This is only a preview of the September 1994 issue of Silicon Chip. You can view 30 of the 96 pages in the full issue, including the advertisments. For full access, purchase the issue for $10.00 or subscribe for access to the latest issues. Articles in this series:
Items relevant to "Automatic Discharger For Nicad Battery Packs":
Items relevant to "Build The MiniVox Voice Operated Relay":
Items relevant to "An AM Radio For Aircraft Weather Beacons":
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Items relevant to "Dual Diversity Tuner For FM Microphones; Pt.2":
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Vol.7, No.9; September 1994
FEATURES
FEATURES
6 How To Use The TEA1100 Fast Nicad Charger IC by Leo Simpson
Versatile chip features switchmode or linear operation
16 Electronic Engine Management, Pt.11 by Julian Edgar
Fueltronics’ Turbo Control Centre
RID YOUR NICAD batteries
of the dreaded memory effect
with this automatic discharger.
It will discharge the pack to its
correct endpoint voltage so that
it can then be recharged to full
capacity – see page 18.
87 Review: Metex M3850 Digital Multimeter by Marque Crozman
All the usual features plus a PC interface
PROJECTS TO
TO BUILD
BUILD
PROJECTS
18 Automatic Discharger For Nicad Battery Packs by John Clarke
Rids your batteries of the dreaded memory effect
31 Build The MiniVox Voice Operated Relay by Darren Yates
Fast-acting unit fits on a small PC board
34 An Image Intensified Night Viewer by Leo Simpson
THIS VOICE OPERATED RELAY
(or VOX) is built on a compact PC
board. It has almost no turn-on
delay & a 3-second release time.
Details page 31.
Lets you see by just the light of the stars
54 An AM Radio For Aircraft Weather Beacons by Darren Yates
Picks up airport weather beacons in the longwave band
66 Dual Diversity Tuner For FM Microphones; Pt.2 by John Clarke
Construction & alignment details
SPECIAL
SPECIAL COLUMNS
COLUMNS
40 Serviceman’s Log by the TV Serviceman
Lightning strikes thrice
63 Amateur Radio by the TV Serviceman
HERE’S A NIGHT VIEWER that’s
ideal for wildlife observations
or any other activity where you
need to see in the dark. It uses a
3-stage image intensifier tube so
that you don’t need a separate
infrared light source. Details
page 34.
Using 2-line Keplerian elements to track satellites
80 Vintage Radio by John Hill
Building a classic crystal set
84 Remote Control by Bob Young
Modellers with dedication; Pt.2
DEPARTMENTS
DEPARTMENTS
2
4
24
53
73
Publisher’s Letter
Mailbag
Circuit Notebook
Order Form
Bookshop
87
90
92
94
96
Product Showcase
Back Issues
Ask Silicon Chip
Market Centre
Advertising Index
YOU CAN USE THIS simple
radio to receive up-to-the-minute
reports from airport weather
beacons. It uses two ICs &
operates in the longwave AM
band – turn to page 54.
Cover concept: Marque Crozman
August 1994 1
Publisher & Editor-in-Chief
Leo Simpson, B.Bus.
Editor
Greg Swain, B.Sc.(Hons.)
Technical Staff
John Clarke, B.E.(Elec.)
Robert Flynn
Darren Yates, B.Sc.
Reader Services
Ann Jenkinson
Sharon Macdonald
Advertising Enquiries
Leo Simpson
Phone (02) 979 5644
Regular Contributors
Brendan Akhurst
Garry Cratt, VK2YBX
Marque Crozman, VK2ZLZ
John Hill
Jim Lawler, MTETIA
Bryan Maher, M.E., B.Sc.
Philip Watson, MIREE, VK2ZPW
Jim Yalden, VK2YGY
Bob Young
Photography
Stuart Bryce
SILICON CHIP is published 12 times
a year by Silicon Chip Publications
Pty Ltd. A.C.N. 003 205 490. All
material copyright ©. No part of
this publication may be reproduced
without the written consent of the
publisher.
Printing: Macquarie Print, Dubbo,
NSW.
Distribution: Network Distribution
Company.
Subscription rates: $49 per year
in Australia. For overseas rates, see
the subscription page in this issue.
Editorial & advertising offices:
Unit 34, 1-3 Jubilee Avenue, Warrie
wood, NSW 2102. Postal address:
PO Box 139, Collaroy Beach, NSW
2097. Phone (02) 979 5644. Fax
(02) 979 6503.
PUBLISHER’S LETTER
Where to now for
satellite TV?
Over the last few months, there has been
a flurry of developments in the pay TV/
satellite TV saga and many people must
be wondering what comes next. When will
they be able to actually start subscribing to
pay TV services? After all, most, if not all,
of the satellite and cable licenses have been
snapped up and people could be forgiven
for thinking that actual services will start “real soon now”. Well the truth is
that some very limited services are about to start and may well have started
by the time this issue goes to press but note the word “limited”. Very few
people will be able to take advantage of them.
For the vast majority of people, pay TV is many years away, as in “turn
of the century” or well after that. It is significant that potentially the biggest
player in the pay TV arena, the so-called PMT (Packer/Murdoch/Telecom)
syndicate, sat on its hands during the recent licence sales. Clearly, they are
not interested in satellite TV and if you hark back to my Publisher’s Letter in
the August 1993 issue, you can see why. With Telecom’s vast phone network
open to it, it has no need for satellites.
And while little may appear to be happening on that front, much is happening behind the scenes. Telecom has let some huge contracts for its CATV
project for the major residential areas of Brisbane, the Gold Coast, Sydney and
Melbourne. As part of that, Telecom Australia has awarded a $160 million
plus contract to Philips to provide the technical equipment and know-how to
deliver full interactive television to Australian audiences. Telecom has also
chosen the Digital Equipment (DEC) Wizard Subscriber Management System,
while Scientific Atlanta has been chosen to supply customer set-top units.
Philips will play a major role in the network upgrade which will involve
a rollout of more than 10,000 kilometres of cable. And nor is optical fibre
the only part of the story. Philips also has been developing the capability of
sending cable TV via twisted wires, so much of the existing network might
also be able to be used eventually. Clearly, Telecom is in the box seat for pay
TV and all the other services to come in the future.
So things are happening but if you want to watch overseas source programming right now and for quite a few years to come, there is only one way
to get it: install your own dish and satellite receiver. There is a large variety
of programs available, beamed into Australia, and more are coming as time
goes on. And this plethora of programming is certain to be available even
after pay TV is up and running. So if you have a hankering for satellite TV,
get into it now. Otherwise, you could be waiting for many years to come.
Leo Simpson
ISSN 1030-2662
WARNING!
SILICON CHIP magazine regularly describes projects which employ a mains power supply or produce high voltage. All such projects should
be considered dangerous or even lethal if not used safely. Readers are warned that high voltage wiring should be carried out according to the
instructions in the articles. When working on these projects use extreme care to ensure that you do not accidentally come into contact with
mains AC voltages or high voltage DC. If you are not confident about working with projects employing mains voltages or other high voltages,
you are advised not to attempt work on them. Silicon Chip Publications Pty Ltd disclaims any liability for damages should anyone be killed
or injured while working on a project or circuit described in any issue of SILICON CHIP magazine. Devices or circuits described in SILICON
CHIP may be covered by patents. SILICON CHIP disclaims any liability for the infringement of such patents by the manufacturing or selling of
any such equipment. SILICON CHIP also disclaims any liability for projects which are used in such a way as to infringe relevant government
regulations and by-laws.
Advertisers are warned that they are responsible for the content of all advertisements and that they must conform to the Trade Practices Act
1974 or as subsequently amended and to any governmental regulations which are applicable.
2 Silicon Chip
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**Illustrations are representative only
MAILBAG
Colour video fader
works well
I wrote to you sometime ago regarding an apparent fault I had with a kit
for the Colour Video Fader featured
in the August 1993 issue of SILICON
CHIP. It was fading/wiping to midgrey rather than black. That letter
was a trifle premature. In a moment
of inspiration, I decided to replace
the two ICs that had come with the
kit. The fault then disappeared and
all is now OK. One of the ICs was
obviously faulty.
Incidentally, I used to work in the
non-technical side of television and
radio, both in several Australian cities and overseas in London. In those
days, the apparatus to enable a broadcast studio to fade to black took up
considerable space in the racks, with
its valves, transformers, large power
supply and all. And it must have cost a
bomb. To think that a handful of small
components in a little black box can
now do the same thing is mind-boggling. Congratulations to the chap who
designed it.
Barry Freeman,
Morphett Vale, Vic.
Thanks for
reader response
Just a short note to thank you for
publishing my letter in the “Ask
SILICON CHIP” pages of the June 1994
issue, asking for a diagram for the
BWD539D scope. The response has
been great and to date I have received
about 10 replies.
The oscilloscope has been fixed and
the fault was a transistor in the trigger
circuit that feeds the timebase.
Bob Riding,
Fingal Bay, NSW.
Basic components
in short supply
I am writing to you with some
concern over the fact that some of
Australia’s major electronic retail
suppliers are going out of some of the
most basic components. While I am
speaking mainly of basic radio parts
such as variable capacitors and ICs
such as the ZN414, some are even
4 Silicon Chip
SILICON CHIP,
PO Box 139,
Collaroy, NSW 2097.
going out of the humble OA90 series
germanium diodes!
I have heard all the old arguments
about “we only stock what the customer wants ... etc” but I am afraid
that this is not good enough. In England and America, you can still buy
things like 415pF metallised variable
capacitors and pre-wound aerial coils
straight from the factories in those
countries.
In all fairness to the importers and
retailers of these products, I can see
their point in not stocking their warehouses with useless products that no
one wants to buy. But what about the
next generation of enthusiasts who
have never ever laid eyes on the most
basic of electronic components, who
have been in the hobby for perhaps
several years, and still don’t know
one end of a crystal set from the other?
I will admit that this all sounds
pretty much like a storm in the electronic teacup but I detect a trend in
the larger suppliers and a dangerous
one wherein we may see the day that
they simply go out of the most basic
lines altogether.
I believe that this situation requires an explanation and perhaps
some action on the part of suppliers
in general. If I were them, and I had
products that weren’t selling well, I
think that I would like to know why.
So perhaps some kind of customer
survey is warranted before we all have
to start junking circuits to get parts that
we could have if the retailers had the
foresight to ask their customers some
questions, instead of their marketing
managers.
Austin Hellier,
Alice Springs, NT.
with reproductions of fabric used in
vintage radios. For example, if I were
to receive a sample of fabric, I would
analyse the types of yarns used and the
pattern and then reproduce the fabric
accordingly.
Ms N. Moore,
PO Box 171, Kyogle, NSW 2474.
Vintage style
fabrics available
Valve technology
still relevant to some
I am a weaver of interesting and
different fabrics. Recent
ly a friend
who is a restorer of vintage radios noticed a particular piece of my woven
fabric and commented that it quite
accurately resembled radio cloth of
1950-60 vintage. He suggested that I
write to you asking whether I may be
able to supply other radio enthusiasts
Series wanted on
telephone technology
Please allow me to offer special congratulations for the excellent series on
the “Evolution of Electric Railways”
and “The Story of Electric Energy”. I
am sure that I am not the only reader
who has learnt a great deal from these
series.
May I suggest that you consider a
similar series on the Telecommunications Network. As a Technical Officer
with Telecom I can assure you that
the vast majority of people, including
those involved with or interested in
electronics, have no idea how complex
the modern system is, or that Australia
has a very extensive fibre optic cable
network.
The recent proposal to lower the
mains voltage to 230VAC seems to
be a recipe for disaster. From my experience it seems that many items of
equipment can barely cope with the
fluctuations in mains voltage currently experienced and surely the lower
mains voltage would be either on the
lower limit or outside the original
design tolerance, thus making this
equipment even more unreliable.
A. Christie,
Boronia, Vic.
Comment: a series on telephone
technology could be worthwhile. Any
volunteers to write it?
When I read your Publisher’s
Letter concerning valve ampli
fiers
in the July 1994 edition, I was flabbergasted. While most of it was fair
and balanced, the last line was, I
feel, over the top. Let’s put the valve
versus transistor amplifiers debate in
perspective, at least from my point
of view.
Why do valves sound different to
transistors? The human ear is more
tolerant of even harmonics as compared to odd harmonics. Valves produce predominantly even harmonics
as a by-product of the amplification
process and transistors produce predominantly odd harmonics. This is
why they do sound different.
I prefer the sound of a valve amplifier. Now I realise that valves do have
some shortcomings. When compared
to a transistor amplifier, large power
valve amplifiers are expensive to
build but let’s face it, I and probably
many other people do not re
quire
powerful amplifiers to enjoy listening
to music.
Most modern speakers are efficient
enough to produce plenty of volume
with only modest power inputs. My
first amplifier produced only 3.5 watts
per channel, for example, and I found
this to be enough for my needs, so
an amplifier of only 20 watts would,
I feel, be enough for most music
listeners.
I realise there are people who feel
that they have to have at least 100 watts
or more per channel and the biggest
possible speakers but I think this is
just hype, or a keep up with the Jones
next door type attitude. The quality
of sound from a reasonably well-designed amplifier is good enough for
me to enjoy and probably many others
as well.
With life in general getting busier
and busier most people don’t get a lot
of time to sit down and do some serious music listening; most people just
have some pleasant music running as
they go about their busy life. I know I
do. So reasonable quality sound is all
I require and most valve amplifiers are
capable of that task.
Valve amplifiers are certainly more
expensive to build than transistor
amplifiers. Parts for a valve amplifier
are not commonly available here in
Australia but they are there if you look
for them in the right places. There are a
growing number of shops specialising
in valves and related components. I
have always found Arthur Courtney
of Resurrection Radio very helpful
and friendly.
If you have any problems in finding
circuits or parts, try looking in some
of the English electronics magazines,
as one of them recently released a kit
and individual major parts for a 20
watts per side amplifier.
The cost of a valve amplifier runs
into many hundreds of dollars sometimes, but it can be spread out to make
it a bit easier. Besides, the thrill of the
chase only makes the final product
more satisfying.
I must admit that these are my
thoughts only, but I am sure many other people probably feel the same way,
and I don’t think that valve amplifiers
should be just brushed off as having
“no place in modern technology”.
Keep up the otherwise good work.
D. Haddock,
Kamerunga, Qld.
Comment: as far as the production
of harmonics is concerned, transistor
amplifiers have a big advantage in
that they can have far more negative
feedback applied to correct the dis
tortion. The very best valve amplifiers
could only have about 20dB of neg
ative feedback because of the phase
limitations brought about by the out
put transformers. Today’s transistor
amplifiers start with pretty linear
performance even in open loop and
may have 60dB or more of negative
feedback. That is one reason why they
are so much better.
Lowered mains voltage
is a lost cause
I have read with interest your recent
passionate editorials on the subject
of the national grid voltage debate. I
am rarely moved to print but on this
occasion you have you lost the plot!
C’mon now, where on earth do you
expect to find commonsense – in a
politicians’ mind?
Now even Blind Freddy knows that
to reduce the grid voltage would cost
us all very dearly and would have the
same meaningless effect as passing a
law to raise the height of every doorway in Australia by 10%. However,
the thin veil of the average Australian
politician’s mind is only known to
cover their personal ego, opportunistic political gain and the securing
of a firm grip on their superannuated
golden egg. No, I think we have a difficult problem here and believe me,
commonsense, the favourite, will be
the last runner.
I noted P. Badham’s Mailbag com-
ments (SILICON CHIP, July 1994) and
whilst in general agreement, I am
disappointed that we are advised to
“accept the inevitability” of European
conversion.
Yes our imported/dumped electronic equipment may well be designed
for 230VAC, but for truly 230VAC
sensitive equipment, how about we
don’t import it in the first place?
That would then create a whole new
market or a conversion after-market
that could be well supported by our
own local electronics industries, and
heavens knows, we need that sort of
employment produc
ing enterprise
here at the moment.
No, Mr Badham, please consider the
bigger picture.
May I also ask you all to consider
one last but very im
portant aspect:
the humble GPO (general purpose
outlet) plug. Since time immemorial
or whenever, we have had in Australia one common, standard design
for a 240VAC GPO plug and socket
arrangement, available from Cairns to
Marble Bar, Darwin to Hobart. Whether by good luck or good judgement it
has stood the test of time. Next time
you visit England, just count up the
number of different variations of this
wee beastie.
My point is this: who is to say that
every X number of years or so the
British Government, whether an EEC
partner or in post partnership disarray,
might not change their voltage standards yet again, like the design of their
GPO plugs?
Surely we can be as independent
of our former colonial masters as the
Americans? Or shall we wait for a
future (and probably somewhat short)
Australian Fearless Leader to pass a
very sensible law to lower the height
of every doorway in Australia by 10%.
They were too high anyway.
C. O’Donnell,
Hoppers Crossing, Vic.
Comment: our much admired GPO
socket will be modified in the nottoo-distant future, as determined by
the same people who want to bring
about the reduction in mains voltage.
Future GPO sockets (ie, mains power
points) will have a circular recess
which will make most presently used
AC & DC plugpacks obsolete and
unusable.
August 1994 5
How to use the
TEA1100 fast nicad
charger IC
The TEA1100 nicad charger IC, as used in
our recent Fast Nicad Charger project, has a
number of interesting features which put it out
in front. These include digital voltage sampling
and filtering as well as switchmode or linear
operation. We look at these in detail and go
through some design examples.
By DARREN YATES & LEO SIMPSON
The Philips TEA1100 Battery charger IC is a 16-pin DIP package which
contains everything to produce a
simple yet highly integrated battery
charger for nickel cadmium (NiCd) and
the new nickel metal hydride (NiMH)
batteries which have a higher capacity
than nicads.
The TEA1100 has three methods of
guarding against over-charging: temperature detection, clock timeout and
an advanced form of voltage detection
referred to as “dV sensing”.
Supply voltage
Unfortunately, the chip has a fairly
awkward supply voltage range, which
is between 5.65V and 11.5VDC. This
makes it not quite suitable for car
operation without supply regulation
circuitry and not low enough to permit operation from a 5VDC regulator.
However, a 7808 or 7809 regulator
will be more than adequate and, in
fact, you can even get away with just
a standard zener diode/transistor
buffer voltage stabiliser such as that
used in the Fast Nicad Charger design
published in the May 1994 issue of
SILICON CHIP.
Linear or switchmode
As we mentioned in the introduction, the TEA1100 IC can run in linear
or switchmode operation. The benefit
of the switchmode option is the efficiency which can be gained by charging lower voltage cells from a higher
Fig.1: this circuit using the TEA1100 in switchmode was the basis for the Fast Nicad Charger published in
the May 1994 issue. The design example in the text will enable you to tailor the circuit to your application.
6 Silicon Chip
Fig.2: this linear version of the
TEA1100 circuit could be used
in RF-sensitive applications. In
this case, the output of the chip
is taken from pin 2 rather than
the PWM output of pin 1.
voltage supply rail. This feature was
used in our Fast Nicad Charger project.
If you’re wanting to charge Nicads
in a noise sensitive application then
you can easily set the IC up to charge
in linear mode, greatly reducing the
circuit noise. The linear circuit uses
less components than the switchmode
circuit but has considerably more heat
dissipation, as you would expect.
Fig.1 shows a sample switchmode
circuit, very similar to that featured
in our May 1994 issue. Fig.2 shows a
linear charge circuit, powered from the
240VAC mains supply. And finally, to
give some idea of the chip complexity,
Fig.3 shows the block diagram of the
TEA1100.
dV sensing
Instead of comparing the voltage of
the battery being charged to a static
voltage reference, the TEA1100 uses a
dynamic process called “dV sensing”.
The “dV” term comes from calculus
and refers to the process of looking for
a very small change in battery voltage.
The TEA1100 compares the present
battery voltage to the previous sampled voltage and checks for a 1% drop.
The theory behind this is that when a
nicad is being charged, its voltage rises
very gradually towards full capacity
but once past this point, the battery
voltage begins to drop slightly.
If a battery charger circuit does not
look for this voltage drop, it will never
give an optimum charge – it will either
under or over-charge. Either way, the
battery life will ultimately be reduced.
Fig.4 shows the characteristic rise in
battery voltage during charge and the
slight droop as it reaches full charge.
The TEA1100 ends the charge cycle
upon sensing a 1% drop in the battery
voltage. That amounts to about 16mV
for a typical nicad cell. Now you might
be wondering how they manage to
reliably detect 16mV when the circuit
lines could be subject to all sorts of
noise and switching frequencies, if the
chip is being operated in switchmode.
The answer lies in the method of sampling the battery voltage.
The PWM (pulse width modulation)
is disabled for 10 clock cycles, after
which the sample and hold amplifier
takes a meas
urement of the battery
voltage. This way, the noise generated
by a “ringing” or decaying supply rail
is removed and a much greater degree
of accuracy maintained.
The 10-cycle delay gives sufficient
time for the inductor to stop ringing
but it does mean that the inductance
must lie within a particular range – it
must be high enough in value so that
it will perform its job as an inductor
in a switchmode circuit but it must
be small enough in value so that the
supply rail is quite stable by the time
10 clock periods have passed. We’ll
talk about this more a little later.
The dV sensing comes under the
block entitled “battery full detection”
in the diagram of Fig.3.
As already noted, the TEA1100
does not compare the battery voltage
to a static reference. Because it is
a dynamic process, the monitored
input voltage need only be between
0.385V and 3.85V. This is fed to pin 7
which is labelled “VAC” for Voltage
ACcumulator.
The way it works is like this: The
VAC voltage is sampled at a rate equal
to the clock frequency divided by 216.
Each VAC voltage sample is digitised
and stored in a register with a quoted
resolution of 12.5 bits. At the time of
the next sample, the stored value is
converted back to an analog voltage
and compared with the voltage on
the VAC pin.
If the VAC voltage is higher than
the stored value, then this new value
is digitised and stored in the register,
overwriting the previous value. If not,
the previous value remains in the
register. The circuit then checks for a
1% drop as we mentioned before and
if found, switches the circuit to trickle
mode and flashes the LED (connected
to pin 15) to indicate that the batteries
are fully charged.
This clever mix of analog and digital
circuitry results in a dynamic process
which takes the battery’s physical
characteris
tics into consideration.
Since no two nicads charge up to
exactly the same voltage, this relative
method provides accurate “full” detection for all cells, regardless of their
final voltage. Incidentally, much the
August 1994 7
VP
12
Vref
10
VS
6
NTC
3
Rn
11
IB
5
CP
9
Vr1
SUPPLY
GND
16
Vhigh
PROTECTION
Vr3
MAINS
ON
RESET
V
In
LSP
Iref
>
t
AO
2
A2
Vr2
Vlow PROTECTION
Vr4
LS
4
A1
>
>
OSC
DISABLE TIME OUT
>
R
s+h
BATTERY
FULL
DETECTION
VAC
7
PWM
1
PWM
&
R
TIME
OUT
PROTECT
>
LED
15
R
1/10
OSC
TO
PWM
:1:2:4
PRESCALER
COUNTER
CONTROL
CURRENTLESS SENSING
AUX PULSES
13
OSC
8
PR
14
SYNC
Fig.3: the block diagram of the TEA1100. This complex chip senses the small
drop in voltage which occurs at the end of charge for nicad & NiMH batteries, so
that the charger can be automatically switched off.
same monitoring method was used in
the “Fast Charger for Nicad Batteries”
featured in the January and February
1991 issues of SILICON CHIP.
The beauty of the dV sensing system is that the VAC input (pin 7) can
be anywhere between +0.385V and
+3.85V. This means that the VAC
resistor divider network can be the
same whether you wish to charge two
or 10 cells, or any number of cells in
between. To satisfy this condition
in the circuit of Fig.1, R14 should
be 47kΩ while R15 should be 10kΩ.
C8, the input filter capacitor, can be
10µF 16VW. Note that to satisfactorily
charge 10 cells, you will need an input
voltage of at least 22V DC when in
switchmode because the maximum
pulse duty cycle is 78%.
The above is based on an overvoltage level of 1.7V/cell and a nominal
battery voltage of 1.2V/cell.
The VAC input has four voltage
thresholds which determine the chip’s
behaviour. Firstly, below 0.3V, the IC
assumes a short circuit (crook) battery
and switches to trickle charge mode;
above 0.385V and below 3.85V, the IC
uses the dV voltage detection method
8 Silicon Chip
to determine the charge state; and
finally, above 4.25V, the IC assumes
open circuit or no batteries present
and switches off. The impedance of
this input is greater than 200MΩ.
Note too that for charging just one
or two cells, the VAC input (pin 7) can
be connected directly to the cell(s).
Output voltage
This brings us to an important
feature of the Fast Nicad Charger published in May 1994 and one which has
caused confusion to many constructors of this circuit. Since the circuit
relies on dV sensing to end the fast
charging mode, it goes without saying
that it will not work unless it is actually charging cells. If you attempt to
test the circuit without a nicad battery
load, it will switch off.
Our testing instructions for the
above circuit would have added to
this confusion by referring to an open
circuit output voltage test. The point is
that you cannot test the charger’s output voltage unless cells are connected.
If you attempt to simulate the presence
of cells with a large electrolytic capaci
tor, the output voltage will rise until
pin 7 reaches +4.25V whereupon the
circuit will switch off.
In fact, the circuit of May 1994 does
not even need the switch to select between two and four cells. The switch
setting for two cells can be omitted and
then circuit will happily charge two,
three or four cells in series without
further modifications.
In admitting this mistake, we can
only plead that it only become obvious after close reading of the copious application information which
Philips has made available on the
TEA1100.
0.5% detection
In some cases, such as “fast-charge”
nicads and NiMH cells, a dV of 0.5%
is more appropriate due to the higher
level of input charge current they can
tolerate. This IC can provide charge
rates up to an incredible five times the
battery capacity or “5C”. An example
of this would be charging a racing pack
in about 15 minutes.
This increased sensitivity can be
easily achieved by inserting a zener
diode of about half the battery voltage
into the sensing resistor string. An example of this can be seen in Fig.5. The
zener diode is selected to be about half
of the fully charged battery voltage,
based on a level of 1.7V/cell.
Protection
Apart from the active protection features already mentioned, the TEA1100
features under-voltage shutdown and
temperature sensing with a thermistor
input circuit.
The first of these, the under-voltage
shutdown, activates when the supply
voltage falls below 5.25V. In this case,
the IC goes into a “power down” mode
in which it becomes non-active and
draws around 35µA (45µA maximum).
The second form of protection
involves a negative temperature coefficient (NTC) thermistor to monitor
the temperature of the battery during
charging. This feature wasn’t included in our May 1994 project to keep
the construction simple. In practice,
where this feature is used, the therm
istor is incorporated into the battery
pack and is automatically connected
when the battery is put on charge.
The temperature monitoring feature
is recommended for batteries which
need to be recharged as soon as they
have been removed from their load.
The classic example of this is
1200mA.h racing packs for electric
model aircraft and cars. The drain on
these batteries is very high - often tens
of amps or more – and so they will be
quite hot (or even stinking hot!) when
they are removed from the load.
The danger is that if you fast-charge
a hot nicad battery, you can damage it.
The temperature protection provided
by the TEA1100 prevents fast charging
from occurring while the battery temperature is outside the specified range.
The NTC thermistor is featured on the
circuit of Fig.1 and is connected to pin
3. If the thermistor is not required, it
can be omitted from the circuit, together with R11.
Fig.4: the
voltage
characteristic
of a 2-cell
nicad battery
back during
charge. If
charging
continues
beyond the
droop in
voltage, cell
damage can
occur.
VOLTAGE (V)
For example, for a 6 cell pack, the
maximum voltage is 6 x 1.7V = 10.2V,
so a zener diode of 5.1V would be
suitable. The maximum voltage level
the VAC input will now see is 5.1V, so
the input resistor divider must now be
recalculated accordingly. R14 on Fig.1
could then be reduced to 22kΩ.
CHARGE TIME (MINS)
capacitor connected to pin 13.
This timeout period is usually set to
about 125% to 150% of the expected
fast charge time but in critical high
charge rate applications, you can set
it to the expected charge time (100%).
In practice, the timeout period
should only be set by adjusting the
capacitor (C at pin 13), as varying the
reference resistor will change other
circuit parameters.
Design example
The easiest way to understand how
to use this IC is to go through a design
example, using the circuit of Fig.1.
This way, you’ll get an idea of what
has to be done and the order in which
you have to do it.
Let’s say we wanted to design the
timeout circuit to run a charger which
will charge up a set of four nicad cells
in one hour. If we use the 150% rule,
then our timeout period, tTO, will be
Timeout counter
Finally, there is the backup protection of a timeout counter, which
automatically shuts down the charger
after a time equal to 226 times the clock
period, has expired. The clock period
is determined by the reference resistor
connected to pin 10 and the timing
Fig.5: a zener diode equal to
half the fully charged battery
voltage can be added to the
circuit to enhance the dV sensing
capability so that it will detect a
drop of 0.5%.
1.5 x 60 mins = 90 mins.
The timeout period is determined
by the following formula:
tTO = 226 x Tosc x p
where Tosc is the clock period and
p is a prescaling factor which you
can program to be either 1, 2 or 4,
depending on how you connect pin
8. By leaving pin 8 open, you set the
prescaling factor to 2. Connecting it
to pin 6 sets it to 1 and pulling pin
8 to ground sets it at 4. The beauty
of this system is that it allows you to
have three different charge periods
without having to change the timing
components.
For our example, let’s connect pin
8 to pin 6 to set the prescaling factor
(p) to 1. The oscillator frequency (1/
Tosc) now needs to be 12.4kHz (ie, Tosc
= (90 x 60)seconds/226). As mentioned
be
fore, this frequency is set by the
time constant formed by the reference
resistor Rref (R13) and the oscillator
capacitor Cosc (C7) based on the following equation:
Tosc = 0.93(Rref x Cosc)
Now Rref is chosen to be within the
range of 12.5kΩ and 125kΩ based on
the necessary charge current. In our
example, let’s assume that the resistor
is 27kΩ. Plugging this value into the
above equation gives a value for Cosc
of .0032µF which we can quite happily
round to .0033µF.
Charge current settings
OK. Let’s say that we wish to charge
our batteries at a fast rate of 700mA.
R4 and R8 are used to set the current.
R4 should be a 5W type. You have
some leeway in picking the value
of this resistor, so long as its value
August 1994 9
Using the TEA1100 fast nicad charger IC
results in a voltage drop of between
50mV and 200mV when the circuit
is in fast charge mode. You can work
out a suitable value for R4 from the
following equation:
Vcs = Ifast x Rcs
where Ifast is the fast charge current
and Rcs is R4. In our design example,
0.1Ω will give us 70mV which is within the desired range. R8 is referred to
as the fast charge current set resistor
Rfc and it can be calculated from the
following equation:
Rfc = (Ifc x Rref x Rcs)/1.25
where Ifc is the fast charge current rate,
Rref is the 27kΩ reference resistor R13,
and Rcs is the 0.1Ω current sensing
resistor R4.
By using this equation, we get a value for Rfc of 1.512kΩ, so a 1.5kΩ 1%
resistor will be perfect for R8.
determined by the worst case ripple
current at the trickle current setting
and follows this equation:
Lmin = Vo’max(1-delta)Tosc/2Iav
where Vo’max is the maximum battery
voltage plus the forward diode voltage drop. For four cells, this works
out to be 6.8V + 0.7V = 7.6V. This is
based on the fact, that the maximum
voltage per cell will be 1.7V; “delta”
refers to a charge current duty cycle
of 50%.
So, using the above equation, we
get a minimum inductance value of:
Lmin = 7.6 x (1-0.5) x 80 x 10-6/2 x
0.35 = 434µH.
Hence the inductor can be anywhere
between 5mH and 434µH. Why not go
for the perfect compromise and settle
upon 2mH?
What inductor?
Winding an inductor presents many
constructors with a problem since they
don’t have access to the necessary
information involving readily available toroids. Indeed, a comprehensive
article on this subject alone could
take many pages. However, to keep it
simple, we’ll just deal with the three
readily available iron powder toroids
made by Neosid and available from
Altronic Distributors and Jaycar Electronics.
The general formula for inductance
using these toroids is:
n = 1000 √(L/AL)
where n is the number of turns, L is
the inductance in millihenries (mH)
and AL is the inductance factor of the
particular core. For the smallest core,
Neosid 17-732-22, 14.8mm OD, AL is
44; for the medium core, Neosid 17742-22, 33mm OD, AL is 59; and for
the largest core, Neosid 17-745-22,
44mm OD, AL is 116.
Having calculated the number of
turns to obtain the required inductance
on the core of your choice, you then
must check whether it is likely to be
saturated at your proposed operating
current. To do this, we calculate the
core energy with the following formula:
E = LI2
where E is measured in joules, L is
the inductance in henries and I is the
current in amps. For the three cores
Earlier on, we mentioned that with
switchmode operation, you have to
be careful in selecting the value of the
inductor – too low a value will result
in the circuit not working efficiently
and too high a value will result in
the dV sensing circuitry picking up
remnants of the switching voltage due
to the “ringing” effect of the inductor.
For this dV sensing to work, the induc
tance current should have decayed to
zero within nine clock cycles. So the
maximum inductance is set by the
following equation:
Lmax = 9 x Tosc x (Vo + Vf)/Io
where Tosc is the period of the clock
frequency, Vo = the flat battery voltage
(around 1V per cell) plus the voltage
drop across the fast recovery diode
D2 (usually taken as 0.8V) plus the
voltage across the current sensing
resistor. Io is the average current
through the inductor which is a fast
charge current.
In the example we’ve been working
through, this would give us a maximum inductance of:
Lmax = (9 x 80µs x 4.8V)/700mA
= 5mH.
This assumes four cells with a flat
voltage of 1V each, plus the 0.8V
drop for the fast recovery diode, D2.
The 80µs figure is the clock period at
12.4kHz.
The minimum inductance value is
10 Silicon Chip
Winding an inductor
under discussion, the maximum
stored energy levels are 0.71mJ for the
14.8mm OD core; 5.1mJ for the 33mm
OD core; and 16mJ for the 44mm OD
core (OD stands for outside diameter).
If the core you have chosen will
saturate at the required current and
inductance, then you will have to use
a bigger core.
One final point must be covered
here before we leave the subject of
inductors and that is that the actual
current flowing in the inductor referred to in the formulas above is the
pulse current; it is not the charging
current. Typically, the pulse current
will be twice the average charging
current.
Trickle charge
When in trickle charge mode, the
TEA1100 continues to pulse the
battery with the fast charge current
but at a much lower duty cycle. As it
seems with just about everything else
on this IC, you have a choice of one
of two ways to set the trickle current,
depending on how you connect pin
11, designated the “Rn” input.
The first method is to leave pin
11 unconnected. In this case, the
repetition and duration of the trickle
current pulses is determined by the
chip itself.
The repetition rate is set as 2-14 x
tTO = 330ms in our example. The duration time is set to 0.75 x 29 x Tosc,
where Tosc is the clock period. In our
example, this works out to be 31ms.
This also gives us a duty cycle for the
trickle current of 9.4%.
The average trickle charge current
based on this duty cycle is set by the
following equation:
Itrickle = Ifc/2 x duty cycle = 30mA.
The second method is to set the
average trickle current yourself by
connecting a resistor Rn to pin 11. The
rule for this resistor is that it must be
within the range of 25kΩ to 250kΩ
and must be greater than the reference
resistor Rref.
The new trickle current equation
looks like this:
Itrickle = Ifc x (Rref/Rn) x duty cycle
With Rn equal to Rref (27kΩ), the
trickle current is 60mA and 7mA with
Rn equal to 250kΩ.
Linear design example
Let’s say that we want to charge
three “AA” cells in one hour, using
the circuit of Fig.2. The required
TABLE 1
Number of cells to be
charged
Transformer
secondary voltage
(V RMS, full load)
Capacitor value
(µF/A)
Capacitor voltage
rating (VDC)
2
7
4000
16
3
9
3000
25
4
11
2400
25
5
13
2000
35
6
15
1700
35
7
17
1500
40
8
19
1300
40
9
21
1200
50
10
23
1100
50
current is based on the following
equation:
Iout = (A.h x 60 x 1.4)/charge time
(mins)
So for a 600mA.h battery, the current
would need to be:
Iout = (600mA.h x 60 x 1.4)/60
= 840mA
In case you’re wondering why it just
isn’t 600mA, the reason is that there
are substantial losses in the battery
when charging takes place, so you
need to increase the charge current
by 40% to make up for these losses
(ie, heat etc.)
At this current, the main pass diode
D5 can still be a 1N4004 but the transistor will have to be something like
a TIP32C, a device which can handle
the current and the power dissipation.
And it will need a heatsink.
Power dissipation
Table 1 gives the required transformer secondary voltage and the
suggested capacitance per amp of
required current and voltage rating of
the filter capacitor. Now for our design
example, to charge up three cells, we
need a transformer secondary voltage
of 9.1V. The power dissipation can be
found from the following equation:
Pdiss = 1.3 x Iout x (Vsec - 2.0)
= 1.3 x 0.84A x (9.1 - 2.0)
= 7.8W
Basing this on a maximum temperature rise of 55°C above ambient, the
required heatsink will have to be better
than 55°C/7.8W or 7°C/W.
Now obviously, this is quite a bit of
power being wasted so you will have
to decide whether the need for a linear
charger outweighs the benefits of the
switchmode alternative.
OK, so we’ve determined the cur-
rent we require and now we have
to tell the TEA1100 what we want.
To do this, we again start with a
reference resistor of 27kΩ, just as
for the switchmode version. Next,
we have to choose the main current
sensing resistor (R1) and again, for
our charge current of 840mA, a 0.1Ω
5W resistor will give us 84mV which
is good enough. Remember that this
resistor doesn’t set the current on its
own. This is done by resistor R3 on
the circuit.
This resistor is determined by the
following equation:
Rfc = (Rref x Rcs x Ifc)/1.25
and in our design example, R3 becomes:
R3 = (27kΩ x 0.1Ω x 0.84A)/1.25
= 1.814kΩ
A value of 1.8kΩ will be close
enough.
Trickle charge
As with the switchmode version,
the trickle charge current can be set
to just about anything you want. By
connecting the prescaling pin (pin 8)
to pin 6 and leaving resistor R7 open
circuit, the TEA1100 will automatically set the trickle charge current to
1/20th of the fast charge rate. In our
example, this would work out to be
42mA.
Now this may be too high, in which
case, you can change the trickle current by connecting resistor R7 from
pin 11 to ground. The relationship
between this resistor and the trickle
charge current is set by the following
equation:
R7 = (1.25 x Rfc x 0.094)/(Itrickle x
Rcs x p)
Let’s say we wanted the trickle current to be 15mA instead of 42mA. By
working through the above equation,
resistor R7 would need to be:
R7 = (1.25 x 1.8kΩ x 0.094)/(15mA x
0.1Ω x 4) = 35.2kΩ.
A 36kΩ 1% resistor will get you
fairly close to the mark.
You should note a couple of things
here. Firstly, we’ve had to change the
prescaling factor to four. Now the
reason for this is that the prescaling
factor not only works on the timing
circuitry but also on the charge current ratio; that is, the ratio of the fast
charge current to the trickle charge
current.
With a prescaling factor of one (pin
8 to pin 6), the maximum ratio is 20:1.
For a prescaling factor of two (pin 8
open circuit), it is 40:1 and for four (pin
8 to ground), it’s 80:1. Now for our design we want a ratio of 840mA/15mA =
56:1. Setting the prescale to either one
or two won’t get us this value so we
have to go to a prescale factor of four.
The reason for the change is that
if resistor R7 is greater than twice
the reference resistor R6, then the IC
automatically selects half of the fast
charge reference current. This gives
us our maximum 20:1 with a prescale
of one, 40:1 with p set to two and 80:1
with p set to four.
In most situations, resistor R7
should not be less than the reference
resistor. If by working through the
equations, you find that R7 is less than
R6, either change the prescaling factor
or remove the resistor from the circuit
altogether.
Timeout counter settings
The last thing to do is to set the
timeout period and since we have
already set the reference resistor R6
to 27kΩ, the only component value
which affects the time is capacitor
C4 and this can be determined by the
following equation:
C4 = (60 x timeout)/0.93 x Rref
x p x 226
Getting back to our design example, let’s say that we’re happy with a
trickle current of 42mA and we want
the timeout period to be 60 minutes.
Capacitor C4 then works out to be:
C4 = (60 x 60)/(0.93 x 27kΩ x 1 x 226)
= .00213µF
(.0022µF will be close enough).
Note too that this capacitor value
will change if you change the pre
scaling factor as in the above example
where we looked at a trickle current
SC
of 15mA.
August 1994 11
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Please feel free to visit the advertiser’s website:
dicksmith.com.au
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Please feel free to visit the advertiser’s website:
dicksmith.com.au
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Please feel free to visit the advertiser’s website:
dicksmith.com.au
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Please feel free to visit the advertiser’s website:
dicksmith.com.au
Electronic
Engine
Management
Pt.12: Fueltronics’ Turbo Control Centre by Julian Edgar
Australian company Fueltronics
has recently released an automotive
turbo
c harger boost control unit.
Called the “Turbo Control Centre”,
the device undercuts its competitors
in price while also providing more
features. It uses a Signetics 80C575
microcontroller and sophisticated
software to control the turbo boost in
modified cars.
The unit consists of two solenoid-operated valves, an elec
tronic
control unit (ECU) housed in a diecast
aluminium box, and a dashboard
mounted liquid crystal display with
control knobs.
Conventional control
Conventional turbocharger boost
pressure control is by a wastegate
– a valve which diverts exhaust gas
around the tur
bocharger’s exhaust
turbine when the appropriate manifold supercharging pressure has been
reached. The wastegate is operated by
a rod connected to a diaphragm, one
The Turbo Control Centre uses a microcontroller & sophisticated software to
modulate turbocharger boost pressure. Note that the board in this photo is not
totally populated, with the output transistors & some ICs still to be added.
16 Silicon Chip
side of which sees manifold pressure.
As boost pressure rises, the diaphragm
deflects and the connecting rod opens
the exhaust turbine wastegate valve.
Electronic control
The Turbo Control Centre makes
use of this conventional mechanical
control but changes the pressure seen
by the wastegate actuator by bleeding
air from the pressure line connecting
the diaphragm to the manifold. A
pulsed solenoid valve is used to do
this and the greater the pulse-width
used, the higher the boost pressure experienced. In order to allow relatively
small valves and plumbing to be used,
a restricting orifice is placed upstream
of the bleed valve T-piece.
There are several advantages in using electronic control of the wastegate.
First, “wastegate creep” – where the
rate of boost increase starts to taper off
before the required level is reached
–is avoided. With electronic control,
the boost level can rapidly rise to the
specified level before wastegate opening occurs. This means that quicker
acceleration is enjoyed.
Second, electronic management allows greater driver control over boost
levels. The Turbo Control Centre uses
two preset levels of boost, which are
initially set with internal potentiom
eters. These preset levels are selected
using a pushbutton switch. Alternatively, the user can select the manual
Turbocharger control is achieved using two solenoid-operated valves. The
smaller valve on the left is used as a pulsed bleed valve & reduces the pressure
seen by the wastegate actuator. The larger valve at right is used as a throttleclosed pressure-relief valve & is designed to give better driving response.
Electronics engineer Jiri Bruderhans was responsible for the hardware
development of the boost controller. The unit has been designed so that it
can be interfaced with engine management software.
boost setting, which allows control
over the supercharging level via a
dash-mounted 10-turn potentiometer.
The other valve used by the Turbo
Control Centre works as a throttle-closed blow-off valve. Conventionally, when the throttle is quickly
closed following acceleration (eg,
during gear changes), the rapid pressure build-up upstream of the turbo’s
compressor slows the turbo. A slight
lag in boost build-up then occurs when
the throttle is opened again.
The Turbo Control Centre blow-
off system senses air pres
sure both
upstream and downstream of the
throttle valve using electronic pressure sensors. When the pressure being
experienced before the throttle blade
is greater than after the butterfly,
the large (25mm plumbing) valve is
opened and this air is bled back to the
turbo air intake. This allows the turbo
to keep spinning at a high speed so
that the boost quickly rises when the
throttle is next opened. The difference
required in the pressures either side of
the throttle butterfly before the blow-
off valve opens is adjustable with an
internal pot.
Shown on the dash-mounted LCD
screen is the boost level in either
numerical or bargraph form, and
the selected boost control (Preset 1,
2 or Manual). In addition, the word
“Blow!” is indicated when the blowoff valve is open. The display is also
used during the setting-up procedure.
The two signal inputs come from
the pressure sensors, both of which
are mounted within the ECU and are
fed by small bore rubber hoses. The
microprocessor and output drive
circuitry is also within this box, with
just the display electronics and input
switches located in the dash-mounted
unit.
Hardware & software
Running at a clock speed of 12MHz,
the Signetics 8051-family 80C575
microcontroller has a tough job to
do, especially in preventing boost
oscillation around the selected boost
level. The 8.5Kb program – which is
written in 805X assembler language
with ‘C’ 805X cross-compiler language
used –required the great
est design
effort in allowing boost to rapidly
rise without over-shooting the preset
value. Inadvertent excessive boost can
cause engine-destroying detonation.
The program uses a differential
equation for convergence, which allows the rising boost level to approach
the preset level in a manner which
allows system damping. The boost
control valve remains closed until
the boost level reaches a “window”
set at 75% of the preset value. When
this occurs, the control valve starts
closing, with the software setting its
pulse width on the basis of the rate of
approach or the distance to the preset
value. When the boost level reaches
95% of the preset value, the valve operation changes again, with a different
feedback loop being employed.
Engine management
Finally, since Fueltronics also
rewrite software chips for factory engine management systems, the Turbo
Control Centre has been designed to
interface with new engine management software. This means, for example, that when the high boost preset
is selected, an engine management
program with the appropriate fuel and
ignition maps can be automatically
SC
brought on-line.
August 1994 17
If you own equipment
which uses nicad
batteries, then this
discharger is for
you. Used correctly,
it will maintain the
full capacity of your
battery pack & extend
its useful life. It can
even rejuvenate an
old battery pack that’s
suffering from the
memory effect.
Automatic discharger
for nicad battery packs
By JOHN CLARKE
While nicad batteries are designed
to provide reliable power over many
charge/discharge cycles, most people
find that their new battery pack starts
to give trouble after only a few such
cycles. This problem is particularly
prevalent in mobile telephone battery
packs. The pack provides a reasonable “talk-time” when new but this
quickly diminishes after a few weeks
of use.
When this happens, many people
assume that the battery pack is crook
and buy a new one. But that’s normally a complete waste of money. As
a general rule, the battery will still be
quite OK and just needs to be revived.
18 Silicon Chip
The problem can usually be attributed to the so-called “memory effect”.
This is a characteristic of the nicad cell
whereby it ceases providing current
when it has discharged to the level
from which it was last charged. Thus,
if a nicad battery pack is repeatedly
recharged with half its capacity still
remaining, it will eventually stop delivering power at half capacity.
This means that, for the example
given above, the battery’s capacity is
effectively halved. Of course, if the
battery is continually recharged from
its 75% level, the problem is exacer
bated. It will now only provide 25%
of its capacity. With that in mind, it’s
not hard to understand why mobile
telephone batteries “run out of steam”
so quickly from new.
The only solution to this problem is
to ensure that the nicad pack is fully
discharged before recharging commences. This will ensure that the pack
can deliver its full capacity every time.
That’s where this Nicad Discharger
comes in. It discharges the nicad pack
until it reaches its full discharge voltage of 1.1V per cell, at which point it
automatically switches off. The pack
can then be removed and recharged
to its full capacity on a charger. By
adopting this technique, the dreaded
memory effect is avoided.
2x1N4004
D2
D3
Q1
BC327
C
E
33k
3.6V
1.5k
910
560
430
330
430
1.8k
A
D1
1N4004
B
3
S1
NOMINAL
BATTERY
VOLTAGE
2
8
IC1a
LM358
1
9.6V
10k
Q2
BC338
B
K
680
C
K
LED2
REVERSE
POLARITY
A
680
CELLS
UNDER
DISCHARGE
D4
1N4004
S2
START
E
4
7.2V
8.4V
LED1
DISCHARGING
33k
4.7k
4.8V
6V
27
5W
2.7k
REF1
LM3362.5
VR1
ADJ 100k
5
6
7
IC1b
470
Q3
BD679
B
E
12V
ADJUST
VR1 FOR
0.49V
1.8k
C
2. 7
B
PLASTIC
SIDE
E
E
C
B
C
VIEWED FROM
BELOW
ADJ
K
A
3-10 CELL NICAD DISCHARGER
Fig.1: the circuit is powered by the battery under discharge. When the START
switch (S2) is pressed, Q1 turns on & the battery voltage is fed to a resistive
divider. The voltage selected by S1 is then compared with a reference voltage
using IC1a, which turns on Q2 to maintain power when S2 is released. IC1b &
Q3 form a constant current source which discharges the battery to an end point
of 1.1V per cell. When this point is reached, Q2 turns off & the discharge cycle
ceases.
Note, however, that several full discharge/charge cycles may be necessary
to fully rejuvenate a battery pack that
is already suffering from the memory
effect. This technique is called “deep
cycling”. Provided that the pack is
OK in other respects, this treatment is
usually completely effective and leads
to a dramatic increase in battery life
and performance. And, of course, you
will save money – nicad batteries are
expensive.
Discharge rate
Our Nicad Discharger discharges
batteries at a nominal 200mA rate until
the end point voltage of 1.1V per cell
is reached. During this time, a LED on
the front panel glows to indicate that
the pack is discharging. When the end
point of 1.1V per cell is reached, the
discharger switches itself off and the
LED goes out to indicate the end of the
discharge cycle.
Thus, for a 7.2V battery pack, the
end point voltage is 6.6V. That’s
because there are six cells in a 7.2V
pack (ie, each cell is at 1.2V when
fully charged). Similarly, the end point
voltage for a 12V pack is 11V. Note
that nicad cells maintain a virtually
constant 1.2V output until they are
almost fully discharged.
The unit is very easy to operate – all
you have to do is connect the positive
and negative leads to the battery pack,
set the range switch to the rated battery
voltage, and press the START button.
The rest all happens automatically and
you simply wait until the DISCHARGE
LED goes out before removing the pack
for recharging.
A second LED on the front panel
lights to warn you if the pack is accidentally connected with reverse polar-
ity. No damage to the Nicad Discharger
(or to the pack) will occur if you do
this – just reverse the connections to
correct the problem.
In fact, this design is based substantially on the Nicad Discharger published in July 1992. This was a popular
unit but, following publication, we
received many requests for two extra
voltage ranges below 6V. This new
circuit adds these ranges and can now
handle nicad packs ranging from 3.6V
to 12V over seven ranges.
In addition, the new design includes
the aforementioned automatic switchoff feature and the reverse polarity
indicator – items that were missing
from the previous design.
Circuit details
Fig.1 shows the circuit details of the
Nicad Discharger. It’s based mainly on
Main Features
•
Seven ranges; suitable for 3.6V, 4.8V, 6.0V, 7.2V, 8.4V, 9.6V & 12V
nicad battery packs
•
•
Discharges battery down to 1.1V per cell
•
•
•
Discharge indicator LED
Automatic switch-off with negligible current drawn after end
point voltage is reached
Reverse current protection & LED indicator
Self-powered from discharging cells
August 1994 19
430
1.8k
430
330
REF1
D3
33k
LED1
10k
VR1
A
K
Q2
560
33k
B C E
1.5k
Q3
Q1
2. 7
D2
680
S2
D1
2.7k
470
910
680
1.8k
4.7k
1
IC1
LM358
S1
K
D4
27W
5W
TO
CELLS
A
LED2
Fig.2: install the parts on the PC board as shown in this wiring diagram. Make
sure that all polarised parts are correctly oriented & mount the 27Ω 5W resistor
slightly proud of the board to allow the air to circulate beneath it for cooling.
Fig.3: check your PC board against this full size etching pattern
before installing any of the parts.
dual op amp IC1, transistors Q1-Q3,
and voltage reference REF1. The op
amp is an LM358 which can operate
from a supply rail as low as 3V. This
allows the circuit to operate correctly
while discharging a 3.6V battery pack
to an end point of 3.3V.
Initially, when a battery pack is
connected, no current flows in the
circuit since all transistors are off. The
circuit is turned on simply by pressing
momentary pushbutton switch S2.
When this happens, base current for
Q1 flows via its 4.7kΩ base resistor,
the base emitter junction itself and the
27Ω emitter resistor. Q1 thus turns on
and applies power to pin 8 of IC1, to
voltage reference REF1 via a 1.8kΩ resistor, and to a resistive divider string
(33kΩ - 1.8kΩ).
REF1 is an LM336-2.5 voltage
reference and this device provides
a constant 2.5V output over a wide
current range from 400µA to 10mA.
This voltage is fed to trimpot VR1
which is adjusted to provide a 0.49V
Fig.4 (above): here are the mounting
details for Darlington transistor Q3. It
must be isolated from the front panel
using an insulating washer & its leads
bent at right angles to mate with the
pins on the PC board – see photo at
left.
20 Silicon Chip
reference for the inverting input (pin
2) of comparator stage IC1a.
IC1a compares the voltage at the
wiper of switch S1 with the 0.49V
reference on pin 2. If the voltage on pin
3 is greater than 0.49V (ie, the battery
is not fully discharged), pin 1 of IC1a
switches high and turns on transistor
Q2 via a 10kΩ base resistor. This in
turn ensures that Q1 remains on and
that the circuit remains powered up
when S2 is released.
At the same time, LED 1 (the DISCHARGE indicator) turns on, since
there is a path to ground via the 680Ω
resistor and Q2.
IC1b and Darlington transistor Q3
form a constant current source which
discharges the battery at a nominal
180mA. The non-inverting input
of IC1b (pin 5) is set at 0.49V (the
reference voltage from VR1), while
the inverting input (pin 6) monitors
Q3’s emitter voltage. IC1b’s output
appears at pin 7 and drives Q3 via a
470Ω resistor.
As a result, a voltage of 0.49V is
maintained across Q3’s 2.7Ω emitter resistor and this sets the current
through Q3 to about 180mA. This
current flows via diode D4 to discharge
the cells. In addition, some discharge
current also flows through LED 1 and
IC1, so that the total discharge current
adds up to a nominal 200mA.
The resistive divider network sets
the cutoff voltages for the various
battery packs. This network is tapped
off using switch S1 and the sampled
battery voltage then fed to pin 3 of
IC1a which operates as described
previously.
In practice, the resistor values
were selected so that, for each range,
the voltage on S1’s wiper is at 0.49V
when the pack has discharged to 1.1V
per cell. These resistor values take
into account the fact that the voltage
across the 27Ω 5W resistor increases
by about 30mV for every volt applied
to the circuit.
When the voltage at S1’s wiper
subsequently drops just below 0.49V
(ie, when the battery pack drops just
below its end point voltage), pin 1 of
comparator IC1a switches low and
removes the drive to Q2. Q2 thus turns
off and so Q1 also turns off and interrupts the power to the circuit.
This also turns off the DISCHARGE
LED and transistor Q3 (since there is
no longer any drive from IC1b), and so
the battery ceases discharging.
PARTS LIST
1 PC board, code 14306941,
101 x 49mm
1 plastic case with aluminium lid,
115 x 65 x 40mm
1 front panel label, 64 x 126mm
2 alligator clips (1 red, 1 black)
1 150mm-length of red hook-up
wire
1 150mm-length of black hookup wire
1 small cordgrip grommet
1 knob to suit
1 single-pole 7-position rotary
switch
1 momentary pushbutton switch
1 TO-126 mica or silicone
insulating washer
1 3mm screw & nut to mount Q3
1 100kΩ vertical trimpot (VR1)
5 PC stakes
This view shows how the fully-assembled PC board appears after the front panel
has been removed. Note that Darlington transistor Q3 should be mounted on the
front panel before soldering its leads to the stakes on the board.
Reverse polarity protection for the
circuit is provided using diodes D1-D4
and the 27Ω resistor. If the battery is
connected with reverse polarity, D1
clamps the voltage across IC1a to just
0.6V, D2 and D3 conduct to prevent
destructive reverse breakdown of Q1,
and D4 prevents reverse current flow
through Q3.
The 27Ω resistor provides current
limiting under reverse polarity conditions. This device dissipates about
3.4W when a 12V battery is incorrectly
connected, hence its 5W rating.
Finally, LED 2 is forward biased
under reverse polarity conditions and
so lights to provide a visual warning.
Board assembly
The Nicad Discharger circuit is built
on a PC board coded 14306941. Fig.2
shows the wiring details.
Begin the construction by installing
PC stakes at the external (plus & minus)
lead positions and at the BCE positions
for Q3. This done, install the resistors,
taking care to ensure that you have the
correct value in each position. Table 1
shows the resistor colour code but it’s
also a good idea to confirm each value
using a digital multimeter, as some of
the colours can be difficult to decipher.
The 27Ω 5W resistor should be
mounted about 2mm above the PC
board so that the air can circulate
beneath it for cooling.
Now install the IC, the diodes and
transistors Q1 & Q2. Make sure that
these components are all correctly
oriented – pin 1 of the IC is adjacent to
a small notch in one end of its plastic
body. Note that Q1 is a PNP transistor
Semiconductors
1 LM358 dual op amp (IC1)
1 LM336-2.5 reference (REF1)
1 BC327 PNP transistor (Q1)
1 BC338 NPN transistor (Q2)
1 BD679 NPN Darlington
transistor (Q3)
4 1N4004 1A diodes, (D1-D4)
2 3mm red LEDs (LED 1,LED 2)
Resistors (0.25W, 1%)
2 33kΩ
2 680Ω
1 10kΩ
1 560Ω
1 4.7kΩ
1 470Ω
1 2.7kΩ
2 430Ω
2 1.8kΩ
1 330Ω
1 1.5kΩ
1 27Ω 5W
1 910Ω
1 2.7Ω
TABLE 1: RESISTOR COLOUR CODES
❏
No.
❏ 2
❏ 1
❏ 1
❏ 1
❏ 2
❏ 1
❏ 1
❏ 2
❏ 1
❏ 1
❏ 2
❏ 1
❏ 1
Value
33kΩ
10kΩ
4.7kΩ
2.7kΩ
1.8kΩ
1.5kΩ
910Ω
680Ω
560Ω
470Ω
430Ω
330Ω
2.7Ω
4-Band Code (1%)
orange orange orange brown
brown black orange brown
yellow violet red brown
red violet red brown
brown grey red brown
brown green red brown
white brown brown brown
blue grey brown brown
green blue brown brown
yellow violet brown brown
yellow orange brown brown
orange orange brown brown
red violet gold brown
5-Band Code (1%)
orange orange black red brown
brown black black red brown
yellow violet black brown brown
red violet black brown brown
brown grey black brown brown
brown green black brown brown
white brown black black brown
blue grey black black brown
green blue black black brown
yellow violet black black brown
yellow orange black black brown
orange orange black black brown
red violet black silver brown
August 1994 21
This view shows how the front panel is attached to
the PC board & secured via the switch bushes. Note
the mounting details for transistor Q3.
Discharge
Current
12V
11V
210mA
8.8V
200mA
8.4V
7.7V
7.2V
6.6V
6.0V
5.5V
4.8V
4.4V
3.6V
3.3V
190mA
180mA
Turn-off accuracy: within 10mV per cell.
Leakage current after discharge: <2µA at 11V;
<0.25µA below 6V.
Reverse battery polarity current: 370mA <at> -12V;
140mA <at> -6V; 70mA <at> -3.6V.
BATTERY VOLTAGE
3.6V .
+
. 8.4V
. 9.6V
. 12V
+
own label from the published artwork
– see Fig.5. Because it handles most
of the current, Q5 requires a modest
amount of heatsinking and this is
achieved by mounting it on the lid of
the case – more on this later.
PRESS TO
START
+
End Point
Voltage
9.6V
+
+
REVERSE
DISCHARGE POLARITY
NICAD DISCHARGER
The unit is housed in a plastic utility
case which has an aluminium lid. This
is fitted with an adhesive label measuring 64 x 126mm or you can make your
Range (Batt.
Voltage)
7.2V
.
Final assembly
Specifications
6.0V .
4.8V .
while Q2 is an NPN type, so don’t get
these two transistors mixed up.
Trimpot VR1 and REF1 can be installed next (watch the orientation of
REF1) but leave Q3 off for now since
it must be mounted on the metal lid
of the case. Switches S1 and S2 are
soldered directly to the PC board – see
Fig.2 and the photos.
The two LEDs can now be installed
in the respective locations but don’t
solder their leads yet. That step comes
later, after they have been pushed
through their mounting holes on the
front panel of the case. Be sure to orient
the LEDs correctly – the anode lead of
each LED is the longer of the two (see
pinout diagram on Fig.1).
Fig.5: this full-size artwork can be used as a drilling template for the front panel.
22 Silicon Chip
Begin the case assembly by attaching
the label to the lid, then drill holes to
accept the two 3mm LEDs, switches S1
and S2, and a 3mm mounting screw
for Q3. Note that it’s best to drill small
pilot holes for the two switches and
then slowly enlarge them to the correct
size using a tapered reamer.
Deburr all holes after drilling and
pay particular atten
tion to the area
around the transistor mounting hole
–it must be perfectly smooth and free
of metal swarf to avoid punch through
of the insulating washer used later
to isolate the transistor from the lid.
A hole should also be drilled in one
end of the case to accept a cordgrip
grommet for the battery leads.
As supplied, the rotary switch will
have 12 positions, so you will have to
adjust the selector ring to change it to
a 7-position type. To do this, simply
remove the nut and lockwasher from
the threaded bush, then lift the selector ring and rotate it so that the
locating pin goes in slot seven.
Check that the switch does indeed now have seven positions,
then trim the length of the shaft
to suit the knob.
Fig.4 shows the mounting
details for tran
s istor Q3. It
must be electrically isolated
from the front panel using a
mica washer. Make sure that
the mounting area is perfectly
smooth and smear both sides of
the mica washer with heatsink
compound (not necessary if a
silicone washer is used) before
bolting the assembly together.
The leads of the transistor are
then bent at right angles so that
Test & adjustment
To test the unit, you will need to
drill a small access hole through the
front panel immediately above VR1.
Alternatively, you will have to temporarily remove the front panel.
Next, connect a 6V battery pack (or
variable supply) to the circuit and
wind VR1 fully anticlockwise to ensure that the discharge transistor (Q3)
remains off. This done, set S1 to the
4.8V range and press S2 to start the
discharger. Check that there is now 6V
between pins 8 & 4 of IC1 and 2.49V
across REF1 when S2 is released. The
DISCHARGE LED (LED 1) should also
be alight.
If everything checks out so far, connect your multimeter across the 2.7Ω
resistor (next to Q3) and adjust VR1
for a reading of 0.49V. This adjustment
sets the reference voltage applied to
IC1a and ensures correct operation
of the constant current source (IC1b
& Q3). Switch off immediately after
making this adjustment and re-attach
the front panel (if necessary).
If you have a variable power supply,
check that the discharger switches off
at the correct voltage for each range selected (see specifications). The reverse
polarity indicator circuit can be tested
by reverse connecting the power and
checking that LED 2 lights.
Finally, always be sure to set S1 (the
range selector switch) to the nominal
voltage of your battery pack before
pressing the START switch to begin
the discharge cycle. For example, if
your nicad pack has a nominal output
of 7.2V when fully charged, then set
SC
S1 to the 7.2V range.
SILICON CHIP SOFTWARE
Now available: the complete index to
all SILICON CHIP articles since the first issue in November 1987. The Floppy Index
comes with a handy file viewer that lets
you look at the index line by line or page
by page for quick browsing, or you can
use the search function. All commands
are listed on the screen, so you’ll always
know what to do next.
Notes & Errata also now available:
this file lets you quickly check out the
Notes & Errata (if any) for all articles published in SILICON CHIP. Not an index
but a complete copy of all Notes & Errata text (diagrams not included). The file
viewer is included in the price, so that you can quickly locate the item of interest.
The Floppy Index and Notes & Errata files are supplied in ASCII format on a
3.5-inch or 5.25-inch floppy disc to suit PC-compatible computers. Note: the File
Viewer requires MSDOS 3.3 or above.
ORDER FORM
PRICE
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Floppy Index (incl. file viewer): $A7
❏
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❏
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❏
Stepper Motor Controller Software (January 1994): $A7
❏
Gamesbvm.bas /obj /exe (Nicad Battery Monitor, June 1994): $A7
❏
Diskinfo.exe (Identifies IDE Hard Disc Parameters, August 1995): $A7
❏
Computer Controlled Power Supply Software (Jan/Feb. 1997): $A7
❏
Spacewri.exe & Spacewri.bas (for Spacewriter, May 1997): $A7
❏
I/O Card (July 1997) + Stepper Motor Software (1997 series): $A7
POSTAGE & PACKING: Aust. & NZ add $A3 per order; elsewhere $A5
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order to (02) 9979 6503; or ring (02) 9979 5644 and quote your credit card number
(Bankcard, Visa Card or MasterCard).
✂
they mate with the BCE PC stakes on
the board.
The front panel can now be attached
to the PC board by fitting the matching
holes over the switch bushes and doing
up the locking nuts. Note that S1 is
fitted with a large star washer, while
S2 has a flat washer fitted to its bush
(these washers all go behind the front
panel). This done, the two LEDs can
be pushed into their front panel holes
and their leads soldered.
The assembly can now be completed
by attaching the battery leads to the
PC board (red for positive, black for
negative). These leads pass through
the cordgrip grommet in one end of the
case and are terminated with alligator
clips or with some other suitable connector for your battery pack.
August 1994 23
CIRCUIT NOTEBOOK
Interesting circuit ideas which we have checked but not built and tested. Contributions from
readers are welcome and will be paid for at standard rates.
VCC
LDR1
IC2d
4093
12
1M
47k
14
13
100k
3
100
270k
47k
0.1
11
6
7
7
IC1
2 LM741
4
4001
6
100k
D2
1N914
D1
1N914
5
2
0.1
10
1
10M
14
IC3b
+12V
4
IC3a
4.7k
3
1
IC2a
8
IC3c
VCC
16
47k
Q1
BC548
7
9
VR1
100k
RLA
D3
1N4001
16
IC4
10 CLK4040O12 1
3
14
CLK
2
10
8
11 D11
1N914
1
IC5 D5
4017 D6 5
D7 6
2
3
10
47k
1
13
12
S1
IC3d
4
5
11
330k
6
8
ENA RST
13
15
22k
+12V
VCC
10M
D10
1N4004
5.6k
1
EXTERNAL
INPUTS
D3 7
D4 10
D8
1N914
1
10k
10M
D9
1N914
VR2
1M
5
47k
IC2b
6
Q2
BC548
6
7
2
4
4
8
IC7
555
4.7k
3
Q3
BC548
5
1
220
RLB
.01
D4-D7
4x1N4004
+12V
IC6
7808
IN
AC
INPUT
1000
GND
OUT
10
Timer for
security lights
This timer can be used to turn on
security lights from dusk until dawn
or for a preset period ranging from
3-7 hours. It also has provision for
connection of a PIR sensor.
LDR1 is connected to the non-inverting input of op amp IC1 which
24 Silicon Chip
VCC
0.1
S1 : 1 : DUSK TO DAWN
2 : 3 HOURS
3 : 4 HOURS
4 : 5 HOURS
5 : 6 HOURS
6 : 7 HOURS
functions as a Schmitt trigger. When
darkness falls, the output of IC1
switches low. During daylight, IC1’s
output is high and this is fed via NOR
gates IC3c & IC3d to hold counters IC4
and IC5 reset. When IC1 goes low, the
reset is removed from IC4 and IC5.
IC2d’s output now goes high which
sets the flipflop consisting of IC3a and
IC3b. Pin 3 of IC3a now goes high and
turns on Q1 and relay RLA. This turns
on the lamps.
IC4 is clocked by Schmitt trigger
oscillator IC2a and provides a division
of 2048. Pin 1 of IC4 clocks decade
counter IC5. Trimpot VR1 is adjusted
so that one pulse per hour is fed to
IC5. As IC5 clocks, each of its outputs
goes high in turn. When the output that
is selected by S1 goes high, flipflop
IC3a/b will be reset which means that
pin 3 will go low. This will turn off
the relay. Nothing more happens now
until night falls again. When it does,
the process will repeat itself.
The 555 timer, IC7, provides for
PIR sensor or light beam relay sensor
control. When a positive going pulse
is applied to either external input, pin
4 of IC2b will go low. This triggers the
555 monostable. Its pin 3 goes high to
turn on transistor Q3 and relay RLB,
for a time period determined by the
components at pin 6 of IC7. Q2 makes
the 555 retriggerable so that further
pulses to the external inputs will reset
the circuit for another period.
A kit comprising all components,
relays and rotary switch but not including the mains transformer or the
boxes is available for $49.95 plus $5
for postage & packing. Contact CTOAN
Electronics, PO Box 211, Jimboomba,
Qld 4280. Phone (07) 297 5421.
Tester for radio
control servos
This circuit can be used
VR1
50k
to check servos for their
maximum throw, direc18k
tion of travel, current consumption, jitters or glitch
es, as well as being used
6
for linkage adjustments in
5
models without the need
to use a transmitter.
In a radio control system the receiver sends
down to each servo a train
of pulses corresponding to the stick
positions on the transmitter, where
the width of each pulse determines
the position of a particular servo.
The pulse width usually varies from
1-3ms with a repetition rate of about
40Hz. The pulses are positive in radios such as JR, Sanwa, Futaba and
Multiplex.
These pulse width commands can
be simulated by a variable-duty cycle
oscillator built around two gates of a
Automotive
voltage regulator
This automotive voltage regulator is based on a circuit sent
in by Bevan Paynter of Williams,
SA. The original version was used
to replace the electromechanical
regulator in his car, although this
revised version has not been built
and tested.
An automotive voltage regulator
works by controlling the current in
the field of the alternator, which in
turn controls the stator output. In
this circuit, ZD1 conducts when
the alternator output reaches 14.2V,
turning on Q3. This turns off Dar
lington pair Q1 & Q2, which were
completing the field circuit.As the
voltage drops below 14.2V, ZD1
ceases conducting, Q3 turns off,
and Q1 & Q2 turn back on again.
500mA
FS
100
10
0.1
D1
1N4001
SIG
.047
4
0.22
5.4V
6V
150k
IC1b
S1
D2
1N4001
OFF
4.8V
4011
2
1
IC1a
3
12
13
14
IC1d
7
11
8
9
SERVO
6V
IC1c
10
0.8-3ms
~25ms
4011 quad 2-input NAND gate IC. The
0.22µF capacitor and 150kΩ resistor
at pin 2 set the ON-period of the oscillator to about 25ms (ie, 40Hz rate),
while the .047µF capacitor at pin 3
together with the associated 18kΩ resistor and 50kΩ potentiometer (VR1)
allow the pulse width to be varied
from 0.8-3ms.
The resulting negative pulse train
from pin 3 of IC1a is buffered and inverted by IC1d, with pin 11 connected
to the positive signal input of the servo
being driven.
IC1c further inverts the signal train
to provide a negative pulse train. A
cheap VU-meter shunted by two 1Ω
resistors provides current monitoring
with a full scale sensitivity of 500mA.
Diodes D1 & D2 and switch S1 make
the circuit able to provide pulse trains
to suit various receiver voltages.
Manfed Schmidt,
Edgewater, SA. ($20)
TO CATHODE-ANODE
This switches the field
JUNCTIONS OF STATOR
ALTERNATOR
DIODES
current back on again
LIGHT
and so the output volt+12V
age settles at 14.2V.
D2
D3
D4
D1 protects Q1 from
3x1N5404
spikes and transients
generated by the field
D1
FIELD
coil switching action.
1.5k
COIL
1N4002
1k
It is absolutely critQ2
BD139
ical to obtain a 12.8V
ZD1
Q3
zener diode for ZD1, to
12.8V
BC337
obtain a 14.2V charg
Q1
ing voltage. All zener
2N3055
1k
1k
diodes vary from their
nominal rating, so
CHASSIS
you will have to test a
Finally, for a 9-diode alternator,
number of 13V zeners
discard diodes D2-D4 (since these
to obtain the correct value. Note:
diodes will already be present in
for zero temperature coefficient of
the alternator). Note that transisthe zener voltage, use two 400mW
tor Q3 should be mounted on a
zener diodes (6.2V and 6.8V nomheatsink.
inal) in series. This will give much
SILICON CHIP.
improved temperature stability.
August 1994 25
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Rod Irving Electronics Pty Ltd
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Rod Irving Electronics Pty Ltd
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Rod Irving Electronics Pty Ltd
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Rod Irving Electronics Pty Ltd
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Rod Irving Electronics Pty Ltd
This tiny board is
a voice-operated
switch designed
to fit into the
tightest space. It
uses a single IC &
includes a SPDT
12VDC relay. It
has almost no
turn-on delay & a
3-second release
time.
By DARREN YATES
S
O WHAT IS A VOX? Well, VOX
stands for voice-operated relay
or switch. They’re most often
used in “hands-free” communication
such as amateur transceivers, mobile
radios and some public address applications. The idea behind a VOX
is that instead of the user pressing a
button on the microphone to speak (ie,
the press-to-talk switch), the sound of
the voice is used to activate it instead.
This leaves the user with an extra hand
free to sit back with scones and a nice
cup of tea.
Our circuit uses one IC and a tiny
SPDT (single-pole dou
b le-throw)
relay which can be used to switch
on or off just about anything you like
(but not 240V equipment). The relay
we’ve used comes from Altronics
(Cat.S-4140) and measures only 16 x 11
x 10mm – pretty tiny for a mechanical
relay with a contact rating of 2A.
In keeping with this, we’ve made
the rest of the circuitry as small as
possible so that you could install the
VOX almost anywhere. It runs from
a 12VDC supply and current drain
is low, about 5 to 7mA quiescent
and around 35mA when the relay is
actuated.
Circuit description
The circuit for the MiniVOX is
shown in Fig.1. As you can see, it
is a “bare-bones” design involving
an LM358 dual op amp (IC1), one
transistor, the relay and a few other
components. Voice signals are picked
up by the electret microphone and fed
to op amp IC1a. This is connected as a
non-inverting amplifier with a gain of
151 or +43.6dB. The 100pF capacitor
across the 150kΩ feedback resistor
rolls off the high frequency response
above 10kHz so that there is no chance
of the circuit responding to spurious
RF signals.
The output of op amp IC1a at pin 1
feeds two diodes, D1 and D2, which
Build the MiniVOX
voice operated relay
All the parts except for the electret microphone are mounted on a small PC
board. Keep the microphone well away from the board, otherwise the relay
noise will repeatedly trigger the VOX circuit. The circuit is suitable for
switching low voltage equipment only (up to about 30V).
function as a half-wave voltage doubler. These rectify the audio signal to
produce a DC voltage across the 2.2µF
capacitor which is directly proportional to the loudness of the sound fed to
the microphone.
This DC voltage is fed to the remaining op amp in the package (IC1b) and
this is connected as a comparator. The
DC voltage from the rectifier is fed to
pin 5 while a resistive voltage divider
applies about +2V to pin 6.
Once the DC voltage across the 2.2µF
capacitor rises above the voltage at pin
6, pin 7 of IC1b pulls high, which turns
on transistor Q1, a BC548 NPN type.
This turns on the relay and lights up
LED 1. Q1 remains on and the relay
is actuated while ever the DC voltage
at pin 5 is above the voltage at pin 6.
Because of the high gain of op amp
August 1994 31
D4
1N4004
10
10k
10k
3
8
IC1a
2 LM358
MIC
1
0.1
D3
1N4004
1k
2x1N914
D2
D1
100pF
6
1M
K
LED1
5
2.2
63VW
A
7
IC1b
12V
PLUGPACK
RLY1
10k
B
C
Q1
BC548
E
4
2.2k
150k
B
1k
2.2
25VW
E
C
E
B
VIEWED FROM BELOW
C
A
K
MINIVOX VOICE OPERATED RELAY
Fig.1: the circuit is based on dual op amp IC1. IC1a functions as a microphone
preamplifier & this drives a diode charge pump based on D1 & D2. When the
voltage across the 2.2µF capacitor on D2’s cathode exceeds a preset level, pin 7
of Schmitt trigger stage IC1b switches high & turns on Q1 & the relay.
PARTS LIST
1 PC board, code 06109941,
code 47 x 44mm
1 electret microphone insert
1 2A SPDT relay (Altronics Cat
S-4140)
Semiconductors
1 TL072, LM358 dual op amp
(IC1)
1 BC548 NPN transistor (Q1)
2 1N914, 1N4148 small signal
diodes (D1,D2)
2 1N4004 rectifier diodes (D3,
D4)
1 red light emitting diode
(LED1)
Capacitors
1 10µF 25VW PC electrolytic
2 2.2µF 16VW PC electrolytic
1 100pF ceramic
Resistors (1%, 0.25W)
1 1MΩ
1 2.2kΩ
1 150kΩ
2 1kΩ
3 10kΩ
IC1a, together with the addi
tional
gain in the half-wave voltage doubler,
the circuit has a very fast response to
audio signals. On the other hand, the
“release” time (the time taken for the
relay to drop out) takes about three
seconds, as determined by the time
constant comprising the 2.2µF capacitor shunted by the 1MΩ resistor and
the threshold voltage of IC1b, as set
at pin 6.
Diode D3 is connected across the
coil of the relay to protect the transistor when it switches off. If the diode
was not there, the inductive kickback
from the relay coil when the current
is switched off could destroy the
transistor.
Power for the circuit can come from
any 12VDC source; eg, car battery, DC
plugpack, SLA battery – whatever
you like. Diode D4 prevents reverse
polarity connections from damaging
the circuit.
Construction
All of the components, including
the LED and the relay are installed
on a small PC board coded 06109941
and measuring 47 x 44mm. Before you
begin any soldering, check the board
thoroughly for any shorts or breaks
in the copper tracks. These should be
repaired with a small artwork knife
or a touch of the soldering iron where
appropriate.
When you’re happy that everything
appears to be OK, you can start construction by installing the wire link,
followed by the resistors, diodes,
capacitors, IC, the transistor, the LED
and finally the relay. Note that to make
the board as small as possible, all of
the resistors and diodes are mounted
on their ends. Each component has a
spacing of 0.2-inch or 5mm between its
pins. Use the overlay wiring diagram
to ensure that each component goes
into the correct position.
You will find that the circuit works
best with the microphone connected
to the circuit via a pair of flying leads
about 50mm long. Don’t make them
too long otherwise the leads may pick
up hum. Because the relay switching
itself makes noise, it’s quite easy for
the circuit to “chatter” because of the
relay sound being picked up by the
mike. So keep the microphone away
from the relay.
RESISTOR COLOUR CODES
❏
No.
❏ 1
❏ 1
❏ 3
❏ 1
❏ 2
32 Silicon Chip
Value
1MΩ
150kΩ
10kΩ
2.2kΩ
1kΩ
4-Band Code (1%)
brown black green brown
brown green yellow brown
brown black orange brown
red red red brown
brown black red brown
5-Band Code (1%)
brown black black yellow brown
brown green black orange brown
brown black black red brown
red red black brown brown
brown black black brown brown
Another place for experimentation is in the threshold
resistors. By adjusting the
A
N/C
RELAY
10kΩ and 2.2kΩ resistors, you
Q1
D3
can adjust the threshold or
N/O
A
1k
more importantly, the on and
10k 10k
10uF
off delay times. Having a higher
2.2k
D2
threshold voltage will mean
K
IC1
that the circuit takes longer to
10k
A LM358
D4
2.2uF
1
MIC
switch on for some sounds and
K
150k
12V
will switch off sooner wherePLUGPACK
D1
as a lower threshold voltage
100pF 2.2uF
(achieved by reduc
i ng the
Fig.2 (left): some of the parts on the PC board are mounted “end-on” to save space, as
2.2kΩ resistor) would result
shown on this wiring diagram. Fig.3 at right shows the full-size PC etching pattern.
in a very quick on time and a
longer release time.
Don’t forget to include the PC stakes immediately and check your circuit
You could also use this circuit as a
as well. These will make it much easier against the overlay diagram for pos- very simple front door light whereby
for you to solder the connecting leads sible errors.
a sound triggers the relay to switch
to the board.
on a 12VDC light globe for say 30 secExperimentation
onds. You could adapt the circuit to
Installation
This circuit provides plenty of do this by simply replacing the 2.2µF
You can easily install the board possibilities for experimentation. By capacitor with a 10µF capacitor and
in existing equipment wherever you using a 150kΩ feedback resistor with increasing the 1MΩ resistor to around
can find enough room and a suitable IC1a, we have fixed the sensitivity of 3.3MΩ. The light globe connects to the
12VDC supply.
the circuit to one which should suit relay outputs.
Again, you can adjust the sensitivity
When the unit is powered up, the most people. Alternatively, you could
quiescent current should be around replace this feedback resistor with so that the circuit picks up sounds
5-7mA, increasing to around 35mA a 200kΩ logarithmic pot which will close to your front door and ignores
with the relay in action. If it is sub- allow you to vary the sensitivity over cars passing in the street. Why not
SC
give it a try?
stantially more than this, switch off a wide range.
COM
0.1
1k
1M
LED1
K
August 1994 33
Night viewers are not new but those
presented in magazines in the
past have really needed an
infrared source to enable
them to see well in the
dark. With the design
presented here, it is
possible to see just by
the light of stars. In fact,
you can even use the tubes
featured here for astronomy.
By LEO SIMPSON
Lift the veil of darkness with an
Image Intensified
Night Viewer
This project employs a 25mm or
40mm 3-stage fibre optically coupled
image intensifier tube. The resultant
cascaded tube has a typical luminous
gain of over 50,000. If all that seems
a mouthful it is because it embraces
some pretty fancy technology which
is still not available to some countries.
Image intensifier and image converter tubes operate on the same
principle. An image is focused by an
34 Silicon Chip
external lens onto the photocathode
target of the tube and this cathode
emits electrons in response to the
incident photons. The electrons are
then accelerated by a cone-shaped
electrode to strike a luminescent
screen. Because each photon landing
on the photocathode target ultimately
gives rise to many photons from the
luminescent screen, the result is a
gain in luminous intensity.
In the tubes being discussed for this
project, the photo
cathode responds
to the infrared region of the spectrum
while the luminescent screen has
TOP OF PAGE: at night, vegetation
which is in complete darkness can be
seen in intricate detail on the green
screen of the Night Viewer. This
simulated shot does not show the
distortion at the edges of the screen
which is really only apparent as you
pan the Night Viewer across the scene.
This is a 25mm version of the Night Viewer, with all components sprayed black.
Note that the Night Viewer must only be used in the dark.
green phosphor (much like the screen
of an oscilloscope) and so the image is
green. Hence, this sort of tube is also
referred to as an “image converter”.
The photocathode is actually
spherical in section, deposited on the
inside face of the window. Ideally,
the luminescent screen should have
the same radius of curvature as the
photocathode but in practice, a flat
screen is used. This results in image
distortion (stretching) at the edges of
the screen. The cone shaped electrode
is held at the same high voltage as
the screen and the voltage between
the photocathode and the screen is
typically 12kV to 15kV.
Typical single stage image converters give a luminous gain of about
75 and in practice, if they are to be
used for effective night time viewing,
they need an infrared light source to
illuminate the scene. For an image
converter to be really effective, it
needs two or three stages, as depicted
in Fig.1. Here, the screen of the first
converter is used as the image input
to the photocathode of the second
converter and so on. The coupling
between stages is in the form of
plano-concave fibre optic lenses.
The tubes supplied for this project
are used and may have some small
but negligible blemishes. Due to the
complexity of the cascaded tube
construction, small blemishes were
acceptable even in new tubes.
Several different tubes are available
for this project, 25mm and 40mm in
screen diameter. Whichever one is
used, an input lens fits at the front
of the case, arranged so it focuses the
scene onto the cathode of the imaging
tube. Therefore, the lens serves the
same purpose as in a camera and the
type of lens is chosen for the application, just as it would be for a camera.
You can have a wide-angle lens for
close-up work, a telephoto lens for
distance viewing or even a zoom lens.
In order to maximise the light being
transferred from the scene to the tube,
fast (large aperture) lenses should be
used. The prototype unit pictured in
this article employs a 100mm f2 lens.
The prototype unit also employs a
low cost dual lens magnifier. If the
eyepiece is removed, the screen of the
imaging tube can be photographed or
videotaped.
These tubes don’t need much light
to operate. 100 millilux (one tenth of
a lux) is the maximum recommended
exposure. The life of a tube is reduced
with prolonged exposure to this light
level. The tube can produce a useful
output down to 500 microlux (0.0005
lux). Starlight is about 0.001 lux.
In comparison, modern colour TV
cameras need about 2 lux and most
sensitive monochrome TV cameras
need at least 0.1 lux.
SCREENS
PHOTOCATHODE
CONE-SHAPED
ELECTRODE
FIBRE-OPTIC
WINDOWS
Fig.1: a 3-stage image converter tube has each section linked
together by fibre optic couplings to markedly increase the
luminous gain.
August 1994 35
C3-C14 220pF-.001 5kV
D3-D14 BY509
D2
1N4007
C14
T1
R1
150
D14
NE1
R2
22k
S1
Q1
2N2219
C1
100
B1
9V
B
C2
.047
350V
NE2
C
SCR1
C106D A
R3
22k
E
C13
G
D12
C11
D11
D10
C10
D9
C9
+13.5kV
T2
C3
C4
D3
K
R4
22k
D1
1N4148
D13
C12
D4
C5
D5
C6
D6
C7
D7
D8
C8
-13.5kV
PCB
GND
B
E
C
VIEWED FROM
BELOW
PASSIVE NIGHT VIEWER POWER SUPPLY
KAG
Fig.2: the EHT supply for the Night Viewer has three sections: a ringing choke
inverter involving transformer T1, a capacitor discharge converter involving
SCR1 & transformer T2, & the voltage triplers.
Just to give some idea of how sensitive these tubes are, we used the
prototype to look at the night time sky
and found that it really accentuated
the detail in the Milky Way!
65mm plastic tubing is used to
house the 25mm image con
verter
tubes, while 90mm stormwater plastic
tubing is used for the 40mm units.
These plastic tubes, their matching
joiners and end caps, are readily available from plumbing suppliers.
The resultant dimensions of the
fully constructed night viewers are
approximately 70mm outer diameter
and 180mm long for the 25mm version,
and 90mm diameter and 280mm long
for the 40mm version.
Required circuitry
As already noted, an image converter requires a high voltage supply of
about 12-15kV but the current needed
is low, less than 10 microamps. The
circuit for the supply produces an
EHT voltage of around ±13.5kV when
powered from a 9V battery. Current
drain is about 14mA, giving a useful
life of around 20 hours from a standard battery or about 60 hours from an
alkaline battery.
The circuit of Fig.2 has three
sections: the inverter, the converter
and the voltage triplers. The inverter
section is a ringing choke oscillator
consisting of transformer T1, R1, D1
and transistor Q1. Resistor R1 provides
bias current to make the oscillator
start, and also supplies feedback to
maintain oscillation. Diode D1 protects the base-emitter junction of Q1
when the base voltage swings negative. The oscillator operates at around
120Hz, set mainly by the transformer.
C14
C13
C12
D13
C11
D11
C10
D9
+13.5kV
C9
D2
T1
100uF
NE1
T2
22k
NE2
D1
Q2
22k
C3
.047
22k
150
B1
D10
D12
D14
S1
The resulting AC voltage at the primary of T1 is stepped up by the secondary
and is rectified by diode D2.
This diode charges capacitor C2 via
the primary winding of transformer
T2. When the voltage across C2 exceeds the breakdown voltage of the
two series-connected neon lamps, NE1
and NE2, (around 150V) the neons turn
on. This triggers the C106D SCR, and
C2 is quickly discharged through the
SCR via the primary winding of T2.
Once the capacitor is discharged, the
neons go out, the SCR turns off and
the charge cycle starts again.
During the discharge cycle of C2, a
high-voltage pulse with a peak-to-peak
voltage of 4.5kV is produced at the
secondary of trigger transformer T2.
This pulse is applied to two separate
3-stage Cockroft-Walton voltage tripler
circuits. The tripler made up by diodes
D4-D9 and capacitors C4-C9 produces -13.5kV. Another tripler made up
by diodes D10-D15 and capaci
tors
G
A
K
SCR1
D3
C4
D5
D4
C6
C5
D7
D6
C7
D8
-13.5kV
C8
GND
36 Silicon Chip
Fig.3: everything
except the voltage
triplers is mounted
on a small PC board
measuring 50 x 28mm.
The triplers are hardwired & then potted in
neutral-cure silicone
sealant although this
step does not take
place until after the
circuit is tested &
connected to the image
converter tube.
This photo of the Night Viewer shows the wiring inside the plastic case before
the triplers are potted.
C10-C15 produces +13.5kV. Voltage
regulation is achieved by the neons,
as the voltage applied to the primary
of T2 is constant at 150V peak. The
circuit will produce a relatively constant output for a DC input voltage
from 7-12V.
Circuit construction
Everything except the voltage triplers is mounted on a small PC board
measuring 50 x 28mm. The wiring
diagram is shown in Fig.3. This board
is mounted, together with the triplers,
in a standard plastic utility box measuring 130 x 68 x 43mm. The triplers
are hard-wired and then potted in
neutral-cure silicone sealant although
this step does not take place until after
the circuit is tested and connected to
the image converter tube.
Several points must be watched
during assembly of the PC board: (1)
Make sure the metal side of the SCR
faces towards the centre of the board;
(2) Make sure that the polarity of diodes D1 and D2 and capacitor C1 is
correct; and (3) Resistor R1 is installed
“end-on”.
The two triplers are hard-wired as
shown in Fig.3. Their wiring should
be kept as compact as possible. A lead
length of 5mm for all components is
OK. Note that the polarity of the diodes
is different in the two triplers.
With the circuitry complete you can
proceed to a test, before any connec-
tions are made to the image converter
tube. The test can be done before the
tripler sections are potted but note that
only one tripler section can actually
be connected at a time in this no-load
condition. Having a supply produce
±13.5kV is possible in free air but a
total of 30kV is not.
When you switch on the power with
either of the triplers connected, it is
most likely that there will be some
corona discharge around the tripler
diodes. This won’t damage anything
but keep a safe distance from this part
of the circuit. The current drawn from
the battery should be about 14mA. If
a wire connected to the circuit earth
is placed close to the relevant EHT
output lead, you should be able to
obtain sparks up to about 5mm long.
After the battery is disconnected, you
should connect the earth wire directly
to the EHT output in order to discharge
all the capacitors.
Note that when the circuit is working, you will not see the neons light.
This is because of the short duty cycle
– you will only see the neons glow
when you look at them in the dark.
If the circuit does not work try measuring the AC voltage at the base of Q1;
it should be around 0.45V RMS measured with a digital multimeter. The AC
voltage measured at the cathode of D2
is about 45V RMS measured with a
digital multimeter. Don’t try measuring the EHT voltages unless you have
a suitable EHT probe, otherwise you
will damage your meter.
If all is well with the preliminary
tests, you can proceed to finish the
project.
As supplied, the image converter
comes prewired. You will need to
mount the image converter in the
The 3-stage image tube is supplied pre-wired. Note that all of the tube
metalwork is connected to the EHT supply and therefore must be fully isolated
so that no user contact is possible in the finished Night Viewer.
August 1994 37
PARTS LIST
This little jig, made of two pieces of scrap PC board, simplifies the hard-wiring
of the two triplers. The hot melt glue is used to pot the triplers after they are
wired into circuit.
1 prewired 3-stage image
intensifier tube
1 objective lens (see text)
1 eyepiece lens (see text)
1 PC board coded OATLEY JM
2 neon lamps (NE1, NE2)
1 inverter transformer (T1)
1 trigger transformer (T2)
1 9V battery and snap connector
1 miniature SPDT toggle switch
3 22kΩ 0.25W 5% resistors
1 150Ω 0.25W 5% resistor
Semiconductors
1 2N2219 NPN transistor (Q1)
1 C106D SCR (SCR1)
1 1N4148 signal diode (D1)
1 1N4007 1A diode (D2)
12 BY509 or equivalent 8kV
3mA diodes (D3-D14)
Capacitors
1 100µF 25V electrolytic
1 0.47µF 350V polyester
12 220pF to .001µF 5kV ceramic
Miscellaneous
Silicone sealant, epoxy
adhesive, hot melt glue, hookup wire, solder, plastic tubing &
fittings, galvanised steel tubing.
A close-up view of the completed EHT supply, showing how the triplers are
potted with hot melt glue in a compartment at the end of the plastic box.
plastic tube, as shown in Fig.4. This
shows the image converter tube suspended in the plastic tube which is
fitted with a sleeve of galvanised steel,
held in place with the plastic fittings.
These fittings will ultimately be glued
into place using plumbers’ PVC glue
(as used for gluing plastic sewer and
stormwater fittings).
At the ends of the plastic tube,
the image converter tube should be
sealed into place using hot melt glue
or silicone sealant. This will do two
things: support the tube mechanically
Where to buy a kit
This project is available in kit form from Oatley Electronics, PO Box 89, Oatley,
NSW 2223. Phone (02) 579 4985; Fax (02) 570 7910
A kit comprising a 25mm prewired 3-stage image converter tube, plastic pipe
and fittings for the tube case, metal X-ray shield sleeve and the EHT power
supply kit is available for $290 plus $10 for postage and packing. The same kit
for a 40mm image converter is $390 plus $10 for postage and packing. Also
available is a suitable eyepiece lens for $18 and an objective lens for $75. The
plastic box for the power supply is $4. Payment may be made by cheque, postal
money order or credit card.
Oatley Electronics also have cheaper kits with single stage image intensifier
tubes. For further details, contact Oatley Electronics.
Note: copyright of the PC board for this project is owned by Oatley Electronics.
38 Silicon Chip
and prevent any user contact with
exposed metal which is connected to
the outputs of the triplers.
However, before you do any work
with glues or sealants, you must drill
holes in the plastic tubing, the metal
sleeve and the plastic case, to allow
the three wires to pass through and
connect to the outputs of the triplers.
Naturally, these holes must line up
precisely.
After the holes have been drilled,
the plastic box is glued to the plastic
ring at the objective lens end of the
tube housing. You can use plumbers’
PVC glue for this job but the box will
need to be held in place temporarily
with strong adhesive tape. After the
PVC glue has set, some hot melt glue
can be used to fill the join between
the plastic box and the metal sleeve.
That done, connect the triplers and
mount them at one end of the plastic
box and partition it off with a piece of
plastic as shown in one of the photos.
Then fill the tripler compartment with
hot melt glue.
-13.5kV
GND
+13.5kV
2mm FOR
PROTOTYPE
40mm FOR
PROTOTYPE
TUBE
1
TUBE
2
PROTOTYPE EYEPIECE
"PEAK" 10x PLALUPE
No.2032-10
OBJECTIVE LENS
EPOXY
TUBE
3
65mm STORM
WATER PIPE
POLYURETHANE FOAM BLOCKS
65mm STORM WATER
PIPE END CAP
SHORT TUBE CUT
FROM A 66mm STORM
WATER PIE JOINER
EPOXY
65mm STORM WATER
PIPE END CAP
METAL X-RAY SHIELD
Fig.4: the image converter tube is suspended in a plastic tube which is fitted with a sleeve of galvanised steel which
functions as an X-ray shield.
-13.5kV
+13.5kV
GND
TUBE 2
TUBE 3
SCREEN END OF TUBE
ANODE END
OBJECTIVE LENS END OF TUBE
CATHODE END
TUBE 1
Fig.5: this diagram shows how the tube sections are wired to the EHT supply.
Mount the PC board and the battery
in the plastic box – they can each
be secured simply by pressing them
into a small blob of Bostik Blu-Tack
adhesive. Remember to connect the
switch in series with the 150Ω resistor
and the battery snap before mounting
these two components.
Finally, you will need to glue your
objective lens and eyepiece lens to the
PVC end caps and these can be secured
to the completed tube assembly with
small self-tapping screws.
You are now ready to use your
completed Night Viewer. Remember
to avoid the temptation to test or use
the Night Viewer during the day time.
Using it under daylight or in brightly
lit rooms will damage the tube. Keep
a lens cap on the objective lens when
not in use as this will also protect the
lens from damage. The prototype was
sprayed with black paint to finish it
SC
off.
WARNINGS
HIGH VOLTAGE: The EHT power
supply used in the Night Viewer is
not capable of delivering any significant current continuously but it
can provide a nasty electric shock.
Make sure that the capacitors are
discharged before working on the
circuit.
LIGHT EXPOSURE: An imaging
tube can be damaged if it is exposed
to bright light. Do not store or use the
tube in daylight. The tube will not be
damaged if it is exposed to normal
room light during construction, but
with no power applied. For longest
life a completed viewer should be
stored in the dark and used in the
dark. Normal night time street lighting levels and street lights are not
a problem. Using it in daylight can
damage it.
X-RAYS: Low level X-ray radiation is
emitted by most imaging tubes. This
radiation is mainly emitted around
the sides of the tubes and not from
the screen or the cathode of the
tube. The radiation level is reduced
to very low levels by housing the
whole tube assembly in an outer
tube made of galvanised steel –
see Fig.4.
EXPORTING: exporting these tubes
to some countries may be prohibited,
or may require special export permits. Do not export these tubes to
any other country prior to consulting
the appropriate authorities.
August 1994 39
SERVICEMAN’S LOG
Lightning strikes thrice
A popular superstition when I was a youngster
was that various calamities – natural or manmade – always happened in threes. Well, that
was according to the adults who knew all about
these things. I never did believe it but a recent
experience does have me wondering a little.
The story is really about video
recorders; and I use the plural term
deliberately because it involves no
less that four machines, all of the
same brand – but different models
– which turned up on the bench in
quick succession. And three of them
had suffered lightning strikes. See
what I mean!
The first one was a Panasonic NVJ1A, a run-of-the-mill model now
about four years old and no longer in
production. It is owned by one of my
regular customers who, incidentally, is
something of a computer buff, a point
of some interest as it transpired.
He came into the workshop one
morning, pushed the machine across
the counter with the cover removed
and said, “Will you put a fuse in it.
It’s stopped and the fuse is blown”,
pointing to the offending component.
Well, he wasn’t wrong; one glance
at the blackened glass was enough
to confirm that. But it was obvious
from the way he spoke that he firmly
believed that the fuse was the only
thing wrong. And when I gently suggested that this was an effect, rather
than a cause, he was quite reluctant
to accept the idea.
There is only one answer in such
cases. I fished out an appropriate replacement, fitted it and applied power.
Splat! – one fuse destroyed. After
that, he didn’t argue. But it was only
then that he told me about the storm
and the fact that his power main had
apparently been struck.
And so he agreed to leave the machine with me. But I warned him that,
if he was lucky, the damage would be
confined to the power supply. If he
wasn’t, it could be a lot more serious.
I didn’t attack it immediately. There
were other jobs ahead of it, the owner
had indicated that he was not in a
hurry, and I was not at all familiar with
this power supply. I had a manual but
had not had occasion to service this
section before. All I knew was that
it appeared to be fairly conventional
switchmode supply.
Strike two
In any case, before I could get it on
the bench, what should turn up but
another Panasonic recorder; an NVFS90A. This is a very much up-market
Super VHS model, with all the bells
and whistles one can imagine – and a
price tag to match. But for all that, its
power supply is almost identical with
the NV-J1A.
And it had also suffered a lightning
strike; not from the same storm but
40 Silicon Chip
Fig.1: the power supply circuit for the Panasonic NV-FS90A video recorder. The components to be checked out
included the mains fuse (F1101), the bridge rectifier (D1102), the starter circuit across the output of the bridge
rectifier, the auto voltage selector IC (IC1101), and safety resistor R1125.
from one a couple of days later. In this
case, however, there were no obvious
symptoms and the fuse was still intact.
Its owner was anxious to get it fixed
as quickly as possible.
In all these circumstances, I decided
to let the FS90A jump the queue. After
all, I had to familiarise myself with
the power supply on one machine or
the other, so it might as well be on the
more urgent one.
The power supply is a self-contained unit which is housed in a metal
box. It sits in the rear lefthand corner
and is easily removed by undoing a
few screws. The box itself measures
about 150 x 50 x 65mm and the bottom cover can be sprung off quite
easily, although the top can present
problems.
Not all models have the same top.
Some, including these two models,
cover all the box and are quite easy
to remove. In other models, they are
only about 50mm long and are quite
tricky to remove. To make matters
worse, there is nothing in the manual
covering this procedure.
The secret lies under a small plastic
label, marked “AC IN”. This can be
peeled off and it is then possible to
see how the cover and body are slotted
together. In all models, the construction is quite compact and this makes
them a little difficult to work on but
not seriously so.
As I have already noted, the mains
fuse (F1101) was intact and there
were no other visible signs of damage.
Well, it didn’t take long to establish
that bridge rectifier D1102 was open
circuit; a rather strange fault in the circumstances – I would have expected
a short circuit.
Anyway, that’s how it was. And,
since I didn’t carry this item in stock,
it would have to be ordered. But what
else could have been damaged? The
next major component after the bridge
rectifier is a small IC (IC1101), which
is described as an auto voltage selector
– more about this later.
There was no conclusive way to test
this IC without a new rectifier but I
made a few resistance measurements
across the appropriate pins and, judging by the transistor configurations
shown within the IC, I suspected that
it may be faulty also. So that was added
to the order list.
So what about the NV-J1A machine?
Like the NV-FS90A, it would almost
certainly need some replacement
parts. Closer exami
nation revealed
one important difference between the
FS90A and the J1A; the J1A was fitted
with a protective thermistor (D1101)
across the mains, a refinement the
FS90A lacked, in spite of its up-market
price tag. I hoped that this might have
prevented further damage.
And yes, this had broken down
and taken out the fuse. So maybe
that was all that was needed. I had
a replacement on hand, fitted it, and
tried again. No joy; another fuse for
the garbage bin.
I moved on to the bridge rectifier
and confirmed that this was the real
culprit – it had broken down. So another bridge was added to the order.
Next to consider was the auto voltage
selector IC, which was a different type
from that in the FS90A. Because the
J1A had apparently suffered a heavier
wallop than the FS90A, I also ordered
a replacement for this IC, just in case.
So the order was duly despatched
and a couple of days later I had the
spares on the bench. Naturally, I went
straight to the FS90A and fitted the
new rectifier. I made a quick check
but no joy. Well, I’d suspected the auto
voltage IC anyway and it was easy to
fit the new one, so that was the next
step. In fact, when I pulled the old
one out and compared measurements
with the new one, my suspicions were
confirmed.
Unfortunately, when the new one
was fitted there was still no response,
so it was back to basics. Measuring
August 1994 41
So that was something I had learned
– the hard way – and is well worth
jotting down for future reference. It
could save an embarrassing bounce.
Back to the J1A
across the bridge rectifier showed
300V plus, which seemed logical, and
so I moved on to pins 3 and 4 of the
auto voltage selector IC, which should
have had essentially the same voltage
between them. In fact, it was zero.
From there it was no great effort to
find the culprit. R1125, a 2.2Ω safety
resistor in the negative line from the
rectifier, was open circuit. Well, that
was no great problem; 2.2Ω safety
resistors are a readily available component and I always have stock on hand.
A new one was fitted and the
machine came to life. A thor
ough
workout confirmed that all functions
were performing correctly and I gave
the machine the usual clean and lube
routine before ringing the owner with
the good news.
A nasty bounce
He came in the following morning,
which was a Saturday, and collected it.
And I naturally assumed that that was
end of that story. Not so – he was on
the phone first thing Monday morning
with the bad news. The thing was dead
at first switch-on.
It wasn’t a good way to start the
week. All I could do was ask him to
bring it back in and assure him that I
would sort it out.
Back on the bench, it didn’t take
long to find the reason; the 2.2Ω safety
resistor I had fitted had failed. I could
find no obvious reason for this, so I fitted another one, switched on, and the
machine came good. I put it through
several on/off cycles – the previous
failure had obviously occurred at
switch-on – and it came good every
time.
42 Silicon Chip
I left it for a while to attend to other
jobs, then tried again. Bingo! It was
completely dead. And yes, it was the
2.2Ω resistor. But why?
With no obvious clues I realised I
needed help. I could spend a week
trying to puzzle this out and more
than likely be no further advanced
at the end of that time. I rang one of
my contacts at Panasonic and put the
problem to him.
His reaction was immediate. “What
kind of safety resistor are you using?”
I replied that it was a standard 2.2Ω
1W type such as one buys at the (electronic) lolly shop; the kind of thing
everyone uses.
“But not from Panasonic?”
“No – does that matter?”
“You fit a Panasonic type and you
wont have any more trouble.”
Sensing a certain amount of incredulity on my part, he went on to
spell out the difference (more on that
in a moment). In any case, I had little
option; I ordered the type he nominated – several, in fact – and when they
came to hand fitted one to the FS90A.
And that really was the end of it; the
machine has given no further trouble.
The crucial difference
So what is so magical about the
Panasonic component? It is a wire
wound type, as distinct from the more
usual metallised types. And, although
it is rated at only 1W, as are the other
types, it is capable of withstanding a
much heavier switch-on surge. And
this particular power supply does
have a heavy switch-on surge. This, in
turn, is a byproduct of the auto voltage
selector system.
In the meantime, I had gone back
to the J1A. I had already replaced the
thermistor, established that the bridge
rectifier had failed, and suspected that
the auto voltage selector IC might be
faulty. In fact, this latter suspicion
proved to be correct.
So the rectifier and IC were replaced
and, on a hunch, I checked the 2.2Ω
safety resistor. I wasn’t really surprised
to find it had failed and was grateful
that I had the correct replacement type
on hand.
And with all that attended to, the
machine came to life. More importantly, it operated in all modes – an
important point, because lightning
strikes don’t always stop at the power
supply. They can pick on odd components anywhere in the system and create faults which can be very difficult
to track down.
So the owners of both the FS90A
and the J1A were lucky; the damage
in either case could have been much
more serious.
Strike three
Machine number three was an NVFS65A. It had also suffered a lightning strike and, as it transpired, had
suffered more damage that the other
two. And, of course, with the first two
under my belt, I was feeling pretty
cocky about this one, the power supply
being essentially the same.
But pride goes before a fall. I went
through the same routine: the fuse,
the rectifier, the safety resistor and the
IC, all of which needed replacement.
But it still wouldn’t deliver voltage
and I began digging deeper into the
circuit.
I didn’t have much luck initially.
Panasonic suggested some likely
components to be either tested or
replaced, as did a colleague who was
also familiar with these units. But none
of the suggestions helped.
So I was at a temporary dead end.
I say temporary, because I was quite
confident that I could track down the
trouble, given time.
But the owner had other ideas. He
called in to see how things were going
and I told him quite frankly that the
job had proved far more difficult than
thermistor across the mains and the
surge protector at the power point. Yet
it was still damaged.
On the other hand, nothing else
in the house was damaged, nor was
there any indication that any of the
surge protectors had been activated.
And by “activated” I mean destroyed
because, as far as I know, all these
surge protectors are sacrificial devic
es; once activated they have to be
replaced.
Fig.2: the power supply for the
Panasonic NV-J1A video recorder is
basically similar to that in the FS90A
but also features a surge protection
thermistor (D1101).
I had originally anticipated.
“Well,” he said. “What about fitting
a new power supply?”
This was the last thing I would
have suggested. I told him that yes,
I could do that, but it would prove
pretty expensive.
He shrugged his shoulders. “Hang
the expense. If that will solve the
problem, go ahead and fit it”.
So that’s what was done. In fact,
Panasonic didn’t supply a complete
replacement; just a new board to fit
in the metal case. And that put the
machine back in operation.
But while having the machine fixed
was gratifying in one sense, it was
somewhat frustrating in another. I was
still keen to know what the problem
really was and anticipated that I could
probably retain the old board and solve
the puzzle at my leisure.
But that was not to be either. Before
I could even raise the matter the owner
indicated that he wanted to take it and,
since it was his property, there was
nothing I could do about it. So that
one must remain a mystery.
Surge protectors
Still on the subject of lightning
strikes, I mentioned earlier that the
owner of the J1A was a keen computer
buff. The significance of this is that he
had become more than usually aware
of the risk of power line surges, of
whatever origin, to his precious computer equipment.
As a result, he had fitted surge protectors to most of his power outlets,
including the one normally used for
the video recorder. So the recorder
had two levels of protection; its own
Machine number 4
Machine number four was a model
NV-L20 and it came in shortly after
the first three. It was completely dead
also but there was no suggestion of a
lightning strike. On the other hand, the
failure did look as though it might be
linked to a mains shut-down, at least
indirectly.
As the owner explained, the machine had been operating normally
immediately prior to a planned maintenance shut-down by the supply authorities. All householders had been
warned and there was no great hassle
involved.
However, when power was restored
a couple of hours later, the machine
was dead. I didn’t attach much importance to this initially, writing it
off as mere coincidence. And it might
have been too but what I found made
me think.
With the previous jobs still fresh in
my mind I went through the power
supply in short order; the fuse, safety
resistor, and rectifier were all intact,
with the usual 300V plus out of the
rectifier. Nor could I find anything
obviously wrong with the voltage
selector IC.
With all those items cleared, suspicion fell on the starter network.
This consists of four resistors (R1102,
R1103, R1123, and R1124) across
the rectifier output and a 1µF 400V
electrolytic capacitor from the junction of R1103 and R1123. The arrange
ment is broadly similar to many starter
circuits used in TV sets. And a common fault is an open circuit or high
value resistor.
In this case, however, all the resistors checked out OK, leaving the
capacitor as the prime suspect. And so
it proved to be. When I pulled it out
and checked it, I could get no reading
at all on the capacitance meter.
So that was an easy one; a new capacitor and the machine came good.
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August 1994 43
SERVICEMAN’S LOG – CTD
I gave it a routine clean and lube and
returned it to the customer.
But where did the mains shut-down
come into this? I have no doubt that
the capacitor was on its last legs anyway and it is important to appreciate
that power is applied to this part of
the circuit at all times, whether the
machine is being used or not. Only
when power is turned of at the mains
is the voltage across the capacitor
removed.
My theory is that this voltage
contributed to a certain amount of
“forming” of the capacitor – enough
to maintain a small amount of capacitance which was sufficient to allow the
system to start. Removing this voltage
for a couple of hours was the last straw
that sank the camel’s hump. But, of
course, it’s only a theory.
Auto voltage selector
Finally, this might be as good a time
as any to expand on the auto voltage
selector system. It is designed to allow
the machine to work on a very wide
range of voltages, although there is no
mention of this in the manual. The
specifications simply say “230-240V,
AC, 50-60Hz.”
However, a practical test confirmed
that it can be plugged into 110V (which
I have available in the workshop) and
still operate quite normally, without
any adjustments.
There is nothing especially new
about this concept; it has been around
in many TV sets for several years now,
although the particular circuit configuration was new to me. Also, it is not
something we think much about in
this country, being blessed with a 240V
50Hz standard which is used virtually
everywhere throughout the continent.
But from a manufacturing and marketing point of view, the advantages
are obvious. Not only does the one
power supply suit all countries but it
is even useful within some countries.
This would be particularly so in countries like Japan, which has a variety
of power supply systems in different
areas. While the 110V 60Hz system is
On Sale Now At
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Or buy direct from SILICON CHIP
Price: $7.95 (plus $3 for postage if ordering from Silicon Chip). Order
today by phoning (02) 979 5644 & quoting your credit card number; or
fax the details to (02) 979 6503; or send cheque, money order or credit
card details to PO Box 139, Collaroy, NSW 2097.
44 Silicon Chip
the one most commonly used, many
areas use 220V 50Hz.
I also understand that there are some
220V 60Hz and 110V 50Hz systems.
It all adds up to a real nightmare, not
only for manufacturers and distributors but also for consumers who wish
to move from one area to another. And
to further complicate matters, the same
type of power outlets are often used
for both voltage systems. It doesn’t
take much imagination to visualise
SC
the problems this can cause.
SILICON
CHIP
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August 1994 53
A long-wave AM
receiver for aircraft
weather information
This simple receiver uses two ICs & will pick
up airport weather beacons in the LW band.
Use it to receive up-to-the-minute weather
reports. It runs off a 9V battery & is easy to
build.
By DARREN YATES
If you’re interested in aircraft or flying then you’ll no doubt already have
a receiver that taps into the airport
frequencies around the country. You
can always pick up interesting information, particularly during aircraft
emergencies and bushfires. Information on the strength and direction of
54 Silicon Chip
the recent NSW fires was broadcast
by pilots back to ground bases and to
nearby airports on this band.
However, there is another band
which gives up-to-the-minute weather
and visibility information and these
stations can be found on the LW
(long-wave) band and are known as
Weather Beacons. They often contain
Morse code information along with a
recorded message about the current
temperature, visibility and cloud levels and current usage of a particular
airport. The weather beacon at Sydney International Airport even has a
computerised voice broadcasting this
information.
This band is located below the
AM broadcast band and ex
t ends
from around 190kHz up to 450kHz.
This low-cost long-wave receiver is
designed to pick up this band and
the bottom of the AM broadcast band,
enabling it to pick up Sydney’s ABC
Radio National station at 576kHz.
Its frequency coverage extends from
below 200kHz up to 580kHz. It uses
D1
1N4004
Q1
BC548
E
C
10
16VW
100
16VW
1.5k
B
S1
9V
A
LED1
RED
470
IC1
ZN414,YS414
IN
COM
L1
220pF
1
VOLUME
VR2
10k
RF GAIN
VR1
10k
.033
100k
0.1
100k
K
1
63VW
OUT
3
8
IC2a
LM358
100k
Q2
BC337
B
5
1
2
6
IC2b
E
B
Q3
BC327
1k
L1 = 200T, 0.2mm DIA ENCU WIRE
WOUND ON A 10mm DIA FERRITE ROD
85mm LONG
1
WEATHER RADIO
YS414
IN
OUT
ZN414
IN
COM COM
100
16VW
E
7
4
100k
C
10
C
8
0.1
B
OUT E
C
A
K
VIEWED FROM BELOW
Fig.1: the circuit is essentially a TRF (Tuned Radio Frequency) design based
on a ZN414 radio IC. This tunes over the long-wave band & feeds the recovered
audio to VR2. The audio stages comprise IC2a & IC2b which drives a pair of
complementary emitter followers (Q2 & Q3).
just two low-cost ICs and three transistors.
Sensitivity of the receiver is very
good – Sydney’s beacon could be
picked up without an external antenna
from the author’s home in Penrith and
Richmond Air Base was no problem
at all.
Circuit description
Let’s take a look at the circuit of the
Weather Radio, as shown in Fig.1. As
you can see, it’s quite straightforward,
using a ZN414 TRF receiver in the
front end and an audio amplifier to
drive the loudspeaker (TRF stands for
Tuned Radio Frequency).
Looking at the circuit, the ferrite rod
antenna L1 and variable capacitor gang
VC1 form a parallel resonant circuit
which tunes the frequency of interest.
The tuned frequency is fed to IC1, the
ZN414 . This IC contains more than a
dozen transistors which amplify and
detect the RF and then amplify the
recovered audio.
The output appears across, and is
filtered by, a .033µF capacitor. The
10kΩ pot VR1 applies DC via a 100kΩ
resistor to the tuned circuit which enables the IC to vary the RF gain.
IC1 only requires about 1.3V at very
low current to work, so the 470Ω resistor provides the load for the circuit
as well as supplying the power to it.
Q1 and LED 1 form a simple voltage
regulator which provides a constant
1.3V output across the 10µF capacitor
to power IC1 (via the OUT pin).
From the 470Ω resistor, the output
signal is AC-coupled to the 10kΩ volume potentiometer, VR2, and then to
the audio amplifier. This consists of
an LM358 (or TL072) dual op amp and
two complementary transistors. The
first op amp (IC2a) is connected as an
non-inverting amplifier with a gain
of 101, as set by the 100kΩ feedback
resistor from pin 1 to pin 2. Pin 1 of
IC2a then drives IC2b. This op amp
drives complementary transistors Q2
and Q3 directly and they operate in
class B mode, without any quiescent
current to minimise crossover distortion. However, the resulting harmonic
distortion is low since the transistors
are included in the feedback network
PARTS LIST
1 PC board, code 06107941,
102 x 44mm
1 57mm 8Ω loudspeaker
2 10kΩ log potentiometers
(VR1,VR2)
1 60-160pF tuning gang (VC1)
1 85mm length of ferrite rod
6 metres of 0.2mm enamelled
copper wire
3 knobs
4 100mm plastic cable ties
1 plastic utility case, 158 x 99 x
53mm
1 front panel artwork
1 miniature SPDT switch (S1)
1 9V battery snap connector
1 9V alkaline battery
Semiconductors
1 ZN414 TRF radio (IC1)
1 LM358, TL072 op amp (IC2)
1 BC548 NPN transistor (Q1)
1 BC337 NPN transistor (Q2)
1 BC327 PNP transistor (Q3)
1 5mm red light emitting diode
(LED1)
1 1N4004 rectifier diode (D1)
Capacitors
2 100µF 16VW electrolytic
1 10µF 16VW electrolytic
3 1µF 63VW electrolytic
2 0.1µF 63VW MKT polyester
1 .033µF 63VW MKT polyester
Resistors (1%, 0.25W)
4 100kΩ
1 470Ω
1 1.5kΩ
1 10Ω
1 1kΩ
Miscellaneous
Screws, nuts, washers, solder.
August 1994 55
10uF
.033
IC1
100uF
Q2
1uF
VC1
4
5
6
7
8
9
1uF
1
100k
7
D1
IC2
LM358
8
100uF
VOLUME
VR2
9
3
Q3
100k
1k
0.1
4
10
1.5k
100k
1
2
100k
470
Q1
RF
LEVEL
VR1
5
0.1
6
1uF
1
2
3
BATTERY
NEGATIVE
LED1
SPEAKER
BATTERY
POSITIVE
L1
Fig.2: install the parts on the PC board as shown here & take care with IC1 as
it looks identical to a TO-92 transistor. VC1 has its two sections connected in
parallel to give a range of 0-220pF, while the leads to the ferrite rod antenna
must be kept well away from the loudspeaker & the rest of the circuit.
of the op amp and since the overall
gain of this stage is a minimum; ie,
100% negative feedback and therefore,
unity gain.
To maintain high frequency stability in the complementary emitter
follower output stage (comprising
transistors Q2 & Q3), a Zobel network
con
sisting of a 10Ω resistor and a
0.1µF capacitor is connected across
the loudspeaker.
Power is supplied from a 9V battery with diode D1 providing reverse
polarity protection. Note that since
IC1 requires only a low voltage and
because the supply voltage to the
audio amplifier is not critical, you
could easily run the circuit from a 6V
supply. However, to do this you would
need more space to fit the batteries
into the case.
Construction
Most of the components for the
Weather Radio are installed on a PC
board coded 06107941 and measuring
102 x 44mm. This is then mounted
inside a standard plastic case measuring 158 x 99 x 53mm. The PC board
is mounted on one side of the case
(behind the front panel), as shown in
the photographs.
Before you begin any soldering,
check the board thoroughly for any
shorts or breaks in the copper tracks.
These should be repaired with a small
artwork knife or a touch of the soldering iron where appropriate.
When you’re happy that everything
appears OK, you can solder in the
resistors and diodes, followed by
the capacitors. This done, install the
transistors and IC1 and IC2. Note that
IC1 has three leads and looks identical to the transistors, so check this
component carefully when installing
it on the board.
Tuning gang
Fig.3: this is the full-size etching pattern for the PC board.
56 Silicon Chip
The tuning gang is a plastic dielectric type with two sections of 0-60pF
and 0-160pF. These two sections are
connected in parallel on the PC board
to produce a variable capacitor of
0-220pF, as shown on the circuit of
Fig.1.
The capacitor is secured to the PC
board with two 2.5mm screws and
then its three tags are soldered to
short lengths of tinned copper wire
The ferrite rod antenna is attached to the rear of the case using plastic cable
ties. Additional cable ties should be used to lace the wiring to the pots, switch,
loudspeaker & LED to maintain a tidy appearance & to prevent tuning drift.
which are passed through the associated holes in the board and soldered
in place.
Drilling the case
Before you go much further, you will
need to do some work on the plastic
case. The board is mounted on one
side of the case, as mentioned above,
along with the RF Gain and Volume
control potentiometers (VR1 & VR2).
The loudspeaker is mounted in the
bottom of the case and when the lid is
attached, the whole assembly is turned
upside down so that the loudspeaker
faces up.
You will need to drill holes for the
loudspeaker grille, the PC mounting
pillars, the knob shafts, power switch
and the LED. The latter two items are
mounted on one end. Perhaps the easiest approach to drilling the case is to
use the front panel artwork (included
with this article) as a template. You
will need to drill a circular pattern
of holes for the loudspeaker and four
holes to mount the ferrite rod antenna
which we will now discuss.
The tuning coil L1 is wound as a
single layer of 200 turns of 0.2mm
enamelled copper wire on an 85mm
length of ferrite rod 10mm in diameter.
If you need to cut the rod to this length,
the way to do it is as follows. File a
nick around the rod at the point you
wish to cut it and then snap it off. If
you try cutting it in any other way it
is sure to shatter.
Start off by winding one turn
around the rod about 13mm from one
end and anchor it with some sticky
tape. This done, continue by winding
on the 200 turns. It doesn’t need to be
exactly 200 turns so if you’re out by a
few turns either way, it won’t matter
too much.
RESISTOR COLOUR CODES
❏
No.
❏ 4
❏ 1
❏ 1
❏ 1
❏ 1
58 Silicon Chip
Value
100kΩ
1.5kΩ
1kΩ
470Ω
10Ω
4-Band Code (1%)
brown black yellow brown
brown green red brown
brown black red brown
yellow violet brown brown
brown black black brown
5-Band Code (1%)
brown black black orange brown
brown green black brown brown
brown black black brown brown
yellow violet black black brown
brown black black gold brown
This close-up view shows the PC board after all the parts have been installed
& the wiring completed. Note that shielded audio cable must be used for all
connections between the pots (VR1 & VR2) & the PC board. The loudspeaker
can be secured inside the case using super-glue.
Make sure that the turns are tight
and close to each other. Once you’ve
wound the turns, anchor the other
end with some more sticky tape
and then carefully cover the whole
winding with tape. This done, strip
the enamel from both ends of the
coil and tin them with solder. The
rod is attached to the side of the case
opposite the PC board, as shown in
the photos, and is secured using two
plastic cable ties.
Before the PC board can be mounted
in the case, you will need to fit a suitable shaft to the tuning gang, to enable
a knob to be fitted. We did this using
a fairly crude but effective method –
super-glue.
First, we roughened the end of the
tuning gang shaft with a file and did
the same to a 15mm long tapped metal
spacer. A dab of super-glue was then
applied to the tuning shaft and the two
Fig.4: this fullsize front-panel
artwork can be
used as a drilling
template for the
various controls
& the indicator
LED.
were butted together and then put to
one side to allow the glue to dry. This
method works surprisingly well.
Mount the PC board using metal
pillars, screws, nuts and lockwashers. Finally, wire in the two pots and
the speaker and then fit knobs to the
shafts of the pots and the tuning gang.
The LED and speaker can be mounted
(permanently) with super-glue, while
the battery can be held in place using
double-sided sticky tape. Alternatively, you can make up a metal bracket to
hold the battery in position.
Testing
Before testing the receiver, check
your work thoroughly for any possible
errors. Once everything is correct, connect your multimeter across the On/
Off switch. This places the multimeter
in series with the supply to allow you
to measure the current drain. Select
a low current range (200mA) on the
multimeter, then connect the battery
and check the current reading.
Depending on where the tuning
gang is sitting, and with the volume
control well down, you should hear
some low-level static coming through
the speaker.
The current consumption should be
about 10mA. Any more than 20mA and
you should switch off imme
diately
and check for errors.
Now advance the volume control
to about half way and then advance
the RF gain control as well. The static
should rise markedly and the loudspeaker may even squeal, depending
on the setting of the tuning gang.
If everything is OK, you should be
able to tune across the long-wave band
and pick up one or two low frequency
AM broadcast stations as well. The
weather beacons will be below these.
Adjust the RF gain control to increase
the signal level until the circuit starts
to oscillate (squeal) and then wind it
back a little. Next increase the volume
until it is at a comfortable level. SC
RF gain
190
580
Weather Radio
Volume
Tuning Frequency (kHz)
August 1994 59
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Please feel free to visit the advertiser’s website:
www.altronics.com.au
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Please feel free to visit the advertiser’s website:
www.altronics.com.au
SILICON
CHIP
If you are seeing a blank page here, it is
more than likely that it contained advertising
which is now out of date and the advertiser
has requested that the page be removed to
prevent misunderstandings.
Please feel free to visit the advertiser’s website:
www.altronics.com.au
AMATEUR RADIO
BY GARRY CRATT, VK2YBX
Using 2-line Keplerian elements
to track amateur satellites
Several low-cost computer programs are now
available to accurately keep track of satellites.
This article explains the origin of this data &
shows how easy it is to put it to use.
Considering the increasing interest
in satellite reception by amateurs, it
is not surprising that the demand for
2-line orbital elements to predict the
location of a satellite at any particular
time is also increasing. In addition, the
prolifera
tion of personal computers
makes the calculation and display of
satellite data in real time a relatively
simple matter.
Fortunately, Keplerian data is freely available to ama
teurs, primarily
through computer bulletin boards.
However, in order to properly understand Keplerian elements, some history is in order. Orbital mechanics, as
applied to artificial earth satellites, is
based largely on celestial mechanics,
initially founded on the work of James
Kepler and Issac Newton and expanded on by mathematicians during the
18th and 19th centuries. Eventually,
the theory became so accurate that
when astronomers observed discrepancies between their observations
and the theoretical results, they were
able to determine that the errors were
caused by variations in their astronomical timescales.
In 1956, astronomers changed the
time scale from one based on the rotation of the Earth (universal time) to a
new scale based on the orbital motion
of the Earth around the Sun (ephemeras time). With the advent of atomic
timekeeping, astronomical timescales
Fig.1: this “screen-grab” shows the menu page for the STSORBIT PLUS satellite
tracking program.
were eliminated completely and the
ability to predict orbital locations
became supremely accurate.
Computer programs
One of the spin-off products of
the US space effort was the creation
of the computer program known as
“STSORBIT PLUS”, designed and used
by NASA to track satellites, including
the Space Shuttle. There is now a
public domain version of this program
available on many computer bulletin
board services. In addition, AMSAT
offer their own program, “INSTANT
TRACK”.
By “plugging in” the latest data sets
or Keplerian elements, it is possible to
very accurately predict the location of
a satellite at any particular time. This
is very useful for tracking amateur
satellites in polar orbits and satellites
used for rebroadcasting television
programs that are not located in geostationary orbit.
In theory, the centrifugal force resulting from the speed of a satellite is
balanced against the gravitational pull
of the Earth and this keeps a satellite
orbit constant. In practice, however,
gravitational forces from the Sun and
the Moon, plus atmospheric drag
(applicable to satellites at an altitude
of 1000km or less), have the effect of
degrading the orbit. For this reason, it
is important to use current elements.
Moreover, some satellites are deliberately launched into low Earth
or polar orbits, in order to provide
coverage over all major land masses.
These satellites might orbit the Earth
once every 90 minutes or so, so a computer “prediction” for future passes is
of paramount importance to amateur
operators.
Table 1 shows the primary orbital
August 1994 63
Table 1: Keplerian Elements
Data for each satellite consists of 3 lines in the following format:
Name
1 NNNNNU NNNNNAAA NNNNN.NNNNNNNN + .NNNNNNNN +NNNNN-N N NNNNN
2 NNNNN NNN.NNNN NNN.NNNN NNNNNNN NNN.NNNN NNN.NNNN NN.NNNNNNNNNNNNNN
COLUMN
DESCRIPTION
LINE 1
1
Line number of element data
2
Blank
3-7
Satellite number
8
Not used
9
Blank
10-11
International designator (last 2 digits of launch year)
12-14
International designator (launch number of the year)
15-17
International designator (piece of launch)
18
Blank
19-20
Epoch year (last 2 digits of year)
21-32
Epoch day (Julian day & fractional portion of the day)
33
Blank
34-43
1st time derivative of mean motion (0.1 revs per day)
44
Blank
45-52
2nd time derivative of mean motion (0.01 x revs per day)
53
Blank
54-61
Radiation pressure co-efficient
62
Blank
63
Ephemeras type (specified ephemeras theory used)
64
Blank
65-68
Element number
69
Checksum
LINE 2
1
Line number of element data (ie 2 for line 2)
2
Blank
3-7
Satellite number
8
Blank
9-16
Inclination in degrees
17
Blank
18-25
Right ascensions of the ascending node in degrees
26
Blank
27-33
Eccentricity in tenths of units
34
Blank
35-42
Argument of perigee in degrees
43
Blank
44-51
Mean anomaly in degrees
52
Blank
53-63
Mean motion in revolutions per day
54-68
Revolution number at epoch
69
Checksum
64 Silicon Chip
parameters used in satellite data elements, while Table 2 shows actual
2-line data elements for a few popular
satellites.
In order to make use of these
Keplerian element sets, which can
be downloaded from their international source on a weekly basis, it
is first advisable to obtain a copy of
a suitable tracking program such as
“ TRAKSAT ”, “ INSTANT TRACK ”,
“STSORBIT PLUS” or “PC-TRACK”.
As elements are distributed, they are
allocated a incremental number such
as TLE428 (the last three numbers signify the set). Of course, downloading
Keplerian elements from computer
bulletin boards does require some
level of computer literacy; ie the
ability to create directories, download data, etc.
Running STSORBIT PLUS
STSORBIT PLUS has the ability to
track multiple satellites in real time.
Fig.1 shows the menu page for STSORBIT PLUS.
At initial installation, create a directory called “STS”. After installation, the program will issue a prompt
for local UTC time offset (eg, Sydney
has +10 hours difference). After
completing this, the main menu of
STSORBIT PLUS will present a variety
of options.
The first and most important step is
to set the Earth station location. F10
from the main menu gives a sub-menu
where F2 allows the user to set new
local co-ordinates. The user can then
insert a capital city location, which
gives the program a base for position
calculations. To do this, the program
searches its internal database of over
1500 locations for a match.
F6 selects the map type used to
view the world and satellite orbits.
Toggling the F6 key allows selection
of either World, Ortho, Quad or Zoom.
For slow PCs, the World map is the
best selection as the program draws a
very impressive and complex map of
the world, complete with city names
and rivers.
After this initial setup, current
Keplerian elements must be down
loaded from an accurate source.
These should be downloaded into
the same directory as STSORBIT
PLUS. To import the 2-line elements
in order to track a satellite, select
F2 from the main menu, then enter
the 2-line element filename and the
satellite name. The program will then
display relevant data on the selected
satellite. By now simply keying ENTER, the program will draw a map
of the world and display the orbital
position of the selected satellite in
real time; eg, the track taken by polar
orbiting satellites can easily be seen.
By selecting F3 from the main menu,
a “pass prediction” will be displayed
for the selected location.
Where to buy software
Other features of this and similar
programs are beyond the scope of this
article. For those interested in obtaining registered copies of the software
mentioned in this article, the following
will be of interest:
• TRAKSAT is available from the
author: Paul E. Traufler, 111 Emerald
Drive, Harvest, AL 35749, USA. A
non-registered version costs $US10,
while a laser-printed operations man
ual will cost an additional $US15. A
registered version costs $US25 (add
$US5.00 for shipping and handling
to Australia). Commercial licenses are
also available from $US50.
• PC TRACK version 3.0 can be obtained from: Thomas C. Johnson, 9920
S Palmer Road, New Carlisle, Ohio
45344, USA. It costs $US45 + US15
for shipping and handling.
• STSORBIT PLUS is available from
the Satcom BBS (phone 02 905 0849)
or from the author: David H. Ransom
Jr, 7130 Avenida Altisima, Rancho
Palos Verde, CA 90274, USA (check
costs with author before ordering).
An additional map database is also
available from the author for $US10.
SC
Allow 3-6 weeks for delivery.
Table 2: Sample 2-Line Elements
Optus B1
1 22087U 92054A 94191.61718487 -.00000112 00000-0 10000-3 0 4146
2 22087 0.0916 108.4637 0002995 329.9719 232.0275 1.00270935 18457
Intelsat 5 F-8
1 14786U 84023A 94190.52379876 .00000053 00000-0 00000+0 0 6425
2 14786 2.7646 69.4432 0046903 321.8887 264.9499 1.00275209 1695
Oscar 10
1 14129U 83058B 94176.41110075 -.00000306 00000-0 10000-3 0 2893
2 14129 27.0856 321.0039 6024383 189.2195 150.8337 2.05882336 54986
UoSat 2
1 14781U 84021B 94190.56754595 .00000133 00000-0 30431-4 0 7063
2 14781 97.7855 204.2441 0011153 193.8486 166.2415 14.69228336553597
Noaa 10
1 16969U 86073A 94193.01550214 .00000098 00000-0 60319-4 0 7694
2 16969 98.5052 201.2581 0012183 257.8226 102.1588 14.24897002406033
RS-10/11
1 18129U 87054A 94191.83829016 .00000023 00000-0 90572-5 0 9258
2 18129 82.9253 311.3579 0011286 326.8723 33.1722 13.72339043353150
Satellite
b
p
y
v
Apogee
a
F2
ra
ea
F1
Perigee
x
rp
Fig.2: this diagram shows the major orbital parameters of a satellite: a =
semimajor axis; b = semiminor axis; ra = apogee radius; rp = perigee radius; F1 =
focal point 1; F2 = focal point 2.
Fig.3: STSORBIT PLUS can display data in several map
formats, including World map as shown at left & Ortho
map as shown at right. Note that the displays are in
colour & are not shown to best advantage here.
August 1994 65
Dual diversity tuner for
FM microphones; Pt.2
Construction & alignment of the Dual Diversity
Tuner does not require any special equipment
or tools apart from an alignment tool & a tuning
wand which can be easily made. There is little
wiring involved since most of the parts are
assembled onto PC boards.
By JOHN CLARKE
The prototype for the SILICON CHIP
Dual Diversity Tuner was built into a
1-unit high black anodised rack case
with screen printed front and rear
panels. Two PC boards are used to
accommodate the components: (1) a
main board coded 06307941 and meas
uring 207 x 161mm; and (2) a satellite
board coded 06307942 and measuring
28 x 49mm. The latter carries the
RF preamplifier components and is
shielded by a boxed section made from
15mm-high single-sided PC board. A
further strip of single-sided PC board
divides this box into two sections, to
provide additional shielding for the
RF preamplifier components.
Following assembly, the shielded
RF preamplifier module is mounted
66 Silicon Chip
directly on the main PC board.
Begin construction by comparing
your PC boards against the published
patterns to verify that all tracks are
intact and that there are no shorts
between tracks. Some holes may need
to be enlarged to accept the relevant
components; eg, the mounting holes
for L10, T1, T2, VC2 and for the PC
stakes. The hole used to secure the tab
of REG1 to the PC board may also need
to be enlarged to accept the mounting
screw.
Note that there are only four holes
in the RF preamplifier board. These
allow short lengths of tinned copper
wire to pass through from the track
(top) side of the board and through
the main board for both mounting and
earthing purposes. Unlike the main
PC board, all components in the RF
preamplifier are mounted on the track
side of the board.
Main board assembly
Fig.7 shows the overlay diagram for
the main PC board. Begin construction
by inserting PC stakes at all external
wiring points and at test points TP1 &
TP GND. This done, install all the low
profile components such as the links,
resistors and ICs. Table 2 shows the
resistor colour code but it’s also a good
idea to check them on your multimeter
as some of the colours can be difficult
to decipher.
Take care to ensure that the ICs are
all oriented correctly and that each is
mounted in the correct location. The
5W resistor is mounted about 1mm
proud of the PC board to allow the
air to circulate beneath it for cooling.
Mount the diodes next but again
be sure to use the correct type at each
location. Diodes D1-D4 are marked
with the BA482 type number and are
smaller than the 1N4148 diodes used
for D6-D8. D5, the BB119 varicap,
looks very similar to a 1N4148, so be
sure to check its type number carefully
6
1
5
4
2
BASE DIAGRAM
TOP VIEW
L1-L4
6T, 0.5mm DIA ENCU WIRE ON
PHILIPS 4313 020 40031 BALUN COR
3
5
before installing it on the board. Take
care with the orientation of each diode
and note particularly that D2 and D3
face in opposite directions.
The capacitors can now be installed. There are several different
types used on the PC board, so make
sure that you always use the correct
type at each location. Ceramic capacitors are mostly used in the FM
tuner section of the board, while
MKT and electrolytic capacitors are
used throughout the remainder of the
circuit. Table 1 lists the relevant capacitor codes and their corresponding
values. Make sure that the electrolytics are correctly oriented.
Note particularly that the 10µF
electrolytic and 0.1µF MKT capacitors near IC3 are installed with their
bodies flat against the PC board. You
will need to bend their leads through
90° to do this, however. The capacitors are mounted in this way so that
the leads to LEDs 1-3 in the bargraph
display can pass over the top of them
– see photo.
Similarly, the 4700µF capacitor near
REG1 is also installed lying down –see
Fig.6. Its body should be secured to
the PC board using silicone rubber
compound to prevent possible lead
damage due to vibration.
The 3-terminal regulator (REG1) is
mounted on a small heatsink. Smear
the mating surfaces with heatsink
compound before bolting the assembly
to PC board.
Coils
Fig.6 shows the coil winding details.
L1-L4 are wound onto a balun former
4
2
3
6
1
2
3
L10
F1,
S1
WINDING: PINS 6 AND 1,
S2
10.5T, 0.5mm DIA ENCU WIRE
T2
WINDINGS: PINS 1, 2 AND 3,
3T, BIFILAR 0.25mm DIA ENCU WIRE
PINS 5 AND 4, 4T, 0.5mm DIA
ENCU WIRE
COILS T1, T2 AND L10 WOUND ON NEOSID TYPE 'A' COIL ASSEMBLY
99-007-96 (BASE, FORMER, CAN AND F29 SLUG)
4
5
6
T1
WINDINGS: PINS 4 AND 6,
3.5T, 0.5mm DIA ENCU WIRE
PINS 3 AND 2, 2T, 0.5mm
ENCU WIRE
NOTE: WIND COILS IN SAME
SENSE AS ABOVE
L5
1.5T
L6
6.5T
1
F2
L7
8.5T
L5-L9 WOUND ON 4mm DIA MANDREL
USING 0.6mm DIA ENCU WIRE
L8
1.5T
L9
6.5T
Fig.6: this diagram shows the winding details for all the coils in the Diversity
Tuner. Be sure to use the wire diameter specified for each coil & make sure
that each winding is wound in the direction shown. A complete description on
winding each coil also appears in the text & this should be closely followed.
(six turns of 0.5mm-dia. ECW), while
L5-L9 are air cored and are made by
winding the appropriate number of
turns of 0.6mm ECW onto a 4mm
(5/32-inch) mandril. You can use a
drill bit for this.
Note that L5, L6 and L7 are wound
in a clockwise direction, while L8 and
L9 are wound anticlockwise. Wind
each turn close to the previous turn
as shown in the diagram.
T1, T2 and L10 are wound on the
Neosid coil formers. Begin by inserting
the coil formers into the bases, then
wind T1 using 0.5mm ECW exactly
as shown. Note that the two windings
are wound in opposite directions and
should be immediately adjacent to
each other. Make sure that you get the
winding phases (directions) correct,
otherwise the local oscillator won’t
work.
Note that the enamelled copper wire
is easily terminated on the base pins by
August 1994 67
S2
.01
D7
10k
.01
1
.01
47
0.1
0.1 0.1
.033
K
1.5k
220k
IC3
LM3914
GND
10uF
1
A
10k
10k
220k
10k
LED1 LED2 LED3 LED4 LED5 LED6 LED7 LED8 LED9 LED10
0.1
2.7k
1.2M
10k
10k
TP
GND
VR3
1
0.1
3.9K
10uF
2.7k
1
330k
IC5
LM393
0.1
VR2
82
5W
10k
2.7k
TP1
VR1
1uF
IC4
LM358
10
300
4.7k
56k
4.7k
1.5k
0.1
47k
220k
.001
0.33
27k
1
1
IC2
TDA1576
750
10k
D8
0.1
0.1
0.1
33pF
.0068
100k
33k
22k
IC6
LF353
100k
560pF
39k
IC11
4017
X1
X2
33pF
L10
100k
SHIELD
47k
10
47uF
1
T2
T1
D5
REG1
7812
0.1
3.3k
33pF
10
0.1
.01
15pF
10
390pF
1
.01
390pF
1.8pF
33pF
6.8pF
L9
IC1
TDA1574
220k
.01
10
.01
220k
VC2 6.8pF
L8
47uF
IC8
74C14
.001
33pF
10uF
.01
10
3.9pF
.01
1
.01
.001
SHIELD
L6
10
SHIELD
VC1
IC12
7555
L5
27pF
.001
4700
0.1
Q1
.001
1
.01
220k
390
L7
2.2k
22k
.01
IC7
4066
.001
SHIELD
D9-D12
.018
IC9
7555
.01
2.2k
12.6VAC
0.1
D4
.01
D6
L4
D1
SHIELD
10k
ANT B
L3
.01
L1
D3
10k
.01
L2
2.2k
.01
.01
IC10
4013
D2
.01
2.2k
ANT A
10
GND
10
GND
O/P
10uF
1
47pF
VR4
A K
A K
LED11
RED
LED12
GREEN
1
Fig.7: install the parts on the main PC board as shown in this wiring diagram.
The RF preamplifier board (top, left) is also mounted on the main board
& is enclosed in a shield made from single-sided blank PCB material (see
Fig.9). Note that the parts in the RF preamplifier are installed on the copper
side of the board, with connections to the main board made via feedthrough
capacitors & wire links.
68 Silicon Chip
Keep all component leads as short as possible when assembling the PC board,
particularly around the FM tuner stages at the top of the PC board. The 4700µF
electrolytic capacitor at bottom right should be secured to the board using
silicone rubber compound to prevent its leads from breaking.
heating the wire with your soldering
iron until the enamel melts and then
applying solder.
T2 must be wound with extreme
care. To wind this coil, first take the
250mm-length of 0.25mm ECW, cut it
in half and twist the two wires together
using a hand drill and a vyce until
there is about one twist per millimetre.
This done, solder one wire end (S1) to
pin 3 of the base and the adjacent end
(S2) to pin 2. Wind on three turns as
shown, then use your multimeter to
identify the other end of the wire connected to pin 3. Solder this end (F1) to
pin 2 and connect the remaining end
(F2) to pin 1.
The other winding between pins 4
& 5 uses four turns of 0.5mm ECW. It
must be wound in the opposite direction to the bifilar winding.
Note that Fig.6 shows a gap between
each turn for the bifilar winding but
this has only been done for the sake
of clarity. In practice, the turns should
all be close-wound (ie, immediately
adjacent to each other), while the top
winding should be immediately adjacent to the bifilar winding.
Coil L10 (the quadrature coil) consists of just a single winding. Wind it
in the direction shown and terminate
the top and bottom leads to pins 1 &
6 respectively.
Once wound, the coils can all be
installed on the PC board. Mount L8
& L9 so that they sit about 1mm above
the board surface.
T1, T2 and L10 can only be installed one way on the PC board since
their middle pins are offset, but make
sure that you don’t get them mixed
up. A metal can is then fitted over
each coil and is secured by soldering
its lugs to the earth pattern of the
board. Finally, the ferrite slugs can
be screwed into the formers using a
plastic alignment tool (available from
TABLE 1: CAPACITOR CODES
Value
0.33µF
0.1µF
.033µF
.018µF
.01µF
.0068µF
.001µF
560pF
390pF
47pF
33pF
27pF
15pF
6.8pF
3.9pF
1.8pF
IEC
330n
100n
33n
18n
10n
6n8
1n0
560p (n56)
390p (n39)
47p
33p
27p
15p
6p8
3p9
1p8
EIA
334
104
333
183
103
682
102
561
391
47
33
27
15
6.8
3.9
1.8
your electronic parts retailer). Do not
use a screwdriver for this job since
this will crack the ferrite.
August 1994 69
S1
NEUTRAL
(BLUE)
CORD GRIP
GROMMET
FRONT PANEL
SECONDARY
LED12
K
ANTENNA
'A'
PAL
SOCKET
LEDS1-10
50 COAX
A
ANTENNA
'B'
PAL
SOCKET
LED11
AUDIO
OUTPUT
RCA
SOCKET
12.6VAC
C
NO
S2
NC
REAR PANEL
VR4
COVER WIRING OF S1 AND F1
WITH INSULATING SLEEVING
BROWN
BLUE
POWER
TRANSFORMER
EARTH
LUG
EARTH
(GREEN/
YELLOW)
ACTIVE
(BROWN)
ACTIVE
(BROWN)
250mA
FUSE
PRIMARY
Fig.8: use 240VAC-rated cable for all mains wiring & insulate all exposed terminals on the fuseholder
& switch S1 using heatshrink tubing (see text) to prevent any possibility of accidental shock. The mains
cord earth lead (green/yellow) must be soldered to an earth lug which is securely bolted to chassis.
70 Silicon Chip
The LED bargraph display and LEDs
11-12 can be installed now. The 3mm
LEDs used for LED 11 and LED 12 are
installed with their leads untrimmed,
so that the LEDs can later be bent over
and pushed through matching holes in
the front panel. Watch the polarity of
the LEDs – the anode lead is the longer
of the two.
The bargraph (LEDs 1-10) must be
mounted so that the front of the display
is 14mm from the edge of board. This
is done to ensure that it will later sit
flush with the front panel – see Fig.8.
To achieve this, it will be necessary to
extend each lead using a short length
(about 25mm) of tinned copper wire.
Bend the leads at right angles about
6mm above the board before soldering
the bargraph in position.
As before, take care with the polarity of this device. As with individual
LEDs, the anode lead of each LED in
the bargraph is the longer of the two
and it is a good idea to mark the anode
end of the device before extending the
lead lengths.
RF preamplifier
The RF preamplifier board can be
assembled now – see Fig.7. Before
This photo shows the method used to mount the bargraph LEDs (LEDs1-10). The
lead lengths must all be extended using short lengths of tinned copper wire &
the leads must all be bent through 90° after soldering so that the bargraph mates
with its front panel cutout.
mounting any of the parts, it must be
mounted copper side up on the main
PC board and secured by passing short
wire links through the four mounting
points (indicated by solid dots on
Fig.6). Solder these links at each end
to the surrounding copper pattern to
secure the two boards together.
This done, the parts can be mounted
onto the preamplifier board by soldering their leads directly to the undrilled
copper lands (ie, the parts are mounted
on the copper side of the board). Keep
all leads as short as possible and take
TABLE 2: RESISTOR COLOUR CODES
❏
No.
❏ 1
❏ 1
❏ 6
❏ 3
❏ 1
❏ 2
❏ 1
❏ 1
❏ 1
❏ 2
❏
10
❏ 2
❏ 1
❏ 1
❏ 3
❏ 4
❏ 2
❏ 1
❏ 1
❏ 1
❏ 1
❏ 9
Value
1.2MΩ
330kΩ
220kΩ
100kΩ
56kΩ
47kΩ
39kΩ
33kΩ
27kΩ
22kΩ
10kΩ
4.7kΩ
3.9kΩ
3.3kΩ
2.7kΩ
2.2kΩ
1.5kΩ
750Ω
390Ω
300Ω
47Ω
10Ω
4-Band Code (1%)
brown red green brown
orange orange yellow brown
red red yellow brown
brown black yellow brown
green blue orange brown
yellow violet orange brown
orange white orange brown
orange orange orange brown
red violet orange brown
red red orange brown
brown black orange brown
yellow violet red brown
orange white red brown
orange orange red brown
red violet red brown
red red red brown
brown green red brown
violet green brown brown
orange white brown brown
orange black brown brown
yellow violet black brown
brown black black brown
5-Band Code (1%)
brown red black yellow brown
orange orange black orange brown
red red black orange brown
brown black black orange brown
green blue black red brown
yellow violet black red brown
orange white black red brown
orange orange black red brown
red violet black red brown
red red black red brown
brown black black red brown
yellow violet black brown brown
orange white black brown brown
orange orange black brown brown
red violet black brown brown
red red black brown brown
brown green black brown brown
violet green black black brown
orange white black black brown
orange black black black brown
yellow violet black gold brown
brown black black gold brown
August 1994 71
iron for this job and run generous fillets of solder along the joints to hold
the shield pieces in position. It is not
necessary to solder along the complete
perimeter; just solder the boards together where you can.
The internal 38 x 12mm board
should be installed with its copper
side facing L5 and L6. Note that the
bottom edge of this board sits about
2mm above the preamplifier board,
to provide clearance for one of the
transistor leads.
With the shield assembly completed, the leads of the ceram
ic
feedthrough capacitors can be connected to the main board and to the
RF preamplifier board using short
lengths of tinned copper wire. The
exception here is the .001µF feed
through capacitor that’s connected
to Q1’s source; it only has one end
connected to the RF preamplifier
board. The lead at the end of the capacitor on the outside of the shield
is simply snipped off.
The two link connections are made
using 0.6mm ECW.
Solder the shield pieces to the RF preamplifier board as shown in this photo &
note that the internal shield piece is installed with its copper side facing L5 &
L6 (to the right). The ceramic feedthrough capacitors are connected to the main
board & to the RF preamplifier board using short lengths of tinned copper wire.
72 Silicon Chip
8
15
A
12
25
15
A
8
care with the orientation of Q1 – its
label should face upwards and the
longest lead should be adjacent to L7.
Do not install the .001µF ceramic
feedthrough capacitors yet, since
these mount into the shield pieces.
Instead, install vertical tinned copper
wire links at each capacitor position
so that these can later be soldered to
the capacitor leads.
The two longest shield pieces can
now be drilled to accept the four
feedthrough capacitors and the two
feedthrough links. Fig.9 shows the
drilling details. Clean away the copper from around the two link holes
using an oversize drill to prevent any
possibility of the links shorting to the
copper. The copper surrounding the
capacitor feedthrough holes should
be left intact and tinned with solder.
You are now ready to install the
feedthrough capacitors. These should
be pushed through so that their
flanges are on the copper side of the
shield pieces – see photos. This done,
the metal bodies of the capacitors
should be soldered to the surrounding
copper.
9
22
27
41
53
COPPER SIDE AT REAR OF PANELS
ALL HOLES 3mm DIA.
REMOVE COPPER AROUND HOLES 'A'
DIMENSIONS IN MILLIMETRES
Fig.9: here are the drilling details for
the two long shield pieces used in the
RF preamplifier.
Once all the feedthrough capacitors are in, the shield pieces can be
soldered to the perimeter of the preamplifier board to form a complete
enclosure. Use a fine-tipped soldering
Final assembly
The completed board assembly is
now ready for installation in the case.
To simplify the description, we will
assume that you are building the unit
from a kit which has pre-punched
holes and screen-printed front and
rear panels. If you are building the
unit from a short-form kit, you will
have to drill the holes yourself using
the PC board and wiring diagram as
a guide.
Assuming that the holes have all
been drilled, assemble the case and
attach the four rubber feet to the base.
This done, install the various items of
hardware on the front and rear panels,
then mount the PC board onto the
baseplate using 5mm standoffs and
3mm screws and nuts. Check that the
LED bargraph display fits neatly into
the slot provided in the front panel
and insert the two 3mm LEDs into
their respective holes.
The transformer can be mounted
next; it is secured using 4mm screws
and nuts. The earth lug is secured
using a 4mm screw, nut and star
washer. Tighten this assembly firmly,
so that there is no possibility of the
earth lug coming adrift. Important:
scrape away the paint or anodising
from around the earth lug mounting
hole before installing the earth lug
SILICON CHIP
BOOK SHOP
Newnes Guide
to Satellite TV
336 pages, in paperback at $49.95.
Installation, Reception & Repair.
By Derek J. Stephenson. First
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Servicing Personal
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Computers are prone to failure
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& includes program listings. 387
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The Art of Linear
Electronics
By John Linsley Hood. Published
1993.
This is a practical handbook from
one of the world’s most prolific
audio designers, with many of his
designs having been published in
English technical magazines over
the years. A great many practical
circuits are featured – a must for
anyone interested in audio design.
Optoelectronics:
An Introduction
By J. C. A. Chaimowicz. First
published 1989, reprinted 1992.
This particular field is about to
explode and it is most important
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subject is comprehensively covered, starting with optics and then
moving into all aspects of fibre
optic communications. 361 pages,
in paperback at $55.95.
Digital Audio & Compact
Disc Technology
Produced by the Sony Service
Centre (Europe). 3rd edition,
published 1995.
Prepared by Sony’s technical
staff, this is the best book on
compact disc technology that we
have ever come across. It covers
digital audio in depth, including
PCM adapters, the Video8 PCM
format and R-DAT. If you want to
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this reference book. 305 pages, in
paperback at $55.95.
Power Electronics
Handbook
Components, Circuits & Applica
tions, by F. F. Mazda. Published
1990.
Previously a neglected field, power
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particularly in the areas of traction
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is an acknowledged authority on
the subject and he writes mainly
on the many uses of thyristors &
Triacs in single and three phase
circuits. 417 pages, in soft cover
at $59.95.
Surface Mount Technology
By Rudolph Strauss. First pub
lish-ed 1994.
This book will provide informative
reading for anyone considering
the assembly of PC boards with
surface mounted devices. Includes
chapters on wave soldering, reflow
soldering, component placement,
cleaning & quality control. 361
pages, in hard cover at $99.00.
Electronics Engineer’s
Reference Book
Edited by F. F. Mazda. First pub
lished 1989. 6th edition 1994.
This just has to be the best reference book available for electronics
engineers. Provides expert coverage of all aspects of electronics
in five parts: techniques, physical
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semicustom electronics & data
communications. 63 chapters, in
paperback at $140.00.
Radio Frequency
Transistors
Principles & Practical Appli
cations. By Norm Dye & Helge
Granberg. Published 1993.
This timely book strips away the
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Written by two Motorola engineers, it looks at RF transistor
fundamentals before moving on
to specific design examples; eg,
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chapters on filtering techniques,
impedance matching & CAD. 235
pages, in hard cover at $85.00.
Newnes Guide to TV &
Video Technology
By Eugene Trundle. First pub
lish-ed 1988, reprinted 1990,
1992.
Eugene Trundle has written for
many years in Television magazine
and his latest book is right up date
on TV and video technology. 432
pages, in paperback, at $39.95.
Title
Price
Newnes Guide to Satellite TV
Servicing Personal Computers
The Art Of Linear Electronics
Optoelectronics: An Introduction
Digital Audio & Compact Disc Technology
Power Electronics Handbook
Surface Mount Technology
Electronic Engineer’s Reference Book
Radio Frequency Transistors
Newnes Guide to TV & Video Technology
$55.95
$59.95
$49.95
$55.95
$55.95
$59.95
$99.00
$140.00
$85.00
$39.95
Postage: add $5.00 per book. Orders over $100 are post
free within Australia. NZ & PNG add $10.00 per book,
elsewhere add $15 per book.
TOTAL $A
August 1994 73
This view clearly shows the three feedthrough capacitors & the feedthrough
link on one side of the shield box. Note that the feedthrough capacitor on the
other side of the shield box is not directly connected to the main PC board.
assembly to ensure a good earth
contact.
Fig.8 shows the final wiring details
for the tuner. Exercise extreme care
with the mains wiring. Begin by stripping back the outer mains cord sheath
so that the leads are free to reach from
the back panel to the mains switch (S1)
on the front panel. This done, push
the mains cord through the entry hole
until about 40mm of the outer sheath
is inside the case and clamp it securely
using a cordgrip grommet.
The Neutral (blue) mains lead goes
directly to power switch S1, while the
Active (brown) lead goes to S1 via the
fuse. The transformer primary connections go to the remaining switch
contacts, while the secondary leads
are twisted together and connected to
the 12.6V AC input on the PC board.
Note that the lead from the centre tap
of the transformer is not used and can
be cut off.
Use heatshrink tubing to insulate
the bare fuse and switch contacts to
prevent accidental shock. This is done
by sliding some heatshrink tubing over
the leads before soldering them. After
the connections have been made, the
tubing is pushed over the switch and
74 Silicon Chip
fuse bodies and shrunk into place
using a hot air gun.
The green/yellow lead from the
mains cord is soldered directly to the
earth lug. Leave a loop in this lead so
that it will be the last lead to come
adrift if the mains cord is wrenched
out of the grommet.
Be sure to use shielded audio cable
for the wiring to the pot and to the
output RCA socket – see Fig.8. This
shielded audio cable should be kept
well away from the power transformer to prevent hum injection into the
audio signal.
The antenna test switch (S2) can
be wired using 3-way rain
bow cable. Note that some switches do not
have the same Common, Normally
Open, Normally Closed (C NO NC)
pin arrangement as shown in Fig.8,
so check your switch before making
the connections. The PAL sockets are
wired with 50Ω RF cable.
Finally, use cable ties to secure the
wiring as shown in the photographs.
Note that the mains leads should be
laced together so that if one lead comes
adrift, it cannot come into contact with
the case.
Before applying power, it is a good
idea to check your work carefully for
wiring and component placement
errors. In particu
lar, check that the
mains wiring is correct, that all parts
are correctly oriented, and that there
are no vacant holes on the PC board.
Note that there are two test points
on the PC board: TP1 and TP GND.
You can connect the negative lead
of your multimeter to TP GND for all
subsequent measurements.
Voltage checks
Apply power and check that +12V
appears at the output of REG1. If it is
below this, switch off immediately
and check the regulator circuit and for
shorts on the +12V rail. If the voltage
is correct, check that +12V is present
on the supply pin of each IC (ie, pin
15 of IC1; pin 1 of IC2; pins 3 & 9 of
IC3; pin 8 of IC4, IC5, IC6, IC9 & IC12;
pin 14 of IC7, IC8 & IC10; and pin 16
of IC11).
The source of Q1 should be at about
4V, which sets the quiescent current
through the device at about 10mA.
You should also be able to measure
4V at G1 of Q1 (and on the other side
of the 220kΩ gate resistor). G2 of Q1
should be at about +12V unless the
tuner happens to be tuned to a very
strong signal. This is very unlikely at
this stage since the tuner has not been
aligned and no antenna is attached.
Fig.10 (above) shows the full-size etching pattern for the main PC
board, while Fig.11 at left shows the etching pattern for the RF
preamplifier board. Check your boards carefully for etching defects
by comparing them with these patterns before mounting any of the
parts.
August 1994 75
Lace the internal wiring together using cable ties & note that the mains leads
should be laced together so that if one lead comes adrift, it cannot come into
contact with the case. The shielded audio cable should be kept well away from
the power transformer to prevent hum injection into the audio signal.
The drain of Q1 should be close to
+12V.
At this stage, one of the active
antenna LEDs should be lit or they
may be alternately flashing at about a
1-second rate. In addition, check that
the Neon lamp in the on/off switch
is glowing but do not expect the signal level LEDs to light at this stage.
Assuming that all is well so far, you
can now move on to the alignment
procedure.
Alignment
Alignment of the tuner requires only
a few simple tools. You will need a
screwdriver-type alignment tool, a
tuning wand, a multimeter and an FM
wireless microphone.
An alignment tool has a plastic
handle and a small tip made of either
brass of tough plastic. It must be used
because an ordinary screwdriver
would detune the coil being adjusted
and, as previously mentioned, could
easily crack the ferrite cores.
The tuning wand (see photo) is used
for aligning the RF preamplifier stage.
It consists of a short length of plastic
tubing with a ferrite core at one end
and a brass screw at the other. This
tool can easily be made as shown in
the accompanying photograph. It decreases the inductance when the brass
end is introduced into an air-cored
76 Silicon Chip
coil and increases the inductance
when the ferrite core is introduced
into the coil.
During alignment, the multimeter
is used to monitor the signal level at
TP1, while the wireless microphone
is used as the signal source. The
step-by-step alignment procedure is
as follows:
(1). Connect a simple antenna to the
antenna A input. A 300mm length of
copper wire plugged into the antenna
socket will do the job.
(2). Adjust VR1 so that the first LED
in the bargraph is just extinguished or
is very dim (FM microphone off). This
will set the meter signal output range.
Adjust VR2 and VR3 so that the wiper
of VR2 is at 0.8V and the wiper of VR3
is at 0.3V.
(3). Connect the multimeter between TP1 and TP GND and set it so
that it will read a 0-3V range.
(4). Switch on the FM microphone
and place it close to the antenna.
Now press and hold the antenna test
switch to select antenna A and adjust
the slug in T1 using the alignment
tool until a voltage appears on the
multimeter.
Depending on the initial state of
tune, the signal strength meter will
either show full scale or only a few
LEDs will be lit. Adjust T1 for a maximum voltage reading.
Note: this maximum voltage must
be less than 2.5V, otherwise the meter
circuit may overrange and a false maximum may be obtained. To overcome
this problem, simply move the FM
microphone further away from the
receiving antenna.
(5). Adjust T2 for a maximum
reading, then adjust L10. This done,
adjust T1 again (this is necessary since
adjustments to L10 retune the local
oscillator due to the AFC).
(6). Repeat step 4 to obtain the maximum signal. Note that it is difficult
to tune L10 if the slug is adjusted too
quickly – tune the slug slowly to avoid
missing the signal peak. Note also that
all three coils may have a small range
over which the signal remains at maximum. In each case, find the centre of
this adjustment range and set the slug
to this position.
(7). L6 and L9 can now be adjusted
for maximum signal. Begin by spreading L6 and L9 so that there is about
0.5mm between each winding turn
and adjust VC1 and VC2 for maximum
signal.
(8). Insert the brass end of the tuning wand into L6. If the signal level
decreases, try the ferrite end of the
wand. If the signal decreases again,
then the coil is correctly tuned. More
than likely, the coil will not be tuned
and will need to be stretched or closed
slightly so that both ends of the tuning wand produce a drop in signal
strength.
If the signal goes down with the
brass end of the wand and increases
with the ferrite end, close the coil
slightly by squeezing it gently with
your fingers. Repeat the above test to
see if the coil is now tuned.
Conversely, if the signal goes up
with the brass end and down with the
ferrite end, then the coil will need to
be stretched slightly. Retest the coil
with both ends of the wand after each
adjustment until the tuning is correct
(ie, both ends of the wand cause the
signal level to decrease).
(9). Repeat step 7 for coil L9, then
repeat the entire alignment procedure
again to make sure that everything is
spot on.
(10). Switch off the FM microphone
and set VR2 (the mute threshold trimpot) fully clockwise. Now adjust VR2
anticlockwise until pin 7 of IC5a just
goes low.
Antenna installation
The antenna requirements for the
SILICON CHIP Dual Diversi
ty Tuner
are not particularly difficult. You can
use commercial FM dipole antennas,
TV “rabbit ears” or 1/4-wave whip
antennas. It is not necessary to use
antennas with gain such as multi-element Yagis.
Dipole and rabbit ear antennas
usually have a characteristic impedance of 300Ω, so you will need to use
a balun transformer (for TV sets) to
match these antennas to the 75Ω input
sockets on the rear panel of the tuner.
TV balun transformers are available
for a few dollars from your local parts
retailer.
A 1/4-wave whip is simply a 300400mm length of wire which plugs
into the rear of the tuner. You can make
one up by connecting a suitable length
of stout enamelled copper wire to the
centre pin of a PAL plug. The second
antenna must be separated from the
first by at least three metres and this
is best done using a PAL plug to PAL
socket extension lead.
When installing the tuner, the antennas should be mounted above the
stage or the audience to minimise
signal attenuation due to people
and room objects. Adjust the audio
level pot so that the signal output
level matches the mixer or amplifier
requirements.
After each setup, always test the
unit by having somebody move
around with the FM wireless microphone. The signal strength meter
on the tuner will give you a good
indication of the signal strength from
each antenna. Use the test switch to
select the second antenna to verify
its performance and check that the
Diversity Tuner automatically switches between the two antennas as the
microphone is moved around.
SC
This home-made tuning wand is used for aligning the RF preamplifier stage
& consists of a short length of plastic tubing with a ferrite core at one end &
a brass screw at the other. It decreases the inductance when the brass end is
introduced into an air-cored coil & increases the inductance when the ferrite
core is introduced into the coil.
August 1994 77
SPECIALS BY FAX
If your fax has a polling function, dial (02) 579
3955 and press your POLLING button to get our latest
specials, plus our item and kit listing. Updated
at the start of each month.
HF ELECTRONIC BALLASTS
Brand new “slim line” cased electronic
ballasts. They provide instant flicker free
starting, extend tube life, reduce power
consumption, eliminate flicker during operation (high frequency operation), and are
“noise free” in operation. The design of these
appears to be similar to the one published in
the Oct. 94 SILICON CHIP magazine. One of
the models even includes a DIMMING OPTION!! Needs external 100K potentiometer
or a 0-10V DC source. We have a good but
limited stock of these and are offering them at
fraction of the cost of the parts used in them!
Type A: Designed to power two 32W - 4’
tubes, will power two 40W - 4’ tubes with
no noticeable change in light output, has
provision for dimming: $26
Type B: Designed to power two 16W - 18"
tubes, will power two 18W - 18" tubes with
no noticeable change in light output: $18
MISCELLANEOUS
FLAT NOSE PLIERS: $4 per pair. BATTERY
CHARGER: S2 accessory set for Telecom
Walkabout “Phones”. Includes cigarette
lighter cable, fast rate charger, and desktop
stand. Actually charges 6 series connected
AA Nicad batteries: $27. BATTERY PACKS:
Contain 6 AA Nicad batteries wired in
series, can easily be pulled apart, used
units, satisfaction guaranteed: $2 per pack.
LITHIUM BATTERIES: Button shaped with
pins, 20mm diameter, 3mm thick. A red led
connected across one of these will produce
light output for over 72 hours (3 days): 4 for $2.
CIGARETTE LIGHTER LEADS: Cigarette
lighter plug with 3 metres of heavy duty fig. 8
flex connected. Should suit load currents up
to 20A: 5 for $5. SUPERCAPS: 0.047F/5.5V
capacitors: 5 for $2. HOUR METER: Non
resettable, mains powered (50HZ), WARBURTON FRANKI, 100,000 Hours maximum,
0.01Hr resolution: $15. PCB MOUNTED
SWITCHES 90 deg. 3A-250V, SPDT: 4 for $2.
AC POWER SUPPLY: Mains in, two separate
8.5V/3A outputs, in plastic case with mains
power lead/plug and output leads/plugs: $15
Ea. MONITOR PCB’s: Complete PCB and
yoke assembly for high resolution monochrome TV monitors (no tube). Operate from
12V DC, circuit and information provided:
$15. MODEMS: Complete mains powered
non standard 1200 baud Telecom approved
modems. We should have brief information
available. Limited stock at below the price of
the high quality case that these are housed
in: $30 for 2 modems.
MEDICAL LASER
One only water cooled medical laser with
selectable outputs: Argon (7W multiline) or
Dye laser (1W red). Large water cooled unit
with a separate control box and accessories
(350kg):
$15,000
LEVEL RECORDER
One only, Bruel & Kjaer level recorder type
2305, in good condition:
$300
78 Silicon Chip
DIE CAST BOXES
These large (187 x 120 x 56mm) aluminium
die cast boxes have several holes drilled in
them and have a C&K toggle switch and a
6.25mm phono socket fitted. New units from
an unfinished production project:
$4 Ea.
WELLER SOLDERING IRON TIPS
New soldering iron for low voltage Weller soldering stations and mains operated Weller
irons. Mixed popular sizes and temperatures.
Specify mains or soldering station type:
5 for $10.
NICAD BATTERY PACKS
Brand new Toshiba 7.2V-2.2AHr Nicad
Battery packs in a plastic assembly:
$20 Ea.
If you purchase three packs we will supply
a matching fast charger (90min.) that can
charge up to three of these batteries (one at
a time). Modern unit that employs “delta V”
voltage detection to terminate charge, needs
an external 12V-2.2A unregulated supply:
$60 for three battery packs and a
three way charger.
PLUGS/SOCKETS
3 pin chassis mounting socket and a matching covered three pin plug. Good quality
components that will handle a few amperes
at low voltage:
$5 for 4 pairs.
DYNAMIC MICROPHONES
Low impedance dynamic microphones
with separate switch wiring, 3.5mm mic.
plug, 2.5mm switch plug, as used on most
cassette recorders:
$4 Ea.
40mW IR LASER DIODES
New famous brand 40mW-830nM IR laser
diodes, suit medical and other applications:
$90 Ea. Constant current driver kit to
suit: $10.
HIGH POWER LED IR ILLUMINATOR
This kit includes two PCBs, all on-board
components plus casing: Switched mode
power supply plus 60 high intensity 880nm
IR (invisible) LEDs. Variable output power,
6-20VDC input, suitable for illuminating IR
responsive CCD cameras, IR night viewers
etc. Professional performance at a fraction
of the price of the commercial product.
COMPLETE KIT PRICE:
$60
LOW COST 1-2 CHANNEL UHF
REMOTE CONTROL
Late in October we will have available a
single channel 304MHz UHF remote control
with over 1/2 million code combinations
which also makes provision for a second
channel expansion. The low cost design
includes a complete compact keyring
transmitter kit, which includes a case and
battery, and a PCB and components kit
for the receiver that has 2A relay contact
output! Tx kit $10, Rx kit $20. Additional
components to convert the receiver to 2
channel operation (extra decoder IC and
relay) $6. INCREDIBLE PRICES:
COMPLETE 1 CHANNEL TX-RX KIT:
$30
COMPLETE 2 CHANNEL TX-RX KIT:
$36
ADDITIONAL TRANSMITTERS: $10
FIBRE OPTIC TUBES
These US made tubes are from used equipment but in excellent condition. Have 25/40
mm diameter, fibre-optically coupled input
and output windows. The 25mm tube has an
overall diameter of 57mm and is 60mm long,
the 40mm tube has an overall diameter of
80mm and is 92mm long. The gain of these is
such that they would produce a good image
in approximately 1/2 moon illumination, when
used with suitable “fast” lens, but they can
also be IR assisted to see in total darkness.
Our HIGH POWER LED IR ILLUMINATOR
kit, and the IR filter are both suitable for use
with these tubes. The superior resolution
of these tubes would make them suitable
for low light video preamplifiers, wild life
observation, and astronomical use. Each of
the tubes is supplied with an 9V-EHT power
supply kit. INCREDIBLE PRICES:
$120 for the 25mm intensifier tube
and supply kit.
$180 for the 40mm intensifier tube
and supply kit.
We also have a good supply of the same
tubes that may have a small blemish which
is not in the central viewing area!:
$65 for a blemished 25mm intensifier
tube and supply kit.
$95 for the blemished 40mm intensifier tube and supply kit.
SIEMENS VARISTORS
420VAC 20 joule varistors that are suitable
for spike protection in Australian 3 phase
systems:
10 for $5.
TAA611C ICs
TAA611C Audio power amplifier ICs, no more
information: 5 for $5.
INTENSIFIED NIGHT VIEWER KIT
SC Sept. 94. See in the dark! Make your own
night scope that will produce good vision in
sub-starlight illumination! Has superior gain
and resolution to all Russian viewers priced
at under $1500. We supply a three stage
fibre-optically coupled image intensifier
tube, EHT power supply kit, and sufficient
plastics to make a monocular scope. The
three tubes are supplied already wired and
bonded together.
$290 for the 25mm version
$390 for the 40mm version
We can also supply the lens (100mm f2:
$75) and the eyepiece ($18) which would
be everything that is necessary to make an
incredible viewer!
MAINS POWERED GAS LASER
Includes a professional potted mains power
supply and a new 3mW red tube to suit. One
catch, this supply requires a 4-6V (TTL) enable input which is optically isolated, to make
the unit switch ON. Very low consumption
from a 4.5V battery.
$100 for a new 3mW tube plus a TTL
mains power supply to suit.
SUPER DIODE POINTERS - HEADS
These pointers probably represent the
best value when you compare them on
a “brightness per dollar” basis. They are
about 5 times brighter than 5mW/670nm
pointers! They have an output of 2.5mW at
650nm, which is about equal in brightness
to a 0.8mW HE-NE tube!! SPECIAL INTRODUCTORY PRICE:
$150
We will also have available some of the
3V diode modules used in these pointers
at approximately $125, and also some
2.5mW/635nm laser diode modules with
special optics at approximately $280.
VIDEO TRANSMITTERS
Low power PAL standard UHF TV transmitters. Have audio and video inputs with
adjustable levels, a power switch, and a
power input socket: 10-14V DC/10mA operation. Enclosed in a small metal box with an
attached telescopic antenna. Range is up to
10m with the telescopic antenna supplied,
but can be increased to approximately
30m by the use of a small directional UHF
antenna. INCREDIBLE PRICING:
$25
TDA ICs/TRANSFORMERS
We have a limited stock of some 20 Watt
TDA1520 HI-FI quality monolithic power
amplifier ICs, less than 0.01% THD and
TIM distortion, at 10W RMS output! With
the transformer we supply we guarantee an
output of greater than 20W RMS per channel
into an 8ohm load, with both channels driven.
We supply a far overrated 240V-28V/80W
transformer, two TDA1520 ICs, and two
suitable PCBs which also include an optional
preamplifier section (only one additional IC),
and a circuit and layout diagram. The combination can be used as a high quality HI-FI
Stereo/Guitar/P.A., amplifier. Only a handful
of additional components are required to
complete this excellent stereo/twin amplifier!
Incredible pricing:
$25
for one 240V-28V (80W!) transformer, two
TDA1520 monolithic HI-FI amplifier ICs, two
PCBs to suit, circuit diagram/layout. Some
additional components and a heatsink are
required.
LIGHT MOTION DETECTORS
Small PCB assembly based on a ULN2232
IC. This device has a built in light detector,
filters, timer, narrow angle lens, and even a
siren driver circuit that can drive an external
speaker. Will detect humans crossing a
narrow corridor at distances up to 3 metres.
Much higher ranges are possible if the
detector is illuminated by a remote visible
or IR light source. Can be used at very low
light levels, and even in total darkness: with
IR LED. Full information provided. The IC
only, is worth $16! OUR SPECIAL PRICE
FOR THE ASSEMBLY IS:
$5 Ea. or 5 for $20
GAS LASER SPECIAL
We have a good supply of some He-Ne laser
heads that were removed from new or near
new equipment, and have a power output
of 2.5-5mW: very bright! With each head
we will supply a 12V universal laser power
supply kit for a ridiculous TOTAL PRICE of:
$89
AA NICADS
Brand new AA size Saft brand (made in
France) 500mA Hr. batteries, also have
solder connections (can be removed):
$2 Ea. or 10 for $ 16.
TWO STEPPER MOTORS PLUS A
DRIVER KIT
This kit will drive two stepper motors: 4, 5, 6
or 8 eight wire stepper motors from an IBM
computer parallel port. Motors require separate power supply. A detailed manual on the
COMPUTER CONTROL OF MOTORS plus
circuit diagrams/descriptions are provided.
We also provide the necessary software on
a 5.25" disc. Great “low cost” educational kit.
We provide the kit, manual, disc, plus TWO
5V/6 WIRE/7.5 Deg. STEPPER MOTORS
FOR A SPECIAL PRICE OF:
$42
CAMERA FLASH UNITS
Electronic flash units out of disposable
cameras. Include PCB/components and
Xenon tube/reflector assembly. Requires
a 1.5V battery.
$2.50
IR LASER DIODE KIT
auto iris lens. It can work with illumination
of as little as 0.1Lux and it is IR responsive.
Can be used in total darkness with Infra Red
illumination. Overall dimensions of camera
are 24 x 46 x 70mm and it weighs less
than 40 grams! Can be connected to any
standard monitor, or the video input on a
Video cassette recorder. NEW LOW PRICE:
$199
IR “TANK SET”
A set of components that can be used to
make a very responsive Infra Red night
viewer. The matching lens tube and eyepiece
sets were removed from working military
quality tank viewers. We also supply a very
small EHT power supply kit that enables the
tube to be operated from a small 9V battery.
The tube employed is probably the most sensitive IR responsive tube we ever supplied.
The resultant viewer requires low level IR
illumination. Basic instructions provided.
$140
BRAND NEW 780nm LASER DIODES
(barely visible), mounted in a professional
adjustable collimator-heatsink assembly.
Each of these assemblies is supplied with
a CONSTANT CURRENT DRIVER kit and a
suitable PIN DIODE that can serve as a detector, plus some INSTRUCTIONS. Suitable
for medical use, perimeter protection, data
transmission, IR illumination, etc.
For the tube, lens, eyepiece and the power
supply kit.
5mW VISIBLE LASER DIODE KIT
We include a basic diagram-circuit showing
how to make a small refrigerator-heater.
The major additional items required will
be an insulated container such as an old
“Esky”, two heatsinks, and a small block
of aluminium.
$40
Includes a Hitachi 6711G 5mW-670nm
visible laser diode, an APC driver kit, a
collimating lens - heatsink assembly, a
case and battery holder. That’s a complete
3mW collimated laser diode kit for a TOTAL
PRICE OF:
$75
BIGGER LASER
We have a good, but LIMITED QUANTITY
of some “as new” red 6mW+ laser heads
that were removed from new equipment.
Head dimensions: 45mm diameter by
380mm long. With each of the heads we
will include our 12V Universal Laser power
supply. BARGAIN AT:
$170 6mW+ head/supply. ITEM No.
0225B
We can also supply a 240V-12V/4A-5V/4A
switched mode power supply to suit for $30.
12V-2.5 WATT SOLAR PANEL
SPECIAL
These US made amorphous glass solar
panels only need terminating and weather
proofing. We provide terminating clips and a
slightly larger sheet of glass. The terminated
panel is glued to the backing glass, around
the edges only. To make the final weatherproof panel look very attractive some inexpensive plastic “L” angle could also be glued
to the edges with some silicone. Very easy
to make. Dimensions: 305 x 228mm, Vo-c:
18-20V, Is-c: 250mA. SPECIAL REDUCED
PRICE until the end of 94!:
$20 Ea. or 4 for $60
Each panel is provided with a sheet of
backing glass, terminating clips, an isolating
diode, and the instructions. A very efficient
switching regulator kit is available: Suits
12-24V batteries, 0.1-16A panels, $27. Also
available is a simple and efficient shunt
regulator kit, $5.
CCD CAMERA
Monochrome CCD camera which is totally
assembled on a small PCB and includes an
SOLID STATE “PELTIER EFFECT”
COOLER-HEATER
These are the major parts needed to make a
solid state thermoelectric cooler-heater. We
can provide a large 12V-4.5A Peltier effect
semiconductor, two thermal cutout switches,
and a 12V DC fan for a total price of:
$45. ITEM No. 0231
RUSSIAN NIGHT VIEWER
We have a limited quantity of some passive
monocular Russian made night viewers
that employ a 1st generation image intensifier tube, and are prefocussed to infinity.
CLEARANCE:
$180
INFRA RED FILTER
A very high quality IR filter and a RUBBER
lens cover that would fit over most torches
including MAGLITEs, and convert them to
a good source of IR. The filter material withstands high temperatures and produces an
output which would not be visible from a few
metres away and in total darkness. Suitable
for use with passive and active viewers. The
filter and a rubber lens cover is priced at:
$11
DOME TWEETERS
Small (70mm diam., 15mm deep) dynamic
8ohm tweeters, as used in very compact
high quality speaker systems: $5 Ea. We
also have some 4" woofers: $5 Ea.
VIDEO ZOOM LENSES
Wire antenna - attached, Microphone: Electret condenser, Battery: One 1.5V silver oxide
LR44/G13, Battery life: 60 hours, Weight:
15g, Dimensions: 1.3" x 0.9" x 0.4".
$25
REEL TO REEL TAPES
New studio quality 13cm-5" “Agfa” (German) 1/4" reel to reel tapes in original box,
180m-600ft: $8 Ea.
MORE KITS-ITEMS
Single Channel UHF Remote Control, SC
Dec. 92 1 x Tx plus 1 x Rx $45, extra Tx $15.
4 Channel UHF Remote Control Kit: two
transmitters and one receiver, $96.
Garage/Door/Gate Remote Control Kit:
Tx $18, Rx $79.
1.5-9V Converter Kit: $6 Ea. or 3 for $15.
Laser Beam Communicator Kit: Tx, Rx,
plus IR Laser, $60. Magnetic Card Reader:
professional assembled and cased unit that
will read information from plastic cards,
needs low current 12VDC supply-plugpack, $70.
Switched Mode Power Supplies: mains in
(240V), new assembled units with 12V-4A
and 5V-4ADC outputs, $32.
Electric Fence Kit: PCB and components,
includes prewound transformer, $28
High Power IR LEDs: 880nm/30mW/12deg.
<at> 100mA, 10 for $9 Plasma Ball Kit: PCB
and components kit, needs any bulb, $25.
Masthead Amplifier Kit: two PCBs plus
all on board components: low noise (uses
MAR-6 IC), covers VHF-UHF, $18.
Inductive Proximity Switches: detect
ferrous and non-ferrous metals at close
proximity, AC or DC powered types, three
wire connection for connecting into circuitry:
two for the supply, and one for switching the
load. These also make excellent sensors for
rotating shafts etc. $22 Ea. or 6 for $100.
Brake Light Indicator Kit: 60 LEDs, two
PCBs and ten Rs, makes for a very bright
600mm long high intensity Red display, $30.
IEC Leads: heavy duty 3 core (10A) 3M
LEADS with IEC plug on one end and an
European plug at the other, $1.50 Ea. or
10 for $10.
IEC Extension Leads: 2M long, IEC plug
at one end, IEC socket at other end, $5.
Motor Special: these motors can also
double up as generators. Type M9: 12V, I
No load = 0.52A-15,800 RPM at 12V, 36mm
Diam.-67mm long, $5. Type M14: made for
slot cars, 4-8V, I No load = 0.84A at 6V, at
max efficiency I = 5.7A-7500 RPM, 30mm
Diam-57mm long, $5.
EPROMS: 27C512, 512K (64K x 8), 150ns
access CMOS EPROMS. Removed from
new equipment, need to be erased, guaranteed, $4.
Green Laser Tubes: Back in stock! The
luminous output of these 1-1.5mW GREEN
laser diode heads compares with a 5mW red
tube!: $490 for a 1-1.5mW green head and
a 12V operated universal laser inverter kit.
40 x 2 LCD Display: brand new 40 character by 2 line LCD displays with built in
driver circuitry that uses Hitachi ICs, easy
to drive “standard” displays, brief information
provided, $30 Ea. or 4 for $100.
RS232 Interface PCB: brand new PCB
assembly, amongst many parts contains
two INTERSIL ICL232 ICs: RS232 Tx - Rx
ICs, $8.
Modular Telephone Cables: 4-way modular
curled cable with plugs fitted at each end,
also a 4m long 8-way modular flat cable with
plugs fitted at each end, one of each for $2.
12V Fans: brand new 80mm 12V-1.6W
DC fans. These are IC controlled and have
four different approval stamps, $10 Ea. or
5 for $40.
Lenses: a pair of lens assemblies that were
removed from brand new laser printers. They
contain a total of 4 lenses which by different
combinations - placement in a laser beam
can diverge, collimate, make a small line,
make an ellipse etc., $ 8.
Polygon Scanners: precision motor with
8 sided mirror, plus a matching PCB driver
assembly. Will deflect a laser beam and
generate a line. Needs a clock pulse and DC
supply to operate, information supplied, $25.
PCB With AD7581LN IC: PCB assembly
that amongst many other components
contains a MAXIM AD7581LN IC: 8 bit, 8
channel memory buffered data acquisition
system designed to interface with microprocessors, $29.
EHT Power Supply: out of new laser printers, deliver -600V, -7.5KV and +7kV when
powered from a 24V-800mA DC supply,
enclosed in a plastic case, $16.
Mains Contactor Relay: has a 24V-250ohm
relay coil, and four separate SPST switch
outputs, 2 x 10A and 2 x 20A, new Omron
brand, mounting bracket and spade connectors provided, $8.
FM Transmitter Kit - Mk.II: high quality high stability, suit radio microphones and
instruments, 9V operation, the kit includes
a PCB and all the on-board components,
an electret microphone, and a 9V battery
clip, $11.
FM Transmitter Kit - Mk.I: this complete
transmitter kit (miniature microphone included) is the size of a “AA” battery, and it
is powered by a single “AA” battery. We use
a two “AA” battery holder (provided) for the
case, and a battery clip (shorted) for the
switch. Estimated battery life is over 500
hours!!: $11.
High Power Argons: the real thing! Draw
pictures on clouds, big buildings etc., with
a multiline water-cooled Argon laser with a
few watts of output. “Ring” for more details.
Argon-Ion Heads: used Argon-Ion heads
with 30-100mW output in the blue-green
spectrum, will be back in stock soon, priced
at around $400 for the “head” only, power
supply circuit and information supplied.
Two only 10:1 video zoom lenses, f=15150mm, 1:1.8, have provision for remote
focus aperture and zoom control: three
motors, one has a “C” mount adaptor, 150mm
diam. by 180mm long:
OATLEY ELECTRONICS
MINIATURE FM TRANSMITTER
Phone (02) 579 4985. Fax (02) 570 7910
$390 Ea.
Not a kit, but a very small ready made self
contained FM transmitter enclosed in a small
black metal case. It is powered by a single
small 1.5V silver oxide battery, and has an
inbuilt electret microphone. SPECIFICATIONS: Tuning range: 88-108MHz, Antenna:
PO Box 89, Oatley, NSW 2223
Bankcard, Master Card, Visa Card & Amex accepted with
phone & fax orders. P & P for most mixed orders: Aust. $6; NZ
(airmail) $10.
August 1994 79
VINTAGE RADIO
By JOHN HILL
Building a classic crystal set
Building a classic crystal set can be a lot of fun.
This unit is based on an old navy design
& offers excellent performance considering
the circuit simplicity.
I recently joined a radio collectors’
club – The Vintage Radio Club of North
East Victoria Inc. This group meets at
various locations around the Sheppar
ton, Benalla and Wangaratta region
and has a membership of about 40.
The North East Club is a fairly active group. Not only do they meet on
a regular monthly basis but they also
put out a monthly newsletter which
is a remarkable effort in itself and a
credit to those concerned. And every
year, the club presents to one of its
members a special achievement award
called the “Hellier Award”.
Les Hellier was a radio pioneer in
the Wangaratta district in the early
1920s. His family were happy to have
his name used by the club for their
annual award and have supplied a
shield for use as a perpetual trophy.
Last year, everyone who wished to
participate in the award activity built
a Little General receiver. This year’s
effort centres around the building of
a crystal set. Personally, I think the
crystal set project is a great idea as it
allows members with little practical
experience to participate in the event.
There are two award categories this
year – vintage and open – so the award
will have joint winners.
Classic crystal set
Anyway, this preamble is simply
a lead up to explain why I have just
finished building a crystal set. I am
pleased to say that my home-made
receiver has turned out to be an outstanding performer and it has been
well worth the effort. What’s more, I
found building this simple little radio
to be an interesting and rewarding
project.
The heart of any crystal set is the crystal
detector. This particular detector uses
a genuine Neutron crystal & bronze
catswhisker. The Neutron crystal is manmade & is not a natural lead sulphide
galena crystal.
80 Silicon Chip
To be perfectly honest, I cannot take
much credit for my crystal set because
it has been built to a well-proven
design. It is a home-made version of
the Technicraft-cum-Orpheus “Super
Crystal Set”, without the spiderweb
coils, plus a few minor modifications
of my own. I also decided on a name
change to distinguish my version and
it is now the “Classic Crystal Set”.
The receiver is of elaborate design
(for a crystal set), having three coils, a
10-position stud switch, two variable
capacitors and four controls on the
front panel. As the set is to be entered
in the vintage category, it has been
built to look like a 1920s production,
complete with a catswhisker type
crystal detector, black bakelite panels
and vintage style control knobs.
The cabinet also follows this pattern; it has a lift up lid and is made of
solid blackwood timber.
Design origins
The previously mentioned Super
Crystal Set was originally designed by
David Whitby and is based on early
navy circuits. The Super Crystal Set, as
well as several other vintage radio kits,
were quite popular about 10 years ago.
In fact, it was these Technicraft kits
that started me in vintage radio. If they
had not come along at the right time, I
would most likely be doing something
else for a hobby today.
David eventually sold his vintage
radio department to Richard Wilson
who then sold the kits through the
Orpheus Radio Museum in Ballarat.
When Richard eventually decided to
get out of the vintage radio business,
the production of Technicraft kits
suddenly came to an end. No doubt
this range of receivers will become
quite collectable.
Retailing at $89, the Super Crystal
Set kit was not cheap and many would-
These ancient aerial and earth terminals are just the thing when building a
1920s style crystal set. The parts used in vintage construction should be from
the right era, or at least look as though they are.
The Classic Crystal Set’s coils were
wound on old (& very rare) 2-inch
diameter black bakelite tubing. A thin
piece of wood has been used to isolate
the coil taps.
This photo shows the two old style variable capacitors used in the crystal set.
The one on the left has a range of about 0-100pF & the larger one a range of
about 0-500pF. Both are plain, single bearing types & both required cleaning &
adjustment before they could be used.
be builders were discouraged by the
price. If you now want to build this
remarkable crystal receiver, simply do
as I have done; build it using conventional coils and utilise what odd bits
and pieces you may have available.
Whether or not the receiver is made to
look like a vintage set or not is entirely
up to each individual constructor and
the components available. Because my
80T
TAPPED 20,10,10
10,10,20
AERIAL
80T
0
receiver has been built as a vintage
replica, the rename to Classic Crystal
Set seemed appropriate.
Design points
I like to think of this particular receiver as being a TRF (tuned radio frequency) crystal set. While some would
argue that the RF section is nothing
other than a loading coil, there really
CRYSTAL
DETECTOR
18T
500pF
10
STUD
SWITCH
100200pF
EARTH
.001
HIGH
IMPEDANCE
'PHONES
Fig.1: the circuit
for the Classic
Crystal set uses
a tapped loading
coil which is
accurately tuned
with a trimmer
capacitor.
is a bit more to it than that.
Sure it is a tapped loading coil but
my design improvement incorporates
a variable capacitor so that the resonance peak can be accurately obtained.
Without this trimmer capacitor, the
eight turns between the taps is much
too coarse if the resonance point of a
particular station is midway between
taps.
As far as I’m aware, a loading coil
is nothing but a tapped coil in series
with the aerial. It is often mounted
on a separate board and operates
independently of and outside the
crystal set.
On the other hand, the accurately
tuned RF coil in the Classic Crystal
Set is inductively coupled to the detector stage by a variable coupling coil
arrangement. That seems like a tuned
non-amplified RF stage to me.
Anyway, whether you agree with
me or not, you would have to admit
that a TRF Crystal Set sounds intriguing and gives the receiver a bit
of class. If anything ever needed its
image lifted in this day and age, it
would have to be the humble crystal
set. So a TRF it is!
Collecting the parts
It is surprising just how long it takes
to bring a simple crystal set project to
completion. Just finding all the necessary bits and pieces was a major operation and quite a few hours were spent
locating the required parts. Knowing
that you have something and knowing where to find it are two different
August 1994 81
A pair of Browns type F high-impedance headphones was used with the Classic
crystal Set. Also shown is an adapter which allows phones with standard lead
tips to be used with a quarter-inch phone jack.
described in crystal set terms as being
mediocre (20 metres long and 6 metres
high), this remarkable little receiver
can even pull in interstate stations.
Adelaide and Sydney stations (5CL,
5AN and 2BL) sometimes come in at
surprisingly good volume levels. Of
course, they often fade to nothing for
lengthy periods too. I must also stress
that these interstate stations are in the
50kW class and this fact allows them
to be received at great distances – even
on a crystal set.
However, the most incredible reception feat that the Classic has managed
so far is 4QD in Emerald, Queensland
– 1500km as the crow files. Once again,
this is a powerful 50kW station. The
original Technicraft Super Crystal Set
will also receive 4QD.
It would appear that I’m in a good
reception area for these particular
transmissions. I might also add that
listening to these distant stations
is not damaging my hearing to any
extent and nor are the headphones
being greatly overstressed. They are
loud enough to identify and that’s
about all.
Detector stage
The variable coupling coil setup was installed in one end of the detector coil. It
is mounted on a hardwood shaft & the coil connections run through the shaft to
the outside. Note that the coil is bound with thread to keep it together.
things. Cleaning and repairing these
parts took up a considerable amount
of time too.
Mention should also be made of
the convenience of having a lathe in
one’s workshop. The variable coupling
coil control, in particular, would have
been difficult to incorporate without
the lathe.
The big advantage of a crystal set of
this design type is that it is so selective,
yet it seems to produce this selectivity
without loss of volume which is contrary to what one would expect.
Selectivity is something that is really important in my locality because
of a local 5kW station, 3CV (Central
82 Silicon Chip
Victoria) on 1071kHz. Not only is 3CV
a mere 6km away from my location but
it also occupies a central position on
the dial. Most single coil crystal sets
cannot handle such a situation and
provide only single station reception
– the strong local.
However, the Classic Crystal Set
with its two tuned circuits, variable
coupling coil and tapped detector coil
enables the operator to tune out the
local station to a remarkable degree.
3CV can be suppressed sufficiently to
receive about eight other stations on
those special nights when reception
is particularly good.
Using an aerial that can only be
Looking at the circuit (Fig.1), one
can say that the detector stage of the
receiver is just about as standard as a
crystal set can be. There are no special
techniques involved and attaching the
antenna to the top of the detector coil
would produce a fairly basic crystal
set.
The secret of the set’s brilliant performance must therefore be in the RF
section ahead of the detector stage.
The tuned RF coil and its accompanying variable coupling coil is where
the performance comes from. This
particular circuitry produces good
selectivity without any significant
loss in volume.
Tuning the receiver is a two-handed
job and it takes a while to pick out
those elusive stations. When a station
is located, it needs to be logged on a
chart so that it can be found again.
This is where it helps if the controls
have numbered dials. In the case of the
Classic, the tuning dial is numbered,
the RF coil trimmer is numbered, the
stud switch is numbered and the coupling coil control knob arrow operates
best at around the 12 o’clock position.
It is therefore easy to return to a station
once these control positions have been
accurately logged.
RESURRECTION
RADIO
Valve Equipment Specialists
Repairs – Restoration – Sales
The finished receiver successfully captures the vintage look of the 1920s. The
crystal detector was mounted high on the back of the front panel where it is out
of harm’s way.
Another stud switch for the detector
coil taps would have been a good idea
but there really wasn’t room to accommodate it on the front panel. Instead,
an internal wander lead and alligator
clip is used. Once set for best results,
it seldom needs moving.
The crystal used in the detector is
not the usual lead sulphide natural
galena type but a genuine “Neutron”
crystal. These special man-made
crystals have a surface which contains
hundreds of small sparkling facets and
good spots abound.
The Neutron crystal was actually
broken in half with a pair of side cutters so that the catswhisker operates
on a freshly exposed surface of the
crystal. When set on a good spot, the
Neutron crystal performs equally as
well as a germanium signal diode,
although an ohm meter indicates
otherwise.
Alternate switching from crystal
to diode produced no difference in
reception quality or sensitivity. However, the signal diode is a bit more
convenient to use.
If you have an interest in simple
radio receivers, then this particular
The parts visible in this photo include the tapped RF coil,
the rear of the stud switch & the trimming capacitor. The
alligator clip at the left is used for selecting the detector
coil taps & once set rarely needs shifting.
VALVES – 1200 types in stock
EL34/BCA7 matched $30 ea.
6L6GC
matched $28 ea.
Parts are available for the enthusiast, including over 900 valve types, high voltage
capa citors, transformers, dial glasses,
knobs, grille cloth etc.
Circuit diagrams for most Australian makes
and models.
Send SAE for our catalog.
WANTED: Valves, Radios, etc.
Purchased for CASH
Call in to our NEW showroom at:
242 Chapel Street (PO Box 2029),
Prahran, Vic 3181.
Phone: (03) 510 4486; Fax (03) 529 5639
circuit will not only test your construction skills but will also reward
you with a top performing crystal
receiver. Whether it is operated in
the city or in some remote country
area, it will give a surprisingly good
account of itself.
So it’s off to the Hellier Award meeting at the weekend. I’ll tell you how it
SC
all went next month.
This view shows the variable coupling coil setup & the
drive shaft to the front panel. Note the brass “clock spring”
connectors on the shaft. Rotation of the coupling coil is
restricted to half a turn.
August 1994 83
REMOTE CONTROL
BY BOB YOUNG
Modellers with dedication; Pt.2
This month, we will look at the work of one
of the most dedicated, versatile & highly
skilled modellers I have ever had the
pleasure to make the acquaintance of, in a
lifetime of active modelling.
For personal reasons he has asked
me to withhold his name so I will
henceforth refer to him only as John.
I first met him when I was operating out of my father’s newsagency at
Tempe back in the mid 1960s. At that
time, he purchased a 10-channel reed
system from me for a model yacht.
Over the years our business relationship grew into one of those friendships
that thrives for a time only to diverge
for a period and then comes back to
life, and always with the feeling that
no real time has elapsed since our last
meeting.
During those years I have watched
his interest in modelling grow and
mature, with his work now at what
I consider to be the level of a master
craftsman.
The staggering thing about John
is the diversity of his interests and
This model racing semi-trailer tractor, built to a scale of 1:12, has an incredible
range of radio-controlled functions, including windscreen wipers, all lights &
the horns.
84 Silicon Chip
the intensity with which he pursues
them. When he decides upon a course
of action it is carried out to the most
unbelievable levels of achievement
and excellence. The photo
g raphs
accompanying this article attempt to
show how diverse are his interests but
they don’t do full justice to the excellence of his workmanship and that is
a great pity for the final products are
a joy to behold.
Model railroads
Possibly his most abiding interest
is in model railroads. His home is a
stunning testimony to a lifetime of
non-stop mod
elling work. His HO
(1:87) scale layout, on which he has
been working for over 25 years (in
between other projects), occupies a
large building dedicated to this layout
alone. It is the only model railroad
layout I have seen which features an
electrical storm complete with a sequence of lightning, thunder and (get
this) torrential rain, over a section of
the track.
My close involvement with John
came about as a result of our mutual
interest in model and full size aviation.
Again, he never did things by halves
and John’s Airforce, as we jokingly
referred to it, featured over thirty
very elaborate R/C aircraft, mostly
true to scale and all built to a level of
excellence that would put most R/C
modellers to shame.
Our midweek flying sessions live
on in my memory as some of the most
interesting and enthusiastic periods in
my modelling career. The energy of
the man was infectious and all of us
in the group at that time worked like
demons, constantly competing to turn
out better and better models.
However, by the early 1980s business life was becoming very tough
and family and business commitments
pulled us apart once more. During this
time the airforce was retired and sold
off and John’s son developed into a
world class R/C car driver and thus
lured John into the international world
of competitive high performance R/C
cars.
Again, nothing was done by halves
and during this time John set up an
engineering section home workshop
that is enough to dumbfound even
the most blase modeller. Actually, I
have seen professional engineering
shops that were nowhere near as well
equipped as John’s playpen. They
certainly are not as neat, as well lit or
as well laid out.
The work that comes out of this
workshop is first class. Possibly my
favourite is his model of a semi-trailer,
complete with working everything!
Constructed totally from scratch from
aluminium stock and sheet, this model
really is a work of art. It is powered by
an O.S. 40 4-stroke engine and really
has to be seen to be believed.
Essentially, it is a model of a racing
car transporter, the trailer being fitted
with working model racing cars and
a workbench complete with a working model vice, a 44 gallon oil drum
with working pump and a contingent
of mechanics, drivers and various
tyre-kickers.
A close-up view of the 16-channel radio control transmitter built by Silvertone
for control of a racing model semi-trailer. It looks as though it might be easier to
drive the full size machine!
Racing truck cab
In his spare time as a lark, John
built a racing truck cab but the concept of model truck racing has never
really caught on. Shown in one of the
accompanying photos is the custom
16-channel Silvertone transmitter
which I built especially for the Semi
Trailer project. The channel logos
give some idea of the complexity of
the finished model: steering, forward
and reverse gear shift, throttle, brakes,
blinkers, horn, fog lights, high and
low beam headlights, parking lights,
hazard lights, windscreen wip
ers,
engine sound and one spare auxiliary
control.
I had to design and build a relay
switching unit which worked directly
from the receiver servo outputs for the
lighting circuits, the receiver being
a custom built Silvertone 16-channel AM unit. This racing truck was
demonstrated several times at model
gatherings but now holds pride of
place in a static collection of models
that range from HO scale tableaus,
through to R/C models of yachts,
This view of the racing model semi-trailer shows the cab tilted forward to reveal
some of the radio control gear.
The engine assembly of the model semi-trailer has a radiator & a belt-driven fan.
Note the servos at the rear for forward/reverse selection of the gear box.
August 1994 85
battleships, tanks, cars, trucks and
aircraft.
However, the piece de resistance
in his home modelling complex is
his garden layout. Here is a backyard
designed to give the maximum pleasure to John and his modelling friends.
The centrepiece of the layout is an
R/C car racing circuit with 1:22 scale
cars around which runs an LGB railroad layout.
Battery power
Radio controlled models coupled together with sound effects have a heightened
sense of realism. The R/C racing circuit has crowd sounds coming from the
pavilion & merry-go-round sounds from the fairground behind.
This general view of the layout shows the car racing track in the centre
surrounded by the LGB (1:32) scale railway layout. The locomotives are battery
powered & radio controlled.
LGB rolling stock is built to Scale 1
(1:32) and has a track gauge of 44.5mm.
The locomotives are battery powered
(essential for outdoor operation) and
operated by radio control, as are the
sound systems. The latter are housed
in enclosed wagons along with a fair
sized speaker to give good bass repro
duction. The sound system responds
to the locomotive speed and throttle
settings, and horns and whistles are
included.
The overall effect of the entire
layout is breathtaking when fully
powered up. I have never fully appreciated sound effects in models,
particularly model trains, but used
skilfully they add a new dimension
to modelling and to my mind they are
now a must in any good modelling
installation.
John uses sound effects in a way
that I have never encountered before.
They include the sound of a helicopter
warming up on the helipad, the roar of
the crowd in the stands, music from
the merry-go-round in the fairground,
the chuff of the steamer climbing an
incline and the burble of a diesel loco
waiting at the level crossing. All of
these effects add a sense of life and
drama to a model complex that is busy
in the extreme.
Future plans
A view inside on of the goods wagons coupled to a diesel locomotive. The wagon
contains the battery packs & radio controlled sound system.
86 Silicon Chip
John’s one complaint with his layout is that the points are manually
operated at the moment, so true to
form he has commissioned Silvertone
to design and build a 20-channel
R/C points control system. I hope to
present the details of this system in a
future column.
However, enough of my account.
The photographs presented tell the
story more effectively than any amount
of prose. Next month I will present
the story of John and his son and their
successes in the field of national and
SC
international R/C car racing.
PRODUCT SHOWCASE
Metex M-3850 digital multimeter
has PC interface
As well as all the
common features
you would normally
expect to find on a
current auto-ranging
digital multimeter,
this Metex M-3850 has
frequency, capacitance
& temperature
measurement, transistor
testing, dual display &
the ability to store data
for later analysis.
The M-3850 has a large back-lit dual
liquid crystal display. The main display is a 4000 count array with 15mm
high digits and it is supplemented with
a smaller 4000 count display in the top
right-hand corner. Small icons show
the current operating mode while a
bargraph provides analog indication
of the measurement. Press
ing the
function button scrolls through the
various modes.
The secondary display can be used
as a data hold facility, to keep account
of a measured maximum, minimum or
a value relative to a preset value, while
the main display shows the current
reading. In dual mode, it allows two
measurements to be displayed at once.
For instance, the primary display can
show a DC supply voltage while the
other displays the frequency of the
ripple on the supply, or the temperature can be displayed in Celsius on
the main display and Fahrenheit on
the secondary display.
As with most DMMs, there are separate terminals for the current ranges
which are used in conjunction with
the large rotary selector switch, the
milliamp terminal is used for current
measurements on the 40mA and
400mA ranges while the Amp terminal
is used for measurements up to 20A
(one range only). The meter can be set
to measure AC or DC using the DCW/
AC button.
For voltage measurements, the
CALLING ALL HOBBYISTS
We provide the challenge and money for you to design and build as many
simple, useful, economical and original kit sets as possible.
We will only consider kits using lots of ICs and transistors.
If you need assistance in getting samples and technical specifications while
building your kits, let us know.
YUGA ENTERPRISE
705 SIMS DRIVE #03-09
SHUN LI INDUSTRIAL COMPLEX
SINGAPORE 1438
TEL: 65 741 0300 Fax: 65 749 1048
August 1994 87
Hakko 926
soldering station
The Hakko 926 is a deluxe
soldering station builffor production work or for use by service
techni
cians and enthusiasts. It
has a 50 watt ceramic element
and a holding temperature accuracy of ±0.5C. Tip temperature
can be varied from 200-480°C.
The iron is well balanced and has
a rubberised grip, while the cord is
burn-proof silicone and has strain
relief at both ends. The 5-pin connector has a locking ring to prevent
accidental disconnection.
The station has a heavy base and
is fully electronically controlled
via the temperature knob on the
front panel. A LED indicates that
the iron is heating. The stainless
steel sponge tray is removable and
has an excess solder tray that overhangs for easy solder collection.
The unit comes with a 3-pin plug
and the tip is grounded for ESD
protection. A 1.6mm conical tip is
K
ALEX
The UV People
ETCH TANKS
● Bubble Etch ● Circulating
LIGHT BOXES
● Portuvee 4 ● Portuvee 6
● Dual Level
TRIMMER
● Ideal
PCB DRILL
● Toyo HiSpeed
MATERIALS
● PC Board: Riston, Dynachem
● 3M Label/Panel Stock
● Dynamark: Metal, Plastic
✸ AUSTRALIA’S NO.1 STOCKIST ✸
K
ALEX
40 Wallis Ave, East Ivanhoe 3079.
Phone (03) 9497 3422, Fax (03) 9499 2381
88 Silicon Chip
supplied but many other styles are
available. The manual is comprehensive and states the specification
and calibration adjustments for all
possible tips. A “CAL” trimpot on
the base of the unit is used for this
purpose.
The holster has been designed to
be placed on either side of the station for ease of use and is angled by
loosening off the adjustment screw.
The Hakko 926 soldering station
sells for $259 and is available from
all Dick Smith Electronics stores
and resellers.
ranges run in the following sequence:
400mV, 4V, 40V, 400V and a maximum
of 1000V DC or 750VAC. The meter is
fully autoranging but has the facility
to lock onto a single range when needed. This is done by selecting the R-H
(Range Hold) mode and then stepping
through the ranges using the Up or
Down button.
When it comes to measuring frequency, the Metex M-3850 really
shines. Most DMMs that measure frequency are hard put to measure up to
1MHz but this unit can go to 40MHz.
Input sensitivity is quoted as better
than 100mV RMS for frequencies up to
30MHz to over 300mV for frequencies
above 30MHz. It has good capacitance
ranges too: 4nF, 40nF, 400nF, 4µF, 40µF
and 400µF (1nF = .001µF).
The resistance ranges run as follows: 400W, 4kW, 40kW, 400kW, 4MW
and 40MW. The meter provides an
audible continuity alarm for resistances below 30W and the diode test
range will light most LEDs. Maximum
open circuit voltage for the diode test
is 2.5V.
Another good feature of the Metex is
the auto-off switch. It turns the meter
off if none of the pushbuttons or the
selector switch has been touched for
10 minutes. Without this feature, most
DMMs become battery eaters and that
becomes frustrating when the battery
dies just as you are about to take a
crucial measurement.
For transistor hFE measurements,
the maximum reading is 4000 which
will allow the Metex to measure many
Darlington transistors. However, the
instruction manual warns that some
Darlingtons have internal resistors
(between base and emitter) and these
can give rise to misleading results.
An interesting mode is the ‘Comparison’ function. The icon ‘CMP’
appears on the display and the meter
uses two memo·ries as high.and low
to test the current reading against and
displays ‘Hi’, ‘Low’ or ‘Pass’ depending on the value. All told, the Metex
has 10 memories for storing data and
these can be stepped through using
the Function button.
Datalogging
Where the Metex is outstanding is
in its ability to be transformed into a
datalogger. It can be connected to a PC
or compatible with an optional serial
interface which is accompanied with
software. This enables measurements
to be stored away with time stamping.
Values can be graphed either in real
time or replayed later.
The software is mouse driven and
has pull-down menus. Two serial
ports are therefore needed to get the
software running, one for the mouse
and another for the meter. Collected
data can be viewed in three modes: a
line graph that autoranges its Y axis
(as the meter does); a time-stamped
history of collected values; and a
large mimicked display of the meter
itself. Collected values are stored in
ASCII files that can be replayed by the
software or loaded into other software
for further analysis.
All told, the Metex M-3850 digital
multimeter is an attractive package
with lots of features. It is supplied in
a vinyl case with separate sections to
store the meter and test leads. Recommended retail price is $229.50 while
the computer interface and software
is a further $18.95. Other options in
clude a rubber holster and an external
temperature probe.
For more information on the Metex
M-3850, contact your local Jaycar
Elec
tronics store or reseller. Phone
(02) 743 5222.
Celestion SRA series
power amplifiers
Celestion’s new SRA series
power amplifiers feature the
com
pany’s dual rail soft-switch
output stage, employing linear,
outputderived class G amplification. The soft-switch design means
that the switch to the upper rail is
inaudible. It provides the advantages of dual rail operation, with
a big increase in efficiency and a
corre
sponding reduction in the
genera
tion of heat, without the
distortion generated by fast-attack
rail switching.
Built to survive the rigours of
touring, all SRA series amplifiers
feature a heavy-gauge steel chassis
coupled to a transverse heatsink
to add rigidity. A continuously
variable cooling fan temperature
con
trolled from the heatsink is
another feature.
Heavy duty output relays are
employed to protect the loudspeaker load and a logic-con-
trolled power-up sequence enables the outputs only when the
amplifier has settled. Outputs are
continuously monitored and are
disabled in the event of operation
outside specified tolerances. Output protection status is provided
on the front panel.
All operational controls, the
fan, filter and tamper-proof bridging and ground lift switches are
accessible from the front panel,
without the need to remove the
amplifier from its rack. The rear
panel has provision for a variety of
New range of low-cost
snap-fitting cases
This new line
of polys tyrol
cases all have
moulded pillars
for mounting
PC boards The
larger cases all
have ventilation slots and
separate plastic front and
rear panels
Sizes available
are 207 x 68 x 179mm, 151 x 58 x 139mm and 94 x 47 x
134mm (W x H x D).
The smaller cases in the range do not have separate
front and rear panels but have moulded slots, as well as
pillars for PC board mounting. There are two different
sized case halves and these may be mixed and matched
to build cases of three different heights. The half case
sizes are 71 x 24 x 123mm and 71 x 15 x 123mm (W x
H x D).
A baby case is also available but is not snap-fitting and is
sized 70 x 47 x 40mm. All cases are available in black and
a grey-white.
For more information on these cases, contact Anton’s
Trains, Cnr Prince & Mary St, North Parramatta, NSW 2151.
Phone (02) 683 3858.
mating connectors, including parallel
latching XLRs for daisy-chaining,
heavy duty binding posts and Neutrik
Speakon connectors.
Presently, two SRA models are
available: (1) the SRA1000 with 510
watts into 4-ohms or 1020 watts
bridged into 8-ohms; and (2) the
SRA1600 with 815 watts into 4-ohms
or 1620 watts bridged into 8-ohms.
For further information contact
Amber Technology Pty Ltd, Unit B, 5
Skyline Place, Frenchs Forest, NSW
2086. Phone (02) 975 1211 or fax (02)
975 1368.
PC COMPUTERS (08) 364 0902 (08) 332 6513
36 Regent St, Kensington, South Australia
High Power 2.5 Watt Transmitter Kit FMTX1
$69
This kit uses a single transistor to provide up to 2.5 watts into a 50-ohm load. It can be
set on the FM band from 88-108MHz. Audio is 500mV P-P with Australian pre-emphasis.
Power supply from 12-24 volts DC. Range up to 100 miles. Leaky coax distribution can
be used with any of our transmitters, terminate up to 2km of coax with a 50-ohm resistor
and no radiation occurs. Use a 150-ohm WW pot and you can set the level of radiation up
to 300 metres from the coax. You can use this method to comply with DOTC schedule 3.
XTAL Locked 30mW Transmitter (The best quality kit transmitter
in Australia) FMTX2B
$49
This transmitter is XTAL-locked on 100MHz (XTAL supplied) and is the most stable kit
transmitter on the market. It features a 3-stage design with only two tuned circuits and
a clean output. This design can be used as the basis of a station exciter.
Digital Stereo Coder (All Digital Design With Australian
Pre-emphasis) FMTX2A
$49
This is a universal stereo coder able to be used with all of our transmitter designs and
many others. Its performance is superior to domestic encoder single chip designs.
Dozens have been sold to FM stations as a standby stereo coder or with the FMTX2B
as an exciter.
Both FMTX2A and FMTX2B on 1 PCB as a complete stereo transmitter FMTX5
$99
MAX I/O Board for PCs (Talk To The Outside World)
$169
This kit features 7 relays, ADC, DAC, stepper motor driver with sample software in
Basic and connects to a PC’s parallel port. Now also available I/O bits software for
MS Windows so you can program functions without being a programmer. Call relays
by a name like stop relay, assign its own icon - uses a simple VISUAL interface to
make your own PLC. Full developer’s version has DOS runtime so you do not require
Windows and optional support for LCD displays. Data logging ADC and DAC boards
and more. MAX version $169.
FM Band Linear Amplifier Kits (All Imported Kits)
New 30mW to 1 watt linear coming in September 1994 (advance orders taken)
500mW to 5 or 10 watts
$199
250mW to 25 watts
15 watts to 110 watts
$599
40 watts to 300 watts
Power supplies and heatsinks not included in short form kit price.
$99
$249
$999
Other kits available. Call for a list or see Silicon Chip April-June 1994 or the
Silicon Chip Model Railway Book.
August 1994 89
Silicon Chip
Mixing Desk, Pt.2; Using The UC3906 SLA Battery
Charger IC.
April 1990: Dual Tracking ±50V Power Supply; VOX
With Delayed Audio; Relative Field Strength Meter;
16-Channel Mixing Desk, Pt.3; Active CW Filter For
Weak Signal Reception; How To Find Vintage Radio
Receivers From The 1920s.
BACK ISSUES
September 1988: Hands-Free Speakerphone;
Electronic Fish Bite Detector; High Performance
AC Millivoltmeter, Pt.2; Build The Vader Voice;
Motorola MC34018 Speakerphone IC Data; What
Is Negative Feedback, Pt.4.
November 1988: 120W PA Amplifier Module
(Uses Mosfets); Poor Man’s Plasma Display;
Automotive Night Safety Light; Adding A Headset
To The Speakerphone.
April 1989: Auxiliary Brake Light Flasher; What
You Need to Know About Capacitors; 32-Band
Graphic Equaliser, Pt.2; LED Message Board,
Pt.2.
May 1989: Build A Synthesised Tom-Tom;
Biofeedback Monitor For Your PC; Simple Stub
Filter For Suppressing TV Interference; LED
Message Board, Pt.3; All About Electrolytic Cap
acitors.
Encoder; Studio Series 20-Band Stereo Equaliser,
Pt.2; Auto-Zero Module for Audio Amplifiers (Uses
LMC669).
October 1989: FM Radio Intercom For Motorbikes
Pt.1; GaAsFet Preamplifier For Amateur TV; 1Mb
Printer Buffer; 2-Chip Portable AM Stereo Radio,
Pt.2; Installing A Hard Disc In The PC.
November 1989: Radfax Decoder For Your PC
(Displays Fax, RTTY & Morse); FM Radio Intercom
For Motorbikes, Pt.2; 2-Chip Portable AM Stereo
Radio, Pt.3; Floppy Disc Drive Formats & Options;
The Pilbara Iron Ore Railways.
December 1989: Digital Voice Board (Records
Up To Four Separate Messages); UHF Remote
Switch; Balanced Input & Output Stages; Data For
The LM831 Low Voltage Amplifier IC; Installing A
Clock Card In Your Computer; Index to Volume 2.
June 1989: Touch-Lamp Dimmer (uses Siemens
SLB0586); Passive Loop Antenna For AM Radios;
Universal Temperature Controller; Understanding
CRO Probes; LED Message Board, Pt.4.
January 1990: High Quality Sine/Square
Oscillator; Service Tips For Your VCR; Speeding
Up Your PC; Phone Patch For Radio Amateurs;
Active Antenna Kit; Speed Controller For Ceiling
Fans; Designing UHF Transmitter Stages.
July 1989: Exhaust Gas Monitor (Uses TGS812
Gas Sensor); Extension For The Touch-Lamp
Dimmer; Experimental Mains Hum Sniffers;
Compact Ultrasonic Car Alarm.
February 1990: 16-Channel Mixing Desk; High
Quality Audio Oscillator, Pt.2; The Incredible Hot
Canaries; Random Wire Antenna Tuner For 6
Metres; Phone Patch For Radio Amateurs, Pt.2.
September 1989: 2-Chip Portable AM Stereo
Radio (Uses MC13024 and TX7376P) Pt.1;
High Or Low Fluid Level Detector; Simple DTMF
March 1990: 6/12V Charger For Sealed Lead-Acid
Batteries; Delay Unit For Automatic Antennas;
Workout Timer For Aerobics Classes; 16-Channel
June 1990: Multi-Sector Home Burglar Alarm;
Low-Noise Universal Stereo Preamplifier; Load
Protection Switch For Power Supplies; A Speed
Alarm For Your Car; Design Factors For Model
Aircraft; Fitting A Fax Card To A Computer.
July 1990: Digital Sine/Square Generator, Pt.1
(Covers 0-500kHz); Burglar Alarm Keypad &
Combination Lock; Simple Electronic Die; Low-Cost
Dual Power Supply; Inside A Coal Burning Power
Station; Weather Fax Frequencies.
August 1990: High Stability UHF Remote
Transmitter; Universal Safety Timer For Mains
Appliances (9 Minutes); Horace The Electronic
Cricket; Digital Sine/Square Wave Generator, Pt.2.
September 1990: Music On Hold For Your Tele
phone; Remote Control Extender For VCRs; Power
Supply For Burglar Alarms; Low-Cost 3-Digit
Counter Module; Simple Shortwave Converter For
The 2-Metre Band.
October 1990: Low-Cost Siren For Burglar Alarms;
Dimming Controls For The Discolight; Surfsound
Simulator; DC Offset For DMMs; The Dangers of
Polychlorinated Biphenyls; Using The NE602 In
Home-Brew Converter Circuits.
November 1990: How To Connect Two TV Sets To
One VCR; A Really Snazzy Egg Timer; Low-Cost
Model Train Controller; Battery Powered Laser
Pointer; 1.5V To 9V DC Converter; Introduction
To Digital Electronics; Simple 6-Metre Amateur
Transmitter.
December 1990: DC-DC Converter For Car
Amplifiers; The Big Escape – A Game Of Skill;
Wiper Pulser For Rear Windows; Versatile 4-Digit
Combination Lock; 5W Power Amplifier For The
ORDER FORM
Please send me a back issue for:
❏ September 1988
❏ November 1988
❏ April 1989
❏ May 1989
❏ June 1989
❏ July 1989
❏ September 1989
❏ October 1989
❏ November 1989
❏ December 1989
❏ January 1990
❏ February 1990
❏ March 1990
❏ April 1990
❏ June 1990
❏ July 1990
❏ August 1990
❏ September 1990
❏ October 1990
❏ November 1990
❏ December 1990
❏ January 1991
❏ February 1991
❏ March 1991
❏ April 1991
❏ May 1991
❏ June 1991
❏ July 1991
❏ August 1991
❏ September 1991
❏ October 1991
❏ November 1991
❏ December 1991
❏ January 1992
❏ February 1992
❏ March 1992
❏ April 1992
❏ May 1992
❏ June 1992
❏ July 1992
❏ August 1992
❏ September 1992
❏ October 1992
❏ January 1993
❏ February 1993
❏ March 1993
❏ April 1993
❏ May 1993
❏ June 1993
❏ July 1993
❏ August 1993
❏ September 1993
❏ October 1993
❏ November 1993
❏ December 1993
❏ January 1994
❏ February 1994
❏ March 1994
❏ April 1994
❏ May 1994
❏ June 1994
❏ July 1994
❏ August 1994
❏ September 1994
❏ October 1994
Enclosed is my cheque/money order for $______or please debit my: ❏ Bankcard ❏ Visa Card ❏ Master Card
Card No.
Signature ____________________________ Card expiry date_____ /______
Name _______________________________ Phone No (___) ____________
PLEASE PRINT
Street ________________________________________________________
Suburb/town ________________________________ Postcode ___________
90 Silicon Chip
Note: all prices include post & packing
Australia (by return mail) ............................. $A7
NZ & PNG (airmail) ...................................... $A7
Overseas (airmail) ...................................... $A10
Detach and mail to:
Silicon Chip Publications, PO Box 139,
Collaroy, NSW, Australia 2097.
Or call (02) 979 5644 & quote your credit card
details or fax the details to (02) 979 6503.
✂
v
6-Metre Amateur Transmitter; Index To Volume 3.
January 1991: Fast Charger For Nicad Batteries,
Pt.1; Have Fun With The Fruit Machine; Two-Tone
Alarm Module; LCD Readout For The Capacitance
Meter; How Quartz Crystals Work; The Dangers
When Servicing Microwave Ovens.
February 1991: Synthesised Stereo AM Tuner,
Pt.1; Three Inverters For Fluorescent Lights; LowCost Sinewave Oscillator; Fast Charger For Nicad
Batteries, Pt.2; How To Design Amplifier Output
Stages; Tasmania's Hydroelectric Power System.
March 1991: Remote Controller For Garage Doors,
Pt.1; Transistor Beta Tester Mk.2; Synthesised AM
Stereo Tuner, Pt.2; Multi-Purpose I/O Board For PCCompatibles; Universal Wideband RF Preamplifier
For Amateurs & TV.
April 1991: Steam Sound Simulator For Model
Railroads; Remote Controller For Garage Doors,
Pt.2; Simple 12/24V Light Chaser; Synthesised
AM Stereo Tuner, Pt.3; A Practical Approach To
Amplifier Design, Pt.2.
May 1991: 13.5V 25A Power Supply For
Transceivers; Stereo Audio Expander; Fluorescent
Light Simulator For Model Railways; How To Install
Multiple TV Outlets, Pt.1.
June 1991: A Corner Reflector Antenna For UHF
TV; 4-Channel Lighting Desk, Pt.1; 13.5V 25A
Power Supply For Transceivers; Active Filter For CW
Reception; Tuning In To Satellite TV, Pt.1.
July 1991: Battery Discharge Pacer For Electric
Vehicles; Loudspeaker Protector For Stereo
Amplifiers; 4-Channel Lighting Desk, Pt.2; How
To Install Multiple TV Outlets, Pt.2; Tuning In To
Satellite TV, Pt.2.
August 1991: Build A Digital Tachometer;
Masthead Amplifier For TV & FM; PC Voice
Recorder; Tuning In To Satellite TV, Pt.3; Step-ByStep Vintage Radio Repairs.
September 1991: Studio 3-55L 3-Way Loudspeaker
System; Digital Altimeter For Gliders & Ultralights,
Pt.1; Build A Fax/Modem For Your Computer; The
Basics Of A/D & D/A Conversion; Windows 3
Swapfiles, Program Groups & Icons.
October 1991: Build A Talking Voltmeter For Your
PC, Pt.1; SteamSound Simulator Mk.II; Magnetic
Field Strength Meter; Digital Altimeter For Gliders
& Ultralights, Pt.2.
November 1991: Colour TV Pattern Generator,
Pt.1; Battery Charger For Solar Panels; Flashing
Alarm Light For Cars; Digital Altimeter For Gliders
& Ultralights, Pt.3; Build A Talking Voltmeter For
Your PC, Pt.2; Modifying The Windows INI Files.
December 1991: TV Transmitter For VCRs With
UHF Modulators; Infrared Light Beam Relay; SolidState Laser Pointer; Colour TV Pattern Generator,
Pt.2; Index To Volume 4.
January 1992: 4-Channel Guitar Mixer; Adjustable
0-45V 8A Power Supply, Pt.1; Baby Room Monitor/
FM Transmitter; Automatic Controller For Car
Headlights; Experiments For Your Games Card;
Restoring An AWA Radiolette Receiver.
February 1992: Compact Digital Voice Recorder;
50-Watt/Channel Stereo Power Amplifier ;
12VDC/240VAC 40-Watt Inverter; Adjustable
0-45V 8A Power Supply, Pt.2; Designing A Speed
Controller For Electric Models.
March 1992: TV Transmitter For VHF VCRs; Studio
Twin Fifty Stereo Amplifier, Pt.1; Thermostatic
Switch For Car Radiator Fans; Telephone Call
Timer; Coping With Damaged Computer Direct
ories; Valve Substitution In Vintage Radios.
April 1992: Infrared Remote Control For Model
Railroads; Differential Input Buffer For CROs; Studio
Twin Fifty Stereo Amplifier, Pt.2; Understanding
Computer Memory; Aligning Vintage Radio
Receivers, Pt.1.
May 1992: Build A Telephone Intercom; LowCost Electronic Doorbell; Battery Eliminator For
Personal Players; Infrared Remote Control For
Model Railroads, Pt.2; Aligning Vintage Radio
Receivers, Pt.2.
June 1992: Multi-Station Headset Intercom, Pt.1;
Video Switcher For Camcorders & VCRs; Infrared
Remote Control For Model Railroads, Pt.3; 15-Watt
12-240V Inverter; A Look At Hard Disc Drives.
July 1992: Build A Nicad Battery Discharger;
8-Station Automatic Sprinkler Timer; Portable
12V SLA Battery Charger; Multi-Station Headset
Intercom, Pt.2; Electronics Workbench For Home
Or Laboratory.
August 1992: Build An Automatic SLA Battery
Charger; Miniature 1.5V To 9V DC Converter;
Dummy Load Box For Large Audio Amplifiers;
Internal Combustion Engines For Model Aircraft;
Troubleshooting Vintage Radio Receivers.
September 1992: Multi-Sector Home Burglar
Alarm; Heavy-Duty 5A Drill speed Controller (see
errata Nov. 1992); General-Purpose 3½-Digit LCD
Panel Meter; Track Tester For Model Railroads; Build
A Relative Field Strength Meter.
October 1992: 2kW 24VDC To 240VAC Sinewave
Inverter; Multi-Sector Home Burglar Alarm, Pt.2;
Mini Amplifier For Personal Stereos; Electronically
Regulated Lead-Acid Battery Charger.
January 1993: Peerless PSK60/2 2-Way Hifi
Loudspeakers; Flea-Power AM Radio Transmitter;
High Intensity LED Flasher For Bicycles; 2kW
24VDC To 240VAC Sinewave Inverter, Pt.4; Speed
Controller For Electric Models, Pt.3.
February 1993: Three Simple Projects For
Model Railroads; A Low Fuel Indicator For Cars;
Audio Level/VU Meter With LED Readout; Build
An Electronic Cockroach; MAL-4 Microcontroller
Board, Pt.3; 2kW 24VDC To 240VAC Sine
wave
Inverter, Pt.5; Making File Backups With LHA &
PKZIP.
September 1993: Automatic Nicad Battery
Charger/Discharger; Stereo Preamplifier With IR
Remote Control, Pt.1; In-Circuit Transistor Tester;
A +5V to ±15V DC Converter; Remote-Controlled
Cockroach Servicing An R/C Transmitter, Pt.1.
October 1993: Courtesy Light Switch-Off Timer
For Cars; Wireless Microphone For Musicians;
Stereo Preamplifier With IR Remote Control, Pt.2;
Electronic Engine Management, Pt.1; Programming
The Motorola 68HC705C8 Microcontroller – Lesson
2; Servicing An R/C Transmitter, Pt.2.
November 1993: Jumbo Digital Clock; High
Efficiency Inverter For Fluorescent Tubes; Stereo
Preamplifier With IR Remote Control, Pt.3; Siren
Sound Generator; Electronic Engine Management,
Pt.2; More Experiments For Your Games Card.
December 1993: Remote Controller For Garage
Doors; Low-Voltage LED Stroboscope; LowCost 25W Amplifier Module; Peripherals For The
Southern Cross Computer; Build A 1-Chip Melody
Generator; Electronic Engine Management, Pt.3;
Index To Volume 6.
January 1994: 3A 40V Adjustable Power Supply;
Switching Regulator For Solar Panels; Printer
Status Indicator; Mini Drill Speed Controller;
Stepper Motor Controller; Active Filter Design For
Beginners; Electronic Engine Management, Pt.4.
February 1994: 90-Second Message Recorder;
Compact & Efficient 12-240VAC 200W Inverter;
Single Chip 0.5W Audio Amplifier; 3A 40V
Adjustable Power Supply; Electronic Engine
Management, Pt.5; Airbags: More Than Just Bags
Of Wind; Building A Simple 1-Valve Radio Receiver.
March 1994: Intelligent IR Remote Controller; Build
A 50W Audio Amplifier Module; Level Crossing
Detector For Model Railways; Voice Activated
Switch For FM Microphones; Simple LED Chaser;
Electronic Engine Management, Pt.6; Switching
Regulators Made Simple (Software Offer).
April 1994: Remote Control Extender For VCRs;
Sound & Lights For Model Railway Level Crossings;
Discrete Dual Supply Voltage Regulator; Low-Noise
Universal Stereo Preamplifier; Build A Digital Water
Tank Gauge; Electronic Engine Management, Pt.7.
March 1993: Build A Solar Charger For 12V
Batteries; An Alarm-Triggered Security Camera;
Low-Cost Audio Mixer for Camcorders; Test Yourself
On The Reaction Trainer; A 24-Hour Sidereal Clock
For Astronomers.
May 1994: Fast Charger For Nicad Batteries;
Induction Balance Metal Locator; Multi-Channel
Infrared Remote Control; Dual Electronic Dice; Two
Simple Servo Driver Circuits; Electronic Engine
Management, Pt.8; Passive Rebroadcasting For
TV Signals.
April 1993: Solar-Powered Electric Fence; Build An
Audio Power Meter; Three-Function Home Weather
Station; 12VDC To 70VDC Step-Up Voltage
Converter; Digital Clock With Battery Back-Up; A
Look At The Digital Compact Cassette.
June 1994: 200W/350W Mosfet Amplifier Module; A
Coolant Level Alarm For Your Car; An 80-Metre AM/
CW Transmitter For Amateurs; Converting Phono
Inputs To Line Inputs; A PC-Based Nicad Battery
Monitor; Electronic Engine Management, Pt.9
May 1993: Nicad Cell Discharger; Build The Woofer
Stopper; Remote Volume Control For Hifi Systems,
Pt.1; Alphanumeric LCD Demonstration Board;
Low-Cost Mini Gas Laser; The Microsoft Windows
Sound System.
July 1994: SmallTalk – a Tiny Voice Digitiser For
The PC; Build A 4-Bay Bow-Tie UHF Antenna;
PreChamp 2-Transistor Preamplifier; Steam Train
Whistle & Diesel Horn Simulator; Portable 6V SLA
Battery Charger; Electronic Engine Management,
Pt.10.
June 1993: Windows-Based Digital Logic Analyser,
Pt.1; Build An AM Radio Trainer, Pt.1; Remote
Control For The Woofer Stopper; A Digital Voltmeter
For Your Car; Remote Volume Control For Hifi
Systems, Pt.2
July 1993: Build a Single Chip Message Recorder;
Light Beam Relay Extender; AM Radio Trainer, Pt.2;
Windows Based Digital Logic Analyser; Pt.2; Quiz
Game Adjudicator; Programming The Motorola
68HC705C8 Microcontroller – Lesson 1; Antenna
Tuners – Why They Are Useful.
August 1993: Low-Cost Colour Video Fader; 60LED Brake Light Array; A Microprocessor-Based
Sidereal Clock; The Southern Cross Z80-based
Computer; A Look At Satellites & Their Orbits.
Au g u s t 1 9 9 4 : H i g h - Powe r D i m m e r Fo r
Incandescent Lights; Dual Diversity Tuner For FM
Microphones, Pt.1; Build a Nicad Zapper; Simple
Crystal Checker; Electronic Engine Management,
Pt.11; Philips’ Widescreen TV Set Reviewed.
PLEASE NOTE: all issues from November 1987 to
August 1988, plus October 1988, December 1988,
January, February, March & August 1989, May
1990, and November and December 1992 are now
sold out. All other issues are presently in stock. For
readers wanting articles from sold-out issues, we
can supply photostat copies (or tearsheets) at $7.00
per article (incl. p&p). When supplying photostat
articles or back copies, we automatically supply any
relevant notes & errata at no extra charge.
August 1994 91
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. Write to: Ask Silicon Chip, PO Box 139, Collaroy Beach, NSW 2097.
Multiple coil version
of transistor ignition
I would like to suggest a redesign
of your Transistor Assisted Ignition as
described in the May and June 1988
issues of the magazine. It has occurred
to me that it would be possible to fit
multiple ignition coils, connected
directly to each spark plug, thereby
effectively bypassing the distributor,
with its inherent losses through carbon
tracking, moisture, rotor to plug lead
contact, etc. Fully electronic systems
such as on the Commodore utilise a
sensor to detect crankshaft angle and
deter
mine the firing point for each
cylinder.
My proposal is to use the existing
distributor for this purpose, which
would no longer be a “distributor”
as such, but more of a rotary switch.
Using four opto or Hall-Effect sensors
(for a 4-cylinder vehicle) within the
distributor, these would ultimately
trigger, in correct order, the appropriate coil for each spark plug. I accept
there may be difficulties in fitting
sensors for 6 or 8-cylinder vehicles
but I am aware that some opto sensors
are quite small and some 8-cylinder
distributors quite large, so I believe
it would be possible. Also, the cost
of multiple coils at around $35 each
1.5V to 9V converter
needs shielding
I recently built one of your 1.5V
to 9V converters, as described in
the August 1992 issue of SILICON
CHIP. It works pretty well, giving
about 8.7V at no load and holding
up quite well up to a load current
of 36mA, at which point the voltage is 8V.
With fingers firmly crossed, I
tried it out on a small radio (Tandy
Realistic 12-719). Much to my surprise, it worked well on FM, with
no interference that I could hear.
92 Silicon Chip
may be a problem but still comparable
or even cheaper in some cases than a
fully electronic system, without the
need to also fit a crankshaft sensor,
with whatever mechanical difficulties
that may present with some vehicles.
I hope you can envisage the advantages of retrofitting a fully electronic
“distributor-less” system to an older
vehicle, and at first glance it would
seen simple and ideal if the exist
ing distributor can be used as the
“crankshaft position” sensor, thereby
avoiding the losses involved in routing the high tension current by this
means, also allowing full coil current
to reach the plugs by close positioning and short leads with regard to the
ignition coils.
Vacuum and centrifugal advance of
the ignition could still be preserved as
with present electronic trigger modifications to points type distributors.
Additionally, each coil would be
operating at only a fraction of normal
requirements, extending its operating
life due to cooler running, with the
added advantage of a much greater
period between firings, allowing each
coil a much longer period to build up
current before it is required.
One other question if I may. I have a
fuel flow sensor, impeller type, specification 22Hz <at> 10 litres/hr. I also have
AM, however, was a completely
different kettle of fish, with a lot of
whistling background noise.
This doesn’t worry me too much,
since I usually listen to FM anyway,
but it would be handy to be able
to hear AM occasionally without
being tortured. Could you suggest
a simple RC filter that would do the
trick? (J. K., Kenmore, Qld).
• It is possible to minimise hash
by installing the device in an
earthed metal box and also keeping the ferrite rod of the radio
as far away as possible from the
converter.
a LED display module which counts
up by 1, with a negative pulse to the
input. I intend testing it to find the
number of pulses per litre flowed, then
to use a counter/divider to convert to
one pulse per litre to trigger the LED
counter to count up by 1. Have you
published a suitable counter/divider
interface which I could use for this
purpose? (P. C., Dundas, NSW).
• You are proposing a very expensive conversion. You would need a
complete transistor assisted ignition
circuit, including the MC3334P chip,
to drive each ignition coil.
Actually, with a “dwell-extended”
design such as our transistor assisted
ignition, the coil is conducting for
virtually all of the time so that its
dissipation is more or less constant,
regardless of the spark rate. Thus,
the coils would not run cooler. This
brings us to a real problem with your
proposed multi-coil system and that
is the total current drain.
Typically, the current drain in a
“dwell extended” system is much
higher than in a Kettering system with
the dwell set by the points. For a single coil, the current can be expected
to be around four or five amps and so
for a 6-coil system the current would
be around 30 amps. This is too much
for the typical car alternator to handle
when the headlights are on – the current drain would simply be too much.
Lastly, while the distributor may
seem like a clumsy mechanical device,
it is actually a very efficient high voltage switch and the losses are of little
importance in a transistor assisted
ignition system.
That is why the vast majority of
cars, one exception being the Holden
Commodore, use a distributor. In fact,
it is a paradox that the Holden Commodore has gone to the refinement of a
multi-coil ignition system when its V6
engine is such a harsh running beast
– a legacy of its 90° angle between the
cylinder banks.
We published a 3-digit counter in
the September 1990 issue. This may
be suitable for your fuel flow sensor.
Using Polyswitches for
loudspeaker protection
I wanted to build the 50W audio
amplifier published on the March 1994
issue and I figured the 2-way bookshelf
speakers published in January 1993
issue would be an excellent match.
I would like to protect the speakers
using Polyswitch protectors but the
thing is, how would I connect the
Polyswitches on the crossovers and
what sort of Polyswitches do I need?
I also want to know what kind of
Polyswitches would suit a “Nippon
America” 10-inch 100W RMS sub
woofer with an impedance of 4Ω?
I would like to run it with the 50W
amplifier. One last question: can Polyswitches be connected in parallel to
double their maximum current rating?
(M. C., Yarraville, Vic).
• We featured Polyswitches in the
50W and 100W amplifier designs
published in the December 1988 issue
of SILICON CHIP. Suitable devices are
stocked by Jaycar Electronics. You
can insert them individually in series
with the tweeter and woofer or just
have one to protect each system. For
the latter approach, we would suggest
the Cat. RN-3415 from Jaycar. These
could also be used to protect your 10inch speakers.
You cannot connect Polyswitches
in parallel as they will not share the
current equally.
Another vote for a signal strength meter
In reference to the letter from B. P.,
of Port Macquarie, in the April 1994
issue, I too would be blessed if you
would design a signal strength meter
and present it as a project. As he states,
commercial units are expensive and
no doubt this is due to their flexibility
and accuracy; a design based around
a tuner/front end from a VCR should
be just as good.
I have included with my letter the
circuit of a tuner/front end which is
made by Sanyo and are easy to come
by secondhand – most of their Beta
machines are fitted with them. The
beauty of this unit is that it only requires +12V for the supply and 0-12V
to tune across the entire band. Band
switching is achieved by taking one of
three lines high as required.
This makes it an ideal choice for
a portable unit as it can then be
Notes & Errata
Microprocessor-Controlled Nicad
Battery Charger, September 1993: a
number of errors have come to light
in the circuit on page 17. Pin 6 of
IC2 should be labelled pin 1 in Fig.1
and the 330Ω resistor associated
with Q3 should be in series with the
emitter resistor. VRI and the 30kΩ
resistor are reversed compared with
the PC board layout on page 20. The
lower of the two series resistors to
earth from pin 9 of IC1 should be
2.2kΩ. Finally, the 100µF capacitor
at the output of the 5V regulator is
shown with incorrect polarity on
the wiring diagram on page 20 and
the 12V relay has been omitted from
the parts list.
4-Bay Bow Tie UHF Antenna, July
1994: readers in eastern states who
are having difficulty purchasing
4.74mm dia, 0.91mm wall thickness
aluminium tube for this project
should note that it can be purchased
from the Alcan Aluminium Centre,
Lidcombe, NSW (Phone 02 647
9900) or ordered from them through
their local Alcan Centre. Readers
in other states may also do this but
they will have to pay freight from
Sydney to their location.
The reflectors and dipoles may
be made from thicker tubing or rod;
eg, 6.35mm diameter with suitable
adjustment being made to the dipole
mounting clip dimensions. The
reflector, dipoles and the connector
harness pieces could also be made
powered by eight 1.5V cells or a 12V
sealed lead acid battery. In designing
the meter, the following should be
taken into account: (1) It needs to
be able to detect and display signal
strength from 1µV up to 2-3V (via a
switched attenuator); (2) It should
have a large, easy to read display,
either a moving-coil meter or a digital
readout (if not both); (3) It should be
easy to calibrate without the use of
expensive test equipment and have
optional outputs at the rear for IF (to
use the meter as a substitute tuner)
and Video/Audio to feed to a monitor
for picture quality evaluation.
Judging by the comments I have
had from others, a project like this
would be extremely popular, as most
from 4.74mm dia aluminium rod.
For the harness pieces this material
will need heating and hammering
on an anvil in the areas where holes
have to be drilled. The connector
pieces could also be made from
3.2mm aluminium rod which is
readily available from CIG welding
centres.
Discrete Dual Supply Voltage Regulator; April 1994: the PC board
pattern and the overlay pattern
featured on page 31 has an error in
that pin 3 of IC1b is not grounded.
The board can be corrected by connecting a short link across to the
adjacent GND track.
Fast Charger for Nicad Batteries,
May 1994: this circuit has caused
confusion to many constructors
because of its method of dV sensing
to end the fast charging mode; it
will not work unless it is actually
charging cells. If you attempt to test
the circuit without a nicad battery
load, the output voltage will rise until pin 7 reaches +4.25V whereupon
the circuit will switch off.
For further background on this
circuit, refer to the article on using
the TEA1100 IC on page 6 of this
issue.
Dual Diversity FM Tuner, August
1994: the varicap diode D5 is
shown on the circuit the wrong way
around. It is shown correctly on
the wiring diagram of this month’s
issue, on page 68.
commercial units start around $1500.
There have been other designs presented before but in general they
were uncalibrated or involved lengthy
construction. (S. W., Hamilton, NZ).
• The problem with designing such an
instrument is not so much the tuner
front end but that of calibration. Without calibration, such instruments are
fairly useless. Tuners do not respond
equally over their band and therefore
it is necessary to produce a calibration
curve for each individual instrument
if the results are to be accurate. This
really does make it difficult for us to
produce a useful product unless we
can come up with a simple calibration
procedure. At the moment, we don’t
SC
have a solution.
August 1994 93
MARKET CENTRE
Cash in your surplus gear. Advertise it here in Silicon Chip.
CLASSIFIED ADVERTISING RATES
VINTAGE RADIO
Advertising rates for this page: Classified ads: $10.00 for up to 12 words plus 50
cents for each additional word. Display ads (casual rate): $25 per column centimetre (Max. 10cm). Closing date: five weeks prior to month of sale.
To run your classified ad, print it clearly in the space below or on a separate
sheet of paper, fill out the form & send it with your cheque or credit card details
to: Silicon Chip Classifieds, PO Box 139, Collaroy, NSW 2097. Or fax the details
to (02) 979 6503.
VINTAGE RADIO SWAP meet/fair.
Inc. military, amateur radio and antique
sound. Sunday 23rd October, 1994
10am to 5pm. Glenroy Technical School
Hall, Melbourne. Bookings: R. Howarth,
PO Box 9, Junortoun 3551. Phone (054)
49 3207.
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
FOR SALE
REAL TIME ICE!!! The only way to go.
MOTOROLA 6805 EMULATOR and
programmers. Prices and data from Graham Blowes, Mantis Micro Products,
38 Garnet Street, Niddrie 3042. Phone
(03) 337 1917 (a/h), (03) 575 3349 (b/h).
Fax (03) 575 3369.
WEATHER FAX programs for IBM XT/
ATs *** “RADFAX2” $35 is a high resolution, shortwave weather fax, Morse
& Rtty receiving program. Suitable for
CGA, EGA, VGA and Hercules cards.
Needs SSB HF radio & Radfax decoder.
*** “SATFAX” $45 is a NOAA, Meteor &
GMS weather satellite picture receiving program. Needs EGA or VGA plus
“WEATHER FAX” PC card. *** “MAXISAT” $75 is similar to SATFAX but needs
2Mb expanded memory (EMS 3.6 or 4.0)
and 1024 x 768 SVGA card. All programs
are on 5.25-inch or 3.5-inch disks (state
which) & include documentation. Add
$3 postage. Only from M. Delahunty, 42
Villiers St, New Farm, Qld 4005. Phone
(07) 358 2785.
Enclosed is my cheque/money order for $__________ or please debit my
RCS RADIO PTY LTD
Card No.
✂
❏ Bankcard ❏ Visa Card ❏ Master Card
Signature__________________________ Card expiry date______/______
Name ______________________________________________________
Street ______________________________________________________
Suburb/town ___________________________ Postcode______________
94 Silicon Chip
RCS Radio Pty Ltd is the only company that manufactures and sells every
PC board and front panel published
in SILICON CHIP, ETI and EA.
RCS Radio Pty Ltd,
651 Forest Rd, Bexley 2207.
Phone (02) 587 3491
Zelcon Technic Pty Ltd
•
•
•
•
PCB Supplier
Photoplotting Services
SMT/Through-Hole Assembly
CAD facilitites
PO Box 149, Glenorchy, Tas 7010
Ph: (002) 71 8120, Fax: (002) 71 8182
BBS: (002) 73 0799
TRANSFORMER REWINDS
350 Watt Power MOSFET Amplifier Module
•
•
•
•
As published in the June 1994 issue
of Silicon Chip. Kit price $159.00.
Postage and handling $8.00.
Payment by M/C, B/C, Visa, Cheque
or Money Order.
3kg O/N Air Bag $10.00
Computer & Electronic Services Pty Ltd
27 Osborne Avenue, Trevallyn Launceston, Tasmania 7250
Phone 003-34 4218; Fax 003-31 4328
MEMORY & DRIVES
PRICES AT AUGUST 1ST, 1994
SIMM (all 70ns)
Parity/No Parity
1Mb 30-pin
$60/54
4Mb 30-pin $208/195
2Mb 72-pin
$135
4Mb 72-pin $235/212
8Mb 72-pin
$470/415
16Mb 72-pin
$900/765
32Mb 72-pin $1690/1590
MAC
6Mb P’BOOK
CO-PROCESSORS
387S/DX to 40
$350
$90
LASER PRINTER HP
with 2Mb
$198
ALL TYPES OF TRANSFORMER REWINDS
COMPAQ
PROLINEA
TRANSFORMER REWINDS
8Mb
$476
EPROM & SRAM EMULATOR: 2K x
8 (or 16) to 64K x 8 (or 16). Download
and verify via standard PC printer port.
Supports Binary, Intel and Motorola
hex formats. Including Binary Editor.
For more information, contact Northern
Eastern Digital, PO Box 1252, Collingwood, Vic 3066. Fax (03) 484 5133/432
1063; Phone (03) 432 1699.
MICASOFT Electronics and Computing
tutor program, written in UK, ideal for
TAFE, schools, or individual use. Now
available in Australia. Send $1.80 in
stamps for demo disk (tell us what size).
$7
$8
IBM PS.2
55 x 65 SXVP 4Mb
L40/N33
4Mb
90/95 PS1
4Mb
$298
$280
$250
TOSHIBA
2000SX
44/6400
$460
$280
8Mb
4Mb
SUN
SPARC 10/20 16Mb
SPARC 10/20 64Mb
$975
$4080
DRIVES – SEAGATE
261Mb 16ms 2yr w
528Mb 12ms 2yr w
1052Mb 9ms 5yr w
$315
$480
$1170
1st Floor, 100 Yarrara Rd, PO Box 382, Pennant Hills, 2120.
Tel: (02) 980 6988
Fax: (02) 980 6991
SUBSTITUTE FOR A HANDFUL OF
ICs: Parallax “BASIC STAMP”. A general
purpose small circuit module, it is really
a 25 x 50mm board with a computer
chip (4MHz PIC 16C56), EEPROM, 8
I/O pins, board space includes prototyping area. Program it on a PC (only
33 instructions) with development kit
which includes one “BASIC STAMP”
($249 plus S/T & post), extra modules
($66 plus S/T & post). Send 45c stamp
for more information. Parallax distributor and technical support in Australia:
MicroZed Computers, PO Box 634,
Armidale, NSW 2350. Facsimile (067)
72 8987.
70ns
70ns
Sales tax 21%. Overnight delivery. Credit cards welcome.
5-Year warranty. Ring for latest prices.
Reply Paid No.7, PO Box 1058,
St Marys, NSW 2760.
Ph: (02) 833 1146. Fax: (02) 623 5559.
SATELLITE TV DX SUPER RX receiver.
Threshold 2.5dB. Also digital picture,
sound, synchron, resolution processors.
Mobile DX receivers, pay TV decoders.
TV, radio, picture, sound modulators.
Digital, analog signal meters. Send $5
for info and catalog/refundable to John
Papp, PO Box 472, Sanderson, NT
0812. Fax/Ph:(089) 27 4985.
DRAM DIP
1Mb x 1
256 x 4
PELHAM
MicroZed Computers, PO Box 634,
Armidale 2350.
FLUORESCENT INVERTER KIT (SC,
Feb 91) (Soft Technology No. 46): 12V,
24V or 48V/16W version. Secondary
wind, board plus components $30 plus
$4 p&p. SOLAR BATTERY CHARGING
REGULATOR: short form kit 12V or
24V (SC, Jan 94) 10A $54 plus $4 p&p.
Additional Mosfet $8 and Schottky diode
$5 to make 20A regulator.
With every kit ordered FREE used LEAD
SEALED BATTERY 12V/4Ah or 6Ah
while stocks last. Good condition but
no warranty. Only p&p is charged for
battery. Ring for postage cost. Cheques
and postal money orders accepted with
mail orders. Send orders to: Otakar
Priboj, PO Box 362, Villawood, NSW
2163, Australia. Phone (02) 724 3801.
INTELLIGENT INFRARED RECEIVER
(ref SILICON CHIP, March 94). Now with
8 outputs. Use your TV or VCR infrared
remote control transmitter to control your
TV or hifi appliances with an intelligent
infrared receiver kit. Also available
infrared transmitters, preprogrammed
and learning models. For details call
BENETRON P/L (018) 20 0108.
MANIPULATE MODELS, Machines,
Men or Mice from the serial port (9600,
N, 8, 1) of your PC using my PICEX
Controller. It’s a tiny computer with its
own Operating System controlling 16
I/O lines. Very simple programming
language. You can even drive it from
any VDU or terminal. Has 3 LEDs, 26pin MAD bus and 34-pin RELAY8 bus.
Up to 256 boards can be driven from
1 serial port. Short form kit includes
programmed PIC16C57-XT chip, board,
4MHz Xtal, and MAX-232 $70, A&T
$130. Promo disk $2. Don McKenzie, 29
Ellesmere Crescent, Tullamarine 3043.
Phone (03) 338 6286.
SILICON CHIP BINDERS
These beautifully-made binders will protect your copies
of SILICON CHIP. They feature heavy-board covers, are
made from a distinctive 2-tone green vinyl & have the
SILICON CHIP logo printed in gold-coloured lettering
on the spine & cover.
To order, just fill in & mail the order
form on page 79, or phone or fax
your order to:
Silicon Chip Publications, PO Box
139, Collaroy Beach, 2097. Phone
(02) 979 5644. Fax: (02) 979 6503.
August 1994 95
Microprocessor For
Stereo Preamplifier
Now back in stock: the 68HC705-C8P
pre-programmed microprocessor for
the Infrared Remote Controlled Stereo
Preamplifier (SILICON CHIP, Sept.Oct. 1993). Also suits the Remote
Volume Control (May & June, 1993).
Price: $45 + $6 p+p
Payment by cheque, money order or
credit card to: Silicon Chip Publications, PO Box 139, Collaroy, NSW
2097. Phone (02) 9795644; Fax (02)
979 6503.
THE HOMEBUILT DYNAMO: (plans)
brushless, 1000 DC watt at 740 revs.
$A85 postpaid airmail from Al Forbes,
PO Box 3919 - SC, Auckland, NZ.
Phone Auckland (09) 818 8967 any
time. Rotor magnets (3700 gauss) kit
now available.
VALVE AMPLIFIERS: Australian
made. Mono, stereo, guitar using 2A3,
211, 6L6 or 807 valves. Williamson
reproductions. Parts available for DIY
constructors. Circuit diagrams and construction details for many types of valve
amplifiers. Valve equipment repairs.
Lancroft Pty Ltd, PO Box 439, Bexley
2207. Phone (02) 567 5390.
THE 8051 MICRO-COMTROLLER
book includes a simulator disk ($40).
ROMLoader EPROM Emulator (EA
Jan/Feb 92, EA June 94) (PCB $30).
8051 Proto-Boards (EA Feb 93) (PCB
$30). Tantau Australia, PO Box 1232,
Lane Cove, NSW 2066. Phone AH (02)
878 4715.
SmallTALK for PCs: voice
digitiser for 286’s and up
Play speech on your PC’s
speaker with no sound card!
3 minute version
$34.95
HDD version
$39.95
Optional QLB/LIB libraries
$14.00
All orders add $3.05 p+p.
Send your cheque/order to:
RAT
Electronics
AUSTRALIA
PO Box 641,
Penrith, NSW 2750
Ph: (047) 77 4745
Fax: (047) 77 4745
Altronics ................................ 60-62
Aust. Audio Consultants...............95
Av-Comm................................57,77
Computer & Elect. Services.........95
David Reid Electronics ..............33
Dick Smith Electronics........... 12-15
E. R. Audio...................................96
Harbuch Electronics....................33
ELECTROSTATIC
LOUDSPEAKERS
3-PANEL FULL RANGE DESIGN,
AVAILABLE IN KIT FORM OR FULLY
ASSEMBLED.
LOCALLY DESIGNED & MANUFACTURED.
FOR INFORMATION BROCHURE,
PHONE/FAX (09) 397 6212 OR WRITE TO:
E. R. AUDIO,
119 BROOKTON HWY, ROLEYSTONE,
WESTERN AUSTRALIA 6111.
Instant PCBs................................95
Jaycar ................................... 45-52
Kalex............................................88
L & M Video.................................43
Macservice....................................3
Oatley Electronics.................. 78-79
PC Computers.............................89
Pelham........................................95
Rat Electronics............................96
RCS Radio ..................................94
UNUSUAL BOOKS: Electronic Devices, Fireworks, Locksmithing, Radar
Invisibility, Surveillance, Self-Protection,
Unusual Chem
istry and more. For a
complete catalog, send 95 cents in
stamps to Vector Press, Dept S, PO Box
434, Brighton, SA 5048.
Rod Irving Electronics .......... 26-30
PRINTED CIRCUIT BOARDS for the
hobbyist. For service & enquiries contact: T. A. Mowles (08) 326 5590.
Silicon Chip Software..................23
2.2kVA VARIAC unenclosed $200. 110V
1kVA transformer enclosed $100. Phone
(047) 87 8968.
SILICON CHIP FLOPPY INDEX
WITH FILE VIEWER
Now available: the complete index to all SILICON CHIP articles
since the first issue in November 1987. Now you can search
through all the articles ever published for the one you want.
The index comes as an ASCII file on a 3.5-inch or 5.25-inch floppy disc to suit
PC-compatible computers and you can use any word processor or our special
file viewer to search for keywords. Simply enter in the keyword(s) and the index
will quickly find all the relevant entries. All commands are listed on the screen,
so you’ll always know what to do next.
Price $7.00 + $3 p&p. Send your order to: Silicon Chip Publications, PO Box 139,
Collaroy 2097; or phone (02) 979 5644 & quote your credit card number; or fax the
details to (02) 979 6503. Please specify 3.5-inch or 5.25-inch disc.
96 Silicon Chip
Advertising Index
Silicon Chip Back Issues....... 90-91
Silicon Chip Binders....................95
Silicon Chip Bookshop.................73
Silicon Chip Projects Book........IBC
Tektronix....................................IFC
Transformer Rewinds...................95
Yokogawa................................OBC
Yuga Enterprise...........................87
Zelcon Technic.............................95
_________________________________
PC Boards
Printed circuit boards for SILICON
CHIP projects are made by:
• RCS Radio Pty Ltd, 651 Forest
Rd, Bexley, NSW 2207. Phone (02)
587 3491.
• Marday Services, PO Box 19-189,
Avondale, Auckland, NZ. Phone (09)
828 5730.
• H. T. Electronics, 35 Valley View
Crescent, Hackham West, SA 5163.
Phone (08) 326 5590.
Especially For
Model Railway
Enthusiasts
Order Direct
From
SILICON CHIP
Order today by phoning (02) 9979 5644 & quoting your credit card number;
or fill in the form below & fax it to (02) 9979 6503; or mail the form to
Silicon Chip Publications, PO Box 139, Collaroy, NSW 2097.
This book has 14 model railway
projects for you to build, including
pulse power throttle controllers,
a level crossing detector with
matching lights & sound effects,
& diesel sound & steam sound
simulators. If you are a model
railway enthusiast, then this
collection of projects from SILICON
CHIP is a must.
Price: $7.95
plus $3 p&p
Yes! Please send me _______ copies of 14 Model Railway Projects
Enclosed is my cheque/money order for $_________ or please debit my
Bankcard Visa Card Master Card
Card No.
Signature_________________________ Card expiry date_____/_____
Name _________________________Phone No (____)_____________
PLEASE PRINT
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