible programmer,
then set VR1 to maximum, place the
search head well away from any metal object and switch the detector on.
It starts up in non-ferrous mode 1,
which should cause non-ferrous metallic objects to be picked up and ferrous objects to be rejected. The current
mode is shown on the left-hand side
of the first line of the LCD.
Move around the half-turn moveable loop of the bucking coil L2 until
the ADC voltage on the right-hand side
of the first line of the LCD reads 2.20-
siliconchip.com.au
2.25V. Then fix the moveable coil in
place using glue. Turn VR1 down until the ADC idle voltage on the LCD is
between 1.95 and 1.99V. The sounder
falls silent when the ADC voltage is
below 2.00V DC.
Now bring a coin close to the centre of the search head. The ADC voltage should increase and LED1 should
light up. At the same time, the sounder
should produce a tone. The closer you
bring the coin to the search head, the
higher will be the frequency of the audio output and the higher the number
of the LED that lights up. Only one of
the LEDs is on at a time.
The bargraph on the second line of
the LCD also proceeds proportionately
from the left to right as the strength of
the field increases. With the strongest
Celebrating 30 Years
signal, LED10 will light up, the sound
frequency will be 2500Hz and the bargraph will fill the width of the LCD.
Now push mode switch S2 to cause
the circuit to switch to the ferrous
metal detection mode, mode 2. Turn
VR1 up to set the ADC idle voltage to
2.01 to 2.05. In this mode, when the
ADC voltage is above 1.99, the sounder
falls silent. Bring a small ferrous object, like an iron screw or bolt, close
to the search head. The ADC voltage
decreases but LED1 will light up and
the sounder will produce a tone.
As the ferrous object is brought closer, the other LEDs will light up in turn
and the tone will increase in pitch. The
bargraph also proceeds to the right.
Mahmood Alimohammadi,
Tehran, Iran. ($80)
March 2018 47
Colour slideshow with alarm clock using an ESP32
A few years ago, I hooked a Raspberry Pi up to a 3.5-inch TFT display
to use as a digital picture frame/slide
show. It loaded pictures from the SD
card in the Raspberry Pi and displayed
them in sequence.
This is a cheaper, simpler version of
that project with even more features.
It uses just a few low-cost modules,
including an ESP32 microcontroller
module with onboard WiFi, to display a series of images as well as an
“analog” clock and it can be used as
an alarm clock too.
This version uses a 3.2-inch colour
TFT based on the ILI9341 controller.
This is similar to the touchscreen used
in the Micromite LCD BackPack from
the February 2016 issue (siliconchip.
com.au/Article/9812) except that it has
no touch sensor.
The same circuit and code should
work with a variety of screens based
on this chip.
One advantage of using the ESP32
is that it starts up instantly and is very
reliable. By comparison, the Raspberry
Pi takes some time to boot since it’s
running a fully-fledged operating system. That also means there’s more to
go wrong.
48
Silicon Chip
I used the Adafruit display library
for Arduino and this incorporates a
bmpDraw() function which makes it
easy to load and display an image.
To add the clock function, I wired
up a DS3231-based real-time clock
module. This is the same module
which has been used in several Silicon Chip projects and it incorporates
an onboard battery back-up to keep
the time correct.
Its internal crystal is very accurate
so it doesn’t suffer from much drift
over time.
I also wired up a piezo buzzer between pin D14 of the ESP32 and
ground, and used the WriteTone()
function to drive this at a particular
frequency for the alarm clock function.
The clock is drawn on the screen
like an analog clock, the date, day
of the week and temperature (as
determined by a sensor on the DS3213
module) are shown as text on the
clock face.
The wiring of the modules is fairly straightforward, with the display
and microSD card module sharing
the same SPI bus consisting of shared
MISO (data in), MOSI (data out) and
SCK (clock) pins which go to D19, D23
Celebrating 30 Years
and D18 on the ESP32 respectively.
They have their own CS (chip select)
pins, with the LCD wired to D4 and
the microSD card to D13.
The LCD also has a DC (data/command) pin and reset pin, which are
wired to D15 and D2 on the ESP32
micro. The DS3231 module uses I2C
communications so its SDA (data) pin
goes to D21 while its SCL (clock) pin
goes to D22.
The remainder of the pins are VCC
and GND which are simply wired to
3.3V and GND respectively on each
device.
All these devices will run off 3.3V.
The LCD I used has an integrated 3.3V
regulator so it can run off 3.3V or 5V.
The ESP32 also has an internal regulator to derive the 3.3V rail from a 5V
USB supply. A 10µF bypass capacitor helps filter this rail. The unit can
be run from a USB charger or similar.
I built my unit on protoboard with
the ESP32 module soldered to one side
and the SD card shield and TFT display on the other.
Some ILI9341-based LCD screens
have an onboard SD card holder and
you could use this instead of the separate module. The total cost of all the
modules in my prototype is around
US$22.
The software is compiled and uploaded to the ESP32 using the Arduino
IDE. The sketch and all required
libraries can be downloaded from the
Silicon Chip website, free for subscribers.
You will also need to enable support
for the ESP32 board in the Arduino
IDE before you can compile it. The
instructions to do so are given here:
siliconchip.com.au/link/aaiw
Once you’ve done that, you will
need to load all the libraries (zipped)
into the IDE before the sketch can be
compiled and uploaded.
All the images for your slideshow
need to be saved in BMP format in
320x240 pixel resolution with 24-bit
RGB colour. They should be placed in
the root directory of the SD card. You
can use free software such as GIMP to
convert images in other formats (such
as JPG and PNG) to BMP.
Here is a YouTube videos showing
the prototype in operation: https://
youtu.be/Wpny5v6ZXoE
Bera Somnath,
Vindhyanagar, India. ($75)
siliconchip.com.au
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GPS RECEIVER
MODULE XC-3712
SCREENS FOR YOUR CAR USING ARDUINO®
A GPS receiver using the NEO6MV2 module,
outputting NMEA data at 9600 baud. Excellent
performance with a 50 channel receiver,
2m position accuracy and 0.1m/s speed accuracy.
• Ceramic antenna
• 4 Pin header for power
and serial data
• 3.3V regulator on board
• Battery backed RAM
$
4995
15 95
$
$
29 95
128 X 128 LCD
SCREEN MODULE XC-4629
240 X 320 LCD
TOUCH SCREEN XC-4630
Compact Colour TFT-LCD display supporting
16 bit colour at 128x128 pixels, and only
needing six pins for full control.
• SPI interface
• 43(L) x 30(W) x 12(H)mm
Colour resistive touch LCD display shield. Piggy-backs
straight onto your UNO or MEGA main board. Fast
parallel interface. microSD card slot.
• Resistive touch interface
• 77(L) x 52(W) x 19(H)mm
BUILD YOUR OWN PARKING ASSISTANT
BUILD A
VEHICLE
TRACKER OR
LOGGER, OR
EVEN USE THE
ACCURATE SPEED
MEASUREMENT
TO CREATE A
SPEEDOMETER.
www.jaycar.com.au/ultrasonic-parking-assistant
7
$ 95
DUAL ULTRASONIC
SENSOR MODULE XC-4442
Finished project.
$
FROM
49
14 ea95
$
95
The popular HC-SR04 ultrasonic distance module
provides an easy way for your DuinoTECH to
measure distances up to 4.5m.
• Uses two digital pins
• 45(W) x 20(D) x 13(H)mm
FROM
12 95
$
REMOTE CONTROL RELAY BOARDS
UNIVERSAL LED FLASHER RELAYS
RELAY MODULES
Add remote control functions to your projects with these
handy relay boards. Set to momentary or latching mode.
• 40m max transmission range
• 12VDC
2 CHANNEL LR-8855 $49.95
4 CHANNEL LR-8857 $69.95
Specifically designed to work with replacement low
current LED indicator lights which may "hyper flash"
when used with your cars standard flasher relay.
• Silent operation
• 40(H) x 30(W) x 30(L)mm
2 PIN 10A SY-4016
3 PIN 20A SY-4018
Control a motor backwards and forwards without speed
contro. Plenty of power (up to 10A at 30VDC), but need a
separate 12VDC power supply to operate the relays. Provide
isolation between the Arduino circuit and switched circuit.
4 CHANNEL XC-4440 $12.95
8 CHANNEL XC-4418 $19.95
12 95
7
$
$ 95
MOTOR CONTROL
MODULE XC-4472
DC-DC STEPDOWN MODULE XC-4514
Has 2 x 5V servo ports connected to the Arduino's highresolution dedicated timer to ensure jitter-free operation.
Control up to four DC motors or two stepper motors.
• 5V to16VDC
• 70(L) x 53(W) x 20(H)mm
Accepts any voltage from 4.5-35VDC, and outputs any lower
voltage from 3-34V. Use it to run your 5V Duinotech projects
from a 6V, 9V or even 12V supply.
• 4.5-35V input voltage, 3-34V output voltage
• 2.5A maximum output current
• 49(L) x 26(W) x 12(H)mm
19 95
$
DC-DC BOOST MODULE WITH DISPLAY XC-4609
Can be used to provide higher voltages for your project,
such as running 5V Arduino projects from Lithium batteries.
• Maximum 2A input current without heatsinking
• Solder terminals
• 66(L) x 35(W) x 12(H)mm
AUTO CIRCUIT PROTECTION
10-WAY BLADE FUSE BLOCKS
AUTOMOTIVE FUSE PACK SF-2142
Perfect for automotive or marine applications. Removable
protective cover and LED indicators for each fuse.
• Input: 100A max
• Output: 30A max per circuit
WITH LED INDICATORS
SZ-2008 $16.95
WITH LED INDICATORS
FROM
& WEATHERPROOF
$
95
SZ-2001 $19.95
120 standard size automotive fuses housed
in a 6 compartment storage box. 20 x 5A, 10A,
15A, 20A, 25A & 30A fuses included.
16
Page 50
$
23 95
Follow us at facebook.com/jaycarelectronics
HEAVY DUTY PANEL
MOUNT CIRCUIT BREAKERS
High quality units with multi-wire
gauge inputs/outputs, perfect for
high powered car audio, automotive
or solar installations.
60A SZ-2081
$
95
120A SZ-2083
ea
200A SZ-2085
39
Catalogue Sale 24 February - 23 March, 2018
PROJECT OF THE MONTH
DUINOTECH MULTIFUNCTION
VOLTAGE GAUGE
NERD PERKS CLUB OFFER
BUY ALL FOR
7995
$
The XC-4284 Round LCD Module for Arduino is an impressive
piece of gear, capable of all manner of graphics, but especially
suited as a round gauge. Here we’ll
show you how to interface the Round
LCD Module to an Arduino® board for
displaying system voltage and in a few
different styles. Ultimately the round
gauge just displays a numerical value,
so any sort of numerical data (e.g.
temperature, velocity etc) could be
added to the gauge.
®
SAVE 20%
VALUED AT $101.85
SEE STEP-BY-STEP INSTRUCTIONS AT:
jaycar.com.au/voltage-gauge
WHAT YOU NEED:
DUINOTECH LITE (LEONARDO)
INTELLIGENT 1.3" ROUND LCD MODULE
28 PIN HEADER TERMINAL STRIP
10K OHM 0.5 WATT METAL FILM RESISTORS - PACK OF 8
1K OHM 0.5 WATT METAL FILM RESISTORS - PACK OF 8
9
$ 95
XC-4430
XC-4284
HM-3211
RR-0596
RR-0572
$29.95
$69.95
$0.85
$0.55
$0.55
ea
1195
SEE OTHER PROJECTS AT www.jaycar.com.au/arduino
14 50
$
$
$
FROM
39 95
MICRO BLADE FUSES
FLEXIBLE DC POWER CABLE
ULTIMATE HEATSHRINK PACK
TRAILER CABLES
SF-2146
Suit newer model cars. The pack contains
one each of 5, 7.5, 25, 30A and two each of
10, 15, 20A.
• Pack of 10
Suitable for general purpose automotive and
marine applications. 15A rated current.
• 10m roll
RED WH-3054
BLACK WH-3055
GREEN WH-3056
WH-5520
1 length each of 7 different colours in 7
different sizes ranging from 1.5mm dia to
20mm.
• Sizes: 1.5, 3, 5, 6, 10, 16 & 20mm
10m length sheathed in a
tough black PVC jacket.
5 CORE WH-3091 $39.95
7 CORE WH-3090 $44.95
MAKE IT A PROJECT!
FROM
6
$ 95
MERIT CONNECTORS
Commonly used in automotive power
connections. Smaller in size, extremely
rugged and provides higher reliability and
current ratings.
15A UNFUSED PLUG PP-2090 $6.95
8A PLUG WITH CIGARETTE LIGHTER
ADAPTOR PP-2094 $6.95
15A PANEL SOCKET WITH COVER
PS-2092 $9.95
15A IN-LINE SOCKET WITH COVER
PS-2096 $6.95
FROM
6
$ 95
19 95
$
WATERPROOF DEUTSCH
2-WAY CONNECTOR SET
12V TO 5VDC
CONVERTER WIRING KIT MP-3675
High quality connectors commonly used in
automotive or marine applications. Perfect
for connecting up sensors/lights in the bay
due to their superior corrosion protection.
• 13A rated.
2-WAY PP-2150 $6.95
4-WAY PP-2149 $8.95
6-WAY PP-2148 $9.95
Get rid of unsightly power cables floating
around car dash that powers GPS, Dash Cam
or mobile device.
• Micro USB Plug
(Mini USB adaptor included)
• 2.5A continuous current
• Cable length 1.3m
To order phone 1800 022 888 or visit www.jaycar.com.au
See terms & conditions on page 8.
$
29 95
SOUND DEADENER
AX-3689
An easy single application solution for
complete sound deadening and isolation that
also offers thermal insulation.
• Combination of butyl and foam
Page 51
FROM
12 95
$
CAR
SECURITY
$
DOOR LOCK ACTUATORS
Used on passenger/driver doors. Durable,
waterproof, dustproof and supplied with
universal mounting hardware. Wiring not
included. Input voltage: 9 - 16VDC.
SLAVE PASSENGER LR-8813 $12.95
MASTER DRIVER
LR-8815 $14.95
FROM
Upgrade to a remote keyless entry! Easy to
install and comes with two remote key fobs.
• Includes master actuator,
wiring and remotes
ea
12 95
9
Upgrade car/caravan/boat interior lighting
with LED technology. Each kit consists of
cool white LEDs with 3M adhesive foam
backing. 12VDC. Universal T10/211/BA9S.
2.5W 260 LUMEN ZD-0585 $9.95
3.0W 310 LUMEN ZD-0587 $12.95
4.5W 450 LUMEN ZD-0589 $14.95
A range of 150 lumens ultra-bright white
LED replacement “festoon” globes
for car interior lights. 120º wide beam.
12VDC.
31MM ZD-0750
36MM ZD-0752
41MM ZD-0754
ONLY
299
SAVE $49.95
CAR
$
249
12 95
TEST &
MEASUREMENT
CAR
ACCESSORIES
Page 52
SAVE $20
H4 HI/LO LED POWERED
HEADLAMP KIT SL-3524 WAS $169
Bright and efficient. Equipped with
advanced Luxeon Z ES LEDs.
• Accurate LED position to ensure correct
beam pattern
• 3800 lumens 40W
• 12/24V
UHF 5DBI
FIBREGLASS
ANTENNA
WITH 5M CABLE
DC-3078
Suitable for cars and
trucks using UHF
transceivers. Flexible
spring base to absorb
and deaden the
vibrations associated
with driving.
• 630mm long
$
$
BATTERY, CHARGER AND
ALTERNATOR TESTER QP-2258
Compact, lightweight, includes 600mm leads
with croc clips, and inbuilt magnet to secure
the unit while taking measurements. 12VDC.
16 95
Play your music from your media player
through your car stereo cassette system.
• No power or batteries required
• Supplied with 1.1m lead &
3.5mm stereo plug
$
39 95
LED VOLTMETER & AMPMETER
Simply plug into the cigarette lighter socket
and get an instant LED readout of the car’s
battery voltage.
• Works on 12/24V vehicles
QP-5584
Monitor battery voltage and current draw.
Supplied with a panel mount and a surface
mount "hood". Connection via three 6.3mm
spade terminals .
$
CD-CASSETTE ADAPTOR AR-1760
RUBBER TOPMOUNT
CAR ANTENNA AR-3260
CAR BATTERY MONITOR QP-2220
19 95
$
18
$
Good for 4WDs etc. Small and flexible.
• 350mm long
99 95
19 95
$
NOW
149
FESTOON LED GLOBES
CANBUS COMPATIBLE
DC-1122
Compact size for under-dash mounting.
Long transmission range up to 20km.
Function buttons/controls are located
on the microphone. Group scan, CTCSS
& DCS,etc.
• 100 user programmable RX channels
• 12/24V
WITH KILL SWITCH LR-8842
Lock and unlock your car doors from
a distance without having to fumble
around with keys. 9 - 16VDC.
• Frequency: 433.92MHz
$
INTERIOR LED
RETROFIT KITS ZD-0585
RADIO +
ANTENNA
89 95
REMOTE CONTROLLED CAR
4 DOOR REMOTE CONTROLLED
CENTRAL LOCKING SYSTEM LR-8839 CENTRAL LOCKING KIT
5W IN-DASH UHF RADIO
$
$
$
$ 95
CAR
LIGHTING
49 95
19 95
$
SPRING CLAMP
UNIVERSAL HEADREST
SUCTION MOUNT PHONE HOLDER TABLET BRACKET HS-9033
HS-9039
Securely mounts to your windscreen with
360° rotation.
• Suits virtually any smartphone
Follow us at facebook.com/jaycarelectronics
Fits just about any vehicle. Padded clamps
to protect your device. 360° rotating
ball-joint.
Catalogue Sale 24 February - 23 March, 2018
TECH TIP:
PORTABLE JUMP STARTER
Ever been stranded on the road with a flat car battery? An emergency portable
car Jump Starter will help you avoid this frustrating situation.
Jaycar has an extensive range of Jump Starters, with some models so small they
can fit in the palm of your hand, but still offer an impressive cranking current of
270A+ (plenty of power for kick starting most motor vehicles).
Higher power models allow you to kick start larger engines and enable you to
use it multiple times before needing to recharge the unit.
Our MB-3736 Jump Starter also has a built in air compressor for inflating flat
tyres too. The 12V/24V MB-3756 is ideal for your car (uses 12V) and your boat
(uses 24V).
All the Jaycar range of Jump Starters are fitted with LED lighting (so you never
have to work in the dark), and handy 5V USB outlets to charge mobile phones
and other portable electronics devices.
Put a Jaycar Jump Starter in your glove box or the boot of your car or van, and
you will never have to worry about a flat car battery again.
FITS IN THE GLOVEBOX!
MB-3760
MB-3757
MB-3758
MB-3736
MB-3756
VOLTAGE
12V
12V
12V
12V
12/24V
24V
CRANKING
CURRENT
270A
300A
350A
400A
400/300A
400A
LiFePO4
Li-Po
Li-Po
SLA
Li-Ion
Li-Po
BATTERY
TYPE
FEATURES
• LED Light
• USB Out
• LED Light
• USB Out
• LED Light
• USB Out
• LED Light
• LED Light
• USB Out
• USB Out
• Air
Compressor
MB-3752
• LED Light
• USB Out
• 19V Laptop
Supply
FITS IN THE GLOVEBOX!
179
$
$
279
189
$
12V 300A LI-PO
12V 350A LI-PO
MB-3757
Will crank an engine up to a 5L petrol, or 3L diesel.
• 300A continuous, 450A peak jump starting
• 2 x USB ports
• LED light
• 66(W) x 142(D) x 30(H)mm
MB-3758
Will crank an engine up to 7L petrol or 4L diesel.
• 350A continuous, 700A peak jump starting
• 2 x USB ports
• LED light
• 85(W) x 216(D) x 36(H)mm
12V 400A SLA
WITH AIR COMPRESSOR MB-3736
Will crank an engine up to 6L petrol or 3L diesel.
• 400A continuous, 1100A peak jump starting
• 2 x USB ports
• LED light
• Built-in air compressor with tyre inflator
• 285(L) x 227(W) x 310(H)mm
FITS IN THE
GLOVEBOX!
119
$
$
12V 270A LIFEPO4
WITH BATT & ALTERNATOR TEST MB-3760
Equipped with a LiFePO4 battery, making it compact &
lightweight but still powerful.
• 270A continuous, 400A peak jump starting
• 2 x USB ports
• LED light
• Reverse polarity and short circuit protection
• 185(L) x 100(D) x 50(H)mm
FROM
3 pr
$ 50
CAR BATTERY CLIPS
Colour coded handles. Sold as a pair.
15A 55MM LONG HM-3010 $3.50
30A 70MM LONG HM-3012 $3.95
50A 98MM LONG HM-3015 $5.50
200A 35MM LONG HM-3060 $9.95
400A 155MM LONG HM-3085 $15.95
NOW
139
$
349
SAVE $20
12/24V 400A/300A LI-ION
24V 400A LI-PO
MB-3756
Suitable for most 12V or 24V vehicles including bus,
trucks, jet ski etc.
• 400A/300A continuous, 800A/600A peak jump starting
• USB port
• LED light
• Carry case included
• 240(W) x 210(H) x 58(D)mm
MB-3752 WAS $159
Will start a Large cruiser boat.
• 400A continuous, 800A peak jump starting
• USB port
• LED light
• 190(L) x 150(H) x 90(W)mm
12 95
$
80A 6 GAUGE TWIN CORE
POWER CABLE WH-3067
For high current applications.
Red & black. PVC installation.
To order phone 1800 022 888 or visit www.jaycar.com.au
$
FROM
34 95
$
FROM
74 95
JUMPER LEADS WITH LEDS
24VDC TO 12VDC CONVERTERS
Heavy duty pair of battery clamps with LED
lights. Surge protected.
400A 3.0M LONG WH-6012 $34.95
700A 4.5M LONG WH-6014 $69.95
Useful for running 12V devices from a 24V
supply in a truck or bus. These converters
have switchmode tecnology for light
weight and compact design.
10A MP-3061 $74.95
20A MP-3063 $119
See terms & conditions on page 8.
Page 53
WORKBENCH
ESSENTIALS
$
24 95
$
1
NOW
29 95
There has been an obvious resurgence in people getting back to the workbench and
reviving skills involving manual dexterity. As you will see across the following pages,
Jaycar has all the DIY tools you'll need to equip your workbench so you can create
projects from the power of your brain and your hands.
5
$
NOW
59 95
SAVE $5
SAVE $10
6
2
$
79 95
4
3
$
NOW
69 95
14 95
$
SAVE $10
NON-CONTACT
THERMOMETER
WITH DUAL LASER
TARGETING
$
QM-7221
Measure temperature from a
safe distance.
• Laser pointing targeting
• Wide temperature range
• 12:1 distance to spot ratio
• 140(L) x90(W)x43(H)mm
2. AUTOMOTIVE DMM QM-1444
• CatIII 600V, 4000 count
• Inductive pickup for RPM measurement
• Dwell angle, duty cycle
• Data hold & relative function
• 146(H) x 66(W) x 42(D)mm
139
5. AUTOMOTIVE MULTI-FUNCTION
CIRCUIT TESTER QM-1494 WAS $64.95
• Designed to test the electrical system of an
automotive vehicle running on 12V or 24V
• Backlit LCD
• 240(L) x 78(H) x 40(W)mm
3. DIGITAL TACHOMETER
QM-1448 WAS $79.95
• Measures up to 99,999 RPM
• Large LCD display, laser pointer, low
battery indicator, memory recall etc.
• 5 Digit LCD display
• Supplied with carry case
• 72(W) x 160(H) x 37(D)mm
FROM
24 95
SELF-POWERED LED PANEL METERS
$
4. AUTOMOTIVE CRIMP TOOL WITH
CONNECTORS TH-1848
• Excellent tool comes with 80 of the most
popular automotive connectors
• Male & female bullets & spades
• Eye connectors
• Butt joiners
1. STORAGE CASE HB-6302
• 4 trays: 233 x 122 x 32mm
• 13 compartments
• Top tray has a generous
265 x 160 x 65mm space
• 270(W) x 260(H) x 150(D)mm
Simple 2 wire connection for voltage readout. Auto zero
calibration and easy to read red LED display. Automatic
polarity sensing. Cutout size 42 x 23mm.
VOLTMETER 8-30VDC QP-5586 $24.95
AMMETER 0-50ADC QP-5588 $39.95
$
6. BENCH VICE TH-1766 WAS $39.95
• Made from hard-wearing diecast aluminium
• Vacuum base and ball joint clamp
• 75mm opening jaw
• 160mm tall (approx)
29 95
HEAVY DUTY STRIPPER,
CUTTER & CRIMPER TH-1827
Strip all types of cable from AWG 10-24 gauge
(0.13-6.0mm).
TYRE PRESSURE TESTER
QP-2287
Keep your tyre pressure in check.
• Measurement range: 5-100psi
• Large LCD readout
• LED light
• Tyre deflation monitoring
$
29 95
16 95
$
19 95
$
12 PIECE
CAR AUDIO TOOL KIT TH-2339
Avoid leaving scars on your cars. This
ABS pry tool kit is extremely useful for
safely removing and installing car audio.
FROM
13 95
$
$
39 95
300PC QC CRIMP CONNECTOR PACK
PT-4536
Contains bullet, ring, fork, spade and joiners in various sizes
and colours.
$
44 95
CORDLESS VOLTAGE TESTER
VERNIER CALIPERS
USB INSPECTION CAMERA
QP-2212
Quick and easy way to locate electrical faults without a
bulky meter. Works on 3-28V circuits.
• Chrome metal construction
• Probe supplied
Calipers with LCD and etched vernier scale. 150mm range.
BUDGET
TD-2081 $13.95
PROFESSIONAL. STAINLESS STEEL TD-2082 $39.95
QC-3373
Inspect or locate objects in hard to reach places.
• Water resistant camera
• Adjustable LED lighting
• 1.5m flexible cable
Page 54
Follow us at facebook.com/jaycarelectronics
Catalogue Sale 24 February - 23 March, 2018
EXCLUSIVE
CLUB OFFERS:
50% OFF
50% OFF
CIRCUIT
F
F
O
50%BREAKERSCI* RCUIT
FOR NERD PERKS CLUB MEMBERS
WE HAVE SPECIAL OFFERS EVERY MONTH.
LOOK OUT FOR THESE TICKETS IN-STORE!
- BLADE FUSE
BREAKERS*
IT *- BLAD
CIRCUSIZE
E FUSE
RS
AKE
BRE
SIZE
EXCLUSIVE
SE
FU
DEOFFER
CLUB
- BLA
EXCLUSIVE
SIZE CL
UB
NOT A MEMBER? Visit www.jaycar.com.au/nerdperks
NERD PERKS CLUB OFFER
OFFER
NERD PERKS CLUB
OFFER
NOT A MEMBER?
Sign up NOW! It’s free to join.
E
EXCLUSIV
CLUB OFFER
FREE
BUY 1 GET 2ND AT
HALF PRICE
NOT
A MEMValid 24/7/17 to 23/8/17
Sign up NOW BER?
! It’s free to
join.
AA-2047
BER?
NOT A MEM! It’s free to join.
Valid 24/7/17 to
23/8/17
Sign up NOW
Valid 24/7/17 to
23/8/17
WIRELESS HEADPHONES*
NERD PERKS CLUB OFFER
2 FOR $348
SAVE
SAVE
25%
$
ONLY
KEVLAR SPEAKERS 4"-6.5"
$
Need two of the same speakers? Buy one, and grab a
second speaker for half price.
e.g. CS-2400 Buy 1 for $79.95, get the second for $39.97 =
$119.93 (Normally $159.90, Save $39.97)
119
6.5" 6300 LUMEN
LED DRIVING LIGHTS
7" TFT LCD COLOUR MONITOR QM-3752
4" CS-2400 $79.95 EA
5" CS-2401 $99.95 EA
6.5" CS-2402 $119 EA
50
Suitable for in-car entertainment.
*AA-2047 valued at $39.95, valid with purchase of QM-3752.
Combo (spot/flood) or spot
available.
COMBO SL-3920
SPOT SL-3921
RRP $199
NERD PERKS
NERD PERKS
NERD PERKS
NERD PERKS
HALF
PRICE!
SAVE
HALF
PRICE!
SAVE
20%
6.5"
30%
JEWELLER'S SCREWDRIVER SET TO-220 TRANSISTOR CLAMP
CONTACT CLEANER
DIGITAL DC POWER METER
TD-2023 REG $9.95 CLUB $4.95
Set of six, housed in a handy storage case.
NA-1012 REG $11.50 CLUB $5.75
175g spray can.
MS-6170 ORRP $69.95 CLUB $46.95
With internal shunt. 5-60VDC.
HH-8602 REG $24.95 CLUB $19.95
Pack of 100.
NERD PERKS
NERD PERKS
NERD PERKS
SAVE
HALF
PRICE!
SAVE
25%
50A CHASSIS MOUNT
ANDERSON ADAPTOR
TD-2055 REG $11.95 CLUB $5.95
Capacitor, diode, transisto checks.
PORTABLE POWER BANK
MB-3723 ORRP $64.95 CLUB $44.95
Solar. 4000mAh.
YG-2738 REG $43.95 CLUB $34.95
50kgs torque at 55RPM.
NERD PERKS
NERD PERKS
SAVE
SAVE
SAVE
15%
30%
12V REVERSIBLE GEARHEAD
MOTOR
NERD PERKS
20%
SAVE
20%
SMART TEST SCREWDRIVER
PT-4460 REG $19.95 CLUB $14.95
Black. Heavy duty.
NERD PERKS
NERD PERKS
SAVE
20%
20%
METAL ENCLOSURE
USB 3.0 4 PORT MINI HUB
6-WAY AUTOMOTIVE FUSE BOX
HB-5442 REG $14.95 CLUB $11.95
150(D) x 61(H) x 102(W)mm. Supplied with
rubber feet.
XC-4952 REG $29.95 CLUB $24.95
Up to 80Mbps transfer rate.
SZ-2002 REG $12.95 CLUB $9.95
32VDC, 15A. 6.3mm QC terminal.
NERD PERKS CLUB MEMBERS RECEIVE:
50%
OFF
CIRCUIT BREAKERS - BLADE FUSE SIZE
*
WITH NETWORK/POE TESTER
TH-1939 REG $69.95 CLUB $54.95
Includes PoE (Power-over-Ethernet) finder.
YOUR CLUB, YOUR PERKS:
REMEMBER TO GET YOUR CARD SCANNED AT
THE COUNTER TO GET POINTS*.
$1 = 1 POINT,
500 POINTS = $25 JAYCOINS GIFT CARD
*Only includes Mini & Standard Blade Circuit Breakers (Manual & Automatic Reset types)
To order phone 1800 022 888 or visit www.jaycar.com.au
MODULAR CRIMP TOOL
See terms & conditions on page 8.
Conditions apply. See website for T&Cs
*
Page 55
WHAT'S NEW
WE'VE HAND PICKED JUST SOME OF OUR LATEST NEW PRODUCTS. ENJOY!
Receiver
$
449
$
Sender
HDMI POWERLINE SENDER & RECEIVER
AR-1903
Watch TV 2 separate rooms! Transmits HDMI signal over your home power wiring up to
300m. Send to a 2nd device in another room via IR signal.
• Supports up to 1080p
• Easy setup, plug and play
$
89 95
$
89 95
USB 3.0 TO DVI/VGA CONVERTER
Extract high quality audio in digital optical,
digital coaxial, or analogue stereo audio.
• Suitable up to 4k2k <at> 60Hz
• Supports: DTS HD, Dolby TrueHD
(via HDMI)
XC-4974
Connect multiple displays and extend
your screen for multi-media and video
conferencing.
• 1080P video streaming
• High definition image
$
59 95
$
3 CHANNEL DJ MIXER AM-4207
39 95
YN-8416
Channel ethernet and power down the same
network cable.
• Input Voltage: 44-57VDC
• Output Voltage: 5VDC
• Network Speed: 10/100Mbps
49 95
MOTION ACTIVATED LED BED
LIGHT ZD-0588
Automatically create a soft glowing light
under your bed. 240 lumens.
• PIR 3m sensing distance
• Self-adhesive, mains powered
Optimise sound waves and prevent losses.
• Foam
• 3M adhesive backing
• Outer ring and inner circle
$
69 95
VISOR MOUNT BLUETOOTH
HANDSFREE KIT AR-3138
Make and receive mobile phone calls
whilst driving.
• Rechargeable battery
• Digital power amplifier
• Connect two phones simultaneously
$
FROM
69 95
CHANGEOVER SOLENOIDS
High-grade industry standard solenoid.
Typically used to operate a winch or a starter
motor.
SINGLE POLE SY-4200 $69.95
DOUBLE POLE SY-4202 $79.95
ARDUINO® COMPATIBLE BOARDS
$
SOUND RING - SPEAKER SINGLE
DOOR KIT AX-3667
• Headphone Socket
• Coloured LED Output Display
• RCA Input Sockets
• Photo / Line and CD Inputs
• 2 x Stereo Line Outputs
5V MICRO USB POE SPLITTER
$
HDMI AUDIO EXTRACTOR AC-1739
29 95
39 95
ESP32 MAIN BOARD
WITH WIFI AND BLUETOOTH®
XC-3800
A powerful dual core microcontroller
featuring WiFi and Bluetooth.
• 3.3V operating and IO voltage
$
24 95
WI-FI MINI MAIN BOARD
XC-3802
Incorporates 80MHz microcontroller
with Wi-Fi into a board. Perfect compact
solution to your IoT sensor node problem.
ld’s
QUEEN ST
AB
ELIZ
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na
cDo
ETH
ST
RRY
THE
ST
TERMS AND CONDITIONS: REWARDS / NERD PERKS CARD HOLDERS FREE GIFT, % SAVING DEALS, DOUBLE POINTS & MEMBERS OFFERS requires ACTIVE Jaycar Rewards / Nerd Perks Card membership at time of purchase. Refer to website for Rewards/Nerd Perks
Card T&Cs. PAGE 3: Nerd Perks Card holders receive special price of $79.95 for Arduino Round Gauge Project (1 x XC-4430 + 1 x XC-4282 + 1 x HM-3211 + 1 x RR-0596 + 1 x RR-0572) when purchased as bundle. PAGE 4: Radio & Antenna Deal includes 1 x DC-1122 &
1 x DC-3078 for only $299. PAGE 7: Nerd Perks Card Holders Buy 1 Kevlar Speakers & Get one at Half Price applies to CS-2400, CS-2401 & CS-2402. FREE Wireless Headphones (AA-2047) with purchased of QM-3752 7” TFT LCD Colour Monitor. 50% OFF Circuit Breakers
includes Mini & Standard Circuit Breakers, Manual & Auto Reset.
LIN
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FRA
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FOR YOUR NEAREST STORE &
OPENING HOURS:
1800 022 888
www.jaycar.com.au
96 STORES & OVER
140 STOCKISTS NATIONWIDE
NEW STORE: FRANKLIN
110 Franklin Street, VIC 3000
PH: (03) 9329 3961
Head Office
320 Victoria Road,
Rydalmere NSW 2116
Ph: (02) 8832 3100
Fax: (02) 8832 3169
Online Orders
www.jaycar.com.au
techstore<at>jaycar.com.au
Arrival dates of new products in this flyer were confirmed at the time of print but delays sometimes occur. Please ring your local store to check
stock details. Occasionally there are discontinued items advertised on a special / lower price in this promotional flyer that has limited to nil stock
in certain stores, including Jaycar Authorised Stockist. These stores may not have stock of these items and can not order or transfer stock.
Savings off Original RRP. Prices and special offers are valid from Catalogue Sale 24 February - 23 March, 2018.
PRODUCT SHOWCASE
Labjack T4 USB or Ethernet DAQ
Labjack have just released their new
low cost USB or Ethernet T4 DAQ
device for data logging, data acquisition, measurement and control applications.
The Labjack T4 comes with up to
12 analog inputs or 16 digital I/Os.
There are four dedicated high voltage
analog inputs (±10V, 12-bit resolution)
as well as up to eight configurable low
voltage analog inputs (0-2.5V, 12-bit
resolution).
It also has two analog outputs (10bit) and multiple digital counters/
timers.
Labjack’s Kipling software is available for basic configuration and testing. The LabJack T4 also comes
with free DaqFactory Express Windows software that allows you to
be quickly up and logging and graphing data.
Free code examples are available
in C/C++, C#, Delphi, Java, LabVIEW,
MATLAB, Python, VB.NET and more.
The T4 is also capable of stand-alone
operation by running Lua scripts and
supports Modbus TCP protocol for industrial applications
Contact:
Ocean Controls
PO Box 2191, Seaford BC, VIC 3198
Tel: (03) 9782 5882
Website: www.oceancontrols.com.au
Shatter-proof mobile phone screens a step closer
with ANU research
“Everyone knows how frustrating it is when you drop your
mobile device and get a large
crack in the screen,” said Dr Le
Losq from the ANU Research
School of Earth Sciences.
New research at the ANU
could lead to shatter-proof glass
for mobile phone screens.
The researchers worked on a type
of glass called alumino-silicate.They
built on the long-standing collaborations from laboratories around the
world.
Dr Le Losq said that the research,
based on experiments and computer
modelling, could be used to alter the
structure of glass to improve resistance to fractures.
Contact:
ANU Research School Earth Sciences
Tel: (02) 6125 2381
email: charles.lelosq<at>anu.edu.au
Altronics auto rescue kit: save $30 in March
We’ve all seen those emergency jump starting kits. And
mini air compressors to get
you out of trouble. Now Altronics combines both with
this nifty emergency pack!
It features a 16800mAh
battery bank plus emergency compressor to top up
tyres, provides 600A peak
siliconchip.com.au
cranking output for cars with flat
batteries,12/16/19V and USB output
provided for powering devices.
Cat No is M-8198; special price in
March is $139.00 - $30 off normal.
Contact:
Altronics Distributors (all stores)
Tel: (1300) 797 007
Website: www.altronics.com.au
Celebrating 30 Years
Electrolube’s new
optically clear, flame
retardant resin
Electrolube has launched a new
encapsulation resin to meet the increasing demands from LED manufacturers for an optically clear, flame
retardant resin.
The optically clear polyurethane
resin, UR5641 is believed to be a
market-first solution.
The two-part, semi-rigid resin
cures to provide a flexible, protective and aesthetically pleasing covering over the luminaire elements
and the aliphatic chemical nature of
the cured resin is naturally resistant
to the yellowing effects of UV light.
This makes it useful for a range
of outdoor as well as indoor applications. UR5641 is also scratch resistant and offers high resistance
to weather, acids and alkalis, water
and mould growth.
UR5641 has a wide operating temperature of -40 to +120 °C
and thermal conductivity of 0.20
W/m.K.
Importantly, UR5641 is flameretardant and UL94 V-0 approved,
making it eminently suitable for the
protection of LED luminaires exposed to hazardous atmospheres,
such as emergency lighting, or
lighting intended for installation in
ATEX rated/zoned environments.
Contact:
HK Wentworth
3/98 Old Pittwater Road, Brookvale NSW 2100
Tel: (02) 9938 1566
Website: www.electrolube.com.au
March 2018 57
SERVICEMAN'S LOG
Squeezing an elephant through the eye of a needle
Dave Thompson*
A while back, I penned a column about some fun I had with some
LED lamps in our range hood; in the editing process, this became a
kind of electronics "whodunit" (a wotdunit?) and it appears some
readers enjoyed the challenge.
The main thrust of that article was
what an idiot I’d been for disassembling the whole thing only to discover the cause was a couple of easily-replaceable blown LEDs. Because
my incompetence apparently knows
no bounds, I have another potential
head-scratcher for those interested in
another challenge.
Sixteen months ago, when we
moved to this house, we left behind
a 100 megabit per second cable internet connection and inherited a slow,
telephone wire-based ADSL pipe instead. This wouldn’t do, so one the
first things I did before we moved in
was to get hold of our ISP and see what
we could do about sprucing things up
a bit internet-wise.
Like many customers, we weren’t
with this ISP by choice. Our original
provider, a small start-up running out
of Auckland was bought out by a bigger local player. They, in turn, were
devoured by an even larger corporation from Australia.
This, as it turned out, was no bad
thing, as this telco brought cablebased internet and related services to
Christchurch and some other centres.
Whether any given street or road
58
Silicon Chip
had the cable ring installed was determined by teams of marketing people literally walking all over the city
and signing people up. If two people
in any given street signed on for the
new cable service, the cable was buried into that street.
Early-adopters like us enjoyed blazingly-fast (for that time) 100Mb/s connections until the ISP did what they
all eventually do and oversold the
system.
It was inevitable, as the likes of VoIP,
internet TV and other web-based services gained popularity, that overall
speeds declined. Eventually, there
was little advantage of this cable connection over the ADSL, ADSL2 and
VDSL technologies that were developing alongside it.
And then this ISP was gobbled up by
an even larger global company, whose
name always reminds me of that Star
Wars character, Yoda. So through no
choice of our own, they are now our
service provider.
The main difference I’ve noticed is
that when I called the smaller ISPs,
I got through to a competent tech
straight away and had problems sorted
within minutes.
Celebrating 30 Years
Then, as the companies got bigger,
support call waiting times got longer
and operators harder to cope with.
I hate advising my clients that they
have to call their ISP when internet
problems arise because the experience
is typically an exercise in frustration.
During our last move, I wanted to
switch over to the then-brand-new fibre-optic internet that was available at
our new home. But my alarm-monitoring company was reliant on the phone
system (as so many are), and the ISP
was adamant that we couldn’t keep our
copper phone lines if we wanted the
fibre-optic internet connection.
That would mean we’d have to scupper alarm monitoring, which was a
deal-breaker for me. I didn’t want VoIP
anyway, and besides, the ISP sold a
so-called "naked" broadband fibre
package right there on their website,
which meant internet-only, yet when
I suggested this option, I was told it
wasn’t possible and that the two systems could not be used side-by-side
and that was that!
What transpired was a lot of wasted time on the phone to their support staff, who all claimed that it was
standard practice that if a technician
siliconchip.com.au
Items Covered This Month
•
•
•
•
Network woes
FM car radio installation
Dab Jetinox pump controller
repair
Chef Heritage oven repair
*Dave Thompson runs PC Anytime
in Christchurch, NZ.
Website: www.pcanytime.co.nz
Email: dave<at>pcanytime.co.nz
came to connect the fibre, he would
remove the copper connections at the
same time. I tried to tell them these
two installations were separate, but
they wouldn’t hear of it.
I had to really dig my toes in and
fight my way up the chain until I finally found someone who would sign
us up for fibre and allow us to keep
the copper wire. This took at least half
a dozen very long and often fraught
phone conversations, just to order a
fibre connection!
When the contracted tech finally
came around to physically install the
fibre, he couldn’t understand why
head office would be telling customers that the two systems couldn’t live
together.
He had no mandate to disconnect
copper lines and said that like me,
many others retained their old lines
for legacy systems or simply to keep
a separate, non-internet dependent
phone line. Honestly, it shouldn’t be
this difficult!
Interestingly, when all this happened, they mentioned that this would
be a 200Mb/s connection. However,
when we moved in and I connected
everything up, we would barely break
siliconchip.com.au
95Mb/s on the usual speed-test sites.
By this time, I was totally done talking to these guys, and since we had
essentially what we’d had at our old
address speed-wise, I didn’t worry too
much about it.
Confessions of a
bandwidth junkie
Fast forward to December 5th this
year. I saw an ad in one of our ISP’s
shopping-mall stores for a new connection plan called FibreX and this
promised speeds of up to one gigabit
per second, a truly marvellous prospect for those of us who consider
100Mb/s “barely adequate”.
They boldly promised three months’
credit if they couldn’t connect us up
in three days, so it sounded too good
to be true.
Obviously, there was small print,
which claimed the offer was only good
for qualifying addresses; apparently
FibreX was not available all over town,
so when I got home, I hit their FibreX
website and entered my address; the
result trumpeted that we could get the
service, so I put my prejudices aside
and got on the phone.
The person at the other end assured
me that we were all set, but they’d need
to send me a new modem to replace
our existing one, which was over a year
old and so obviously now redundant.
Fine by me, and so with a rosy feeling of accomplishment, I sat back and
waited, anticipating how wonderful a
one-gigabit connection must be.
A few days later, the modem arrived.
However, as soon as I unpacked it, I
saw a problem. It was a cable modem,
designed for the same, older-style cable connection we’d had at our old
address.
I promptly called the ISP and after
the usual 30-minute wait told them I
Celebrating 30 Years
thought they’d sent the wrong modem.
They assured me that was the right
modem and that within a few days a
technician would be out to put in the
cable and away we would go.
By now mightily confused, I asked
why a technician would have to come
out when we already had a fibre connection and all that is required is a
push-button speed increase at the ISP
or exchange.
I was somewhat hampered by not
knowing how these systems work
beyond the connection to the house,
but I assumed there was nothing required here for this speed increase
to happen.
They insisted that a new cable had
to be installed for the system to work
and when I started asking questions,
they kept bumping me around different departments until finally, after
about two hours, I talked to someone
who cottoned on that what had happened was that the person I talked to
originally didn’t double-check that we
could actually get FibreX here, even
though the system seemed to think
we could.
We couldn’t; FibreX is simply a
hardware/speed upgrade to the old
cable internet system, and it is still
only available to customers in those
streets it originally was installed in,
and we didn’t have it here. Excellent!
What a complete waste of time; and I
let them know in no uncertain terms
what I thought about them and their
“support”.
To placate me, this operator told me
about a super new product they were
now implementing called FibreMax.
This used our existing fibre connection
and could also give us gigabit speeds,
and that quietly this was even faster
and cheaper than the FibreX system!
Somewhat mollified, I signed up on
March 2018 59
the spot, with the operator claiming it
would all go through on the nod within
three days. All I had to do was wait.
Hurry up and wait
And so I waited; after a week of nothing happening speed-test-wise, I called
them back (and by this time I was really disliking having to call them).
And once again, I had to start at the
beginning and tell my story and then
ask what was happening. Ah, the operator said, by the looks of it I was getting FibreX installed, and she could
see the technician was due to come
out and install it in a few days, so I’d
just have to wait until then.
I couldn’t believe what I was hearing. I very politely informed this person that I wasn’t getting FibreX, I was
supposed to be getting FibreMax, and
that no technician was required.
This phone jockey didn’t even know
what FibreMax was, and after putting
me on hold multiple times, she finally
came back and transferred me to someone else, who again wanted the whole
story and put me on hold for ages before returning to tell me there’d been
a muck up in the provisioning, but
now it was all sorted and it would be
on within 24 hours.
It was also at this time I learned we
were supposedly already enjoying a
200 megabit connection, as originally
installed, so perhaps there was something wrong with our setup somewhere.
My modem was more than capable
of these speeds and all my routers,
switches and network cards are gigabit
types so I just couldn’t understand it.
My contact made some notes and
suggested they’d sort the speed change
first, then we’d see if there was something else holding our speed back. This
sounded reasonable, so I left it at that
and went back to waiting.
60
Silicon Chip
The following afternoon, I did another speed test and noticed that while
our download speed hadn’t changed,
our upload speed had doubled to just
under 90Mb/s, so something had definitely happened.
Still, our download speed stayed
stubbornly shy of 100Mb/s and this
whole thing was really starting to rot
my togs.
Once more, I stepped into the breach
and called the ISP. Another long hold
later I was told I’d have to call the contracted telecommunications people
who partnered with the ISP to provide
this gigabit product.
My arguments about why I had to do
this when I was paying them for this
service fell on deaf ears, so all I could
do was phone this other company.
At least the help desk technician
who answered the phone after two
rings knew his oats. While looking
through the files, he could see two different orders had been put in for our
address and the cancellation of FibreX
and connection of FibreMax was causing all sorts of provisioning problems.
People were just pushing it back
and forward to each company without actually doing anything. Unless I
called, nothing would be done at all.
Outstanding!
We were now about a week before Xmas and still, the speed test remained under 100Mb/s. Calls to the
ISP and the contractor confirmed that
everything was all-go at their respective ends, but nothing had happened
here. They couldn’t explain it. I tried
another, different modem to no avail.
So, dear reader, have you solved the
diabolical mystery of who killed my
bandwidth? Because at this stage, I
still hadn’t.
On the last workday before Christmas, I tried calling again. After yet
Celebrating 30 Years
more buck-passing from the ISP and
assurances from the contractor that
all was OK, I accepted that I’d have
to leave it until after Christmas. And
when I sat down and thought about it,
there are people really struggling out
there, or even having no Christmas at
all, and here I am whining about not
having faster Internet.
It’s such a first-world problem and
that really put things into perspective for me.
After Christmas, we braved one of
the local malls and stopped in at another corner kiosk, figuring that we
could at least talk to someone who had
access to all the records. At this stage,
all the guy we talked to could do was
apologise for the events preceding all
this. He also arranged to have their
technical support guys call us back,
the first time anyone had actually offered to do this.
We accepted that the Wednesday
after New Year’s Day was likely the
earliest time they could help us and
left it at that. However, shortly after
returning home, I got a call from the
help desk to see if we could do something about it now. I was fine with that
(it must have been a slow day on the
help desk!) and sat down at my computer to assist him with setting up the
remote login he’d use to have a look
at our network.
After a few minutes, I could see him
driving the computer and as we chatted on the phone, he looked at some
of the settings and status information
on the modem, pulling up a hidden
screen that I’d not encountered on my
travels through it. This page gave all
the technical statistics of the network
connections, protocols, packets and
speeds up and down the pipe.
And within just a few minutes,
"samurai" Josh, no doubt wielding his
razor-sharp troubleshooting katana,
had pinpointed the cause of our problems, leaving me very embarrassed and
choking on a huge slice of humble pie.
You probably guessed the issue long
ago; I didn’t, and I call myself a tech. It
turns out the “enhanced” Cat5e cables
I’d used throughout the office when
I set it up several years ago weren’t
that enhanced after all, and the routers were sensing this and throttling
our local network speeds to 100Mb/s!
I simply had to change all the cables – those between the incoming fibre terminal and the new modem, and
the computers and a couple of gigabit
siliconchip.com.au
switches through to the modem itself
– to proper Cat6 cables, which in theory, would allow us to upgrade to 10
gigabits in future (when one gigabit
becomes barely adequate...).
But for now, this has opened the
floodgates and now our speed test has
a much healthier 800Mb/s average.
The devil is in the details, and while
they might have messed things up,
I did too. Who would have thought
a few measly cables would prove so
troublesome…
Speaking from up high
F. W., of Moonee Valley, Vic, an
experienced technician, recently set
about installing a replacement radio in
his grandson’s new (second-hand) car,
only to be stymied not once but twice.
Here is how it went down...
My 18-year-old grandson just got
his first car, a 2000 VT Holden Commodore, from a friend of the family.
When he got it, the radio was missing,
with a hole in the dashboard. Apparently, the original radio stopped working and was removed.
His mother bought him a new Pioneer radio and fitting it is where his
father and I came in. I am a retired licensed aircraft engineer and car enthusiast and as my grandson has limited resources (ie, little money), the
job was left to me.
I have fitted a lot of radios into cars
and caravans over many years including the more modern ones with remotes, USB inputs and Bluetooth and
have never had any problems. One
thing I have found over the years is the
difference between licensed aircraft
engineers and some keen amateurs is
that aircraft engineers work to a better
standard. Anyway, I digress.
As the old radio had been removed
and disposed of "because it didn't
work" we were starting from an unknown base. First thing I figured out
was that the original radio car loom
plug had been cut off and a plug from
some other radio had been "attached".
I put attached in quotes because the
plug had been connected to the car
loom using the best wire twisting techniques known to man and covered in
some cases with insulation tape. So I
decided to obtain an original VT Commodore radio loom plug and re-wire
it properly to the car loom.
In the old days, one identified the
12V, earth and speaker wires on the car
and joined the new radio wiring loom
siliconchip.com.au
to the car wiring loom, all of which
took about 30 minutes. A permanent
power supply was not required for earlier radios as they had no computers
or memory to keep alive. A soldering
iron, solder and some heat shrink tubing were the only tools required.
Then some smart people at a company
called Aeropro decided to make things
a bit easier by making adaptor looms
and plugs to go between the vehicle
wiring loom and the new radio. This
speeds up the process dramatically
and it only takes about 30 seconds.
I have installed several radios using
Aeropro looms without any problems,
so I decided to take the same approach
this time. With the Aeropro looms fitted, I attached the aerial connector and
we turned the ignition on.
In contrast to the radios of my youth
which would immediately spring
into life, the new ones have to be programmed first by carefully following
the installation instructions in the
book. Luckily, these steps are fairly
straightforward.
The radio display started in a demo
mode and then we completed the programming procedure. We selected a
strong FM station and turned the volume up, but we were met with stony
silence.
I removed the plug from the back
of the radio and performed a series of
checks which confirmed the following:
• we had 12V DC, both the switched
(accessory) and permanent supplies.
• we had earth continuity to the car
frame
• all speakers appeared OK, except
for the passenger side front door
speaker
• the antenna connection had continuity and no short to earth
• all the Aeropro leads had good continuity and the pins and sockets
were all in good condition
I then hooked up all the plugs and
looms and did a wiggle test with power on but still no sound, not even a bit
of static.
As one speaker appeared to be faulty,
we removed the interior panel (door
card) to access the driver. We found
the terminal block on the speaker
(where the car wiring plug connects)
had broken away from its mount and
was literally floating around on the
speaker cone wires.
As a consequence, it was most likely
that the speaker cone wires were
touching, causing a short circuit, or
possibly they had dislodged from under the goop on the cone. The easiest
solution was to get another speaker
from the local wrecker’s yard, which
we duly did. We confirmed it operated
on the bench and installed it.
We then re-installed the radio, programmed it and selected the same
strong FM station but were once again
greeted with more stony silence. As
my grandson had to get to football and
basketball practice, we called it a day.
The next morning, a web search confirmed that modern radios will typically refuse to work if there is a problem with any of the speakers, as they
go into a protection mode. I assume
this is intended to prevent damage to
the amplifier section.
We had replaced the suspect speaker
Servicing Stories Wanted
Do you have any good servicing stories that you would like to share in The Serviceman
column? If so, why not send those stories in to us?
We pay for all contributions published but please note that your material must
be original. Send your contribution by email to: editor<at>siliconchip.com.au
Please be sure to include your full name and address details.
Celebrating 30 Years
March 2018 61
so I didn’t know what else could be
wrong.
Then it hit me; I had not re-checked
the speaker and wiring continuity after replacing the faulty driver. I once
again checked all the speaker connections and once again, found a fault in
the passenger-side front door speaker.
That meant there must have been two
problems in the same circuit!
Investigation showed a broken wire
in the door opening. I repaired it and
the radio then sprang into life. By
the way, my grandson’s football team
won the Premiership, and he came
runners-up in basketball, so we had
wins all-round.
Pump controller repair story.
B. D., of Mount Hunter, NSW, had a
problem with an irrigation pump controller that burnt out during use. The
service agent was too busy to fix it but
he had a go and managed to do it himself. His story is as follows...
I have a Dab Jetinox automatic pump
which I use for irrigation on my small
acreage. After a recent watering episode, I noticed that the pump had
stopped after running for a couple
of hours. On closer inspection, I saw
that the pump warning light had come
on and that pressing the reset button
would not restart the pump.
I called the local agent and spoke
to a technician who said that it was
most likely a fault in the controller.
The options were to replace the complete controller for around $200 or bypass it altogether and just operate the
pump with the mains power switch
for about $60 labour. The latter option
would be OK as I was using it in that
manner anyway.
These pumps have a pressure switch
which stops the pump when the taps
are turned off and a flow meter which
stops the pump if it can't draw any
liquid. I have the pump connected to
quite an extensive PVC pipe network
which won't hold pressure and causes the pump to cycle on and off fairly
regularly if left on, so I switch it off
unless I’m watering.
It is also unlikely to run dry as the
suction line siphons from a dam. The
controller also has some other functions to do with slow flows to reduce
the amount of cycling. But I can get
away without the controller, so next
day I took it back to the agent to let
him fix it.
I spoke to a sales assistant, as the
62
Silicon Chip
technician was out in the field, and his
response was less than enthusiastic.
He told me that they were snowed
under because of all the dry weather
we were having and they couldn't look
at for a week or so. Well, I thought I
may as well have a look at it myself
as bypassing the controller should be
pretty straightforward.
I took it home to my workshop. I
thought I would just power it on before
I start dismantling. To my surprise,
the pump turned over. I quickly reconnected the water supply and tried
again. Under load, the pump started,
accompanied by fireworks from the
controller and then it went dead.
I then started work on the controller which required me to use my set
of special screwdriver bits to remove
the cover. I noticed a circuit board covered in black soot, as well as a large
capacitor and motor terminal. I photographed the board and made a sketch
of the wiring connections.
I soon realised that the wires marked
“nero” (black in Italian) and “maroon”
(brown) were connected to the main
relay and were the power wires for the
pump. I disconnected these from the
board and joined them together after
insulating the join. I tried the pump
and it ran without any problems and
I used it to do a couple of hours of
watering.
Since I had removed the circuit
board from the controller, I thought
I would have a look at it anyway. It
consisted of a 240V relay which powers the pump, inputs for the pressure
switch (“pressostato”) and flow meter
(“flussostato”) and a logic chip controller. The relay coil is switched by 24V
DC which is produced on the board.
I cleaned up the board and I could
see on the underside that one of the
240V pins of the relay was surrounded
by air as the solder had gone. I then
The circuit board from the controller
after it had been cleaned.
Celebrating 30 Years
removed the relay and saw the entire
track on the top side of the board from
this terminal to the spade connector
had completely burnt away. It also took
a 100kW resistor with it.
This pump draws about 8A and this
current was being carried by a top and
bottom track about 1cm wide. Not surprising it failed eventually. I replaced
the resistor and re-soldered the relay,
this time including some reasonable
size wires from the relay terminals
to the spade lugs in parallel with the
board tracks.
After re-fitting the repaired board to
the controller, I tried the pump and it
ran and cycled off and worked satisfactorily. Although I could have used
it without the controller, I am glad
it is fully operational as it could be
used as a spare domestic water supply if required.
I am also glad that I didn't replace
the controller as more than likely the
replacement would have the same
problem.
Not so hot by the seaside
B. C., of Dungog, NSW, recently
did battle with a top-of-the-line oven,
which contained not just one but two
different faults just waiting to spoil
dinner. Of course, he wasn’t going to
allow that to happen. Here is how he
fixed it...
The day before an important family
get-together, my friend’s Chef Heritage
gas oven and range went into a “limp”
mode. Over the telephone, she said
that this had happened before.
Usually, it would fix itself, but now
she could not trust it anymore. As we
were due to arrive there later that day,
a request was made to bring my toolbox and soldering iron.
On arrival, I wasted no time and
started my assessment of the fault.
Fortunately, she still had the original
Chef user’s manual for the gas/electric range.
The original invoice was still enclosed, for $1178 plus $12 delivery
charge. It was the flagship model made
by Chef in 1984 and it had all the bells
and whistles.
In addition to the four-burner gas
hob and grill, there was also an electric party oven at the top and a fan
forced gas oven below. An electronic
clock/timer controlled both the grill
and oven, and electronic spark ignition was used to automatically light all
the gas burners. It stood at 1700 mm
siliconchip.com.au
high and was mostly made of enamelled steel.
An extra mechanism, in the centre
of a double power outlet, was used to
isolate the mains power for the gas
range. After turning the electricity
on, a buzzer made a series of beeps.
Then a few seconds later, the clock/
timer would stabilise and “HELP” was
shown on the display.
After rotating the manual/auto
switch to the set mode, I tried to use the
“display set” up/down pushbuttons to
set the current time. There was no response and the display was starting to
flicker. The buzzer was now randomly
beeping, no matter which position the
rotary switch was set to.
There was no spark ignition available when attempting to light the gas
oven or any of the hobs. The gas oven
fan would not run and the party oven
would not turn on.
However, the gas oven light was still
working! Using a handheld gas lighter,
it was still possible to light all the
gas burners. Well, at least that meant
that the gas part of the range was still
working.
I carefully manoeuvred the range
out from the gap where it had been
installed. The removal of a large sheet
metal cover then allowed access to the
wiring in the rear of the unit. All the
neutral wiring was blue and the active
wiring was orange, with the exception
of one red wire (that went to the party
oven thermostat).
I disconnected and removed the
clock/timer module from behind the
range and took it to a workbench in
the garage. The module case split into
two halves, revealing a couple of PCBs.
One was a power control/linear power
supply PCB and the other, a microprocessor/display PCB.
I started by testing the power supply electrolytic capacitors with an ESR
meter. They were all above specification, especially the 10µF/63V elec-
tro next to the 7805 voltage regulator. There were also 470µF/25V and
1000µF/63V electros near the rectifier
diodes. I replaced them all as a matter
of course. Any suspect solder joints
were resoldered.
I then turned my attention to the microprocessor/display PCB. There was
one PCB pad (near the 8MHz quartz
crystal) where only two of the three
trimmed pigtails had taken solder
properly. This joint was resoldered.
Both the rotary selector switches were
also spray cleaned with solvent.
I connected a suitable mains power
lead (terminated with insulated spade
terminals) to the A and N input terminals on the power supply board.
After initialisation, the display was
stable and the buzzer only beeped
briefly when changing modes. The
time could be set and the clock ran
correctly, even when switched back
to manual mode.
It was now time to reassemble and
re-fit this clock/timer module back into
the range. The brackets and screws
were refitted. All the leads were reconnected and the mains power switched
on. Every function appeared to be
working normally again, and the range
was left to soak test.
Then disaster struck! During the
evening meal preparation, the electric
party oven refused to work. Hastily, a
toaster oven was temporarily pressed
into service.
After the meal was finished, I
clocked on for the afternoon shift.
Upon examination, the clock/timer
appeared to be working in its various
modes but it was not controlling the
electric party oven.
There was no way of avoiding it;
the module would have to be taken
out again! On my way back out to the
shed, I pondered, were there still some
other dry solder joints?
Using a fluorescent desk lamp and
some magnifiers, I found nothing obvi-
ous. It was time to bench test the outputs. There were two relays that basically controlled the two ovens; when
the relay output (for the electric party
oven) was checked, with a 100W lamp
load, it did not light.
With the mains power turned off,
a multimeter showed no continuity
through the relay coil. As I re-soldered
the coil pins, one fell over at an angle.
When this relay was removed from
the PCB, only three of the four pins
were intact.
Under magnification, I could see
that the fourth pin had corroded away
close to where it entered the plastic
case.
Now, where was I going to find a
suitable relay at this time of the evening? It was a 12V DC SPST 10A type. I
went out to the courtyard (behind the
house), into the appliance graveyard.
There I found an early model Sharp
convection/microwave oven. After removing its top cover, I found an interface PCB inside with relays. This was
removed and taken back to the shed.
Amongst these, thankfully, there
was a suitable relay. With some modifications, it was fitted in place of
the original relay. Bench testing then
showed that the lamp would light
when this output was selected.
The clock/timer module was reassembled and taken back into the kitchen. The module was re-fitted back into
the range and it was with a great sense
of relief to find everything was back
to normal.
After prolonged soak testing and
with occasional on/off cycling of the
mains power, it continued to play
ball. Early the next morning, the sheet
metal back cover was re-fitted and the
Chef Heritage range was pushed back
into place.
Later it was put through a workout
as a baked dinner for six people was
prepared. It was the best baked dinner
SC
I had eaten for a long time!
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Celebrating 30 Years
March 2018 63
Want your own wireless station? Build this
We’ve designed this low-power AM Radio
Transmitter for the opposite ends of
the age spectrum! First, it’s every
kid’s dream to play disc jockey and
transmit programs around the
house or maybe even next door.
And the second, (mainly for our
older readers) to let you “listen
in” to the programs of your
choice on that vintage radio set
that you’ve lovingly restored.
AM Radio
Transmitter
By JIM ROWE &
NICHOLAS VINEN
W
hy would you want a broad- when you’re out driving – but the car
cast band AM transmitter radio lacks direct audio inputs. With
with a power output so low this little transmitter, that’s no problem.
In short, the whole idea of this prothat it can only be received within a
ject is to allow any line-level audio
radius of just a few metres?
Well, apart from wanting to keep it signal to modulate an RF carrier in the
all legal, let’s say you’ve just finished AM broadcast band so that it can be
building a replica of a classic 1940s’ played through a nearby conventional
era AM radio, which you’re entering a AM radio.
The carrier frequency of the transmitclub competition. Wouldn’t it be great
if you could tune it into an “authentic” ter can be tuned over most of the broadold time radio program, to recreate the cast band, ie, from 650kHz to about
way it might have sounded back then? 1500kHz. This allows you to choose
With this little transmitter, you’ll a frequency that’s away from any of
be able to do just that, by rebroadcast- the broadcasting stations operating in
ing historic radio programs like those your area, to ensure interference-free
reception.
available on CD from Screensound
Australia or even downloaded
from the internet (eg, www. Features & specifications
archive.com). Or you could
play some classic tunes that Transmission range: ~20cm (ferrite rod only),
~2-4m (with wire antenna)
you happen to have on CD or
Tuning
range:
650-1500kHz (typical)
in MP3 format.
Supply
voltage:
9-24V
Alternatively, you might
9mA <at> 12V DC
want to play the music from Operating current:
tuning, fine tuning, modulation
your personal MP3 or CD Adjustments:
depth
(volume), carrier balance
player through your car radio
64
Silicon Chip
Celebrating 30 Years
The audio quality from the transmitter’s signal is very close to that of the
program material you feed into it because it uses a special balanced modulator IC.
There’s also a modulation level control, so you can easily adjust the transmitter for the best balance between audio volume and minimum distortion.
But the best part is that the whole
transmitter uses just a handful of parts
and fits inside a standard UB3 sized
plastic jiffy box. It’s low in cost and
easy to build, as all the parts fit on a
small PCB. And there are no SMD components to worry about! You can run it
from a plugpack power supply or a 9 or
12V battery, so safety isn’t a problem,
even for beginners.
How it works
Although it’s designed for very low
output power, this transmitter uses
the same basic principles as a highpower AM radio transmitter.
Fig.1 shows the details. It consists
of an RF (radio frequency) oscillator,
siliconchip.com.au
a modulator and an RF output amplifier or “buffer”.
The RF oscillator generates a sinewave of constant amplitude, with a
frequency in the AM broadcast band.
This provides the transmitter’s RF carrier, which is the frequency you tune
your AM radio to.
In most full-size AM transmitters,
the RF oscillator uses a quartz crystal
and is fixed in frequency, so the station
concerned is always found at exactly
the same place on your radio’s tuning
dial. However, in this case, the oscillator is tunable, so that you can set the
transmitter’s frequency to a part of the
band that’s unoccupied in your area,
for clear reception.
The signal produced by the RF oscillator is fed into the modulator, which is
the heart of the transmitter. As shown
in Fig.1, this also receives the audio
signal.
Stereo signals from the audio source
are blended to mono via a simple mixing circuit. The resulting mono signal is
then fed to the modulator via potentiometer which sets the modulation level.
Incidentally, if you wanted to transmit voice, you could use a microphone
preamplifier to boost the tiny microphone output to a level that the transmitter can use (a microphone by itself
would not be enough).
And if you wanted to do the whole
“disc jockey” thing (voice AND music),
you could use an audio mixer to handle
both a microphone and a music source
(for a suitable mixer, see siliconchip.
com.au/Article/644).
The modulator uses the audio signal
to vary the amplitude of the RF signal.
the carrier).
Fig.1: the block diagram for the AM Transmitter. A tunable RF oscillator
sets the carrier frequency and this is amplitude-modulated by the audio
signal. The modulator’s output is then amplified and fed to an antenna.
When the audio signal swings positive, the amplitude of the carrier is increased and when it swings negative,
the carrier’s amplitude is reduced. In
other words, the RF carrier is “amplitude-modulated”. The waveforms in
Fig.1 show the basic concept.
Amplitude modulation or AM is just
one way of using an RF signal to carry audio or other kinds of information
from one place to another.
The amplitude-modulated RF output
from the modulator is very weak, so
before it can be fed to our transmitting
antenna (which is just a short length of
wire), we have to increase its level by
passing it through the third building
block: the RF buffer amplifier.
This stage amplifies the modulated RF signal to a level that’s just high
enough to cause weak radio signals to
Scope1: this shows the oscillator waveform at the junction of
T1 and the 4.7nF capacitor. The amplitude is around 100mV
RMS, reduced from the 1V RMS at Q1’s emitter due to T1’s
turns ratio. This is at the bottom end of the tuning range
(around 650kHz) and the sinewave is quite clean.
siliconchip.com.au
be radiated from the antenna.
Circuit details
The full circuit of the AM Transmitter is shown in Fig.2. The RF oscillator is a Colpitts configuration, based
around transistor Q1.
This uses the primary winding of
RF transformer T1 as the inductive
arm of its resonant circuit, along with
fixed 470pF and 22pF capacitors and
a miniature tuning capacitor (VC1). T1
is a local oscillator transformer from a
low-cost AM receiver coil kit.
The output of the oscillator is taken from the secondary winding of T1.
This is then fed through a 4.7nF DC
blocking capacitor and a series 1kΩ resistor to one of the two carrier inputs
(pin 10) of IC1, an MC1496 balanced
modulator which has been designed
Scope2: an audio signal that we fed into the transmitter is
shown in yellow at the top while the AC voltage across the
ferrite rod coil (L1) is shown below in green. Due to the long
timebase, you can’t see the carrier sinewave but you can see
how its amplitude is being modulated by the audio signal.
Celebrating 30 Years
March 2018 65
Scope3: the same signal as in Scope2 but shown at a
much faster timebase, so you can see the sinewave carrier
waveform (in green). Over such a short period, the audio
signal (in yellow) is not varying.
specifically for this kind of use.
The second carrier input of IC1, pin
8, is tied to ground as far as RF signals
are concerned, via a 10nF capacitor.
However, the IC needs both its carrier inputs held at a DC bias level of
about +6V and that’s the purpose of
the voltage divider network involving
the 1.5kΩ, 560Ω and 1kΩ resistors between +12V and ground.
The 22µF capacitor filters out any
low-frequency variations in this bias
voltage.
The 1kΩ resistor between pins 8 and
10 ensures that both carrier inputs are
biased at the +6V level. It also forms a
voltage divider with the 1kΩ resistor
from T1, to reduce the unmodulated
carrier level at IC1’s inputs to below
60mV RMS – the maximum level
which can be applied to its carrier inputs for undistorted output.
You can see an example of the signal
at the output side of T1 in the screen
grab, Scope1.
IC1’s audio modulating signal inputs are at pins 1 and 4 and these have
to be biased lower than the carrier inputs, to about +4V DC.
The 560Ω and 1kΩ resistors form a
divider between the +6V DC bias point
and ground to derive the +4V DC bias
voltage. This is applied to the two audio signal input pins (pins 1 & 4) via
1.5kΩ resistors.
The two 10kΩ resistors connected to
trimpot VR1 reduce the bias voltage at
these two inputs slightly but VR1 also
allows the DC offset between these two
pins to be adjusted over a small range.
This affects the minimum carrier
modulation level and careful adjustment of VR1 allows for a minimum
66
Silicon Chip
Scope4: this shows the modulated carrier across ferrite rod
L1 but the scope was set up to overlay subsequent traces.
The resultant “jitter” in the waveform is due to the audio
modulation.
carrier signal feed-through with maximal negative swing of the input audio signal.
The stereo audio input signal is fed
into the unit via jack socket CON2 and
mixed together via two 10kΩ resistors
to form a mono signal. This signal is
then fed to modulation depth (volume)
control VR2.
Two 10kΩ resistors have been connected between the audio inputs of
CON2 and ground. These are used to
provide suitable loads for your signal source.
In some cases, if you are using the
headphone output of a CD/MP3 player,
mobile phone etc, its output amplifier
may not operate if the load impedance
is too high. 10kΩ will be sufficient for
many devices but if necessary, these
two resistors can be reduced in value
(eg, to 1kΩ).
Keeping It Legal
This AM transmitter has very low RF
power output (a tiny fraction of a watt)
and is specifically designed to have a
range of no more than a few metres,
thus keeping it legal.
Do not attempt to modify the circuit
with the aim of increasing its power output or to increase its range by feeding
its output into any form of gain antenna,
because this would greatly increase the
risk of interfering with the reception of
licensed broadcasting stations.
It would also make you liable to
prosecution by the broadcasting and
spectrum management authorities and
probable confiscation of your equipment as well.
Celebrating 30 Years
As shown in Fig.2, the modulating
signal from VR2 is fed to just one of the
modulator’s audio input pins – in this
case, to pin 1 via a 4.7µF DC blocking
capacitor. The second input (pin 4) is
tied to ground via a 100µF capacitor,
so the full audio (AC) voltage from VR2
is effectively applied between the two
input pins.
The 1kΩ resistor connected between
pins 2 & 3 of IC1 is used to set the internal gain of the modulator, while
the 10kΩ resistor from pin 5 to +12V
sets the IC’s internal bias and operating current level.
Modulated carrier outputs
The modulated carrier outputs from
IC1 appear at pins 6 & 12, which are
both connected to the +12V rail via
3.3kΩ load resistors.
In this circuit, we only use the output from pin 12 and this drives the
base of RF amplifier transistor Q2 via a
220pF capacitor. The transistor’s base
bias is supplied by the 2.2MΩ connected to the +12V supply
Q2 is connected as a common-emitter amplifier and its output is developed across the collector load formed
by L1, a broadcast-band antenna coil
wound on a small ferrite rod.
As well as forming Q2’s collector
load, L1 actually forms part of the
transmitter’s antenna, because the
ferrite rod inevitably radiates some
RF energy.
However, its very small size makes
it a rather poor radiator, so an external
wire antenna (about two metres long)
is also connected to Q2’s collector via
a 10nF coupling capacitor.
This dual-antenna system gives the
siliconchip.com.au
Fig.2: the circuit uses a Colpitts oscillator based on transistor Q1 to generate the carrier frequency which is then
modulated by the audio signal fed into pin 1 of IC1 (MC1496). The modulated RF signal is then amplified by commonemitter amplifier stage Q2 and fed to the antenna. Potentiometer VR2 sets the modulation depth.
transmitter a range of about three or
four metres, despite its very low RF
power output.
You can see an example of the modulated carrier at the antenna terminal
in screen grabs Scope2, Scope3 and
Scope4.
Power supply and polarity
protection
The circuit is powered by a regulated rail, shown as +12V in Fig.2
for simplicity, but it’s actually set to
around 11.7V. The reason for this is
that we want to ensure a stable, regulated DC voltage even if a 12V supply
is used. So we’ve arranged for 300mV
of “headroom”.
This not only suits regulated 12V
DC mains supplies but also most 12V
batteries and it has a negligible effect
on the operation of the AM transmitter.
This requires the use of a low-dropout regulator and in this case, we are
using a low-cost, micropower LP2951
adjustable regulator which can supply
up to 100mA.
But normally this circuit only draws
a few milliamps which means it has a
siliconchip.com.au
“dropout voltage” under 200mV.
The input supply is connected via
CON1 and Mosfet Q3 provides reverse polarity protection. If the supply is connected correctly, current
flows through Mosfet Q3’s parasitic
diode and simultaneously, its gate is
pulled to ground via the 100kΩ resistor, switching it on.
When on, the Mosfet channel
“shorts out” the internal diode, resulting in almost no voltage drop across
Q3. Hence, it does not raise the required supply voltage for regulation.
But if voltage is applied with the
wrong polarity, the internal diode is
reverse-biased and does not conduct.
And with the gate pulled high, the
Mosfet is switched off and so no current can flow through the channel.
The 12V zener diode between gate
and source prevents damage to Q3
if a supply voltage beyond its +16/5V gate-source rating is applied and
the 100kΩ resistor limits the current
through ZD1 in this condition.
The output voltage of REG1 is set to
11.7V by adjusting VR3. This forms a
divider with the 100kΩ resistor across
Celebrating 30 Years
the output and controls what proportion of the output voltage is fed to feedback input pin 7. The regulator uses
negative feedback to maintain this pin
at a nominal +1.23V.
So we need a division ratio of 9.5
times (11.7V ÷ 1.23V) and this will be
achieved when VR3 is adjusted for a
resistance of 850kΩ [100kΩ x (9.5 – 1)].
Hence the use of a 1MΩ potentiometer.
We need some extra adjustment range
to account for variations in the internal 1.23V reference voltage.
Note that the 100kΩ/1MΩ divider
resistor values are quite high and this
is because REG1 has a minimum load
specification of just 1µA and a quiescent current of around 70µA.
By keeping the resistor values
high, we reduce the amount of current “wasted” in the feedback divider, which could otherwise swamp the
quiescent current.
LED1 provides power-on indication.
It’s connected across the 12V supply in
series with a 47kΩ current-limiting resistor (ie, the current through the LED
is around 0.25mA).
By using a blue LED, we can get a
March 2018 67
Fig.3: Use this component overlay, along with the
photo below, to assemble your AM Transmitter. This
overlay is also printed on PC boards available from
the SILICON CHIP Online Shop.
Note there are some minor differences between the
overlay and the early prototype photo.
sufficiently bright indicator without
wasting too much current.
current. The resistors are chosen to
give an output very close to 5V.
Optional USB supply for
Bluetooth receiver
Construction
The PCB has provision for a second LP2951 regulator to provide a 5V,
100mA output. This is intended to
power a Bluetooth audio receiver, so
that you can wirelessly transmit audio from a mobile phone (or similar)
to the AM Transmitter. The audio output of the Bluetooth receiver can be
fed to CON2, so that the audio is then
re-broadcast.
This only requires five extra components and is quite convenient since the
Bluetooth receiver then simply plugs
into the AM Transmitter and a separate
power supply is not required.
These extra components are REG2,
CON3, two resistors and a 100µF filter capacitor. Again, we’ve used an
LP2951 since it has a low quiescent
68
Silicon Chip
Construction is easy, with all the
parts mounted on a small PCB measuring 122 x 57.5mm. This board has
cutouts in each corner, so it fits inside
a standard UB3 size jiffy box. The overlay diagram, Fig.3, shows where each
component goes on the board. The extra components for the optional USB
power socket are shown in RED.
Start by fitting the 26 small resistors.
The resistor colour code table shows
each value’s colour coding bands.
However, it can be difficult to distinguish certain colours even under the
best conditions, so we strongly recommend that you check the value of
each resistor with a digital multimeter (DMM) to verify it is correct before
soldering.
Remember that you don’t need to fit
Celebrating 30 Years
the 10kΩ and 30kΩ resistors nor the
100µF capacitor near REG2 if you are
not building the unit with the USB
power output option.
Follow with zener diode ZD1,
ensuring that its cathode stripe is
orientated as shown in Fig.2 before
soldering. The ceramic and MKT capacitors can go in next. Like the resistors, these are not polarised and
can again go either way around but
be sure to fit the correct value in
each position.
Solder IC1 in place now, with its
pin 1 dot or notch as shown in Fig.2.
We don’t recommend that you use
a socket. Having done that, fig REG1
in a similar manner – again, making
sure it’s orientated correctly. And if
you’re building it with the optional
USB power supply, also fit REG2 in
the location shown, then follow with
the USB socket. Solder its two larger mounting pins first, then the four
smaller signal pins.
Bend the leads of Mosfet Q3 so that
it fits onto the board as shown, then attach its tab with an M3 screw and nut.
Do the nut up tight and ensure the Mosfet is sitting straight before soldering
and trimming the three leads.
Now fit jack socket CON2, ensuring it is sitting flat on the board and
aligned with the edge before soldering its five pins. Proceed by installing
trimpots VR1 and VR3; these are different values, 50kΩ for VR1 and 1MΩ
for VR3 so don’t get them mixed up.
Mount the two small transistors next.
They are the same type but you may
need to crank their leads out with small
pliers so they fit the patterns on the
board before soldering.
The electrolytic capacitors can now
be fitted, including the 4.7µF tantalum
type. The aluminium types, in cylindrical cans, have a stripe on the negative side and a longer lead on the positive side, so ensure the positive lead
goes through the pad marked “+” on
the PCB, as shown in Fig.2. The tantalum type will have a “+” printed on
its body and this should be lined up
with the corresponding marking on
the PCB.
One of the 100µF capacitors only
needs to be fitted if you have already fitted REG2; its position is shown in Fig.4
You can now fit DC input connector
CON1, again, making sure it’s pushed
down fully and aligned with the edge
before using plenty of heat and solder
to form good fillets between the three
siliconchip.com.au
flat tabs and the PCB pads.
The final capacitor to fit is tuning capacitor VC1. This fits on the top of the
board, with its spindle stub shaft and
three connection tabs passing down
through matching holes in the board.
Turn the board over and attached
the tuning cap body to the board using two of the M2.5 x 4mm screws
supplied with it. Don’t lose the third
screw, though – you’ll need it later to
attach the disc knob to VC1’s spindle.
Now solder VC1’s three pins to their
corresponding board pads.
The oscillator coil T1 is next on
the list. This is effectively polarised
because there are three connection
pins on one side of its base and only
two on the other – be sure to orientate
it correctly before pushing it all the
way down onto the board. There are
seven solder connections to make in
all; five pin connections plus two for
the can lugs.
You will need to cut the shaft of
pot VR2 short, to around 10mm from
the threaded ferrule, so that the knob
doesn’t stick out too far later. It’s easier to do this before mounting VR2 although it can be done later if necessary.
Having cut the shaft to length, solder
VR2 in place.
Then fit LED1 with its body about
20mm above the board, making sure
that the longer lead (anode) goes into
the pad marked “A”. Then bend its
leads down through 90° about 14mm
above the board, so that the LED faces away from the board and will later
protrude through a matching hole in
the side of the case later.
Antenna rod & coil
The final component to fit to the
transmitter board is the antenna rod
and coil assembly (L1). This is secured using two small cable ties, each
of which loops around under the board
through the pairs of 3mm holes provided for this purpose.
Do not replace the cable ties with
wire or any other metal bands. A metal
loop would form a “shorted turn” and
this would absorb RF energy and seriously degrade the performance.
Unfortunately, making the coil’s connections to the board can be a bit tricky.
In most cases, there are four leads and
it’s not easy to work out which are the
correct two to use – ie, the actual start
and finish of the coil.
With the ferrite rod we used, the
wires were marked with black, green,
red and unmarked and the two we used
were the black and unmarked wires.
But other coils may use a different colour scheme.
In fact, the only reliable way to identify the start and finish leads is to check
all lead combinations with an ohmmeter and go with the combination that
gives the highest reading – typically
around 11Ω.
Another little trap is that with many
of these coils, the intermediate leads
actually consist of two fine gauge insulated wires, twisted tightly and soldered together at their outer ends.
This means that if you decide to cut
these leads short, they must be bared
and soldered together again – otherwise, you’ll find that the coil has become an open circuit between start
and finish. And of course, the transmitter won’t function very well with
L1 open circuit!
A word of advice: if you do shorten
any of the coil leads, it’s a good idea
to check the coil continuity with your
multimeter before you solder the start
and finish leads to the board.
Then it’s time to fit the tuning disc
(thumbwheel) to VC1’s shaft and fasten
it in place using the remaining M2.5 x
4mm screw.
A wire antenna is not strictly necessary as long as you can place ferrite
rod L1 near the receiving radio’s own
ferrite rod or antenna (within 10cm or
so). If you need a longer range, solder
Vintage Australian
Radio Programs On CD
If you’d like to rebroadcast genuine
old time Aussie radio programs through
your AM Transmitter, you should know
that many of the programs are available
from ScreenSound Australia (the National
Screen and Sound Archive).
You can purchase CDs with classic
“golden age of radio” programs, including
quiz shows, serials like Dad & Dave and
Mrs ’Obbs, comedies like The Bunkhouse
Show and McCackie Mansion, and so on.
For more information on what’s available,
visit the ScreenSound website at https://
shop.nfsa.gov.au/
That’s not the only source of music –
as mentioned earlier, the US site www.
archive.org has an enormous library covering just about everything ever recorded.
And most countries have, or are working
towards, archives of their own.
a 2m length of insulated hookup wire
to the antenna terminal now.
The board assembly is then ready to
attach to the box lid (used here as the
transmitter’s base). Before doing this,
however, you may need to drill and
cut the various holes in both the lid
and the box itself, if you’re building
the project from scratch. The location,
size and shape of each of the holes is
shown in Fig.5.
The PCB assembly is secured to
the lid using four M3 x 10mm tapped
spacers and eight M3 x 6mm machine
screws.
Once that’s been done, it’s time to
check the transmitter’s operation.
Checkout & adjustment
The first step is to set the supply
voltage and for this, you will need a
source of 12-20V DC power and a multimeter set to read volts.
Rotate VR3 fully anti-clockwise,
connect the DMM between TP1 (red)
There are only two connection points on the PCB: sockets for This photo shows the optional USB (5V) power supply for
the audio input (left) and 12V DC power (right).
Bluetooth receivers, etc. If you don’t need it, leave them out.
siliconchip.com.au
Celebrating 30 Years
March 2018 69
and TPG (black) and apply power.
LED1 should light up and you should
get a reading of around 1.23V. Slowly
rotate VR3 clockwise until you get a
reading close to 11.7V.
If you have fitted the optional USB
power output, now would be a good
time to move the DMM’s red lead to
pin 1 of REG2 (the square pad at lower
right) and verify that you get a reading
between 4.75V and 5.5V. No adjustment should be necessary.
For the remaining steps, you will
also need a reasonably sensitive
AM radio receiver. Switch off, then
follow this step-by-step adjustment
procedure:
(1) Adjust the two fine tuning capacitors on VC1 so that the metal halfdiscs do not overlap.
(2) Switch the radio on and tune it to
a convenient frequency in the lower
section of the broadcast band, away
from any of the local broadcasting
stations (in Sydney, you can tune to
about 820kHz).
(3) Turn the volume up (you’ll just
hear static at this stage) and position the radio near the transmitter,
orientated so that its internal ferrite
Parts list – AM Radio Transmitter
1 double-sided PCB, code 06101181, 122 x 57.5mm
1 UB3 Jiffy box (130 x 67 x 44mm)
1 ferrite rod, 55mm long, with broadcast band coil (L1)
1 mini RF oscillator coil in can with red slug (T1)
4 M3 x 10mm tapped spacers
9 M3 x 6mm machine screws
1 M3 hex nut
1 2.1mm or 2.5mm ID DC barrel socket, PCB-mount (CON1)
1 3.5mm switched stereo jack, PCB-mount (CON2)
1 small knob (to suit VR2)
2 100mm cable ties
1 2m length of insulated hookup wire (for antenna)
Semiconductors
1 MC1496 balanced modulator, DIP-14 (IC1) [SILICON CHIP Online Shop Cat SC4533]
1 LP2951 adjustable micropower regulator, DIP-8 (REG1)
2 PN100 NPN transistors (Q1,Q2)
1 IPP80P03P4L04 P-channel Mosfet (Q3) [SILICON CHIP Online Shop Cat SC4318]
1 3mm blue LED (LED1)
1 12V 1W zener diode (ZD1)
Capacitors
1 220F 25V electrolytic
3 100F 16V electrolytic
1 22F 16V electrolytic
2 4.7F 16V electrolytic or tantalum
2 100nF ceramic (disc or multi-layer)
2 10nF MKT
1 4.7nF MKT
2 470pF NP0/C0G ceramic
1 220pF NP0/C0G ceramic
1 22pF NP0/C0G ceramic
1 mini tuning capacitor 60-160pF, with thumbwheel and mounting screws (VC1)
Resistors (all 0.25W 1% metal film)
1 2.2M 2 100k 1 47k 2 15k 7 10k 2 3.3k 3 1.5k 4 1k 1 560
1 50k horizontal trimpot (VR1)
1 50k 16mm PCB-mount logarithmic taper potentiometer (VR2)
1 1M horizontal trimpot (VR3)
Optional extra parts for USB power output
1 LP2951 adjustable micropower regulator, DIP-8 (REG2)
1 horizontal PCB-mount type A USB socket (CON3)
1 100F 16V electrolytic capacitor
1 30kΩ 0.25W 1% metal film resistor
1 10kΩ 0.25W 1% metal film resistor
70
Silicon Chip
Celebrating 30 Years
rod antenna is roughly parallel to
the transmitter’s ferrite rod.
(4) Turn the transmitter’s tuning control (VC1) to one end of its range,
set trimpot VR1 well away from its
centre position (this is important)
and set VR2 (modulation depth) to
its midrange position.
(5) Turn the adjustment slug in T1 anticlockwise until it stops rotating
(do this gently or you could crack
the ferrite slug).
(6) Feed an audio signal into the transmitter by plugging the audio cable
from your signal source into CON2.
Start the source up and make sure
it has a sufficiently loud (high amplitude) output signal.
(7) Apply power to the transmitter.
Check that the voltage at pin 8 of
IC1 is close to +6V; you can again
use TPG as a ground reference. If
this is correct, your transmitter is
very likely to be working properly.
(8) Listen carefully to the radio while
you turn the transmitter’s tuning
knob very slowly towards the other
end of its range. At some point, you
should start to hear the music from
your MP3 or CD player, after which
you should be able to tune the transmitter so that its signal is received
at a good strength.
(9) If you have trouble getting the tuning exactly right, you can use the
two small trimmers on VC1 and/
or the adjustment slug in T1 to fine
tune the oscillator but be gentle
with T1’s slug (remember that we
already set it fully anti-clockwise)
and note that this will shift the overall tuning range down slightly (ie,
you may no longer be able to tune
up to 1500kHz).
Troubleshooting
Can’t find the signal? The first thing
to do is to try tuning the transmitter
back the other way but even more
slowly and carefully than before. If this
still doesn’t bring success, try turning
the adjustment slug in oscillator coil
T1 anticlockwise another half-turn
(or even a full turn if this later proves
necessary).
This will shift the oscillator’s tuning
range up in frequency and should allow you to correctly adjust the transmitter when you tune VC1 over its
range again.
Once you’ve found the signal and
adjusted the transmitter’s tuning control for the best reception, try turning
siliconchip.com.au
Inside the MC1496 Double Balanced Mixer IC
The circuit opposite shows what’s inside the MC1496 IC which
forms the “heart” of the AM Transmitter. Compared to some other
ICs which may have thousands or even millions of components,
this one is dead simple!
It comprises eight transistors (nine if you count the diode, which
is almost certainly a transistor with its collector and base shorted)
and three resistors.
Given the relatively low operating frequency in this circuit (sub1MHz), the transistors don’t even need to be a particularly special
type. So you could build a double-balanced mixer from discrete
components fairly easily. But why do that?
The MC1496 basically consists of adouble differential amplifier
(the top four transistors), a standard differential amplifier (the two
below these) and a current mirror for biasing the different amplifiers (the bottom section).
Starting at the bottom, an external current source is applied
to pin 5 (Bias). This current flows through the diode and series
500Ω resistor to VEE (normally ground). This sets up a base bias
voltage for the two transistors to the right. Since they also have
500Ω emitter resistors, and since their base-emitter voltage drop
will be the same as the diode forward voltage, their collector currents will match the bias current.
The collector currents of these two transistors are ultimately
sourced from the two outputs, at pin 6 (Vo+) and pin 12 (Vo-),
shown at the top of the diagram. There is one current path from
each output to each bias transistor. So say you supply 1mA to
the Bias input.
That means that a total of 2mA will be drawn from Vo+ and Vo-,
to supply the two 1mA current sinks at the bottom of the diagram.
However, they will not necessarily be equal currents. For example,
one could be 0.5mA and the other 1.5mA.
Notice that the upper two differential amplifiers are wired differently. In the left-hand differential amplifier, pin 8 (carrier +) drives
the base of the transistor which controls current from pin 6 (Vo+)
while in the right-hand differential amplifier, pin 8 (carrier +) drives
the base of the transistor which controls current from pin 12 (Vo-).
So essentially, changes in the voltage of the + carrier input have
the opposite effect on the differential output voltage compared to
the – carrier input. And as you would expect, if you leave the signal inputs floating and simply apply a carrier, one output will simup the transmitter’s modulation control (VR2). This should make the reception even louder and clearer but
if you turn the control up too far, the
music will become distorted. Just
back it off again until the distortion
disappears.
Now is a good time to adjust trimpot
VR1 for the best audio quality (maximum clarity).
We found that its optimum position
was about halfway between the centre
and one of the end positions of the rotor (on either side).
Don’t set this trimpot (VR1) too
close to its midway (centre) position,
because this balances out the RF carrier altogether and gives double sideband (DSB) suppressed carrier modsiliconchip.com.au
ply duplicate the carrier signal while the other output will carry an
inverted version of the same signal.
That just leaves us with the question of what the two extra transistors in the middle of the diagram do. These are connected to the
signal inputs. The current through each transistor would be essentially fixed, because their emitters are connected to constant current
sinks, except for the pin 2 & 3 connections, labelled “gain adjust”.
A resistor is connected across these two pins and that allows
current to flow from one side to another of the circuit, depending
on which voltage is higher. And which voltage is higher depends
on whether the voltage at pin 1 (signal input+) or pin 4 (signal input -) is higher, because these transistors are operating as emitter-followers.
Therefore, the differential input signal causes a differential voltage shift at the bottom of each of the differential amplifiers at top.
And that shifts the current sharing between the two outputs, effectively controlling the gain of those upper pairs.
This has the effect of modulating the carrier signal which appears at the outputs, by an amount that depends on the resistor
value between the gain adjust pins, because that controls how
much current is shifted from one side to the other for a given signal input voltage swing.
The lower the resistor value, the greater the modulation (to a
point).
And voila, we have generated a modulated RF carrier based on
the applied signal.
ulation. And that gives quite a high
distortion when you’re using a normal
AM receiver.
Once all the adjustments have been
made, your AM Transmitter is working correctly and you’re ready for the
final assembly.
Final assembly
If your UB3 box has vertical PCB
mounting ribs inside, you’ll also have
to cut some of these away.
That’s because the transmitter board
assembly is a fairly tight fit inside the
box and the ribs foul the ferrite rod
and its coil.
The ribs to remove are mainly those
at the rear side of the box, where they
interfere with the ferrite rod. HowCelebrating 30 Years
ever, it’s also a good idea to cut away
any ribs on the end near the holes for
CON1 and CON2 because these can
make final assembly more difficult.
You should also cut away any ribs on
the front of the box, around the holes
for LED1 and VR2, as this makes the
final assembly even easier.
The ribs are easy to remove. The
ABS material used in these boxes is
fairly soft and can be cut away using a
sharp hobby knife, small wood chisel
or a rotary tool such as a Dremel.
Once the ribs are gone, remove the
knob from modulation pot VR2 (if you
have fitted it for the checkout) and unscrew the nut from VR2’s ferrule.
You can now introduce the box to
front of the lid/board assembly at a
March 2018 71
The PCB mounts upside-down
on the Jiffy box lid via screws
and nuts – here it is shown
in position before being
fastened in place. Suitable
holes for the modulation
pot and power LED must
be drilled (along with
holes for the input and
power sockets in the
end; along with a
slot for the tuning
capacitor.
(Drilling templates
and panel art
are available at
siliconchip.com.au)
suitable angle, passing VC1’s disc knob
through its slot and LED1 and VR2’s
shaft through their respective holes.
Next, swing the box down over the
board assembly, pulling the remaining antenna wire through its hole as
you do so. As it comes down, slide it
slightly towards the CON1/CON2 end,
so that the ferrule of CON2 enters its
clearance hole.
That done, you can fit the nut to
VR2’s threaded ferrule. Tighten it firmly and then refit the knob. Finally, turn
the assembled box over and fit the four
supplied self-tapping screws supplied
to fasten everything together.
Connecting a
Bluetooth receiver
A typical Bluetooth audio receiver
is powered from a USB socket and has
a 3.5mm stereo jack socket for the audio output.
Once you’ve paired your phone or
tablet with it (see the supplied instructions) and your device is in range, it
should connect automatically and any
audio output will be received wirelessly and appear as a line-level signal at
the output socket.
So, if you
build this unit with
the optional USB power socket, assuming your
Bluetooth receiver draws
no more than 100mA (most will be
well under this), all you need to do
is plug it into the power socket and
connect a cable with 3.5mm stereo
jack plugs at each end between the
Bluetooth receiver audio output socket and the AM Transmitter’s audio input socket.
You can verify the receiver is working by plugging a pair of headphones
or earphones into its output socket
and if so, you should have no trouble getting it to work with the AM
Transmitter.
Just keep in mind that you will probably want to turn the Bluetooth and
receiver volume controls right up and
use the modulation depth control on
the unit, to get the best audio quality.
Running it from a 9V battery
The AM Transmitter will operate
from a 9V battery with slightly re-
Resistor Colour Codes
Qty. Value
o 1 2.2MΩ
o 2 100kΩ
o 1 47kΩ
o 0/1 30kΩ
o 2 15kΩ
o 7/8 10kΩ
o 2 3.3kΩ
o 3 1.5kΩ
o 4
1kΩ
o 1 560Ω
72
Silicon Chip
4-Band Code (1%)
red red green brown
brown black yellow brown
yellow violet orange brown
orange black orange brown
brown green orange brown
brown black orange brown
orange orange red brown
brown green red brown
brown black red brown
green blue brown brown
5-Band Code (1%)
red red black yellow brown
brown black black orange brown
yellow violet black red brown
orange black black red brown
brown green black red brown
brown black black red brown
orange orange black brown brown
brown green black brown brown
brown black black brown brown
green blue black black brown
Celebrating 30 Years
duced output power and thus range.
You just need to adjust VR3 to give
around 8.5V at TP1.
The current consumption drops
to around 7mA, giving more than 24
hours of runtime from a typical 9V alkaline battery.
Also, note our warning earlier about
attempting to run from a higher voltage to achieve more output (and range).
This would almost certainly make
your transmitter illegal.
Tuning it to lower frequencies
It may be useful to modify the Transmitter to tune to around 450-455kHz,
to allow you to inject a modulated test
signal directly into a radio set.
This can be achieved by replacing
the 22pF coupling capacitor with a
470pF ceramic capacitor. This should
allow you to tune between 440kHz
and 600kHz.
We do not suggest you add any extra
capacitance across VC1 as it may prevent the oscillator from running.
SC
Small Capacitor Codes
Qty. Value
F
EIA
IEC
Code
Code
Code
o 2 100nF 0.1µF
104
100n
o 2 10nF .01F
103
10n
o 1 4.7nF .0047F 472
4n7
o 2 470pF N/A 471 or 470 470p
o 1 220pF N/A 221 or 220 220p
o 1 22pF N/A 220 or 22 22p
siliconchip.com.au
Using Cheap Asian Electronic Modules Part 14: by Jim Rowe
Banggood’s
RF Detector
This nifty RF Detector module from Banggood can measure the power of
RF signals from 1MHz to 8GHz, over a range of 60dB. It is on a tiny PCB
measuring 33 x 24.5mm and has an SMA RF input connector attached
to one end. It’s based on the Analog Devices AD8318 chip, which is an
enhanced version of the AD8307.
A
s a matter of interest, we used the
Analog Devices AD8307 chip in
the RF Level and Power Meter project
of October 2008 (siliconchip.com.au/
Article/1971) and also in the Arduino Multifunction Measuring Shield
of April-May 2016 (siliconchip.com.
au/Series/299).
Both the AD8318 and AD8307 are
logarithmic amplifier/detectors which
provide a DC output voltage proportional to the RF input power level.
But the AD8318 has a much wider
bandwidth of 1MHz to 8GHz, compared with the DC-500MHz range of
the AD8307.
While the AD8307 has a range of just
over 90dB, the AD8318 has a smaller
dynamic range of about 60dB (necessary to get the improved frequency
range).
Unlike the AD8307, which operates from a nominal supply voltage of
3V, the AD8318 is designed to operate
from 5V. It also has a typical supply
current of 68mA, compared with the
7.5mA drawn by the AD8307.
But perhaps the most important
functional difference between the two
devices is in terms of the output circuitry. The AD8307 has a current mirror in the output circuit which provides a positive slope to the DC output voltage. So the output voltage is
directly proportional to the RF input
level, with a slope of 25mV/dB.
In contrast, the AD8318 has a different output circuit designed to alsiliconchip.com.au
low it to be used for power amplifier
gain control. As a result, it provides
an output voltage which is inversely
proportional to the RF input, with a
slope of -25mV/dB. Is this a problem?
Not when you are going to use it in
conjunction with an Arduino or other
microcontroller.
Fig.1 shows a simplified version
of the circuitry inside the AD8318. It
has nine detector stages, interspersed
with eight cascaded gain stages. The
nine detector outputs are fed to an adder which drives a current-to-voltage
converter to produce the output voltage, Vout.
The V-I (voltage-to-current) converter at upper right allows adjustment
of the slope of Vout in measurement
mode. For example, the output slope
of -25mV/dB is achieved when the Vset
pin and the Vout pin are tied together.
Higher output slopes can be obtained by connecting a voltage divider
between the Vout pin and ground, and
feeding a fraction of Vout back to the
Vset pin. So if the voltage fed back to
Vset is Vout ÷ 2, this changes the output slope to -50mV/dB.
However, the output voltage is always in the range of 0.5-4.6V, so beyond -55mV/dB, the dynamic range
will be reduced as the output at lower
RF levels will be pegged at 4.6V.
Note that the AD8318 includes an
internal temperature sensor as well
as bias stabilisation circuitry for the
cascaded gain stages so that changes
Fig.1: simplified block diagram of the AD8318 logarithmic detector/controller. It
has nine detector stages interspersed with eight gain stages.
Celebrating 30 Years
March 2018 73
Fig.2: circuit diagram of the log detector module. Clpf and Cobp are optional
capacitors used to filter ripple from IC1’s output. Suitable values are 1nF for
Clpf and 10nF for Cobp with pads provided for mounting on the PCB.
in ambient temperature do not unduly
affect accuracy.
All this is squeezed into a tiny 4 x
4mm 16-lead LFCSP (SMD) package;
much smaller than the 8-pin SOIC/
PDIP packages used for the aforementioned AD8307.
Now have a look at the circuit for the
Banggood log detector module shown
in Fig.2. Apart from the AD8318 chip
itself (IC1), there is not much to it. The
only other IC is REG1, a 78L05 regulator in a SOT-89 3-pin package with tab.
This provides a regulated 5V rail for
IC1. But the 78L05 has a nominal dropout voltage of 2V, so the module needs
a power supply (Vcc) of at least 7.5V.
As with many modules, there’s one
LED to indicate when power is applied. LED1 is connected directly be-
tween the Vcc input and ground with
a 10kW series resistor.
CON1 is the RF input, an SMA edgemount socket. This is terminated via
a 51W resistor and then coupled to
the INhi input (pin 14) of IC1 via a
1nF capacitor, with a second 1nF cap
coupling the INlo pin of IC1 (pin 15)
to ground.
As the input resistance of IC1 between pins 14 and 15 is close to 1200W,
this gives the input circuit a low-frequency cutoff of around 300kHz. The
effective input resistance at frequencies below about 100MHz is around
49W (51W || 1200W).
Pin 16 of IC1 is the enable input,
which can be used to switch the device into a low-current standby mode
if desired, by pulling it to ground.
However, in the Banggood module, it’s
connected to the +5V line, so the chip
always functions while the module is
powered up.
But what’s the purpose of that 510W
resistor connected between pin 10
(Tadj) of IC1 and ground? It allows adjustment of the chip’s internal temperature compensation, to optimise
its operation at different frequencies.
A value of 510W apparently gives
very close to optimum compensation
at frequencies up to 2.2GHz, and also
at 8GHz, while optimum operation at
3.6GHz and 5.8GHz can be achieved
by changing RTadj to 51W or 1kW, respectively.
Even so, a value of 510W apparently
gives acceptable performance over the
whole range.
The two capacitors shown in red,
Clpf and Cobp, are used for filtering
any ripple in the output from IC1. If
both capacitors are omitted, the nominal output video bandwidth of the
AD8318 is around 45MHz, making it
suitable for demodulating pulse signals.
But if you’re using it purely for
measuring unmodulated RF, this wide
bandwidth can allow significant second-harmonic ripple to appear in the
output for input signals below 22MHz.
Since this ripple can cause measurement jitter, the simplest way to reduce its effect is to add either Clpf or
Cobp, or both. A suitable value for Clpf
is 1nF, while that for Cobp is around
10nF and these values give an output
bandwidth of around 100kHz.
By the way, neither of these capacitors are fitted to the module board
(even though pads are provided for fitting them as 0603 SMD components)
Banggood’s logarithmic RF Detector module detector module is based on the Analog Devices AD8318 chip. It has an
RF bandwidth of 1MHz to 8GHz with a range of -65dBm to +5dBm and an input impedance of 50W. These photos are
almost twice actual size.
74
Silicon Chip
Celebrating 30 Years
siliconchip.com.au
which is why we’ve shown them in
red in Fig.2.
Trying it out
To check out this module, I hooked
it up to a suitable 9V DC power supply and connected its RF input up to
a VHF/UHF signal generator.
Then I monitored its output using
a 4.5-digit bench DMM while varying
the RF input level over the range from
+10dBm to -70dBm, for four different
frequencies: 100MHz, 1GHz, 2GHz
and 4GHz.
I wasn’t able to go above 4GHz because that’s the highest frequency my
signal generator provides.
These measurement runs were used
to plot the module’s transfer characteristic at each of the four sample frequencies and the results are shown in
Fig.3. The four plots are very close to
linear between RF input levels from
-5dBm down to -60dBm and only
curve gently away at the upper and
lower extremes.
Although the truly linear part of
the module’s transfer characteristic
only covers about 55dB, the curved
sections at each end give it a useful
range of about 70dB as claimed in the
data sheet.
The linear sections of all four plots
are well within ±1dB of each other
and have a slope of -24.33mV/dB; very
close to the expected -25mV/dB.
Note that we’ve mentioned a 60dB
range before, as this is the practical
range over which you can expect to
get an accurate result.
Connecting to an Arduino or
Micromite
Interfacing this module to a micro is
straightforward. Just feed the module
with 7.5-9V DC and connect its Vout
to either one of the micro’s own ADC
inputs directly, or to a higher-resolution ADC coupled to the micro via an
SPI or I2C interface.
Then it’s just a matter of writing a
firmware sketch or MMBasic program
to read the analog Vout signal and convert it into an RF power level.
So this module should be suitable
for use as the sensor section of a homebrew VHF/UHF level and power meter.
You could even use it as an RF sensor
head for our Arduino Multifunction
Measuring Shield (MFM), although
its negative-slope transfer characteristic would require some changes to
the MFM’s firmware sketch.
Other uses would be in an RSSI (received signal strength indicator) for
UHF base station receivers and WLAN
routers. In short, it seems to represent
good value at around $16.50.
SC
Fig.3: plot of
the transfer
characteristic
for the AD8318
at four
different input
frequencies.
Note the
excellent
linearity.
siliconchip.com.au
Celebrating 30 Years
March 2018 75
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and more! Stows away in a hard
plastic carry case.
March
60
$
T 2120
289
NEW!
189
$
$
T 2444A
X 4306
299
$
N 1120
120W Portable Folding Solar Power Kit
Going bush? Have power wherever you go on your next 4WD adventure.
This complete power kit includes 120W panel, solar regulator, battery connection
cables and canvas carry case. 3 stage solar charger ensures your batteries are alway
performing at their peak! Adjustable stand for finding best
sun placement. 720x520x70mm (folded).
$119
Brilliant Battery
Powered Work
Lights
30% OFF!
80
Super bright LED floodlamps coupled with a
rechargeable battery
offering up to 6 hours use.
Includes car charger &
plugpack. Great for work
sites & service vans.
$
Massive 200x
Magnification
Get a close up view with
a desktop microscope
This high resolution 12 megapixel USB micrsocope
allows close up inspection of just about anything!
USB PC interface, plus HDMI output for monitor
connection. 220x magnification with 10-50mm
focal length. 2.4” LCD.
Whisk away those soldering fumes!
#1 choice for schools! This 60W soldering station has a
powerful in-built fume exhaust fan which sucks away the
smoke when soldering. The active filter helps to reduce
airborne pollutants. Durable metal construction.
NEW!
A 1101
SAVE 30%
Bluetooth 3.5mm Jack
X 2321 20W
120
35
$
19.95
X 3250 Warm White
X 3251 Natural White
$
SAVE 15%
Perfect for lighting cabinets and
workspaces at home or in vehicles. Up
to 4 strips can be daisychained together using
X 3255 joiner ($2.95). Suggest M 8936B 2A plugpack
($21.50) to power 4 strips. Provide a crisp 975 lumen output.
25Wx10Hx500Lmm.
$
M 8880
5 Way Intelligent USB Charger
‘Charge IQ’ feature charges a connected device at
the fastest speed. 7.8A max current. 110-240V great for travel. Includes mains lead. 73x73x34mm.
SAVE $30
139
$
Includes air compressor
& ultra compact lithium
jump starter!
M 8198
E
land
Mid
DS
AL
ON
BUNNINGS
CD
M
LEACH HIGHWAY
GT. EASTERN HWY
Inflate a flat tyre. Start a flat battery.
MYAREE
5A 116 North Lake Rd.
MIDLAND
212 Gt Eastern Hwy.
Includes
charging
case
Scoop purchase!
Why pay $179?
99
$
C 9037
No headphone jack
on your phone?
No worries! These new Jabees Shield ‘true wireless’
bluetooth earbuds are perfect for exercise - they’re
sweat resistant, light weight and provide 9hrs of
listening time. Great alternative to Apple Airpods!
Includes charging case and replacement earbuds.
COPE ST
MIDLAND
GATE
LOTON AV
ee
Myar
LLOYD ST
NEW stores now open in WA!
MCCOY ST
29.95
$
Instantly add Bluetooth wireless audio streaming to any
3.5mm input, whether it be your car, your favourite headphones or home amp. Internal battery provides 5 hours of
listening time and is USB rechargeable. Just 40mm long!
$175
X 2320
10W
Modular
Aluminium
12V LED
Strips
NORTH LAKE ROAD
SAVE $50
A complete auto rescue kit for the car boot. Features a
16800mAh battery bank plus emergency compressor to
top up tyres (max 8 mins run time). Provides 600A peak
cranking output for cars with flat batteries. 12/16/19V &
USB output provided for powering devices.
To find your nearest store, visit: www.altronics.com.au/storelocations
Bluetooth FM
Audio Player
Transmits bluetooth audio
from your phone (music,
phone calls etc) to your cars
FM radio. Plus it’s also a
dual USB charger!
X 0604A
44.95
$
Sale pricing ends March 31st 2018.
pROTEcT YOUR HOME OR BUSINESS.
599
$
SAVE $100
Why settle for just
HD? This system
features 30% more
detail and clarity.
SAVE $200
699
$
Affordable 4 Megapixel
CCTV Surveillance System.
A 2562
Pro-Grade 22 Input Mixer With USB
A professional 22 input mixing desk with mic pre-amps and compressors, plus British style EQs and 24-bit multi effects processor. Great
for bands, home studios and function centres. Easy to use, uncluttered
control layout. USB audio interface hooks up to a PC or Mac. Can be
rack mounted or bolted into a mobile stand such as H 5510 ($89.95).
Includes power supply.
20
$
SAVE 22%
22%
OFF
A 3051
33
$
A 2620
Phono Pre-Amp
Portable Micro Mixer
A low noise pre-amp with
RIAA circuitry for connecting
a turntable to a line input.
Requires 9V battery (S 4970B).
Powered by 9V battery or plugpack
(M 8923 $17.95) this tiny mixer is
perfect for small productions. Mixes
four 6.35mm mics.
BEcOME THE NExT BIg
THINg IN pODcASTS!
4 Channel
USB Mixer With
EQ & Effects.
C 9014B
SAVE 24%
SAVE $15
Add security to your home
or business with our high
resolution 4 megapixel
(1080p) CCTV pack. Wireless
cameras cut down installation
time and effort! Pack includes
power supplies for each camera,
a network video recorder
(expands to 9 channels!) and
four compact bullet cameras.
Nothing else to buy!
pre-installed with 1TB
hard drive.
NEW MODEL!
1199
$
HALF pRIcE!
peace of mind
for the family!
219
$
129
Colour 7” LCD Video Door Intercom
Vari-Focal
1080p/960H
Camera
SAVE $50
A high performance
1080p AHD camera
with adjustable focal
length (3-12mm).
Switchable between
1080p and 960H
modes depending on
DVR capability.
SB9123F
99
$
NEW!
A safe & easy way to monitor the front door. Records photos
of visitors when you’re not home. Includes power supply,
hookup cable, base station & camera unit. Remote door
latching*. Expandable to 4 base stations & 2 cameras.
*When used with optional door strike S 5385 $46.95.
Just the shot for monitoring your mixing
efforts. Deep bass with crisp treble
and full midtones. Very comfortable!
Detachable lead with durable woven braid
sheath.
Mini Desktop
Mic Holder
Great for keeping a
microphone steady on
your desktop whilst
recording.
150mm max height.
15
$
79.95
SAVE
40%
This handy balun converts
DC power and coaxial video
into an economical Cat5e
cable for transmission
up to 300m. Includes
transmitter &
receiver.
X 2382 54 LED
NEW!
29.95
$
S 9240A
40
C 0383
Tough grill and diecast body resists damage, even when dropped on hard
floors - schools love ‘em! Includes 5m XLR lead.
Remote Motion
Activated Camera
Records 720p video or 8MP
still shot photos to internal SD
card when motion is detected.
Runs off batteries, so its quick
& easy to set up anywhere
you need to keep an eye on
things. Weatherproof case with
LCD screen. Requires 8xAA S
4955B 4pk, $3.95 & DA0322
16GB SD card $16.95.
54.95
$
Cut Cabling Costs!
C 0493
$
Tough Drop Resistant Microphone
S 9941
S 9406A
Stunning Monitor Headphones
75
4 Channel Wireless
CCTV System
$
Want to get into recording
A 2548
podcasts, voice overs or
making audio samples? This mini
USB mixer connects directly to
your PC or Mac, takes up very little
desk space and is powered directly
from USB - making it highly portable. Includes 3 band EQ/effects.
124W x 157D x 40Hmm.
$
S 9900G
4 Domes
Simple to install with instructions supplied. Cameras can be remote viewed on iOS/Android. Each
pack includes: • HD digital video recorder • Pro grade 4MP resolution weatherproof cameras • 20m
S 9901G
connection leads • Power supply • HARD DRIVES TO SUIT: 1TB $119 (D 5514), 2TB $189 (D 5516). 4 Bullets
SAVE
$40
159
$
S 9444
$
X 2381 20 LED
Instant Outdoor Lights.
No Electrician Required.
39.95
$
X 2380 8 LED
Dusk or motion
activated
Solar powered with in-built rechargeable batteries.
These stylish motion activated LED lights are fantastic for
lighting up outdoor areas such as entryways, paths etc.
Three operating modes - see web for full details.
Wireless Shop
Door Alert
33
$
A handy motion
activated chime unit
for shops to notify staff
when customers arrive.
120m range. Requires
3xAAA batteries
(S 4949B 4pk $3.95)
& 3xC batteries
(S 4960B 4pk
SAVE 22%
$7.90).
Shop online 24/7 <at> www.altronics.com.au
S 5322
1300 797 007
QUALITY TEST gEAR FOR THE
WORKBENcH OR FIELD KIT...
Includes padded
carry case to
protect your
investment!
Q 1289
SAVE $60
139
$
20 only at
this price.
2 year warranty.
Q 0200B 25MHz
499
$
Perfect for those in R&D, product development or servicing. 2 channels with real-time
1GSa/s sampling. Colour 7” TFT screen simultaneously displays waveform plus the measured wave voltage, peak to peak plus RMS, frequency, duty cycle etc. Realtime adjustments can be made using included PC software. Stored data can be saved to a USB stick.
Measures cable length,
traces cable location,
finds cable breakages
& provides PoE/ping
testing. Provides a
suite of test functions for
comms/CCTV installers
with easy on-screen
adjustments. It even
logs readings to Micro
SD card (16GB D 0328
$13.95).
Q 1346
145
$
Twin laser beams for precise
measurement between
-50°C and 1050°C with
30:1 optical resolution.
Adjustable emmisivity to
cater for different surfaces. It
even connects to an external
probe. 2% accuracy.
25MHz Dual Channel Digital Storage Oscilloscope
Make coax
& data cable
testing easy.
SAVE $44
Measure
temperature
without touching.
SAVE $50!
Q 0966
315
88
60
$
Q 1242A
SAVE $19
Q 1074A
39.95
$
SAVE
$50
NEW!
This top quality anemometer measures
up to 45m/s (162km/h). Sensor is on
curly cord for external measurement. Also
measures temperature. Perfect for ventilation monitoring, experiments etc.
A high accuracy model
for those requiring
true RMS ac waveform
measurement. Huge
feature list - check online
for more info. Relative
function, backlit LCD, USB
datalogging. Cat III 600V.
SAVE $27
$
SAVE $34
120
$
Autoranging
True RMS
Multimeter
A bargain for the
electrical tradesman, this
model features 200MΩ
& 2000MΩ ranges
with 100, 250, 500 &
1000V test voltages. A
must have for insulation
breakdown. Includes
leads & case.
A must have for data
& comms techs.
SAVE $39
Professional Wind
Speed Meter
Accurately measures AC or DC
current to a MASSIVE 600A!
Includes advanced True RMS
AC measurement, resistance,
temperature, capacitance, zero
& hold functions - All supplied
with carry case & test leads.
Professional
Insulation
Tester
$
Q 1252
AC/DC Clamp Meter
39.95
$
T 2186A
165
$
10 Crimping Tools In One!
101 Pc Ratchet Driver Kit
A tool for every occasion! Features 95 security, philips,
pozi and slotted bits made from tough S2 alloy. Includes
two way ratchet handle with comfy rubber grip. See web
for full contents list.
T 2178
NEW!
79
T 5021
.95
185
$
M 8254
A fixed voltage output power supply designed
for powering automotive, marine and comms
equipment. Low noise and ripple design
(<100mV) offers excellent efficiency and
performance.
33
$
11 Pc Insulated Tool Kit
Ideal for technicians working on mains
powered equipment. Includes cutters, pliers,
wire strippers, 5 screwdrivers plus a neon test
driver and 2 rolls of insulation tape - all in a
handy carry case.
38
$
T 5036A
Fixed 13.8V 20A
Bench Power Supply
T 2175
T 4021
19
$
With tool pocket &
customisable foam
inner to keep equipment
secure and safe. Ext. size:
445x330x128mm.
.95
X 0432
This jumbo 5x loupe with LED provides
a crisp clear view of fine print,
circuit boards, small parts etc. USB
rechargeable. Includes carry case.
Virtually every crimper you’ll ever need! 10
sets of quick change magnetic jaws to suit
kwik crimps, uninsulated lugs, telephone lugs,
ferrules, coax crimps, D-Sub pins and RJ plugs.
Lockable Tool
Field Case
$
No More Eye Strain!
SAVE
33%
NEW!
Double Sided Parts Case
Perfect for working in the field! 15 compartments on one side, plus 10 removable containers on the other side.
Shop online 24/7 <at> www.altronics.com.au
SAVE 20%
ESD Safe Workbench Matting
An electronics workbench essential! 1m x 0.5m
with anti-static wrist strap.
1300 797 007
pOWER YOUR EASTER ROAD TRIp!
D 0505A 1A 4000mAh
SAVE 22%
NEW!
24.50
$
NEW!
Z 6303
55
$
33.95
$
Raspberry Pi Zero W Starter Kit
®
D 0507A 2A 8000mAh
Super Slim Battery Banks
Emergency pocket power supply for your
phone or tablet. Slimline aluminium design.
SAVE 25%
22
$
M 8630
Multi-Stage Weatherproof
Vehicle Battery Chargers
99
$195
$
Each model utilises a microprocessor to M 8534 6/12V 4.5A 7 Stage
ensure your battery is maintained in tiptop condition whenever you need it. Helps
to extend battery service life. Suitable for
permanent connection. Great for boats,
M 8536 12V 10A 10 Stage
caravans & seldom used vehicles.
Huge 4.8A output! Ideal for use with QC3.0
devices for ultra fast charging.
64.50
$
NEW!
M 8194
15.95
$
Triple Car Accessory Adaptor
Plus dual USB charger for keeping your
devices powered up on the road.
SAVE 20%
NEW
LOWER
pRIcE!
HALF pRIcE!
QC 3.0 USB Car Charger
M 8606
The Pi Zero W offers amazing power and features from a compact board including
Bluetooth and 802.11b/g /n wi-fi. 1GHz CPU with 512MB of RAM. Mini HDMI & USB
OTG on board. Kit includes Zero W board, case, 16GB SD card (with NOOBs), mini
HDMI adaptor and USB adapter.
USB Car
Jumpstarter
& 2-in-1 Floodlight
50
$
K 9615
Arduino Starter Platform Kit
A handy starter kit for educators or Arduino newbies. Includes an Arduino UNO
compatible board, blue acrylic base, 5V 2A power supply, USB lead, breadboard,
65pcs of jumper leads & hardware.
SAVE 22%
A must have for any road trip! Starts most
4 & 6 cylinder cars from dead flat. • 300 cranking amps
• Fits in your glovebox • High power LED flood light
• USB phone charging • Suits 12V vehicles only. • Includes
carry case, battery clips, mains charger & USB lead.
469 279
$
$
N 1112
50W
80
$
N 1114 100W
44
$
The Tremor
Effect Pedal Kit
M 8627A
Laptop & USB Car Charger
Simply plugs into a car accessory socket.
Voltages 15, 16, 18, 19, 20, 22 and
24VDC, up to 120W. Includes 8 adaptors to
suit most laptops.
SAVE $20
33
$
N 0704
NEW!
Portable Fold Up Solar Power ‘Blankets’
The perfect go-anywhere power accessory - use it to charge
batteries when you go bush! If you don’t want a permanent
solar panel on your 4WD, car or caravan, this fold up solar
blanket is a great option. It includes 10A regulator and croc clips
for direct hookup to your battery.
K 8122
Build your own analog effects
pedal and tweak it you suit your
needs! Controls level, depth,
velocity, hard/smooth & true
bypass. Tough diecast case
Audio Spectrum Analyser Kit
Give your homemade audio gear a high-tech
upgrade. This compact unit is ideal for panel
mounting. 127 x 64mm white backlit LCD. Auto
or manual range selection. Measures:
• Peak power RMS power • Mean dB • Peak
dB • Linear audio spectrum • 1/3 octave
audio spectrum
NEW!
NEW!
K 9705
Plugs into an Arduino UNO to provide high
accuracy inductance and capacitance measurement. 5 digit resolution, 1% accuracy.
10nH to 100mH+. 0.1pF to 2.7µF+.
26.95
M 8017A 12V
440
$
or M 8018A 24V
B 0092
Produces up to 400mA charge current. Ideal
for maintaining a 12V lead acid battery.
465W x 320H.
$480
Get Pure AC Mains Power From a Car Battery
BIG & BEEFY 3000W SURGE RATING! Delivers pure sine wave
AC power to difficult loads, such as laptops & game consoles.
12V input, 1000W continuous rated. 274 x 131 x 83mm.
Sale Ends March 31st 2018
Phone: 1300 797 007 Fax: 1300 789 777
Mail Orders: mailorder<at>altronics.com.au
26.95
$
LC Meter Shield Kit
SAVE $119
$
5W Solar Charger Module
59
$
K 8102
12.95
$
K 9650
Arduino Keypad Plate
Pefect for Arduino based access
control, security and automation
designs, this handy wallplate
has the atmega328p chip on
board and is suitable for use with
standard shields.
K 9805
Heart Rate For Arduino Kit
(DIYODE Nov ‘17) A simple kit design for
biometric Arduino projects - or anything where
measuring a heartbeat is required. Requires
9V battery (S 4970B $3.95)
Find your nearest reseller at:
www.altronics.com.au/resellers
Please Note: Resellers have to pay the cost
of freight and insurance and therefore the
range of stocked products & prices charged
by individual resellers may vary from our
catalogue.
© Altronics 2018. E&OE. Prices stated herein are only valid until date shown or until stocks run out. Prices include GST and exclude
freight and insurance. See latest catalogue for freight rates.
View ANY program – even digital TV – on a Vintage TV Set with this
Analog TV audio/
video modulator
1950s’ and 1960s’ TVs are now old enough (and rare enough) to be regarded
as collectable. But how do you enjoy them? You certainly can’t use off-air
signals – they’re now all digital. And the output from a modern VCR or settop box can be far from optimal for driving these old TV sets. This design will
process that signal to provide optimum picture and sound quality.
T
elevision first appeared in Australia in 1956 and was a great
boon for the Australian electronics industry.
As with a vintage radio, you can restore a 1950/60s TV to working order
and an increasing band of collectors
and enthusiasts are doing just that.
But unlike AM radio (where analog
and digital signals still happily coexist), vintage TVs can no longer be
used as originally intended because
of the shut-down of analog TV transmissions.
Of course, it is not only vintage TV
collectors who may need a good signal for displaying on an old TV set.
Every time you see a TV series
which might happen to show a working TV set of the era means that there
80
Silicon Chip
is a need for an optimal signal.
Museums face this problem too and
it is sometimes apparent that their display is far from optimum. After all,
back in the days of black & white TV,
people did not habitually watch poor
quality pictures.
So what is the use of a beautifully
restored TV if you can’t watch anything on it?
The obvious approach is to use a
commercial VHF TV RF modulator or
the modulator in a VCR.
Either of these will accept a composite video signal and audio, which
can come from a digital TV set-top
box (allowing you to watch current
TV channels), a digital media player
By Ian Robertson
Celebrating 30 Years
or a DVD player.
In most cases, provided your TV can
tune to a channel your modulator can
generate, you may get an acceptable
picture and sound on your vintage TV
this way. But chances are that the results will be disappointing.
Depending on the TV and the material you are playing, you may notice symptoms such as diagonal white
lines and buzzing interference in the
sound, spoiling your enjoyment of that
classic movie or TV show. (See adjacent photo.)
Why does this happen?
Well, the short answer is that modern analog TV signals are different to
those that were broadcast in the 1950s
and 1960s.
siliconchip.com.au
The diagonal white lines often seen on older sets are retrace
lines, which are normally hidden but can manifest themselves due to the VBI not being fully blanked. By the way, the
blue cast on these screens is quite typical for sets of the day.
Here’s a “test pattern” which displays a lot of information
about the signal (in this case, after being processed by our
new Video/Audio Modulator). The moiré pattern is caused
by an interaction between screen and camera.
Firstly, in the late 1960s, in readival Test Signal, Time Code and once
ness for colour, the transmitted sound
home video recorders appeared, a
carrier power was quietly reduced
number of copy protection schemes,
from 25% of peak vision power to
notably Macrovision.
10%.
All these systems have three main
The main effect at the time was that
attributes: They became embedded in
many older TVs became more critical
the recorded video, they were virtually
to tune for good sound quality. That
ubiquitous and the VBI portion of the
could be tricky because the tuning for
signal was no longer below ‘‘black”.
best picture (with minimum snow)
Why should this be a problem, since
could result in poor sound.
even vintage TVs have vertical retrace
The second change was the “disblanking circuits?
covery” in the mid-1970s of the VerThe answer is, it turns out to be altical Blanking Interval (VBI) in the
most impossible to fully blank peak
TV signal.
white signals that occur in the VBI
The VBI is effectively the time that
using available internal signals in the
was included in the TV signal to allow
TV with passive circuits.
the scanning beam in the receiver’s
CRT time to return from the bottom
to the top of the screen (vertical
retrace).
Prior to the mid-1970s,
the VBI contained no
information, just a
black signal; actually, it was below the
black signal level.
Then John Adams at Philips in
the UK came up
with the idea of
transmitting text
data in this otherwise wasted interval and Teletext was
born.
Other uses soon This is actually the rear
appeared for the panel of the Modulator – you’d
VBI. Amongst these normally bring all cables in here so it
were Vertical Inter- would be hidden.
siliconchip.com.au
Celebrating 30 Years
Because such VBI manipulation
hadn’t been thought of, early TV designs simply didn’t do it. Even some
early colour TV designs were embarrassed by signals in the VBI and required field modifications.
VBI signals cause another problem.
When fed to most RF modulators, the
peak white excursions of the data in
the VBI completely cut off the AM vision carrier.
This action “punches holes” in the
FM sound carrier, causing an annoying
buzz in the sound. You might remember this buzz from the days when you
operated your TV through the VCR.
So what can be done about it?
You could modify the TV to bypass
the entire RF section and
feed vision and
sound directly to the video
and audio amplifiers.
When done
properly, this
can work very
well but it does
require specific
modifications to
each TV and arguably ruins the originality and authenticity of the set.
And since most vintage TVs used the AGC
to provide contrast control, you will usually lose
this control.
March 2018 81
Fig.1: the structure of an analog video signal around the time of the vertical
blanking interval (VBI), ie, the time between the transmission of each field
(half of an interlaced image). This interval contains a negative sync pulse
(much longer than the horizontal synchronisation pulses) plus a number of
nominally blank lines. In many cases, they might not actually be blank and
that can upset older TV sets.
What is really needed is a device
that will convert modern video signals
into a form suitable for any vintage TV.
To do so, we need to remove all signals during the VBI and return it to
black, clip any peak white excursions
above 1V peak, so they don’t affect the
sound, and generate a TV signal with
a “B&W era” 25% sound carrier.
Then it should provide the best possible picture and sound quality. And
ideally, it should be simple, inexpensive and easy to build!
Many possible design choices were
evaluated. The video processor could
have been implemented digitally but
an analog solution was chosen because
of the lower cost and complexity.
is essentially the same but much longer, lasting for 160s, which is the time
normally taken to scan 2.5 lines.
The remainder of the third line,
plus lines 4 to 17 are blank and finally, the next field starts with line 18. So
it’s these blank lines which may con-
tain unwanted signals that we need
to suppress.
The rest of the time, during normal
picture scanning, it needs to clamp
the maximum signal level to the correct white level and by implication, it
must also adjust the signal to achieve
the correct black level.
Vintage TVs don’t all display an accurate black level but it’s needed anyway to ensure the minimum vision
carrier level of 20% on peak white is
observed, so that the sound is not affected.
Fig.2 shows the signal voltage during the scanning of one line. It starts
with the horizontal blanking interval,
during which time the CRT electron
beam is being swept back to the start
of the next line.
During this time, you can see there
is a short pause (the front porch), followed by the short, negative horizontal
synchronisation pulse, the back porch
(which for colour signals, incorporates
the PAL or NTSC colour burst), then
the visible line interval, during which
the video signal provides the brightness (luminance) information via its
amplitude and, in the case of colour
sets, the chrominance information via
the phase information.
How it works
To reach the goals outlined just
above, three main circuit sections are
required: video processing, audio processing and RF modulation.
The video processing circuitry must
detect the vertical synchronisation
pulse and start a timer which lasts for
the duration of the VBI (1.28ms) so that
it can suppress any extraneous video
signals during this time.
This is illustrated in Fig.1, which
shows how the last two to three lines
of each field are normally blank, containing only horizontal synchronisation pulses, which are negative excursions in the video signal, below
the black level.
The vertical synchronisation pulse
82
Silicon Chip
Fig.2: a PAL image contains 625 lines and each one is transmitted with a
signal as shown here. The front porch and back porch provide a reference
black level for the rest of the signal. The peak-to-peak amplitude, from the
horizontal sync pulse to the white level, is normally 1V. Sometimes signals
can exceed 1V; one of the jobs of the circuit described here is to prevent that
as it can badly affect sound quality by blanking the audio FM carrier.
Celebrating 30 Years
siliconchip.com.au
Fig.3: this
waveform is
a single video
line showing
the relationship
between the
various levels
which can range
between peak
white (1.073V)
and the sync tip
level (0V).
The synchronisation pulses are
nominally 285mV below the black
level while the maximum white level should be about 715mV above the
black level, giving a peak-to-peak voltage of around 1V.
The black level can be determined
by monitoring the average signal level
during either the front porch (just before the horizontal sync pulse) or the
back porch (just after it). This design
uses the back porch since it’s easier
to detect.
The overall design of the unit is
shown in the block diagram, Fig.4.
This shows how the vertical synchronisation pulse is detected by IC2 and
then used to trigger pulse generator
IC5a, which switches the video output
between the version with the limited
white level (clamped by diode D1) to
the version with everything but the
sync pulses removed (clamped by diode D2) during the VBI.
IC2 also detects the back porch period and this is fed to the circuit which
normalises the black level so that the
two clamps limit the video signal at
the right levels.
The processed video and sound are
then fed into audio/video modulator
IC6. This includes an FM audio modulator with tunable carrier oscillator,
RF oscillator for the video carrier and
a double-balanced mixer. The two
variable inductors, L1 and L2, allow
the TV channel and FM sub-carrier
to be tuned.
The sound is processed by applying
an adjustable level of gain and then
passing it through the correct pre-emphasis filter and this is then fed to the
A/V modulator.
The RF modulated output passes
through a low-pass filter and then to
the RF output, which goes to the antenna input of the TV.
siliconchip.com.au
So now that we have discussed what
processing must be done, let’s look
at the operation of the complete circuit, starting with the video processing section.
Circuit description
The full circuit is shown in Fig.5.
The composite video and audio signals
to be sent to the TV are fed into dual
RCA socket CON1. A 75Ω termination
resistor sets the load impedance correctly for the video signal, to eliminate
reflections in the cable.
The video signal is then AC-coupled
to non-inverting input pin 3 of IC1 via
a 47µF capacitor and biased to 2.5V
(half the 5V supply) by a pair of 10kΩ
resistors.
IC1 is a video (wide-bandwidth)
op amp which acts as a non-inverting
buffer and also provides a gain of two,
ie, doubling the signal amplitude.
The gain is set by the ratio of feedback resistors (1 + 4.7kΩ ÷ 4.7kΩ) and
the 47µF capacitor at the bottom of this
divider chain will charge up to the
same bias level as applied to pin 3, so
that the gain is not applied to the DC
offset. That would cause output pin
1 of IC1 to be pegged to the +5V rail.
The signal at this output pin goes to
two different sub-circuits; via a 100nF
capacitor to IC2, the sync separator,
and via a 4.7µF capacitor to emitterfollower buffer transistor Q1.
Let’s look first at what happens
to the signal buffered by Q1. As explained below, the base of Q1 is held
at +1.5V during the back porch interval. This charges up the 4.7µF coupling capacitor.
Because the average voltage of the
back porch is the black level, the black
level of the signal at the base of Q1 becomes 1.5V.
Given the ~0.7V drop between its
base and emitter, that sets the black
level at its emitter to around 0.8V.
The signal at Q1’s emitter passes
through two 1kΩ resistors and then
into inputs B0 and B1 of multiplexer
IC3 (pins 1 & 2).
But there are also two dual schottky
diodes, D1 and D2, connected to these
pins. They are wired in parallel, so
that they act like a single diode with
a higher current rating and lower forward voltage.
Let’s consider the signal at input pin
Fig.4: block diagram of the Modulator. IC2 detects the vertical sync pulse
and starts timer IC5a, which controls an analog switch that changes the
video output to a version containing only sync pulses during the vertical
blanking interval. The rest of the time, D1 and IC2 combine to prevent
signal levels above the maximum white level from passing through to the
modulator, which also receives the processed audio. Variable inductors L1
and L2 allow the two carriers to be tuned.
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March 2018 83
B0 (pin 2) first. The cathodes of D1 are
held at 2V by buffer op amp IC4c.
This reference level is generated
from a string of four resistors across
the regulated 5V rail. Given that schottky diode D1 will have a forward voltage of around 0.2V when conducting,
this means that input pin B0 will be
clamped at a maximum of around 2.2V.
This is 1.4V above the black level that
we determined earlier would be present
at the emitter of Q1 (ie, 2.2V - 0.8V).
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Silicon Chip
Since we’ve applied a gain of two to
the signal, that represents an increase
of 700mV (1.4V ÷ 2) above the black
level in the original signal; very close
to the 715mV mentioned earlier for the
correct white level. So D1 prevents the
signal at pin 2 of IC3 from exceeding
the desired white level.
During active line scanning, the signal at input pin 2 (B0) is fed through
to output Bn (pin 15), which drives
the base of PNP emitter-follower Q2.
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Thus, Q2 buffers the video signal
which is then fed through a 75Ω impedance-matching resistor and 470µF
DC-blocking capacitor to the video
output socket.
Note that the 75Ω resistor will form
a voltage divider with the 75Ω cable
impedance/input impedance of the TV.
Since IC1 already applied a gain of
two to the video signal, the TV will
receive a signal with the correct amplitude.
siliconchip.com.au
Fig.5: complete circuit of the Modulator. The video signal is buffered by IC1 (which also applies some gain), then
buffered again by Q1 and clamped by diodes D1 & D2 before passing to analog multiplexer IC3. Its video output is then
fed to another buffer transistor, Q2, and then onto the A/V modulator, IC6. It then generates a signal which is fed to the
RF output, CON2, via a low-pass filter. The audio level is adjusted using VR1 and processed by IC4b before also being
fed to modulator IC6.
Actually blanking the Vertical
Blanking Interval
As mentioned earlier, the video signal from input buffer IC1 also passes
through to IC2.
This is an LM1881 sync separator
and this detects two control signals:
the vertical synchronisation pulses
(shown in Fig.1) and the colour burst/
back porch (shown in Fig.2).
Its pin 3 output goes low for a fixed
period when a vertical synchronisation
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pulse is detected while the pin 5 output goes low during the back porch/
colour burst period.
The vertical sync pulse output from
pin 3 is stretched by IC5a, a 4538 retriggerable monostable multivibrator.
The length of the output pulse is set
by the combination of a 22nF capacitor
and 68kΩ resistor and this time constant was chosen to be equal to the remainder of the VBI.
The signal from the Q output of IC5a
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(pin 6) is fed to logic input S1 of multiplexer IC3 (pin 10). This switches
the source of the video fed to buffer
transistor Q2 to be from input pin B1
(pin 1) rather than Y0 (pin 2) so that
during the VBI, the video signal sent
to the TV set contains only the horizontal synchronisation pulses and is
otherwise black.
The signal fed to input B1 is similar
to the signal described earlier at B0,
except that it is clamped by diode D2
March 2018 85
Fig.6: use this PCB overlay diagram as a guide during assembly. Most of the
passive components, with the exception of the electrolytic capacitors, are
surface-mounted, as are all the semiconductors, with the exception of IC6. Be
careful to fit the ICs and electrolytic capacitors with the correct polarity.
rather than D1. D2’s cathode is connected to a 0.6V reference level which is
buffered by op amp IC4a (derived from
the same divider string as the 2.0V reference mentioned earlier).
Since the black level of the video
signal at the emitter of Q1 is around
0.8V, taking into account the ~0.2V
forward voltage of D2, this diode will
prevent any signal levels above the
black level from passing through to
input B1. Thus, the synchronisation
pulses (which are negative) can get to
input B1 but anything else during the
VBI will be clipped off.
As a result, anything other than the
sync pulse that may come from the
video source during the VBI is not fed
through to the TV.
By the way, because of the bias requirements of the vision modulator
and the need to allow for diode drops,
the reference voltages generated by the
resistor chain are quite critical and inter-dependent.
A spreadsheet was used to calculate
the best fit, using preferred-value resistors, to avoid the need for adjustments.
The back porch and
black reference level
I explained earlier that the base of
Q1 is held at +1.5V during the back
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Silicon Chip
porch to set the correct black reference
level. This reference level comes from
the output of op amp IC4d, which is
in turn driven from the same four-resistor reference divider that produces
the other two reference voltages.
The output of IC4d drives the base of
Q1 when input A0 (pin 12) of analog
multiplexer IC3 is connected to its
respective An output (pin 14) when
logic input S0 (pin 11) is low. This
logic input is driven by the Cn output of the multiplexer, (pin 4). This
part of the multiplexer is being used
as a logic gate.
Since input C1 (pin 3) is tied high to
+5V and input C0 (pin 5) is connected
to the back porch/colour burst output
of sync separator IC2, output Cn will
only be low during the back porch period (ie, output pin 5 of IC2 is low) and
when input S2 (pin 9) is low.
And input S2 is low most of the
time but is driven high during the VBI,
by the output of IC5a that was mentioned earlier.
So basically, the base of Q1 is held
at the +1.5V reference level during the
back porch, except for during the VBI.
This means that the black level of
the signal is “reset” at the beginning
of each horizontal scan line but it is
left unaltered during the VBI since
other signals that are present during
the VBI can be falsely detected as the
back porch and thus could result in
incorrect biasing.
The 4.7µF capacitor at the base of
Q1 has a high enough value to preserve
the correct DC levels during the VBI.
Audio processing
The audio signal from CON1 is fed
to audio gain/volume control pot VR1
and then AC-coupled to non-inverting
input pin 5 of the remaining op amp,
IC4b. The signal is biased to a halfsupply (~2.5V) level using two 100kΩ
This same-size
photo matches
the above
component
overlay in most
respects, but
is of an early
prototype and
so has a number
of patches
and added
components
(particularly
around IC3).
The final PCB
design above has
these changes
incorporated.
Celebrating 30 Years
siliconchip.com.au
resistors. A fixed gain of 11 times is
applied, set by the ratio of the 100kΩ
and 10kΩ resistors. Again, the bottom
end of the divider is connected to a capacitor to ground, so that the DC bias
of the inverting input and the output
will also settle at 2.5V.
A simple filter network comprising a
parallel 1nF capacitor and 56kΩ resistor provide audio pre-emphasis with a
time constant of 50µs (treble boost), as
required for the following FM modulator. The audio signal is AC-coupled
to the modulator via a 470nF series
capacitor so that the signal can be biased to 1.7V, to suit the modulator; this
level is derived from the 12V rail using 180kΩ and 30kΩ resistors.
RF modulator
IC6, the MC1374, is designed specifically for this sort of job. Along with
the audio signal just mentioned, which
is fed into pin 14, The video signal at
CON4 is also fed into IC6, at input pin
11. A 47pF capacitor to ground filters
out any RF which may be present in
the video signal, preventing it from affecting the operation of the modulator.
The MC1374 contains an RF oscillator, RF modulator and a phase shift
type FM modulator, arranged to permit
good PC board layout of a complete
TV modulation system. The RF oscillator can operate up to approximately
105MHz, which makes it suitable for
Band 1 VHF. The video modulator is
a balanced type.
The choice of the MC1374 may seem
unwise as this part is no longer in production. However, it is readily available from many sources on the web
at a reasonable price. This is a much
better situation than most that TV restorers have experienced!
SILICON CHIP will have a stock of
this IC available in the Online Shop,
so you can order it at the same time
as the PCB.
The modulated sound carrier and
composite video information are fed
in separately, to pins 1 and 11 respectively, to minimise crosstalk. The RF
output is a current sink which can
drive a 75Ω load.
Note that the PNP video buffer transistor, Q2, is not just used to provide
a low impedance drive for the output
socket. It also allows us to shift the
video signal DC bias level to around
3.9V, as is required by IC6, to set the
correct black level. (Note that due to
the way IC6 works, the same DC bias
siliconchip.com.au
Parts list – Audio/Video Modulator
for Analog (Vintage) TV sets
1 130x100x50mm light grey ABS instrument case [Altronics H0371]
1 double-sided PCB, 100 x 88mm, code 02104181
1 150nH variable inductor (L1) [CoilCraft 7M2-151] OR 1 SBK-71K coil former pack
(SILICON CHIP Online Shop Cat SC2746) plus 100mm length of 0.25mm diameter
enamelled copper wire
1 10H variable inductor (L2) [CoilCraft 7M2-103] OR 1 SBK-71K coil former pack
[SILICON CHIP Online Shop Cat SC2746) plus 900mm length of 0.25mm diameter
enamelled copper wire
2 220nH SMD inductors, 2012/0805 package
1 2-way PCB-mount RCA socket, red/white (CON1) [Altronics P0210]
2 black PCB-mount low-profile RCA sockets (CON2,CON4) [Altronics P0207]
1 2.1mm or 2.5mm ID PCB-mount DC socket (CON3)
1 12V DC regulated plugpack with plug to suit CON3
5 No.4 x 6mm self-tapping screws
Semiconductors
1 LMH6642 high-bandwidth op amp, SOT-23-5 (IC1)
1 LM1881 sync separator, SOIC-8 (IC2)
1 74HC4053 triple two-channel analog multiplexer, SOIC-16 (IC3)
1 MCP6004 quad op amp, SOIC-14 (IC4)
1 74HC4538 dual monostable multivibrator, SOIC-16 (IC5)
1 MC1374P A/V modulator, DIP-14 (IC6) [Silicon Chip Online Shop Cat SC4543]
1 LM7805S 5V 1A regulator, TO-263 (REG1) OR
1 7805 5V 1A regulator, TO-220, with leads cut short and bent to fit (see text)
1 BC847 NPN transistor, SOT-23 (Q1)
1 BCX17 PNP transistor, SOT-23 (Q2)
2 BAT54C dual schottky diodes, SOT-23 (D1,D2)
1 40V 1A SMD schottky diode, SMA package (D3) [MBRA140T3 or similar]
Capacitors (all SMD 2012/0805, 16V X7R unless otherwise stated)
3 470F 16V radial electrolytic
5 47F 16V radial electrolytic
1 4.7F
6 470nF
2 100nF
1 22nF
3 10nF
3 1nF
1 68pF
3 47pF
1 39pF
1 22pF
Resistors (all SMD 2012/0805, 1%)
1 680kΩ
1 180kΩ
3 100kΩ
1 68kΩ
1 56kΩ
1 30kΩ
1 18kΩ
3 10kΩ
1 6.34kΩ
1 5.6kΩ
2 4.7kΩ
2 3.3kΩ
1 3.0kΩ
2 2.2kΩ
2 1kΩ
3 470Ω
2 150Ω
1 100Ω
3 75Ω
1 10kΩ 9mm horizontal log pot with long 18-tooth spline shaft (VR1) [Altronics
R1918]
level is used for pin 1).
This shift is due partly to the ~0.7V
base-emitter junction forward voltage
and partly because of the voltage divider comprising two 150Ω resistors
between Q2’s emitter and the 5V rail.
These two resistors also reduce the AC
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amplitude of the video signal by half,
compensating for the gain of two that
was applied earlier by IC1.
IC6 contains two internal oscillator
amplifiers which drive the RF tank
between pins 6 and 7, to generate the
video carrier, and the FM carrier tank
March 2018 87
supplies the rest of the circuitry. It too
has a 470F output filter capacitor.
Construction
The PCB attaches to the rear panel via a single screw on the input socket; the
assembly is held in the case via four self-tapping screws while the rear panel
slots into the vertical guides in the case. This holds the whole thing rigid.
between pins 2 and 3, to generate the
audio carrier.
Both of these tanks are based on
variable inductors, to allow them to
be tuned to the required frequencies,
as well as capacitors, to make them
resonant.
Since the video carrier, at 50100MHz, is at a much higher frequency
than the audio carrier (5.5MHz), the inductance value of L1 (0.15µH) is much
lower than L2 (10H).
This unit is not crystal locked
but tuned to operate on channel 2
(64.25MHz), since this channel is now
unused and able to be tuned by any TV.
It is a simple matter to re-tune it to any
band 1 channel (1, 2 or 3).
Note that it may be possible to tune
to channels 0 or 4 but neither of these
can be received by early TVs with
10-channel VHF tuners, so they would
not be good choices. Later Australian
sets had 13-channel tuners.
The design could have used a crystal for maximum stability but a suitable custom crystal would be expensive and the LC oscillator stability is
excellent anyway. A PLL could also
have been used but would have greatly
increased complexity.
The configuration of the video RF
tank (a parallel resonant circuit) is
pretty much identical to the sample
circuit in the MC1374 datasheet, with
the exception being the 10nF capacitor; its suggested value was 1nF in
the data sheet. Its purpose is to filter
the applied supply voltage, so a larger
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Silicon Chip
value should be better.
Similarly, the FM carrier oscillator components (series resonant) are
very similar to those specified in the
MC1374 data sheet with the only real
difference being the values of the 47pF
and 68pF load capacitors, which have
been tweaked to work better with the
properties of inductor L2.
The balanced modulator gain resistor is the recommended value, at
2.2kΩ. This controls the modulation
depth at the output.
The output is terminated with a
75Ω resistor from the 12V rail, which
also supplies current to the modulator circuitry.
The output signal then passes
through a double-pi low-pass LC filter (fifth order) to clean up the sidebands. It would have been better to use
a proper “vestigial sideband filter” but
these require tuning.
The downside of this simple approach is that it’s possible to tune the
TV to the opposite sideband. However, this will result in poor picture and
sound quality which is easy to identify. In this respect, it’s no different to
typical VCR modulators.
The power supply is simple. We rely
on the plugpack to supply a regulated
12V rail which is used to power the
A/V modulator (IC6) more-or-less directly, via reverse polarity protection
schottky diode D3.
A 470F filter capacitor is provided,
which also acts as the input bypass capacitor for 5V regulator REG1, which
Celebrating 30 Years
As all components mount on a single PCB, construction is relatively
straightforward. The PCB then fits
neatly into the plastic instrument case.
The PCB overlay diagram Fig.6 and
photograph show where all the components go.
Most of the parts are SMDs (surface-mount devices) but there are
some through-hole parts too, notably
the connectors, electrolytic capacitors and IC6.
Because most of the SMDs have
widely-spaced pins, you shouldn’t
have any difficulty soldering them in.
IC1 is the one exception, with closelyspaced leads, but since it only has five
pins (two on one side and three on the
other), it shouldn’t prove too difficult.
Soldering IC1 is a good place to
start. Since it has a different number
of pins on each side, its orientation is
easy to figure. Tack-solder one of the
corner pins (on the side with two pins)
and then check that the other pins are
correctly aligned over their pads using a magnifier.
If not, re-heat the solder and nudge
it into place. Repeat until it’s properly aligned, then solder the other four
pins. This is easier if you apply a little flux paste to the pins first.
Don’t worry about bridging the three
that are close together; if this happens,
simply apply a little flux paste and
then apply some thin solder wick and
heat and the bridges should disappear.
Add some flux paste and re-heat the
initial pin that you tack soldered to
ensure the joint is not cold.
Clean off any residue using alcohol
or flux cleaner and check carefully
under magnification (and with good
light) that all five solder joints have
good fillets. You can then move on to
the other SMD ICs, IC2-IC5.
You can use a similar approach but
you should find these considerably
easier due to the larger pin spacings.
Watch the polarity though; all the other
ICs can be soldered in one of two orientations and only one is correct. Refer
to the photo and the overlay diagram,
Fig.6, to see the correct orientations.
In each case, pin 1 should go towards
the top edge of the board.
Pin 1 of the IC is normally indicated with a dot or divot in that corner,
as well as the pin 1 side having a bevsiliconchip.com.au
elled edge. Make sure the orientation
matches that shown in Fig.6 before
soldering all the pins.
Next, fit diodes D1 & D2 and transistors Q1 & Q2. These are all in 3-pin
SOT-23 packages, similar to IC1 but
since they have fewer pins, the spacings are larger, making them quite easy
to solder.
Just don’t get them mixed up since
they look virtually identical. Use the
same technique as before, tack soldering one pin and then soldering the rest
before reflowing the first joint.
It’s best to solder the passive SMDs
next, ie, the resistors, ceramic capacitors and the two 0.22H chip inductors, L3 & L4. The technique is essentially the same but this time you only
need to make two solder joints per
component.
In each case, make sure it is sitting
straight and flat on the PCB before soldering the second pin.
Also, it’s best to wait for a few seconds after making the first joint before
attempting the second, since if it’s still
liquid, you will end up nudging the
part out of place.
If the component moves when you
go to make the second solder joint,
even though you’ve waited a few seconds, that suggests the first joint hasn’t
adhered to the PCB pad properly.
The SMD resistors will have a code
printed on them to indicate their resistance. For example, a 47kΩ resistor will be marked with either “473”
(ie, 47 x 103) or “4702” (ie, 470 x 102).
However, SMD capacitors will probably not have any markings and the
smaller inductors may not either. If
your DMM has provision for it, measure them to confirm their value before
placement.
The final SMD component is the
regulator, REG1. We have specified
an SMD version of the 7805 since that
is what was used to build the prototype, however, it is possible to mount
a standard 7805 regulator if you bend
the leads so that they will sit against
the PCB and then cut them short so
that they don’t protrude past the ends
of the mounting pads.
Regardless of whether you use an
SMD regulator or adapt a through-hole
type, the tab has a lot of thermal inertia
so we suggest that you spread a thin
layer of flux paste on the large tab as
well as the three smaller pads, turn up
your soldering iron’s temperature and
then solder one of the smaller pins.
siliconchip.com.au
And here’s how it all fits together, immediately before the case top is placed
in position (it only fits one way) and the two case screws are inserted from
underneath and tightened.
You can then check if the tab is properly located and start applying solder
to the junction of the tab and the PCB.
You will probably have to hold the
iron there for some time (10 seconds
or more) to get the regulator and PCB
hot enough for the solder to flow.
Once that happens, feed the solder
in and then quickly remove the iron
and you should get a nice fillet between the tab and PCB. You can then
solder the remaining pins.
Alternatively, if you have a hot air
rework station, you can apply solder
paste and then carefully heat the regulator and surrounding PCB area with
hot air until the solder melts.
Through-hole parts
There are just a few through-hole
parts and most of them are easy to
solder. Start with IC6, being careful to
ensure it’s correctly orientated before
soldering it in place. We don’t suggest
that you use a socket; it’s better to solder the IC directly to the PCB.
Follow with the electrolytic capacitors. They are different sizes so
it should be obvious where each one
goes but do pay careful attention to
orientation. The longer lead goes into
the hole marked + on the PCB and in
Fig.6, while the opposite side (ie, negative end) of the can should be marked
Celebrating 30 Years
with a stripe.
Fit RCA connectors CON2 and
CON4 next, followed by DC socket
CON3. In each case, ensure the connector is pushed fully down onto the
board before soldering the pins.
Inductors L1 and L2
While you can purchase these inductors from the CoilCraft website, if
you’re only buying two then the postage charge will be prohibitive.
Luckily though, the CoilCraft parts
have an identical footprint to the SBK71K coil formers that we already stock
in the SILICON CHIP Online Shop for
other projects. These are supplied with
a ferrite slug which can be adjusted
for tuning the oscillators, just like the
CoilCraft parts.
Wind inductors L1 and L2 using the
following procedure:
1) cut a ~900mm length of 0.25mm diameter enamelled copper wire and
strip the insulation off one end (by
about 5mm) using a sharp hobby
knife or emery paper.
2) tin the end of the wire and wrap it
around one of the pins at either end
of the side which has three pins (ie,
not the middle pin).
3) push the wire as close to the base
of the former as possible and solder
it to the pin. Be quick since if you
March 2018 89
apply too much heat, the pin could
come out of the former.
Try to avoid getting too much solder on
the rest of the pin since that could
prevent it from being inserted into
the PCB later.
4) pass the wire up the side of the former, through the notch in the base
and wrap it around the cylindrical shaft.
5) wind 45 turns as neatly as possible. With wire this fine, it’s almost
impossible to do it layer-by-layer
but it’s best to avoid making it a total jumble.
Keep the turns below the collar that’s
about 2/3 of the way up the cylinder,
so that they can’t slip over the top.
6) bring the last turn down to the opposite pin on the side with three
pins and cut the remainder off. Strip
the insulation from the end of the
wire, tin it, wrap it around that pin
and solder it in place as you did
the other end. See the below photo
for an idea of what the finished coil
should look like.
7) measure the resistance between the
two pins. You should get a reading
of 0.25-0.3Ω (remember that your
multimeter leads will have some
resistance so if possible, short them
and null/zero it before making the
measurements).
If you have an inductance meter, you
can measure the coil now. It should
be around 8µH.
8) screw the ferrite slug into the top
of the former until it’s fully inside
and then place the shield can over
the top, with its mounting flanges
on the sides not occupied by pins.
9) L2 is now complete. Use the same
procedure to wind L1, except that
only five turns of wire are required.
The resistance should be much lower – under 0.1Ω.
Having finished winding the two
coils, solder them in place where
You can buy L1 and L2 pre-made but
winding them yourself, using SBK-71K
coil formers from the SILICON CHIP
Online Shop, will prove much cheaper.
L1, 150nH, (5 turns) is on the left, while
L2, 10µH, (45 turns) is on the right.
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Silicon Chip
shown in Fig.6. Make sure you don’t
get them mixed up. L2 is the one with
more turns and a higher winding resistance.
Final assembly
All that’s left now is potentiometer
VR1 and dual RCA socket CON1. Fit
these both where shown in Fig.6; try to
keep the pot shaft parallel to the PCB
while you solder its mounting pins.
You can then slip the rear panel over
the connectors and pot shaft and lower the whole assembly into the bottom
of the case.
Affix it to the base using four selftapping screws.
Tuning and testing
There are only three adjustments
to make: tuning the vision carrier and
sound sub-carrier by adjusting the
values of L1 and L2 respectively and
adjusting pot VR1 to give the correct
sound level.
Our prototype drew 42mA at 12V,
so a good way of checking that you
have assembled your unit correctly is
to connect a DMM set to measure milliamps in series with the 12V power
supply when you first power it up.
If you get a reading between about
30mA and 50mA then that suggests
there are no serious faults and it’s probably working correctly.
Having verified that the circuit is
drawing an appropriate amount of
current, the next step is to adjust the
two oscillators by turning the tuning
slugs in L1 and L2 with a plastic adjustment tool.
We’ve come up with three procedures for this, depending on what
equipment you have.
The easiest one is if you have a spectrum analyser. Connect it to the RF output, power the unit up and adjust L1
so that the largest peak is centred on
64.25MHz. Adjust L2 so that the smaller peak is centred on 69.75MHz. You
will likely see an image of the carrier
11MHz below this (ie, 5.5MHz below
the main peak); ignore that one.
If you have a 100MHz+ oscilloscope, connect a tight loop of wire to
the end of one of the probes and place
it near the 39pF capacitor just above
L1. Don’t make a direct connection to
the circuit or you may pull the oscillator off-frequency.
Adjust L1 to read 64.25MHz on the
scope display. Then move the probe
coil near the 68pF capacitor between
Celebrating 30 Years
L2 and IC6 and adjust L2 for a reading of 5.5MHz.
If you don’t have equipment that can
read these frequencies, the simplest
approach is to hook the RF output of
the unit up to the antenna input on an
analog TV that you know works, tune
the TV to channel 2 and feed some
video into the input.
If TV has automatic fine-tuning
(AFT), turn it off.
Adjust L1 so that image just breaks
up at the edge of the sound carrier.
Back it off until you have a clear image.
If you encounter significant ringing
in the image while you are tuning, you
are attempting to tune to the wrong
sideband. Wind the core right out and
start from the top position.
Once you have a clear picture, you’ll
need to tune the sound. It helps to display an image with a lot of white text,
such as a DVD copyright message.
Tune L2 for minimum noise in the
sound – the correct adjustment is a
definite null, either side of which the
noise increases.
Connect an audio signal to the unit’s
input and turn up VR1 (to about halfway) to verify that the sound is properly fed through.
If you adjusted L1 and L2 without using a TV, now is a good time to
hook the unit up to a TV and tune in
to channel 2.
With nothing connected to the video or audio inputs, you should get a
black screen and silence. Then all you
need to do is plug in a video and audio
source and verify that you get a clean
picture and sound.
As for setting VR1, which controls
the audio modulation depth, basically, you just need to turn it up as high
as possible before you notice any distortion in the sound, then back it off
a little bit.
If you can’t get the unit to work,
feed the Video Out signal to the A/V
input on a modern TV while feeding a
video signal into the input and check
that you get a good picture. That will
verify that the video processing circuitry is working OK. If not, check the
circuitry around ICs1-5.
If you can verify that the video output is working correctly but you still
can’t tune into a signal on your vintage
TV, that suggests a problem with IC6
or one of its associated components,
including L1 and L2.
Re-check that you have tuned the
two oscillators correctly.
SC
siliconchip.com.au
Vintage Radio
By Associate Professor Graham Parslow
Philips 1953 portable
5-valve model 148C radio
Photo courtesy of Kevin Poulter, President of HRSA
The Philips 148C was one of a series of portable radios produced by
Philips under different brand names, including Mullard and Fleetwood.
All had the same construction and broadly similar circuitry. Their
common case was an interesting design, with all controls and the
dial concealed by a shutter. Finally, the case panels were made from
aluminium, a fairly exotic material in the later 1940s and 1950s.
We now take the aluminium can
for granted since billions of them are
made every year. However the first
aluminium products were extremely
expensive. The original Auld Mug of
1857 (The America’s Cup) was made
of aluminium and predated industrial production that commenced
in 1888.
Two world wars necessitated quantity production of aluminium for aircraft. Aluminium gathered mystique
from its use in aircraft while becoming
ever more available for other uses in
siliconchip.com.au
the 1940s. It is surprising that Philips
were one of the few radio manufacturers to use it for making a case, although RCA in America manufactured
a nearly identical case.
Regardless of the lightness of aluminium, the weight of the Philips 148C
is a substantial 6.3kg, even without
batteries. In fact, it is only the outer
panels which are made from aluminium while the end panels are of Bakelite. The chassis is steel and the internal construction is fairly conventional
for the time.
Celebrating 30 Years
The Philips 148C is a full-featured
superhet with an RF stage. With the
exception of the full-wave rectifier
(which is a 6V4 in my set but could be
an EZ82), all of the miniature valves
are battery types such as 1T4 and 1R5.
Its RF stage makes it a sensitive performer and it readily pulls in weak stations. While it might be thought that
the aluminium panels would offer a
degree of shielding and would thus
reduce signal pickup by the aerial
coils, they have little practical effect
in this regard.
March 2018 91
changing the volume control on one
of these radios because of the way the
shutter-operated switch made access
to the volume pot so difficult.
The front end has two separate
loop coils for the aerial and these are
built into both ends, using the Bakelite mouldings as retainers. Although
the ends look the same externally, the
left and right differ internally to accommodate the coils and their terminations.
As can be appreciated from the accompanying photographs, having two
aerial coils added to the challenge to
set up this radio on the workbench,
after the casing was disassembled for
restoration.
The short fly leads from the radio to
the aerial coils must be unsoldered to
remove the chassis. This means that
temporary wiring is needed to connect the aerial coils for working at
the bench.
Circuit details
Since the Philips 148C has its two aerial coils integrated into the case,
temporary wiring was needed to connect the coils up for testing.
Opening the shutter on the front of
the case reveals the two controls (one
for volume and one for tuning), at opposite ends of the slide-rule dial.
The shutter actually operates the
On-Off switch while the changeover
from battery to mains operation is
achieved by inserting the mains plug
into the socket on the rear of the case.
These switches are worked by
springs and levers that add complexity to the mechanical construction of
the radio. A friend who ran a radio repair shop told me that he spent a day
The aerial coils are wired in series
and act with the first gang of the three
gang tuning capacitor (C1) to provide
RF input to the 1T4 RF preamplifier
valve. A second tuned circuit involving (C2 and L5) feeds signal to the grid
of the 1R5 mixer-oscillator valve. The
1R5 additionally receives tuned input from the local oscillator formed
by C3 and L8.
Apart from the full-wave rectifier which enabled operation from the 240VAC mains, all the valves are miniature battery
types and it is a conventional superhet with a tuned RF amplification stage.
92
Silicon Chip
Celebrating 30 Years
siliconchip.com.au
The intermediate frequency is
455kHz and is selectively passed on
by the first IF transformer to the IF amplifier valve, another 1T4. The two IF
transformers are of the relatively miniature type that Philips developed in
the early fifties. The preceding model,
type 148 of 1950, featured full-size cylindrical IF coils.
The tuning capacitor is also relatively small, with brass plates (not aluminium). Even so, this is still a cluttered
layout with difficult access to many
components, as can be seen from the
picture of the front of the chassis with
the speaker removed.
The 1S5 detector and audio preamplifier has only one diode that serves
the double function of detection and
providing AGC to the first two valves
via resistors R6 & R1 and inductor L5.
The volume control potentiometer changes the signal level fed to the
grid of the 1S5. The preamplified audio signal then passes to a 3V4 pentode output stage proving a modest
level of 250mW or so. In practice this
is quite satisfactory when coupled to
the 6-inch Rola type H speaker.
Oddly, Philips reduced the speaker to a 5-inch unit in later variations
of this radio (model 168). To my ear,
the later ones do not sound as good
as this one.
The one series valves (1T4, 1R5 and
1S5) are the standard set for portables
of the late 1940s and the 1950s, used
by almost every manufacturer. In combination with the 3V4 output pentode
these valves were a proven combination for performance and efficient
battery usage. They are not rare but
the 1R5 and particularly the 3V4 are
prone to fail and are becoming harder
to obtain.
The radio ran at 90V HT with a
drain of 10mA and 9V LT with a drain
of 50mA. For portable operation, the
battery was a combination type incorporating 90V and 9V sections, such as
the Eveready 753, and was connected
via a single plug.
For mains operation, the 6V4 full
wave rectifier produces the HT and
the LT, using ballast resistors to reduce the voltage to 9V for the seriesconnected valve filaments. The “one”
prefix on the valves indicates a nominal filament voltage of 1V, but these
valves barely operate at one volt.
Greater than 1.2V is needed to ensure efficient emission from the filaments. The 3V4 (V5) nominally resiliconchip.com.au
The unrestored aluminium case with the dial shutter closed and badge removed.
The radio does not have an on/off switch, but instead is turned on by opening
the shutter.
quires 3V for the filament, however
this is two 1.5V filaments in series
and in parallel the filaments can work
from 1.5V.
Restoration work
The anodised aluminium case had
developed a patina of green and looked
tired. After cleaning with a degreaser
it was resprayed with an automotive
chrome finish.
Editor’s note: some readers may
object to using a sprayed metal
finish rather than restoring the
original aluminium finish. However, after many decades of use,
surface corrosion, deep scratches
and pitting make it very difficult to obtain anything like the
original finish. Anodising
is not a simple process
and it involves dyes. This
is a satisfactory and practical compromise.
The Bakelite end
pieces were polished
with car wax. The
yellowed dial
cover with a hole (see picture of the
front of the chassis before restoration)
was replaced with acetate sheet, heatmoulded to shape.
This was challenging because the
width needs to be precise to fit into the
This end view
shows part
of the mains
on/off switch
which was
operated by the
shutter at the
front of the case.
Celebrating 30 Years
March 2018 93
This view shows the front of the chassis with speaker removed. Interestingly,
the tuning gang has brass plates, whereas most production tuning gangs at the
time used aluminium plates.
small channels at either end of the dial
and the bottom lip must be reinforced
to remain straight across the span.
A new Philips logo for the centre of
the speaker grille was created by using laser-printed acetate sheet glued
to metal-coated card.
Troubleshooting the circuit
The electrical restoration of this radio proved more challenging. Initially there was no sound at all from the
speaker, using bench supplies to pro-
vide 9V LT and 90V HT via the battery
plug (see the picture of the bench arrangement).
The 9V supply current was 50mA,
indicating continuity of the heater
filaments. In valve portables there is
no visible glow of the filaments to indicate open-circuit heaters so current
measurement is an important diagnostic tool.
But the 90V line was drawing only
3mA (whereas it should have been
10mA or more, if everything was work-
ing). For reasons that I suspect relate
to operating at a relatively low voltage, portable valves have a high frequency of failure of pin connections
and I routinely clean the pins before
powering up.
A signal tracer at the volume control
showed that detected (rectified) audio was being delivered from the 1S5.
Since there was absolutely no sound
from the speaker, it was detached and
its voice coil checked for continuity.
It was OK.
Detaching the speaker also gave access to many components otherwise
inaccessible (see the picture of the
front of the chassis).
The next fault possibility suggested
by the low HT current was an open-circuit primary in the output transformer.
This annoyingly common fault
proved to be the case. When the output transformer is open-circuit there
is no HT to the anode of the 3V4 output valve so it cannot conduct current.
Then came an “Oh bother” moment
because the speaker transformer nuts
and bolts were buried behind other
components and the upper superstructure made the transformer captive, even if the bolts were removed.
The practical solution was to add a
replacement transformer to a bracket
below the speaker mounting and leave
the original in place.
This will prevent a standard size
battery being housed in that space.
However, this set has a mains power
Even though the case was manufactured from aluminium panels, the chassis was made from plated steel and in other
respects the construction was entirely conventional. Surprisingly, not many of the paper capacitors needed to be replaced.
94
Silicon Chip
Celebrating 30 Years
siliconchip.com.au
supply, so it was a reasonable sacrifice.
But sadly the radio was still not
working after replacing the output
transformer. This led to measuring
voltages around the 3V4 and checking whether audio was delivered to
the grid.
The result was flabbergasting. A blue
wire from IF transformer 2 might have
provided screen voltage but it was soldered to pin 6 which is not connected. The audio feed from the 1S5 was
connected to pin 3 (the screen) rather
than pin 6 (the grid) that had nothing
at all connected.
My first thought was that the cowboy who did this had incorrectly
counted the pins anticlockwise rather than clockwise to create this mess,
but that did not explain the mistakes.
It was a case of that person having the
wrong data for the valve and/or incomprehensible stupidity.
The picture of the components under the chassis shows the radio after
the correct pin connections were sorted out for the 3V4. But even then, the
radio still did not work. The feed capacitor from the 1S5 to the 3V4 (C20)
was replaced but there was no audio
signal passing through.
Finally, checking voltages at the 1S5
revealed the last problem. There was
no screen voltage because R9 (3MW)
had gone open-circuit. Replacing R9
was the last step to restoring normal
function.
Luckily, the 1S5 still acted as a detector even when it could not function
as an audio preamplifier.
After fixing the problems, the radio
was run from the 230VAC mains using a proprietary plug inserted into the
rear of the case. The power transformer and mains socket are awkwardly
tacked on below the main chassis at
the left-hand side and multiple wires
lead up to the 6V4 rectifier and switching circuit mounted at the top.
Everything about the mechanical
and electrical construction of this radio
is challenging. However, all is well that
ends well. It was gratifying to restore
this radio to a good final appearance
and excellent performance.
SC
Not all of these portables made by Philips were equipped for mains operation
as can be seen by the add-on section above involving the 6V4 full-wave rectifier
just below the orange label.
Philips sold this radio under three
brand names: Philips Model 148C (as
shown to the right), Fleetwood Model
1052D and Mullard Australia MABS
1052. The valve line-up was the same
for each brand.
siliconchip.com.au
Celebrating 30 Years
March 2018 95
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PRE-PROGRAMMED MICROS
Price for any of these micros is just $15.00 each + $10 p&p per order#
As a service to readers, SILICON CHIP ONLINESHOP stocks microcontrollers and microprocessors used in new projects (from 2012 on) and
some selected older projects – pre-programmed and ready to fly!
Some micros from copyrighted and/or contributed projects may not be available.
PIC12F675-I/P
PIC12F675-I/P
PIC16F1455-I/P
PIC16F1507-I/P
PIC16F88-E/P
PIC16F88-I/P
PIC16LF88-I/P
PIC16LF88-I/SO
PIC16LF1709-I/SO
UHF Remote Switch (Jan09), Ultrasonic Cleaner (Aug10),
Ultrasonic Anti-fouling (Sep10), Cricket/Frog (Jun12), Do Not Disturb (May13)
IR-to-UHF Converter (Jul13), UHF-to-IR Converter (Jul13)
PC Birdies *2 chips – $15 pair* (Aug13), Driveway Monitor Receiver (July15)
Hotel Safe Alarm (Jun16), 50A Battery Charger Controller (Nov16)
Kelvin the Cricket (Oct17), Triac-based Mains Motor Speed Controller (Mar18)
Courtesy LED Light Delay for Cars (Oct14), Fan Speed Controller (Jan18)
Microbridge (May17)
Wideband Oxygen Sensor (Jun-Jul12)
Hi Energy Ignition (Nov/Dec12), Speedo Corrector (Sept13),
Auto Headlight Controller (Oct13), 10A 230V Motor Speed Controller (Feb14)
Automotive Sensor Modifier (Dec16)
Projector Speed (Apr11), Vox (Jun11), Ultrasonic Water Tank Level (Sep11)
Quizzical (Oct11), Ultra LD Preamp (Nov11), 10-Channel Remote Control
Receiver (Jun13), Revised 10-Channel Remote Control Receiver (Jul13)
Nicad/NiMH Burp Charger (Mar14), Remote Mains Timer (Nov14)
Driveway Monitor Transmitter (July15), Fingerprint Scanner (Nov15)
MPPT Lighting Charge Controller (Feb16), 50/60Hz Turntable Driver (May16)
Cyclic Pump Timer (Sep16), 60V 40A DC Motor Speed Controller (Jan17)
Pool Lap Counter (Mar17), Rapidbrake (Jul17)
Garbage Reminder (Jan13), Bellbird (Dec13), GPS Analog Clock Driver (Feb17)
LED Ladybird (Apr13)
Battery Cell Balancer (Mar16)
6-Digit GPS Clock (May-Jun09), Lab Digital Pot (Jul10), Semtest (Feb-May12)
Batt Capacity Meter (Jun09), Intelligent Fan Controller (Jul10)
GPS Car Computer (Jan10), GPS Boat Computer (Oct10)
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
Micromite LCD BackPack [either version] (Feb16), GPS Boat Computer (Apr16)
Micromite Super Clock (Jul16), Touchscreen Voltage/Current Ref (Oct-Dec16)
Micromite LCD BackPack V2 (May17), Deluxe eFuse (Aug17)
Micromite DDS for IF Alignment (Sept17)
PIC32MX170F256B-I/SP
Low Frequency Distortion Analyser (Apr15)
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)
Digital Effects Unit (Oct14)
PIC32MX470F512H-120/PT Micromite PLUS Explore 64 (Aug 16), Micromite Plus LCD BackPack (Nov16)
PIC32MX470F512L-120/PT Micromite PLUS Explore 100 (Sep-Oct16)
dsPIC33FJ128GP802-I/SP Digital Audio Signal Generator (Mar-May10), Digital Lighting Controller
(Oct-Dec10), SportSync (May11), Digital Audio Delay (Dec11)
Quizzical (Oct11), Ultra-LD Preamp (Nov11), LED Musicolor (Nov12)
dsPIC33FJ64MC802-E/P
Induction Motor Speed Controller (revised) (Aug13)
dsPIC33FJ128GP306-I/PT CLASSiC DAC (Feb-May 13)
ATTiny861
Thermometer/Thermostat (Mar10), Rudder Position Indicator (Jul11)
PIC16F877A-I/P
PIC16F2550-I/SP
PIC18F4550-I/P
PIC32MX795F512H-80I/PT
When ordering, be sure to nominate BOTH the micro required AND the project for which it must be programmed.
SPECIALISED COMPONENTS, HARD-TO-GET BITS, ETC
NEW THIS MONTH:
AM RADIO TRANSMITTER
- MC1496P double-balanced mixer IC (DIP-14)
VINTAGE TV A/V MODULATOR
- MC1374P A/V modulator IC (DIP-14)
- SBK-71K coil former pack (two required)
P&P – $10 Per order#
STATIONMASTER (CAT SC4187)
(MAR 18)
$2.50
(MAR 17)
Hard to get parts: DRV8871 IC, SMD 1µF capacitor and 100kW potentiometer with detent
$12.50
ULTRA LOW VOLTAGE LED FLASHER (CAT SC4125)
(FEB 17)
kit including PCB and all SMD parts, LDR and blue LED $12.50
$5.00
$5.00 ea.
SC200 AMPLIFIER MODULE (CAT SC4140)
(JAN 17)
hard-to-get parts: Q8-Q16, D2-D4, 150pF/250V capacitor and five SMD resistors
$35.00
ALTIMETER/WEATHER STATION
(DEC 17)
Micromite 2.8-inch LCD BackPack kit programmed for the Altimeter project
$65.00
60V 40A DC MOTOR SPEED CONTROLLER (CAT SC4142)
(JAN 17)
GY-68 barometric pressure and temperature sensor module (with BMP180, Cat SC4343) $5.00
hard-to-get parts: IC2, Q1, Q2 and D1
$35.00
DHT22 temperature and humidity sensor module (Cat SC4150)
$7.50
Elecrow 1A/500mA Li-ion/LiPo charger board (optional, Cat SC4308)
$15.00
VARIOUS MODULES
WiFi Antennas with U.FL/IPX connectors (Water Tank Level Meter with WiFi, FEB18)
PARTS FOR THE 6GHz+ TOUCHSCREEN FREQUENCY COUNTER
(OCT 17)
5dBi – $12.50
2dBi (omnidirectional) – $10.00
Explore 100 kit (Cat SC3834; no LCD included)
$69.90
NRF24L01+PA+NA transceiver with SNA connector and antenna (El Cheapo 12, JAN18)
$5.00
one ERA-2SM+ & one ADCH-80A+ (Cat SC1167; two packs required)
$15.00/pack
WeMos D1 R2 board (Logging data to the ‘net using Arduino, SEPT17)
$15.00
Geeetech Arduino MP3 shield (Arduino Music Player/Recorder, VS1053, JUL17)
$20.00
DELUXE EFUSE PARTS
(AUG 17)
IPP80P03P4L04 P-channel mosfets (Cat SC4318) $4.00 ea. AD9833 DDS module (with gain control) (for Micromite DDS, APR17) $25.00
$15.00
BUK7909-75AIE 75V 120A N-channel SenseFet (Cat SC4317) $7.50 ea. AD9833 DDS module (no gain control) (El Cheapo Modules, Part 6, APR17)
CP2102 USB-UART bridge
$5.00
LT1490ACN8 dual op amp (Cat SC4319) $7.50 ea.
microSD card adaptor (El Cheapo Modules, Part 3, JAN17)
$2.50
ARDUINO LC METER (CAT SC4273)
(JUN 17)
DS3231 real-time clock with mounting spacers and screws (El Cheapo, Part 1, OCT16)
$5.00
1nF 1% MKP capacitor, 5mm lead spacing
$2.50
TOUCHSCREEN VOLTAGE/CURRENT REFERENCE
(DEC 16)
MICROBRIDGE COMPLETE KIT (CAT SC4264)
(MAY 17)
Micromite LCD BackPack kit (programmed to suit) PLUS UB1 Lid (Cat SC4074)
$70.00
PCB plus all on-board parts including programmed microcontroller (SMD ceramics for 10µF) $20.00
Laser-cut matter black or blue lid (to suit UB1 Jiffy Box)
$10.00
SHORT FORM KIT with main PCB plus onboard parts (not including BackPack
MICROMITE LCD BACKPACK V2 – COMPLETE KIT (CAT SC4237)
(MAY 17)
includes PCB, programmed micro, touchscreen LCD, laser-cut UB3 lid, mounting hardware,
module, jiffy box, power supply or wires/cables) (Cat SC3987)
$99.00
SMD Mosfets for PWM backlight control and all other on-board parts $70.00
MICROMITE PLUS EXPLORE 100 *COMPLETE KIT (no LCD panel)* (SEP 16)
(includes PCB, programmed micro and the hard-to-get bits including female headers, USB
POOL LAP COUNTER
(MAR 17)
and microSD sockets, crystal, etc but does not include the LCD panel) (Cat SC3834)
$69.90
two 70mm 7-segment high brightness blue displays plus logic-level Mosfet (Cat SC4189) $17.50
laser-cut blue tinted UB1 lid, 152 x 90 x 3mm (Cat SC4196) $7.50
(MAR 18)
THESE ARE ONLY THE MOST RECENT MICROS AND SPECIALISED COMPONENTS. FOR THE FULL LIST, SEE www.siliconchip.com.au/shop
*All items subect to availability. Prices valid for month of magazine issue only. All prices in Australian dollars and included GST where applicable. # P&P prices are within Australia. O’seas? Please email for a quote
03/18
PRINTED CIRCUIT BOARDS
NOTE: The listings below are for the PCB only – not a full kit. If you want a kit, contact the kit suppliers advertising in this issue.
For more unusual projects where kits are not available, some have specialised components available – see the list opposite.
NOTE: Not all PCBs are shown here due to space limits 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!
PRINTED CIRCUIT BOARD TO SUIT PROJECT:
PUBLISHED:
PCB CODE:
Price:
CLASSiC DAC MAIN PCB
APR 2013
01102131 $40.00
CLASSiC DAC FRONT & REAR PANEL PCBs
APR 2013
01102132/3 $30.00
GPS USB TIMEBASE
APR 2013
04104131 $15.00
LED LADYBIRD
APR 2013
08103131
$5.00
CLASSiC-D 12V to ±35V DC/DC CONVERTER
MAY 2013
11104131 $15.00
DO NOT DISTURB
MAY 2013
12104131 $10.00
LF/HF UP-CONVERTER
JUN 2013
07106131 $10.00
10-CHANNEL REMOTE CONTROL RECEIVER
JUN 2013
15106131 $15.00
IR-TO-455MHz UHF TRANSCEIVER
JUN 2013
15106132
$7.50
“LUMP IN COAX” PORTABLE MIXER
JUN 2013
01106131 $15.00
L’IL PULSER MKII TRAIN CONTROLLER
JULY 2013
09107131 $15.00
L’IL PULSER MKII FRONT & REAR PANELS
JULY 2013
09107132/3 $20.00/set
REVISED 10 CHANNEL REMOTE CONTROL RECEIVER
JULY 2013
15106133 $15.00
INFRARED TO UHF CONVERTER
JULY 2013
15107131
$5.00
UHF TO INFRARED CONVERTER
JULY 2013
15107132 $10.00
IPOD CHARGER
AUG 2013
14108131
$5.00
PC BIRDIES
AUG 2013
08104131 $10.00
RF DETECTOR PROBE FOR DMMs
AUG 2013
04107131 $10.00
BATTERY LIFESAVER
SEPT 2013
11108131
$5.00
SPEEDO CORRECTOR
SEPT 2013
05109131 $10.00
SiDRADIO (INTEGRATED SDR) Main PCB
OCT 2013
06109131 $35.00
SiDRADIO (INTEGRATED SDR) Front & Rear Panels
OCT 2013
06109132/3 $25.00/pr
TINY TIM AMPLIFIER (same PCB as Headphone Amp [Sept11])OCT 2013
01309111
$20.00
AUTO CAR HEADLIGHT CONTROLLER
OCT 2013
03111131
$10.00
GPS TRACKER
NOV 2013
05112131
$15.00
STEREO AUDIO DELAY/DSP
NOV 2013
01110131
$15.00
BELLBIRD
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 refer above [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
Li’l Pulser Mk2 Revised
JAN 2014
09107134
$15.00
10A 230VAC MOTOR SPEED CONTROLLER
FEB 2014
10102141
$12.50
NICAD/NIMH BURP CHARGER
MAR 2014
14103141
$15.00
RUBIDIUM FREQ. STANDARD BREAKOUT BOARD
APR 2014
04105141
$10.00
USB/RS232C ADAPTOR
APR 2014
07103141
$5.00
MAINS FAN SPEED CONTROLLER
MAY 2014
10104141
$10.00
RGB LED STRIP DRIVER
MAY 2014
16105141
$10.00
HYBRID BENCH SUPPLY
MAY 2014
18104141
$20.00
2-WAY PASSIVE LOUDSPEAKER CROSSOVER
JUN 2014
01205141
$20.00
TOUCHSCREEN AUDIO RECORDER
JUL 2014
01105141
$12.50
THRESHOLD VOLTAGE SWITCH
JUL 2014
99106141
$10.00
MICROMITE ASCII VIDEO TERMINAL
JUL 2014
24107141
$7.50
FREQUENCY COUNTER ADD-ON
JUL 2014
04105141a/b $15.00
TEMPMASTER MK3
AUG 2014
21108141
$15.00
44-PIN MICROMITE
AUG 2014
24108141
$5.00
OPTO-THEREMIN MAIN BOARD
SEP 2014
23108141
$15.00
OPTO-THEREMIN PROXIMITY SENSOR BOARD
SEP 2014
23108142
$5.00
ACTIVE DIFFERENTIAL PROBE BOARDS
SEP 2014
04107141/2 $10/SET
MINI-D AMPLIFIER
SEP 2014
01110141
$5.00
COURTESY LIGHT DELAY
OCT 2014
05109141
$7.50
DIRECT INJECTION (D-I) BOX
OCT 2014
23109141
$5.00
DIGITAL EFFECTS UNIT
OCT 2014
01110131
$15.00
DUAL PHANTOM POWER SUPPLY
NOV 2014
18112141
$10.00
REMOTE MAINS TIMER
NOV 2014
19112141
$10.00
REMOTE MAINS TIMER PANEL/LID (BLUE)
NOV 2014
19112142
$15.00
ONE-CHIP AMPLIFIER
NOV 2014
01109141
$5.00
TDR DONGLE
DEC 2014
04112141
$5.00
MULTISPARK CDI FOR PERFORMANCE VEHICLES
DEC 2014
05112141
$10.00
CURRAWONG STEREO VALVE AMPLIFIER MAIN BOARD
DEC 2014
01111141
$50.00
CURRAWONG REMOTE CONTROL BOARD
DEC 2014
01111144
$5.00
CURRAWONG FRONT & REAR PANELS
DEC 2014
01111142/3 $30/set
CURRAWONG CLEAR ACRYLIC COVER
JAN 2015
SC2892 $25.00
ISOLATED HIGH VOLTAGE PROBE
JAN 2015
04108141
$10.00
SPARK ENERGY METER MAIN BOARD
FEB/MAR 2015
05101151
$10.00
SPARK ENERGY ZENER BOARD
FEB/MAR 2015
05101152
$10.00
SPARK ENERGY METER CALIBRATOR BOARD
FEB/MAR 2015
05101153
$5.00
APPLIANCE INSULATION TESTER
APR 2015
04103151
$10.00
APPLIANCE INSULATION TESTER FRONT PANEL
APR 2015
04103152
$10.00
LOW-FREQUENCY DISTORTION ANALYSER
APR 2015
04104151
$5.00
APPLIANCE EARTH LEAKAGE TESTER PCBs (2)
MAY 2015
04203151/2
$15.00
APPLIANCE EARTH LEAKAGE TESTER LID/PANEL
MAY 2015
04203153
$15.00
BALANCED INPUT ATTENUATOR MAIN PCB
MAY 2015
04105151
$15.00
BALANCED INPUT ATTENUATOR FRONT & REAR PANELS MAY 2015
04105152/3
$20.00
4-OUTPUT UNIVERSAL ADJUSTABLE REGULATOR
MAY 2015
18105151
$5.00
SIGNAL INJECTOR & TRACER
JUNE 2015
04106151
$7.50
PASSIVE RF PROBE
JUNE 2015
04106152
$2.50
SIGNAL INJECTOR & TRACER SHIELD
JUNE 2015
04106153
$5.00
BAD VIBES INFRASOUND SNOOPER
JUNE 2015
04104151
$5.00
CHAMPION + PRE-CHAMPION
JUNE 2015
01109121/2 $7.50
DRIVEWAY MONITOR TRANSMITTER PCB
JULY 2015
15105151 $10.00
DRIVEWAY MONITOR RECEIVER PCB
JULY 2015
15105152
$5.00
PRINTED CIRCUIT BOARD TO SUIT PROJECT:
PUBLISHED:
MINI USB SWITCHMODE REGULATOR
VOLTAGE/RESISTANCE/CURRENT REFERENCE
LED PARTY STROBE MK2
ULTRA-LD MK4 200W AMPLIFIER MODULE
9-CHANNEL REMOTE CONTROL RECEIVER
MINI USB SWITCHMODE REGULATOR MK2
2-WAY PASSIVE LOUDSPEAKER CROSSOVER
ULTRA LD AMPLIFIER POWER SUPPLY
ARDUINO USB ELECTROCARDIOGRAPH
FINGERPRINT SCANNER – SET OF TWO PCBS
LOUDSPEAKER PROTECTOR
LED CLOCK
SPEECH TIMER
TURNTABLE STROBE
CALIBRATED TURNTABLE STROBOSCOPE ETCHED DISC
VALVE STEREO PREAMPLIFIER – PCB
VALVE STEREO PREAMPLIFIER – CASE PARTS
QUICKBRAKE BRAKE LIGHT SPEEDUP
SOLAR MPPT CHARGER & LIGHTING CONTROLLER
MICROMITE LCD BACKPACK, 2.4-INCH VERSION
MICROMITE LCD BACKPACK, 2.8-INCH VERSION
BATTERY CELL BALANCER
DELTA THROTTLE TIMER
MICROWAVE LEAKAGE DETECTOR
FRIDGE/FREEZER ALARM
ARDUINO MULTIFUNCTION MEASUREMENT
PRECISION 50/60Hz TURNTABLE DRIVER
RASPBERRY PI TEMP SENSOR EXPANSION
100DB STEREO AUDIO LEVEL/VU METER
HOTEL SAFE ALARM
UNIVERSAL TEMPERATURE ALARM
BROWNOUT PROTECTOR MK2
8-DIGIT FREQUENCY METER
APPLIANCE ENERGY METER
MICROMITE PLUS EXPLORE 64
CYCLIC PUMP/MAINS TIMER
MICROMITE PLUS EXPLORE 100 (4 layer)
AUTOMOTIVE FAULT DETECTOR
MOSQUITO LURE
MICROPOWER LED FLASHER
MINI MICROPOWER LED FLASHER
50A BATTERY CHARGER CONTROLLER
PASSIVE LINE TO PHONO INPUT CONVERTER
MICROMITE PLUS LCD BACKPACK
AUTOMOTIVE SENSOR MODIFIER
TOUCHSCREEN VOLTAGE/CURRENT REFERENCE
SC200 AMPLIFIER MODULE
60V 40A DC MOTOR SPEED CON. CONTROL BOARD
60V 40A DC MOTOR SPEED CON. MOSFET BOARD
GPS SYNCHRONISED ANALOG CLOCK
ULTRA LOW VOLTAGE LED FLASHER
POOL LAP COUNTER
STATIONMASTER TRAIN CONTROLLER
EFUSE
SPRING REVERB
6GHz+ 1000:1 PRESCALER
MICROBRIDGE
MICROMITE LCD BACKPACK V2
10-OCTAVE STEREO GRAPHIC EQUALISER PCB
10-OCTAVE STEREO GRAPHIC EQUALISER FRONT PANEL
10-OCTAVE STEREO GRAPHIC EQUALISER CASE PIECES
RAPIDBRAKE
DELUXE EFUSE
DELUXE EFUSE UB1 LID
MAINS SUPPLY FOR BATTERY VALVES (INC. PANELS)
3-WAY ADJUSTABLE ACTIVE CROSSOVER
3-WAY ADJUSTABLE ACTIVE CROSSOVER PANELS
3-WAY ADJUSTABLE ACTIVE CROSSOVER CASE PIECES
6GHz+ TOUCHSCREEN FREQUENCY COUNTER
KELVIN THE CRICKET
6GHz+ FREQUENCY COUNTER CASE PIECES (SET)
SUPER-7 SUPERHET AM RADIO PCB
SUPER-7 SUPERHET AM RADIO CASE PIECES
THEREMIN
PROPORTIONAL FAN SPEED CONTROLLER
WATER TANK LEVEL METER (INCLUDING HEADERS)
10-LED BARAGRAPH
10-LED BARAGRAPH SIGNAL PROCESSING
NEW THIS MONTH
TRIAC-BASED MAINS MOTOR SPEED CONTROLLER
VINTAGE TV A / V MODULATOR
AM RADIO TRANSMITTER
JULY 2015
18107151 $2.50
AUG 2015
04108151 $2.50
AUG 2015
16101141 $7.50
SEP 2015
01107151 $15.00
SEP 2015
1510815 $15.00
SEP 2015
18107152 $2.50
OCT 2015
01205141 $20.00
OCT 2015
01109111 $15.00
OCT 2015
07108151
$7.50
NOV 2015
03109151/2 $15.00
NOV 2015
01110151 $10.00
DEC 2015
19110151 $15.00
DEC 2015
19111151 $15.00
DEC 2015
04101161
$5.00
DEC 2015
04101162 $10.00
JAN 2016
01101161 $15.00
JAN 2016
01101162 $20.00
JAN 2016
05102161 $15.00
FEB/MAR 2016
16101161 $15.00
FEB/MAR 2016
07102121 $7.50
FEB/MAR 2016
07102122 $7.50
MAR 2016
11111151
$6.00
MAR 2016
05102161 $15.00
APR 2016
04103161
$5.00
APR 2016
03104161
$5.00
APR 2016
04116011/2 $15.00
MAY 2016
04104161 $15.00
MAY 2016
24104161
$5.00
JUN 2016
01104161 $15.00
JUN 2016
03106161
$5.00
JULY 2016
03105161
$5.00
JULY 2016
10107161 $10.00
AUG 2016
04105161
$10.00
AUG 2016
04116061
$15.00
AUG 2016
07108161
$5.00
SEPT 2016
10108161/2 $10.00/pair
SEPT 2016
07109161 $20.00
SEPT 2016
05109161 $10.00
OCT 2016
25110161
$5.00
OCT 2016
16109161
$5.00
OCT 2016
16109162
$2.50
NOV 2016
11111161 $10.00
NOV 2016
01111161
$5.00
NOV 2016
07110161
$7.50
DEC 2016
05111161 $10.00
DEC 2016
04110161 $12.50
JAN 2017
01108161 $10.00
JAN 2017
11112161 $10.00
JAN 2017
11112162 $12.50
FEB 2017
04202171 $10.00
FEB 2017
16110161
$2.50
MAR 2017
19102171 $15.00
MAR 2017
09103171/2 $15.00/set
APR 2017
04102171
$7.50
APR 2017
01104171 $12.50
MAY 2017
04112162
$7.50
MAY 2017
24104171
$2.50
MAY 2017
07104171
$7.50
JUN 2017
01105171 $12.50
JUN 2017
01105172 $15.00
JUN 2017
SC4281 $15.00
JUL 2017
05105171 $10.00
AUG 2017
18106171 $15.00
AUG 2017
SC4316 $5.00
AUG 2017
18108171-4 $25.00
SEPT 2017
01108171 $20.00
SEPT 2017
01108172/3 $20.00/pair
SEPT 2017
SC4403 $10.00
OCT 2017
04110171 $10.00
OCT 2017
08109171 $10.00
DEC 2017
SC4444 $15.00
DEC 2017
06111171 $25.00
DEC 2017
SC4464 $25.00
JAN 2018
23112171 $12.50
JAN 2018
05111171
$2.50
FEB 2018
21110171
$7.50
FEB 2018
04101181
$7.50
FEB 2018
04101182
$5.00
MAR 2018
MAR 2018
MAR 2018
PCB CODE:
10102181
02104181
06101181
Price:
$10.00
$7.50
$7.50
LOOKING FOR TECHNICAL BOOKS? YOU’LL FIND THE COMPLETE LISTING OF ALL BOOKS AVAILABLE IN THE BOOKS & DVDs” PAGES AT SILICONCHIP.COM.AU/SHOP
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
Receiving vertically
polarised VHF TV
I am very interested in the 6-element
VHF TV antenna featured in the February issue. It looks as though it could
solve some TV reception problems that
we are experiencing.
However, the VHF TV transmitters
in the Manning Valley in NSW are
vertically polarised, not horizontally
polarised, as is the case in Australian
metropolitan areas. So can I just mount
the antenna so that all the elements are
vertical or is it more complicated than
that? (T. D., Taree, NSW)
• Unfortunately, it is more complicated. As presented in the February
issue, the mast is shown as attached
to the boom between the folded dipole
and first director element.
That's fine when the antenna is set
for horizontally polarised TV broadcasts but if the attachment is placed
in the same position on the boom
when the antenna elements are vertical, the metal mast will interfere with
the operation of the folded dipole and
all the other elements, to a greater or
lesser extent.
The normal way to avoid this problem is to use a non-metallic mast
which could be made of fibreglass or
timber. Where do you get a fibreglass
mast? One suitable source would be
to adapt the telescopic handle from a
long-handled pruner.
Of course, the conventional approach is to attach the mast to an extension of the boom, behind the reflector
element. This was done with the vertically polarised DAB+ antenna which
we presented in the November 2015 issue (siliconchip.com.au/Article/9394).
However, the boom of the 6-element
VHF TV antenna is considerably longer than that for the DAB+ antenna and
overall it is quite a lot larger and heavier and it would have a lot more windage when used in vertical mode. You
could make the boom from 25mm or
larger square tubing but using a nonmetallic mast is probably the simplest
and best option.
98
Silicon Chip
If you use a timber mast, we suggest
it must be at least 35mm in diameter,
made of durable hardwood and painted to preserve it from weathering.
Currawong has hum in
one channel
I have finally got my Currawong
stereo valve amplifier (November
2014-January 2015; siliconchip.com.
au/Series/277) up and running.
However, I've got hum in the left
channel which is not influenced by
the volume control and it gets worse if
I remove LK4. I have no hum whatsoever in the right channel, regardless of
whether LK5 is fitted. Is there a fix for
this? (C. B., Gillieston Heights, NSW)
• This could have a number of causes, including a faulty solder joint or
bad valve pin connection to the socket, faulty valve or bad wiring. It could
also be caused by unusually high levels of hum pickup from wiring near
the transformer.
We suggest you try temporarily removing V1 and connect a clip lead
across the 100kW resistor that goes to
pin 6 on V1. This resistor is to the right
of V1 (the right-most of three there).
Be careful because HT is applied to
this resistor.
Make sure the clip lead (or whatever
you use to short it) has sufficient insulation and don't touch it when power
is applied.
This will mean that there is no signal at the input of V2. If the hum goes
away, that suggests a problem with V1
or its socket soldering or the surrounding circuitry. If you still have significant hum then try removing V2. That
will eliminate the signals driving V7
and V8. If that fixes it, then V2 or an
associated component is suspect.
If none of that helps, rotating the
transformer may also reduce or eliminate the hum. Keep in mind that the
transformer lead lengths may limit the
amount of rotation possible and make
sure to loosen the mounting bolt before
rotating and tighten it again when you
have finished.
Celebrating 30 Years
Whatever changes you make, switch
off the power, unplug the unit and
make sure the HT capacitors have discharged before removing the insulating panel to work on it.
Note: we received subsequent correspondence that the cause of the hum
was due to the pins in the left-hand
speaker connector not being a tight
enough fit into the socket. Replacing
the pluggable terminal block on that
side eliminated the hum.
Jacob’s Ladder does not
work
My 10-year old son built your Improved Jacob’s Ladder project from
the February 2013 issue (siliconchip.
com.au/Article/2369). It didn’t work,
so we built another one, with the same
result. There just doesn’t seem to be
any power to either one, no matter
what we do. (B. B., via email)
• If there is no power then either the
10W resistor supplying the circuit is
open-circuit or there is a short on the
regulator output. Check that IC1 is
oriented correctly. Check that there
is 12V at the input to REG1 and 5V at
its output.
Make sure the ignition coil connections are correct, with the coil primary
negative terminal to the coil primary
negative on the PCB and the coil primary positive to the +12V via a 10A
fast-blow fuse. It is possible that you
have connected the coil primary positive to ground instead.
Having checked all this, adjust the
dwell as described in the middle of the
left-hand column on page 65.
Curing on/off thump in
the Active Crossover
I built the 3-way Active Crossover
from the September and October
2017 magazines (siliconchip.com.au/
Series/318) and really like it. It works
beautifully.
The only problem I have is that if
the speaker amplifiers are left on and
turned up when the crossover is powsiliconchip.com.au
ered off or on, it can produce a big
“thump” in the output. I have to make
sure the main amp volumes are down
before powering on/off the crossover.
It sounds like a capacitor charging;
sometimes this happens with subwoofers.
I was wondering whether John
Clarke might know how to mute this
output pulse somehow. (B. S., Torrens
Park, SA)
• The switch-off thump can usually
be reduced if the positive and negative supplies both decay at the same
rate. The 15V supplies can be balanced
to discharge at a particular rate with
a resistor across one of the 15V regulator outputs (ie, between the output
and GND). You would need to measure which supply rail falls the slowest,
positive or negative, and add a resistor
across that output.
The resistor value will need to be
adjusted so that the decay rate matches the other supply. An oscilloscope
monitoring both supplies will reveal
the difference in voltage fall rates.
Switch-on (and also switch-off)
thumps can generally also be reduced
by adding a 100nF capacitor across
each of the low voltage power switch
terminals. That provides an amount
of switch contact de-bounce and also
provides some quiescent current to the
power supply.
Having said that, normally the
Crossover should be switched on
and off at the same time as the power
amplifiers (eg, using the same mains
switch), thus allowing the thump removal circuitry in the amplifiers or
corresponding speaker protectors to
solve the problem.
10MHz GPS-locked
frequency standard
I have had my Amateur Radio License now for 57 years and have always enjoyed reading electronics magazines, starting with “Radio & Hobbies”. Haven’t we seen a lot of changes
since then? In recent times, I have enjoyed the Micromite projects, having
built three of them now.
With Amateur Radio equipment getting more exotic over the years, have
you ever described a 10MHz GPSlocked frequency standard? With amateurs going higher in frequency, into
the microwave bands, it’s becoming
critical to have an accurate standard
to work with.
siliconchip.com.au
Keeping short links for posterity
In recent times, you have started
publishing short links to internet
content which work through your
own web presence, which is grand
for now. It would be more useful for
people accessing the online version
rather than the paper version I guess.
I'm thinking about what happens
should there be a disaster similar in
nature to what happened to EA, ETI,
RTV&H and every other relevant
magazine ever published (or so it
seems). Should the business cease
to exist or the website be altered in
some way (eg, change of name), then
all those short links become useless.
Have you considered providing a
summary of the short links and the
actual URL being referenced, perhaps
as an ever growing list, on an annual
basis (January to December inclusive
and resetting each January), or per
issue, within the printed edition at
least? It might take a similar form to
the advertisers’ index, normally facing the inner back cover.
I have a Marconi frequency generator that goes up to 1500MHz and it
would be nice to be able to lock it to
an accurate standard. Like most, it has
a socket on the rear to attach a reference oscillator.
Please keep up the good work with
the magazine. (T. H., Kingston, SA)
• Please see our GPS-based Frequency Reference project in the March,
April and May 2007 issues and the subsequent update in the September 2011
issue: siliconchip.com.au/Series/57
Discrepancies in
Touchscreen Altimeter
Is it correct that the AM2302 temperature and humidity sensor supplied for the Touchscreen Altimeter/
Weather Station (December 2017;
siliconchip.com.au/Article/10898) is
not mounted on the circuit board as
shown on photos per the article in the
December issue?
The small PCB appears to contain
some additional components and only
three connection pins.
Anyway, I proceeded to finish construction using the DHT22 datasheet
pinout and that function seems to
be working OK. However, there are
Celebrating 30 Years
It’s just an idea but it would hopefully not cost much and would make
the paper magazine useful beyond
the life of your current website. I
find I refer back to 1980s and 1990s
EAs and ETIs at times.
If they had used short links then,
they would be useless now. (P. G.,
Ardross, WA)
• Even if Silicon Chip magazine
ultimately became financially nonviable and ceased publication (perish the thought), the website could
be spun off and operated as an independent entity.
Having said that, you can get an
up-to-date list of all short links from
www.siliconchip.com.au/l/ and you
can download them in CSV file format at www.siliconchip.com.au/l/csv
Mind you, even the full links have
a finite life. In fact, the most common reason why short links fail is
that the original link no longer works
and probably this will be because the
particular website no longer exists.
some discrepancies with the Altimeter function.
In the magazine, the opening screen
reads "metres above GND" while my
screen shows "metres above QNH"
What is QNH? Similarly, on the
CHANGE MODE OR UNITS screen,
the magazine shows "GROUND REFERENCE" while my screen shows "Input QNH Reference".
When the "Input QNH Reference"
button is touched, a numeric keypad is
shown. I thought the keypad expected
an input referring to the actual location altitude variation.
However, when I entered a negative
value (my location was about 25 metres lower than the altitude shown),
the system crashed showing 00.00
metres and I could get no response
from screen touches. I had to reset the
Micromite.
I did make a couple of structural
alterations to allow the unit to be
placed on a shelf laying on its side; I
mounted the power switch on the front
panel to the right of the touchscreen
and instead of using screws to secure
the battery holder, I used hot melt glue.
I have recently built Kelvin the
Cricket which entertained my whole
family over the Christmas holidays.
March 2018 99
Every time he chirped the crowd went
quiet to hear what the temperature
was. The children learnt to count by
fives as well. Kelvin regularly compares notes with the Altimeter/Weather Station and they are usually within
about 1.5°C of each other.
I really appreciate Silicon Chip publishing articles on the Micromite as I
do not want to go down the Arduino
or Raspberry Pi trails. I will stick with
Micromite and PICAXE for economy
and simplicity.
I am more than happy with using
BASIC coding as I can make some
sense of it. Thank you all for a great
read being highly educational and entertaining. (S. S., Barrington, NSW)
• There was some confusion over the
DHT22 sensor as the circuit diagram
shows a “bare” DHT22 (with the pins
labelled correctly but in the wrong order!) while the overlay diagram and
photos show a DHT22 mounted on a
small breakout board with two additional components.
We sell the bare DHT22 but as you
point out, it can be made to work with
the correct wiring. We’re publishing
errata in this issue regarding these
discrepancies.
We explained the addition of the
QNH feature post-publication in the
Mailbag section of the January 2018 issue (page 4). According to Wikipedia,
QNH is “a Q code indicating the atmospheric pressure adjusted to sea level”.
When you bring up that keypad,
enter the atmospheric pressure at sea
level at your location for corrected altitude readings.
This is available to pilots in flight
over the radio, allowing them to correct their altitude readings before
landing.
The software presumably can’t handle the entry of a negative barometric pressure. You can set the software
back into the original mode shown in
the magazine by selecting "MSL Reference" mode via the menu.
Altimeter chip does not
need reprogramming
I received your kit for the Touchscreen Altimeter (December 2017;
siliconchip.com.au/Article/10898)
early this week.
Today the January 2018 edition of
the magazine arrived. I saw the comments in Mailbag on page 4 about
the revised software. I had wondered
about the absence of a QNH adjustment function.
I am an ultralight pilot and am interested in using the project in my plane
to compare with the inbuilt altimeter
as a matter of interest.
However, I have currently no computer and have no experience in program loading, therefore can't update
the software myself. Can I send the
chip back to be reprogrammed with
the updated version of the software?
I have not removed it from its package at this stage.
Please advise on how we can solve
this dilemma. I am happy to reimburse
you for any shipping costs.
My second question concerns the
Elecrow charger module. I see no reference to the solar panel voltage in
the article. I assume the input voltage
is 12V DC. I keep the plane's battery
charged with an 80-watt solar panel/
charger controller whilst it is not in
use. Can I connect this Elecrow board
to that solar panel?
• No software update is required. All
chips supplied for the Altimeter project have the QNH feature mentioned
in Mailbag.
Are brushless DC motors similar to induction motors?
In reading the Lathe-E-Boy project (January 2018; siliconchip.
com.au/Article/10933) and subsequently the earlier 1.5kW Induction Motor Speed Controller articles
(April-May 2012; siliconchip.com.
au/Series/25), maybe the penny has
dropped!
We are now surrounded by "brushless DC" power tools, electric skateboards with "brushless DC" motors,
battery electric garden equipment,
inverter air conditioners and fridges
and I suppose there are more.
Having recently repaired a Fujitsu inverter aircon which used a
Fairchild FSBS10CH60 IGBT motor
controller and comparing the circuit with the 1.5kW Induction Motor Speed Controller, the power circuitry is almost identical in design
philosophy.
The associated motor winding
connection explanation makes more
sense than that which I read (not
from Fujitsu) regarding inverterdriven aircons which mentioned
100
Silicon Chip
"3-phase DC motors" and showed a
schematic with a star connected motor and no connection to the common winding.
A lot of this jargon seems a bit esoteric but when read in the light of the
motor explanation in the April 2012
issue on the 1.5kW Induction Motor
Speed Controller, it seems that all
the motors are only size variants of
a delta-wound 3-phase motor connected to a suitably-sized IGBT and
controlled by a fast digital switcher
for speed control. Is that right? (P.
C., Ormiston, Qld)
• The driving circuitry for brushless DC motors and 3-phase induction motors is quite similar. They
both typically have a number of
driven coils which is usually a multiple of three.
The difference is that the rotor
field of a BLDC motor is provided
by permanent magnets while the rotor field of an induction motor is induced by the rotating magnetic field
of the stator coils.
Celebrating 30 Years
For current to be induced in the
rotor conductors of an induction
motor (whether it is off squirrel cage
construction or has wound coils),
there must be some "slip" (ie, a delay between the rotating field of the
stator and the induced field in the
rotor) in an induction motor, whereas a BLDC motor will be essentially
synchronous.
Speed control of an induction motor requires varying the voltage and
frequency applied to the windings
and while there are various ways to
do this, high-frequency PWM using
IGBTs in bridge circuits is the most
practical method and it's how almost
all these controllers work.
Whether the motor is delta-wound
or star-wound really only affects
the voltage required. The way the
windings are driven is essentially
identical.
A star-wound motor does not require a neutral connection to the
common windings; without one, a
“virtual neutral” exists.
siliconchip.com.au
The charger module expects a solar
panel voltage of around 5-6V. There are
numerous small panels available with
an open-circuit voltage of around 6V,
including one that we sell in our Online Shop, Cat SC4339.
Note that you will probably need
to wire more than one of these small
panels in parallel to supply sufficient
current to operate the unit.
By the way, please check the errata
for that project on page 104 of this issue regarding the wiring of the DHT22
temperature and humidity sensor.
High-Energy Ignition
System with 6V battery
I want to build the Jaycar KC5513
High-energy Electronic Ignition kit
(based on your November-December 2012 design; siliconchip.com.au/
Series/18) for an old motorcycle with
a 6V system using a standard points
arrangement.
Does the kit need any modification
to cope with a 6V rather than 12V
system?
Harley Davidson 1927 J Models used
points without a distributor but a dual-lead coil and were thus a “wasted
spark” arrangement. I don’t see any
issues using your ignition system on
those old V-Twins. (K. D., via email)
• That ignition system can be used
at 6V. The LM2940 is a low-dropout
regulator and it will be OK with a 6V
battery.
However the battery voltage will inevitably drop below 5V during cranking (if there is a starter motor) and will
reduce the available spark energy until the engine fires up. Make sure the
points are correctly gapped otherwise
starting may be problematic.
Frequency Switch kit is
not working
I have a Jaycar KC5378 Frequency
Switch which I cannot get to work.
It’s based on the article you published
in the June 2007 issue and also in the
book Performance Electronics for Cars
(siliconchip.com.au/Article/2261).
Having built it, I powered the unit
up and connected a voltmeter between
ground and TP1. There was no voltage present and adjusting VR1 did not
affect this.
If I rotate VR2 anti-clockwise, the
relay will latch; then clockwise it will
unlatch. However, any input method
I have tried will not trigger the relay.
Please advise of any checks I could do
to rectify this. (A. C., Swan Hill, Vic)
• If there is no voltage at TP1, check
that there is 7.4V at the cathode (K)
of diode D2 and 8V at the output of
REG1. Varying VR1 will not affect the
TP1 voltage.
It appears that VR2 does change the
TP1 voltage since you can get the relay
to switch on and off with adjustment.
If you apply an AC signal to the input, the voltage at pin 4 of IC1 should
rise; the higher the signal frequency,
the higher the voltage at pin 4. It’s this
relationship which VR1 adjusts. VR2
simply sets the threshold where the
relay switches on or off.
Adapting 12V battery
charger for 24V
I want to build the Jaycar KA1795
12V Battery Regulator kit, based on the
article published in Electronics Australia, July 1997.
I want to use it to charge a 24V 4.5Ah
lead-acid battery.
Could you please suggest which
component values need to be changed
and/or upgraded to give the correct
regulated voltage.
I am using an Arlec battery charger
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Celebrating 30 Years
March 2018 101
with the 2 x 12V windings in series,
giving about 28VAC. (B. C., Dungog,
NSW)
• We suggest that you change the
following resistors: R5 to 12kW, R7 to
1.2kW and R8 to 68W 5W. Note that
we cannot guarantee that these mods
will work; they might need tweaking.
SC200 Amplifier
questions
I have been reading the article on
building the SC200 Amplifier which
was re-published in the January 2018
issue of EPE Magazine. The power output transistor FJA4313 appears to be
unobtainable. I can’t find a supplier
that stocks this transistor.
Also, there is also a mistake in the
article. ±56.6V is derived from 40-0-40
AC secondary transformer, not 45-0-45
AC; this would give ±63.6V.
LED1 is specified as SMD 3216/1206
blue and there are different version
of this with 20mA or 30mA forward
current.
The typical forward voltage ranges
from 3.2V to 3.6V. Which one is the
correct LED and does it matter? (A.
W., Wimborne, UK)
• FJA4313OTA is available from DigiKey (Catalog code FJA4313OTU-ND)
or as part of a set of hard-to-get parts
from our Silicon Chip Online Shop
(Cat SC4140). You are right, the transformer should have been specified as
40-0-40V; not 45-0-45V.
LED1 is supplied with around 2mA
so any blue LED of that size should be
fine. The forward voltage is not important as it's supplied from a constant
current source.
High Energy Ignition
systems with points
I have a 1978 Datsun 200B with
points. Will the High-Energy Ignition
System you published in the November
and December 2012 issues (siliconchip.
com.au/Series/18) work with points?
(W. O’D., Cartwright, NSW)
• All of our High Energy Ignition
systems can be used with points as
well as reluctor, Hall effect and optical triggers.
Will SC200 transformer be overloaded at 200W into a 4W
4W load?
I am an EPE subscriber emailing
from England. I have recently thoroughly enjoyed the brilliant Silicon
Chip SC200 amplifier constructional
project published in EPE over the
last three months. Congratulations to
both Nicholas Vinen and Leo Simpson for yet another job well done.
However, I have a technical query
which has been troubling me concerning the power supply for this
project. My calculations imply that
the transformers specified for this
project are underpowered. If there
is an error in my calculations below, I would be pleased if you could
correct me.
A 300VA, 80V transformer is capable of supplying a maximum current
of 300 ÷ 80 = 3.75A RMS. When the
SC200 is supplying the maximum
stipulated 135W into an 8-ohm load,
135W = 8 × I2 and therefore I = 4.1A.
However, in the push-pull amplifier output stage, 4.1A is only drawn
from each secondary for half the
time. Therefore, the average DC current drawn by each half of the output stage is 2.05A.
Now, there is a 1.7 multiplication
scaling factor from the DC load current to the transformer AC RMS current for this configuration of power
supply.
Therefore Irms = 2.05 × 1.7 = 3.5A
which is less than the 3.75A RMS
available from a 300VA transformer.
All appears well for an 8-ohm load.
However, going through the same
102
Silicon Chip
calculations for the rated 200W,
4-ohm load,
200W = 4 × I2 gives I = 7A, which
is on for only half the time in each
half of the transformer secondary.
Therefore average DC current in each
half of the output stage is 3.5A. Multiply by the 1.7 scaling factor, 3.5A ×
1.7 = 6A RMS, which is much more
than the 3.75A RMS available from
a 300VA transformer.
It appears to me that a 500VA (80V
<at> 6.25A) transformer is required to
supply 200W into 4-ohms.
If the 1.7 scaling factor is omitted
then the transformers specified in
EPE appear to be powerful enough.
Has Nicholas omitted to include the
1.7 scaling factor in his calculations?
Likewise, by similar calculations, for the low-power version of
the PSU/amplifier, it appears to me
that a larger transformer is required
to supply the rated power into four
ohms, ie, larger than the specified
160VA transformer.
I would be very thankful if you
could consider my theory and point
out to me if and where I have made
an error in my calculations. This
has been puzzling me! I suspect
that I'm missing something. (C. H.,
London, UK)
• Strictly speaking, you are correct.
When delivering 200W into a resistive load, the amplifier will draw
more than 300W. But even though
we state that the amplifier can do
this (and it can), the assumption is
Celebrating 30 Years
that the normal load will be a loudspeaker and therefore partly inductive rather than purely resistive.
Second, unless you intend using
the amplifier with a constant sinewave signal (perhaps driving a vibration table), the actual power delivered to the load will be substantially less.
Third, normal program signals are
complex and typically have a dynamic range of more than, say, 30dB.
Putting it another way, the full
power duty cycle will be quite low
and the average power drawn by the
amplifier, even when driven to the
point of clipping on audio programs,
will be quite small; perhaps only a
few watts. So in practice, for normal domestic audio use, the 300VA
transformer is quite adequate. In
fact, a 300VA transformer would be
quite adequate for a stereo pair of
these modules.
On the other hand, if you intend
using the amplifier module with a
4-ohm loudspeaker load for music
instrument applications, particularly for bass guitar or electronic
organ, we would recommend going
for a 500VA transformer.
As a final comment, if you did intend to drive the amplifier for a longterm continuous output of 200W,
we'd be more concerned about the
ratings of the main filter capacitor,
the output power transistors and
their heatsinks and the risks of overSC
heating than the transformer.
siliconchip.com.au
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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
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siliconchip.com.au
Celebrating 30 Years
March 2018 103
Coming up in Silicon Chip
Rohde & Schwarz RTM3004 oscilloscope review
Advertising Index
We take an in-depth look at one of Rohde & Schwarz's newest scopes, the
RTM3004, with 1GHz bandwidth, 5GHz sampling, 10-bit vertical resolution,
16 digital channels and an 80Msample memory.
Altronics.................................. 76-79
Facett Hearing Aids from Blamey Saunders
Electrolube................................... 11
Ross Tester reports on his experiences with the latest set of hearing aids from
leading Australian supplier Blamey Saunders hears.
Hare & Forbes............................. 2-3
Introduction to programming the Cyprus CY8CKIT
Keith Rippon Kit Assembly......... 103
This low-cost module incorporates a 32-bit microcontroller and a set of
reprogrammable analog circuitry which can be used for a wide range of tasks.
We show you how to use the free Integrated Development Environment.
Dave Thompson......................... 103
Digi-Key Electronics....................... 5
Jaycar............................... IFC,49-56
LD Electronics............................ 103
LEACH Co Ltd................................ 9
LEDsales.................................... 103
Radiant Heater Controller
It will be winter in just a few months. Staying comfortable at night can be a
challenge. This new Heater Controller design takes care of that, adjusting
the heating power while you are sleeping to provide gentle heat without any
clicking thermostats or blinking lights which may wake you up.
El Cheapo Modules – RF attenuators
Jim Rowe describes a programmable, 63-step, 4GHz RF digital step attenuator
module with a range of applications. Plus he also looks at a fixed four-range
DC-4GHz attenuator
Microchip Technology...........OBC,21
Ocean Controls............................ 13
Pakronics..................................... 11
PCBcart...................................... 33
Sesame Electronics................... 103
SC Online Shop...................... 96-97
SC Radio, TV & Hobbies DVD.... 101
Note: these features are planned or are in preparation and should appear
within the next few issues of Silicon Chip.
The Loudspeaker Kit.com............ 75
The April 2018 issue is due on sale in newsagents by Thursday, March 29th.
Expect postal delivery of subscription copies in Australia between March
29th and April 13th.
Vintage Radio Repairs............... 103
Tronixlabs................................... 103
Wagner Electronics........................ 7
Notes & Errata
Lath-e-Boy High-power Lathe Controller, January 2018: the wiring colours shown in the photos on pages 40, 41 and 43
and in the lower-right corner of the circuit diagram on page 39 are not safe. The four wires to the induction motor should be
colour coded red, white, dark blue (from pin 2 of CON7 to the motor) and brown. Green/yellow striped wire must be used
for earthing the motor frame (and only for earth!).
Touchscreen Altimeter and Weather Station, December 2017: there are some inconsistencies and ambiguities between
the circuit diagram (Fig.1), sensor wiring (Fig.3) and parts list, regarding the temperature and humidity sensor. The circuit
diagram on page 25 showed a bare DHT22/AM2302 sensor with correctly wired pins, however, pin 4 was shown on the left
side of the device and pin 1 on the right, the opposite of how they are numbered on the physical module.
Also, the module shown in Fig.3 and the accompanying photo is mounted on a small breakout board with two extra
components which were not shown on Fig.1 and not mentioned in the text or parts list. The sensor we supply does not come
with the breakout board.
The circuit diagram in the online edition has been corrected to show the two extra components. If the sensor you’ve
purchased does not come on a breakout board, simply solder a 100nF capacitor between pins 1 and 4 of the DHT22/AM2302
and a 1kW resistor between pins 1 and 2. Note that the 1kW resistor could just as easily be fitted between the +5V and pin
21 (DATA) connections on the BackPack module.
High-Power DC Fan Speed Controller, January 2018: the IPP80N06S2L-07 Mosfet is listed in the parts list as being in a
TO-92 package but it is actually in a TO-220 package.
Arduino Mega Box Music Player, February 2018: the Arduino Uno and Mega do not share the same SPI pin connections. Pins
50, 51 & 52 must be connected by flying leads to digital pins 12, 11 & 13 respectively before the SD card will work on the Mega.
SC200 Audio Amplifier, January-March 2017: the power supply is mistakenly listed as 45-0-45V to provide ±57V
on page 32 of the January issue and page 85 of the February issue. The transformer is actually 40-0-40V as described in
the parts list and circuit diagram in the March issue where the power supply is described in full.
104
Silicon Chip
Celebrating 30 Years
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