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Vol.8, No.3; March 1995
Contents
FEATURES
4 Electronics In The New EF Falcon, Pt.1
New engine management system has triple coil ignition – by Julian Edgar
11 Protection For Toroidal Power Transformers
Fuse selection for short circuit & overload protection – by Michael Larkin
16 The Latest Trends In Car Sound, Pt.3
Building a Tube Sub-Woofer – by Julian Edgar
58 A Look At The 68000 Microprocessor
Interface buses & registers – by Elmo Jansz
85 Tektronix TDS 784A TruCapture Oscilloscope
TUNE SUB-WOOFER FOR CAR HIFI
SYSTEM – PAGE 16
Can display up to 400,000 acquisitions per second – by Leo Simpson
PROJECTS TO BUILD
20 Subcarrier Decoder For FM Receivers
Tune into hidden FM transmissions – by John Clarke
32 50W/Channel Stereo Amplifier, Pt.1
Easy-to-build, no setting-up adjustments – by Leo Simpson & Bob Flynn
40 Build a Lightning Distance Meter
It measures flash distances up to 19km – by Darren Yates
52 Wide-Range Electrostatic Loudspeakers, Pt.2
Building the treble & bass panels – by Rob McKinlay
69 IR Illuminator For CCD Cameras & Night Viewers
Use it for security or wildlife observations – by Branco Justic
TUNE INTO HIDDEN FM
TRANSMISSIONS – PAGE 20
SPECIAL COLUMNS
46 Serviceman’s Log
Doing the rounds with remote control – by the TV Serviceman
63 Remote Control
Building a remote control system for models; Pt.3 – by Bob Young
72 Computer Bits
Record real-time video with the Video Blaster FS200 – by Darren Yates
BUILD THIS 50W/CHANNEL
STEREO AMPLIFIER – PAGE 32
74 Vintage Radio
The innaugural vintage radio swap meet – by John Hill
80 Amateur Radio
Build a simple 2-transistor CW filter – by Darren Yates
DEPARTMENTS
2 Publisher’s Letter
9 Mailbag
10 Circuit Notebook
50 Order Form
82 Product Showcase
90 Ask Silicon Chip
93 Notes & Errata
94 Market Centre
96 Advertising Index
REMOTE CONTROL RECEIVER FOR
MODELS – PAGE 63
March 1995 1
Publisher & Editor-in-Chief
Leo Simpson, B.Bus.
Editor
Greg Swain, B.Sc.(Hons.)
Technical Staff
John Clarke, B.E.(Elec.)
Robert Flynn
Reader Services
Ann Jenkinson
Advertising Enquiries
Leo Simpson
Phone (02) 979 5644
Regular Contributors
Brendan Akhurst
Garry Cratt, VK2YBX
Marque Crozman, VK2ZLZ
Julian Edgar, Dip.T.(Sec.), B.Ed
John Hill
Jim Lawler, MTETIA
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
NSW's new truck
monitoring system
Most people love to see the introduction of new technology. It usually
brings improvements in the way that
things are done and in the long run,
usually produces economic advantages, both to those directly using the
new technology and to the community
at large. But there are times when the
introduction of new technology gives
cause for alarm and perhaps, concerted
opposition.
What prompts this thought is the introduction by the Road Transport
Authority in New South Wales of a new computer linked monitoring system for trucks and buses. The idea is that there will be 20 speed cameras
throughout the state that will be linked to a central bureau at Flemington
in Sydney. Four of these cameras are now operating, at Bargo, Gundagai,
Wyong and Deepwater, near Tenterfield.
Not only will this system's cameras be able record any truck or bus
travelling at excess speeds but by calculating the time of transit between
any two monitoring cameras, it will be able to tell whether the vehicle has
been speeding at other times along the way. By subsequently examining the
vehicle's logbooks, the bureaucrats will also be able to tell if the driver has
taken the regulation breaks.
Now, given that there have been a number of very serious accidents
involving trucks and buses in New South Wales and other states, you
might think that this is desirable innovation by a government bureaucracy.
Well, I don't think it is. In order to be able to work, the system will not just
photograph those vehicles which are speeding - it will have to photograph
every truck and bus which passes by. I reckon that this constitutes a gross
invasion of privacy. In the past, if you exceeded the speed limit, you might
expect to be caught by a speed camera operated by the police. But now,
if you are a truck or bus driver, you will be photographed whether or not
you are speeding!
And why should the system be confined to trucks and buses? Obviously,
with the capabilities of a modern computer network, there is no reason why
it could not be used to track all cars travelling along the highways. Now you
might be fairly relaxed about trucks and buses being continually monitored
but think it through. This means that all trucking operations along major
highways can be monitored by the State. The possibilities for abuse and
corruption of this system are hair-raising. And when it is extended, as it
surely will, to private cars, the police state will have finally arrived.
If you're happy with that, fine. But if you're not, take a photocopy of this
editorial and send it to your local politician along with a covering note that
you want it stopped!
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
Electronics in the
The XR6 is a factory-produced, high-performance
version of the EF Falcon. Its 4-litre engine produces
164kW under the control of the newly-introduced
EEC-V engine management system.
The latest EF Falcon has a new engine
management module with 88Kb of onboard memory. In addition, the system
now features sequential fuel injector
operation & triple-coil ignition.
Pt.1: the engine management system
4 Silicon Chip
The EEC-V Ford engine management system (pronounced ‘Eck-5’)
replaces the EEC-IV system introduced
on the Falcon in 1985. Initially used for
controlling ignition and fuel delivery
only, the system was subsequently upgraded in 1992 to also control automatic transmission and air-conditioner
compressor operation. However, with
these additional demands, the system
was at its limits in terms of both input/output (I/O) and microprocessor
throughput.
The new EEC-V system now allows
the incorporation of knock detection
and control, as well as a multi-coil
distributorless ignition system. In
addition, the system’s greater pro-
e new EF Falcon
By JULIAN EDGAR
Above: the EF Falcon 6-cylinder engine uses a new engine management system
& a triple-coil ignition system to eliminate the distributor.
cessor speed has translated directly
to improvements in vehicle perfor
mance, drivability, fuel economy and
emissions.
Microcontroller I/O
The microprocessor in an engine
management system must be able to
sense physical parameters in the form
of electrical signals. Two different
types of sensors are used: analog and
digital.
Analog sensors provide a varying
output voltage and measure factors
such as throttle position, engine
coolant temperature and intake air
temperature. Digital sensors, on the
other hand, provide either an “on”
(logic 1) or “off” (logic 0) signal, or
can deliver a variable frequency digital
pulse train. The square-wave output
from a speed sensor is a good example
of this latter type.
Analog sensors are read via analog
to digital (A/D) convertors, while on/
off binary signals can be read by a low
speed digital input port. The micro
controller software reads the input
port periodically to determine the
state of the switch but this approach
is appropriate only for inputs which
change state at a frequency of less than
2Hz. For signals which change more
rapidly than this, a high speed digital
input is used. This allows an event to
be captured closer to the time at which
the transition took place.
Output ports must also be suited to their specific applica
tions. A
low speed digital output (LSDO)
is appropriate for the control of an
air-conditioning compressor clutch,
for example. On the other hand, a
high speed digital output (HSDO) is
necessary for a function that requires
accurate timing control (such as fuel
injector operation).
For an output which repeats at a
fixed time interval, it would be possible to use an HSDO and continually
schedule the output events to generate an appropriate signal. However
the software requirement makes this
undesirable. Instead, circuitry which
is activated once and then “forgotten” until a change in periodicity
is required is used. These outputs
use pulse width modulation (PWM)
and are referred to as “Duty Cycle
Outputs”.
The 8065 microprocessor
The 8065 microprocessor is based
on the previous system’s 8061 but
March 1995 5
MISSING
TOOTH
6.5 AMP
COIL PRIMARY CURRENT
(WITH DWELL)
Vp-p
6.5 AMP
Fig.2: the
coil primary
current ramp
is controlled so
that it reaches its
target value at
the point where
it will be fired.
This reduces the
load on the car’s
electrical system.
TOOTH
CENTRE
Fig.1: the crankshaft position sensor output
waveform is used by the ECU to time the ignition
and fuel injection systems.
with several enhancements. The
8061 was a reasonably powerful 16bit chip which was optimised for
high-speed, real-time applications.
However, depending on which I/O
mode it is operated in, the 8065 can
offer substantially more input and
output channels. Table 1 shows the
configuration chosen for the EF Falcon
EEC-V system.
A/D conversion
The 20 channels of A/D conversion
offer 10 bits of accuracy over the range
from 0-5V. The time required for conversion is less than 30 microseconds,
while events on HSDI ports have a
capture resolution of 2 microseconds.
HSDO’s are also accurate to within
2 microseconds. In addition, the 32Kb
PROM of the previous system has been
replaced with an 88Kb memory, which
Fig.3: the electronic
ignition system uses a
knock sensor to help
determine the ignition
timing advance. The
sensor is screwed into
the engine block.
6 Silicon Chip
EDIS COIL PRIMARY CURRENT
WAVEFORM
allows for much greater software design flexibility.
Ignition system design
The EEC-V system uses a new
distributorless ignition system on
the 6-cylinder engine. Previously,
most of the ignition-related activities
were controlled by the EEC-IV’s 8061
micropro
cessor, whereas the new
system uses its own CPU.
The ignition system, termed the
Electronic Distributorless Ignition
System (or “EDIS” in Ford parlance),
replaces the conventional distributor
with three individually controlled
ignition coils. Each of these coils fires
two spark plugs (in two cylinders) at
once, with one cylinder fired on its
compression stroke and the other on
its exhaust stroke. The spark plug fired
on the compression stroke uses far
more of the available energy
than the other simultaneously fired plug.
The engine crankshaft
position is sensed by
a variable reluctance
pick-up which is excited
by a rotating sprocket with teeth spaced
at 10° intervals. A
KNOCK
missing tooth
SENSOR
is positioned at
60° before top
dead centre for
No.1 cylinder and
this results in a distorted waveform (see
Fig.1) which the EDIS
CPU can sense. The
EDIS CPU also calculates
engine rpm from this sensor
and this is then passed on to the 8065
CPU.
The 8065 takes this speed information and, along with other information
such as throttle position and intake
air temperature, uses it to calculate
the desired spark advance angle. This
infor
mation is then passed back to
the EDIS CPU which carries out the
necessary calculations to provide a
spark at the desired angle of advance.
The EDIS system also energises the
coil primary in a way different to conventional ignition systems. Generally,
the primary side of the coil is energised
well in advance of the required firing
point. By contrast, EDIS uses a method
of dwell control which predicts when a
given coil should be turned on so that
it reaches its target primary current at
the point where it will be fired – see
Fig.2. This not only reduces the load
on the car’s electrical system but also
reduces the need for current-limiting
circuitry in the ignition system.
Knock detection
Spark timing has a major influence
when it comes to obtaining the best
fuel economy and performance. At the
same time, engine knock (detonation)
must be avoided to prevent engine
damage.
Detonation can occur due to variables in engine build, the fuel octane
rating, the air/fuel ratio and internal
carbon build-up. In fact, the need for a
safety margin between engine-damaging detonation and optimal outcomes
has seen the ignition timing retarded
by as much as 6° in some cars, with a
consequent reduction in performance.
To overcome this problem, EDIS
uses a knock detector to sense engine
detonation. The sensor is attached
to the engine block and is used to
measure vibration within a specific
frequency range. This frequency range
was chosen by analysing the frequency
of engine block vibration both with
and without percepti
ble knock and
then selecting the range in which
there was the most noticeable change.
Specifically, a band about 600Hz wide
and centred on 7.5kHz is used.
Detonation occurs only during the
firing stroke, hence the background
noise of the valve train, crankshaft
rotation and so on can be measured
separately and used as a reference
value. During firing, the knock sensor
signal is constantly compared to this
reference signal. If the threshold is
exceeded, knock is deemed to have
occurred and the EEC-V processor
retards the timing for the next cylinder
by 1°. If knock continues to occur, the
spark advance is then retarded by either an additional one or two degrees
for each cylinder, depending on speed
and load conditions.
When knocking is no longer detected, the spark timing for each cylinder
is advanced in 0.25° increments until
knock is again detected. As a result,
the spark advance hovers just below
the level at which audible detonation
occurs.
Fuel injection
Two different systems of fuel injection are used in the EF Falcon range,
one for the V8 engine and the other
for the 6-cylinder engine. The V8
uses sequential injection with airflow
measured by a hotwire mass airflow
meter. The 6-cylinder engine, on the
other hand, uses a combination of
manifold absolute pres
sure (MAP)
sensing, intake air temperature sensing and an rpm signal to calculate the
airflow mass.
In the case of the 6-cylinder engine, the fuel injection system uses a
heated exhaust gas oxygen sensor to
provide constant feedback of the air/
SPARK PLUG
LEADS
DOUBLE-ENDED
IGNITION COILS
Fig.5: the 6-cylinder engine is fitted with triple double-ended ignition
coils, with each coil used to fire two spark plugs simultaneously.
In this system, one cylinder is fired on its compression stroke & the
other on its exhaust stroke.
TABLE 1: I/O Channels For EEC-V ECM
fuel ratio to the
Number of Channels
ECU. This oxyType of I/O
EEC-V
(8065) EEC-IV (8061)
gen sensor is also
used to provide
A/D Conversion
20
13
information to an
Low-speed digital input
13
0
adaptive learning
mechanism.
High-speed digital input
8
8
This works as
Low-speed digital output
24
8
follows. The sensor output values
High-speed digital output
16
10
during closed loop
operation are com
Duty cycle output
9
0
pared with those
predicted by the ECU as needed un- mixtures, then the correction values
der the current operating conditions. are stored and applied when the enIf there is a difference between the gine is later being driven in open-loop
amount of fuel the ECU predicted mode. This occurs under full throttle,
would be required and the amount during cold conditions and when the
being used to provide the appropriate engine is in lean cruise mode.
ADVANCE (ø)
KNOCK IDENTIFIED,
TIMING RETARDED
IN STEPS
KNOCK AGAIN
IDENTIFIED
1-2ø, DEPENDANT
ON SPEED/LOAD
TIMING RAMPS UP
IN STEPS UNTIL KNOCK
AGAIN IDENTIFIED
0.25ø
KNOCK STOPS
TIME (PIP SIGNALS)
Fig.4: when knock (or detonation) is detected by the knock sensor, the ignition timing is initially retarded in steps of either
1 or 2 degrees (depending on the engine speed & load) & then re-advanced in 0.25 degree increments.
March 1995 7
This photo shows the new
EEC-V electronic control
unit (ECU) on the left, while
the older EEC-IV ECU is on
the right. The EEC-V uses
an 8065 microprocessor
capable of over a million
operations per second & has
88Kb of memory.
Fig.6: a heated exhaust gas oxygen
sensor is used to provide vital
feedback on the air/fuel mixtures.
The fuel injectors are fired in two
banks, with cylinders 1, 3 and 5 operating as one bank and cylinders 2,
4 and 6 as the other. The banks are
fired in response to the ignition signal
pulses derived from the EDIS, with
the injectors in each bank opening on
every third pulse (ie, once per rev).
During cranking, the firing frequency
is increased to give better starting.
Operating modes
A number of different modes of
operation are employed by the ECU:
(1). Closed Loop Mode. This is where
the oxygen sensor input is used to
determine the air/fuel ratio being used.
This will normally occur after the first
few minutes of engine operation, when
the sensor has reached its operating
temperature.
(2). Open Loop Mode. The input from
the oxygen sensor is disregarded in
this mode. This occurs for two reasons:
(a) either the sensor has not reached
its operating temperature; or (b) it is
necessary to run the engine at air/
fuel ratios other than stoichiometric
(that is, other than at a 14.64:1 air/
fuel ratio).
(3). Crank Mode. This occurs during
engine starting. In this mode, the
ignition advance is set at 10° BTDC,
the idle speed control bypass valve is
fully open, and the evaporated fuel
canister purge is closed. The injector
pulse width (and thus fuel flow) is
dependent on engine coolant
temperature.
(4). Run Mode. Once the car
has started (and if it doesn’t
there is an Underspeed Mode
to cater for this), the ECU
switches to Run Mode. In this
condition, the throttle position has a large controlling
influence on fuel injection
behaviour.
(5). Cruise Mode. When
the throttle position sensor output is
within a certain range, the ECU selects
this mode. The ignition timing is now
calculated as a function of RPM, load
and the coolant and intake air temperatures. The fuel flow is derived from
the calculated airflow and then made
richer or leaner to suit the coolant
temperature.
(6). Wide Open Throttle Mode. This
mode is selected when the throttle
position sensor exceeds a prescribed
value. It selects a richer mixture than
in other running modes to increase
engine power. Note that the ignition
timing remains the same, as it is already at optimal levels.
(7). Limp Home Mode. If an electronic
malfunction occurs, the system reverts
to the following settings: the ignition
timing is fixed at 0° BTDC; the canister
purge is locked out; the injector pulse
width is fixed at 3ms; the injectors are
fired on the rising edge of each ignition
signal; and the idle speed control valve
duty cycle is set to 75%.
A very rich mixture which is characterised by black exhaust smoke
results, although the car can still be
driven at speeds of up to 100km/h in
this mode.
SC
Acknowledgement
Fig.7: the injector firing modes for the 6-cylinder engine show that the
injectors are operated in two banks of three. During normal running, they
operate alternately on the rising edge of each third ignition pulse. During
cranking, however, the firing frequency is increased (ie, each bank operates
briefly on each ignition pulse) to give better starting.
8 Silicon Chip
Thanks to Ford Australia and the
Society of Automotive Engineers
for permission to use material from
the “SAE Australasia” journal of
October/November 1994.
MAILBAG
Fax/modems can
cause problems
Your editorial of October 1994 mentions difficulties with sending facsimiles to people who don’t know how to
operate their facsimile machine.
I would like to whinge about the
generally unsatisfactory way many
people are using their facsimile machines. Amongst my pet hates are
those who think they have sent me
a facsimile, then ring a week later:
“Didn’t you get my fax?” These people have their machine set so that it
does not print a “satisfactorily sent”
report. OK that is a waste of paper but
most machines allow printing of an
“inability to send” slip. To turn off all
reporting is irresponsible.
On a humorous note, with a happy
ending, I recently received a sequence
of facsimiles from a person who on
several occasions sent me two blank
sheets from a machine he was not
familiar with. It turns out that the machine was a recent installation. Eventually, someone set the firm’s name and
number in the facsimile’s handshake
routine. Armed with this information
I was able to send a facsimile which
read “please stop sending blank pages,
they are too hard to read”. He rang me
and we worked out that he was sending
facsimiles to everyone with the pages
in wrong side up and was wondering
why he had got no answers!
Then there is the problem you refer
to, caused by those who use a common
line for voice and facsimile. They answer the phone and usually there is
only one person in the establishment
who knows how to handle the call if
it is other than a speech call.
I sometimes get up in the middle of
the night to handle matters that may
have been nagging my mind. Have
you ever accidentally sent a facsimile to someone with a combined line
at 1.00am? I have. My effort was not
well received. Some machine-phone
combinations handle this problem
by answering the call, listening for
a facsimile tone, then connecting to
the facsimile machine, or ringing a
handset, if it is a voice call. However,
if the call has been launched through
STD, the caller is being charged from
when the ringing tone stops. This is
exacerbated where a voice answering
machine is used too.
Then there is the unsolicited and
inappropriate junk mail, pages of
useless information – these go straight
into the bin and a mental note is made
not to deal with that firm. Courteous
firms ring first and ask “will you give
us your fax number and accept our
regular transmissions?” A conversation usually follows, establishing our
mutual interest or not and consequent
cost saving for both of us. I may be
old-fashioned but courteous treatment
by a firm is usually an indication of
how they are likely to do business
with me.
How about the person who sends
a full A4-size page with one or two
lines on it? – usually accompanied
by a “Fax Cover Sheet” with fancy
graphics and information that would
have been better received as a 2-line
header! Why not use a pair of scissors
to cut the sheet short and save costs
at both ends?
Many problems are caused by facsimile cards in a PC. I tried one a long
time ago, on a line common with my
normal phone, and although the idea
seemed to be working from my end, I
soon realised that there were problems
out in the real world I was trying to talk
to. The cost of these “cheap” units is
deceptive. I found out that a separate
line cost me no more to install, with the
ongoing rental costs being worth the
convenience the separate line gave me.
Another not so obvious point is that
some firms seem to think that separate
voice and facsimile numbers are an
indication of how serious one is about
one’s business. If you have separate
numbers, you will be treated with
more care and respect.
Bob Nicol,
Armidale, NSW.
Solar tracker
could be a hot box
I would like to offer some comments
about the Solar Tracker in the January
1995 issue. In full sun, the temperature
in that electronics box will exceed
100°C, which may prove to be destructive. I suggest it be placed under
SILICON CHIP,
PO Box 139,
Collaroy, NSW 2097.
the panel or fitted with a sun screen
so that only the sensors are exposed.
It seems to me that a sun-tracker
only needs to operate when there is a
sun to track; at other times the panel
should centre. The mercury switches
could be arranged to do that. The night
sensor could face south and operate
a comparator which would switch
from the centre position mode to the
tracking mode whenev
er the direct
sunlight exceeded the average reflected southlight.
B. Jolly,
Tranmere, SA.
Sun tracker
circuit query
I have waited for some time for a
construction article on a sun-tracker.
Now you have published one which is
very good but I am puzzled by a couple
of things about the circuit. Why is pin
4 of the 555 not connected to pin 8 as
recommended in the National Semiconductor application notes for this
device? And why is there no bypass
capacitor on pin 5?
I also believe it would be normal
practice to provide separate gate resistors for the FET switches. Finally,
why are there no power supply filter
capacitors across the 12V supply?.
Other than this I intend to build the
unit as soon as I can get my hands on
a PC board from RCS Radio.
Cliff Wylie,
Leumeah, NSW.
Comment: while National Semiconductor do recommend that pin 4 is
tied high, it is not mandatory for it
to be so. Nor is a capacitor at pin 5
mandatory. Individual gate resistors
for the Mosfets would normally be
used in a switching circuit but since
the voltages in this circuit are so static,
they are not required.
Bypass capacitors for the supply are
also not mandatory since the circuit
is powered directly from a lead-acid
battery. Having said that, there is no
reason why you should not change the
circuit to tie pin 4 high, add a capacitor to pin 5 and so on. We understand
that RCS Radio Pty Ltd has produced
a PC board with these modifications
included.
March 1995 9
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.
Pump control system
uses LDT
Most country households get their water supply from
tanks via an automatic pump. This cycles on and off if
the demand is less than the supply capacity of the pump.
The resulting pressure variations can be mildly annoying
when under the shower and extended periods of cycling
leads to premature pump failure. This control system
overcomes both problems by returning the surplus output
of the pump to its inlet whenever the flow sensor detects
a demand on the system.
The flow sensor uses a linear differential transformer to
detect flow. This device has a central primary winding to
magnetise a core and two identical secondary windings,
one each side of the primary, connected in series but in
opposite phase. With the core positioned equally in both
secondary windings there is no output. Displacement of
the core by the flow sensor valve produces a nett output
from the secondaries and when this reaches 2 volts the
Triac will fire on each half cycle. The Triac turns on a
solenoid valve which then returns unwanted flow from
the pump back to its inlet.
The solenoid valve used is the 24VAC type commonly
found in garden irrigation systems and this is rated for
both inrush (at switch on) and steady currents. As the
interrupted current from the Triac makes the solenoid
just rattle, it is rectified and smoothed by the 470µF
25VW capacitor. To provide the required inrush current,
Adjusting pulse-train
mark-space ratio
This circuit adjusts the
mark-to-space ratio of
an incoming pulse train
with
o ut affecting the
fin
frequency. Hex Schmitt 15Hz-150kHz
trigger IC1 is connected
SQUARE
WAVE
to buffer the incoming
signal and the paralleled
inverters drive C1 and
the associated constant
current source, Q1.
What happens is that
the output of IC1 pulls C1 and the
collector of Q1 low on each negative
transition of the input signal. Q1
then recharges C1, ready for the next
negative transition of the input signal.
If trimpot VR1 is set for its highest
resistance condition, Q1 is unable to
turn on and therefore the waveform
10 Silicon Chip
4x1N4001
15VAC
IC1
74C14
3
24VAC
SOLENOID
TR1
SC141D
DIFFERENTIAL
TRANSFORMER
8VAC
1500T
500T
1500T
0V
PUMP
OUTLET
FLOW
SENSOR
VALVE
BACKPRESSURE
VALVE
SOLENOID
VALVE
PUMP
INLET
TO HOUSE
a non-linear resistor in the form of a lamp is used. This
has a cold resistance of 3Ω and hot resistance of 20Ω.
For construction details of the flow sensor and back
pressure valves, send a stamped self-addressed envelope
to the designer.
W. Jolly, 2 Hextall Ave,
Tranmere, SA 5073. ($40)
4
6
IC1a
2
470
25VW
+5V
14
5
1
LAMP
6.2V 0.3A
12
13
11
10
470
D1
1N914
C1
.001
150
68k
Q1
BC557
1k
2
MARK/SPACE
VR1
10k
12
13
IC2a
8
3
1
7
passes through unchanged.
VR1 controls the amount of current
available to recharge C1 during the
space period. The effect is to vary the
space period from about 100ns minimum to the maximum stipulated by
the incoming waveform. IC2a, a quad
exclusive-OR gate, buffers the output
10
OUTPUT
9
5
8
9
IC2
4030
14
11
N
S1
6
4
7
INVERT
signal and also provides the facility
to invert the output waveform. This
means that the mark-space ratio can be
varied over the full range, by use of the
invert switch and VR1. The maximum
input frequency is 150kHz.
G. Freeman,
Nairne, SA. ($40)
Protection for toroidal
power transformers
Toroidal power transformers are well known
for the advantages of compact size, low hum
radiation & good efficiency. However, they also
draw heavy surge currents at switch-on & this
can cause problems. This short article discusses
fuse selection for short circuit and overload
protection.
By MICHAEL LARKIN*
Simple fuses in the secondary leg
of a transformer may only provide
short circuit protection. Such fuses
may not provide adequate overload
protection in many cases. Australian
Standard AS3108-1990 calls for both
short circuit and overload protection
for transformers (refer clause 14). It
is required by Australian Standard
AS3000 wiring rules that one leg
of an extra low voltage transformer
secondary winding be fused. This
is a minimum but it may not be the
whole answer.
For example, consider a 240V 300VA
toroidal transformer supplying a 12V
track lighting system. Normally, this
track would take six 50W lamps but because the track may be physically quite
long, the user may have seven, eight
or more lamps plugged in. Hence, we
now have a situation where the fuse,
due to its lack of sensitivity, does not
act and the transformer will overheat.
There are several possible answers
to this problem: (a) put a fuse in the
primary; (b) put a thermal cutout in
the transformer; (c) put a thermal protective device in lieu of a fuse in the
secondary leg of the AC circuit; and
(d) fit a one shot fuse in the primary
winding.
Table 1 below is a summary of
the recommended mains fuses to be
placed in the primary toroidal transformer circuit. The fuse should be a
slow-blow or anti-surge type to avoid
being blown by the inrush current at
switch-on.
This switch-on surge is much higher
than the inrush cur
rent for typical
conventional transformers. If too low a
fuse rating is chosen, intermittent fuse
operation will occur during “switch
on” of the transformer. This is the
nub of the problem. It is a matter of
discriminating between genuine fault
Table 1: Fuse Ratings
Toroid Rating
Fuse Type
625VA
Slow Blow or Anti-Surge
500VA
Slow Blow or Anti-Surge
300VA
Slow Blow or Anti-Surge
225VA
Slow Blow or Anti-Surge
160VA
Slow Blow or Anti-Surge
120VA
Slow Blow or Anti-Surge
80VA
Slow Blow or Anti-Surge
50VA
Slow Blow or Anti-Surge
30VA
Slow Blow or Anti-Surge
15VA
Slow Blow or Anti-Surge
conditions and large inrush currents.
The best options are (b) or (c), from
a technical point of view. Option (c)
may also be the best option from an
economical viewpoint.
Option (d) is not really a practical
approach because once the primary
fuse is blown the transformer is useless. Table 1 should be regarded as a
guide only and is based on a standard
3AG fuse size 5mm diameter by 20mm
long. These fuses are for the 240VAC
side of the toroidal transformer. Ratings should be tested in the practical
circuit. This is most important.
Table 2 shows the characteristics of
typical slow-blow fuses. Note that with
a current equal to 50% over the rating,
the fuse will take a minimum of 60 minutes to blow, or in other words, it takes
virtually forever. This is an essential
characteristic for the fuse in the primary
of a toroidal power transformer.
However, while a correctly specified slow-blow fuse will protect a
toroidal power transformer against a
short circuit in the secondary it will
not protect it against overheating
where the overload is, say, 33%. This
is equivalent to the
overload quoted for
the 300VA toroid in
Current Rating
the example above.
To cope with this
8.0A
situation, designers
5.0A
need to specify a
3.0A
thermal cutout in
the primary wind2.5A
ing. This will be
2.0A
sensitive to any
over-temperature
1.0A
situation within the
0.8A
primary wind ing
of the transformer.
0.315A
The normal tem0.25A
perature setting is
0.125A
110°C but for high
ambient situations,
130°C devices may be used.
* Michael Larkin is the managing
director of Tortech Pty Ltd, manufacturers of toroidal and conventional transformers. Their address
is 24/31 Wentworth Street, Green
acre, NSW 2190. Phone (02) 642
6003. Fax (02) 642 6127.
Table 2: Slow Blow Fuse Duration
Rated
Current In
1.5
2.1 x In
2.75 x In
4 x In
10 x In
Min
Max
Min
Max
Min
Max
Min
Max
125mA-10A
60 min
2 min
200ms
10s
40ms
3s
10ms
300ms
March 1995 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
Car Sound, Pt.3:
Building A Tube
Sub-Woofer
Car sub-woofers are now very widely
used by those who wish to listen to music
containing sub-100Hz frequencies. In
this article, we show you how to build a
car sub-woofer capable of reproducing
frequencies down to 25Hz.
By JULIAN EDGAR
The vented tube-type sub-woofer
design shown here has several advantages over a conventional, built-in
box design. These advantages are as
follows:
(1). compact size compared to many
sub-woofer installations;
(2). portability – the sub-woofer can
be easily removed when more boot
space is required;
(3). can be used in cars with folddown rear seats, hatchbacks, station
wagons, and mid-engine cars;
(4). low cost (around $200 each);
(5). effectiveness, with response down
to 25Hz; and
16 Silicon Chip
(6). good power handling capability,
allowing the use of high-pow
ered
bridged amplifiers.
Subwoofer design
A large diameter, suitably enclosed
woofer will generate good bass.
However the problem is in fitting the
required large enclosure into a car.
As an example, the recommended
vented box size for a typical 15-inch
sub-woofer is 222 litres. That’s equivalent to a box size of 100 x 50 x 44.4cm,
which means goodbye to the back seat
or boot!
On the other hand, a 10-inch driver
with suitable specifi
cations can be
accommodated in a vented enclosure
of just 50 litres. That’s less than one
quarter the size required for a 15-inch
driver! If two such 10-inch sub-woofers are used, their enclosures occupy
less than half the volume of the 15-inch
unit with only a slight reduction in
effective cone area.
Consequently, I decided to use two
10-inch sub-woofers, each with an
enclosure volume of about 50 litres
in my own car. However, the in-car
results were so good that only one unit
is really required – unless you want to
shake the rear vision mirror so much
that it is impossible to use! But how do
you build-in two enclosures of about
50 litres each and still leave room to
carry luggage if required?
The answer is to build the sub-woofers into two 12-inch diameter tubes,
one running down each side of the
boot. The accompanying photos show
how the tubes were fitted into the boot
of my Subaru Liberty. The tubes are
held in place by aluminium straps
and, when bulky loads need to be
carried, can be easily removed in just
a few minutes.
Plastic storm-water pipe (78cm long) is used for the main
body of the enclosure. The end-pieces are cut from 16mm
MDF & the speaker end-piece is shown here being trialfitted before being finally attached. Make sure that the end
pieces are not undersized – it’s better to have to sand them
back to ensure a tight fit. A sealant/glue such as “Liquid
Nails” should be used to form an airtight seal & at least 16
countersunk screws (see text) should be installed around
the periphery of the tube.
The drivers are mounted at the front
of the tubes and normally pump bass
through the back of the rear seat. Alternatively, if the rear seat is folded,
the sub-woofers pump bass straight
into the cabin.
Building the unit
The bass tubes are made from heavywalled (5mm thick) 32cm diameter
plastic stormwater pipe. The cost
from a plumbing supply house was
$55 a metre. Note that this material
The vents were made from 50mm-diameter plastic pipe
fitted with an outside ring cut from a plumbing adapter
fitting. Each vent was cut to a length of 54mm & sprayed
with black paint before being fitted to the end-piece
opposite the driver.
is also available in sewer pipe form
with a slightly thicker wall but the
cost escalates to almost $80 a metre!
The bass tubes were each cut to
78cm long, giving an internal volume of about 60 litres with the end
pieces in place. Once these pieces
had been cut, the two 32cm-diameter
end pieces for each tube were cut
from 16mm-thick medium-density
fibreboard (MDF). One end-piece
has a hole cut into it to accommodate the driver, while the other has
This view shows the completed enclosure, before the installation of the driver.
The inside of the enclosure was lined with acoustic material to damp out
reflections. This material is actually dressmaker’s quilt wadding, which is about
a quarter of the price of Innerbond. In addition, a thin layer of car carpet has
been used to cover the outside of the tube & this was glued into place using
contact adhesive.
Parts List & Costs
1 10-inch sub-woofer, Jaycar
Electronics Cat. CW-2166,
$109
1 1-metre length of 32cm-dia.
stormwater pipe, $55
1 10-inch speaker grille, Jaycar
Electronics Cat. AX-3522, $14
1 1-metre length of 150cm-wide
quilt wadding, $5
1 1-metre length of car carpet,
$5
Miscellaneous: screws, “Liquid
Nails” glue, scrap 16mm-thick
medium-density fibreboard
(MDF) for tube end pieces,
loudspeaker terminal, speaker
cable, $20
Total Cost: $208 each
a 50mm-diameter hole to accept the
vent tube. An electric jig-saw was used
to make these cutouts.
The end pieces are held in place by
countersunk wood screws inserted
from the periphery of the pipe, with
16 screws and a sealant/adhesive (eg,
“Liquid Nails”) used to ensure an airtight seal at each end. Note that screws
with parallel sides (not tradition
al
woodscrews) should be used to get
maximum purchase when screw
ing
March 1995 17
The two bass tubes are
held in position inside
the boot using brushed
aluminium straps. On
the left is the amplifier
which drives both the
bass tubes & also the
rear deck-mounted
3-way loudspeakers.
into MDF. The large number of screws
(16) proved necessary to ensure an
airtight seal. Even tiny leaks can allow
whistles and buzzes.
Each tube was lined with a soft
acrylic filling. This prevents reflections within the tube, which colour
the sound and give the bass a hollow
timbre. Innerbond speaker-box filling
is available for about $9 a metre but
very similar material can be bought
from dressmaking shops under the
name of quilt wadding. In this form,
it’s about a quarter of the price.
After testing various drivers, it was
decided that the Jaycar CW-2166 had
the right mix of low cost ($109) and
performance. This woofer uses a rigid
cast frame and has a polypropylene
cone. Its free air resonance is 31Hz,
while its power handling capability
is quoted as 120 watts RMS and the
sensitivity as 91dB. In addition, its Qts
is a low 0.33, allowing it to be used in
compact enclosures.
In fact, the enclosure design recommended by Jaycar is perfect for use
as a bass tube – a volume of 45 litres
(with the acrylic filling, the tube I used
would be very close to this figure),
coupled with a vent 50mm in diameter
and 54mm long. The speaker’s impedance is 6 ohms.
Testing
Testing was initially done using an
Akai 45W RMS/channel home stereo
amplifier and a standard graphic
equalizer. Also used was a frequency
generator. By feeding the frequency
generator output to the sub-woofer
via the amplifier, the frequency re
Fig.1: this graph plots the performance of the author’s system. With the +12dB at 45Hz amplifier
equalization switch activated, there is a peak in the frequency response of about 12dB at 31.5Hz.
18 Silicon Chip
This is the view from the inside of the cabin when the rear seat is folded down.
The sub-woofers are reasily removed when the full volume of the boot is needed
by undoing eight wing-nuts & unplugging two cables. Even with the seat back in
its normal position, the bass is sufficient for most people!
sponse (and any peaks or troughs)
could be roughly determined by ear.
In a domestic situation, the response
sounded smooth but with plenty of
punch. The next step was to mount
one of the tubes in a car.
My car sound system uses a mix of
original and aftermarket equipment.
The original Subaru front-end comprising a radio-cassette player and
single CD player has been retained.
The two front channels of this original
system are used to drive the original
dual-cone 6-inch speakers mounted
in the front doors, along with a pair
of Jaycar Super Tweeters which have
been added to the front door sail areas
(the triangular areas where the rear
vision mirrors are).
The two rear channels are used
to drive the speaker-level inputs
of a Coustic AMP-268 4 x 45W car
amplifier and two of its outputs in
turn drive rear deck-mounted Jaycar
6 x 9 3-way speakers. The other two
channels of this amplifier were used
to drive the twin sub-woofers via a
built-in variable low-pass crossover
network.
With just one of the bass tubes connected, the bass was superb. The driver
A steel mesh grille costing $14 was
used to protect the driver. It is held
in place using brackets & roundhead
screws.
showed no signs of being overloaded,
even when driven by the amplifier in
high-power bridged mono mode. In
fact, my reaction was that if the bass
was this good with just one bass tube,
what would it be like with two? The
answer is even better.
Frequency response plot
A visit to Adelaide car sound dealer
Cartronics was made so that a Coustic
Real Time Analyser could be used to
check the system. This is effectively a
spectrum analyser which records and
prints the system’s in-car response.
With the system being driven by a
CD-recorded pink noise signal, and
with the +12dB at 45Hz amplifier
equal
ization switch activated, the
graph showed a peak in the frequency
response of about 12dB at 31.5Hz.
Being the sort of person who likes
lots of bass, I am happy to leave the
system with this boosted low-frequency response. On the other
hand, purists could simply reduce
the switched amplifi
er bass boost
to achieve a flatter response. Either
way, the sub-woofers showed that
they were capable of reproducing low
SC
frequencies with ease.
March 1995 19
This photo shows the prototype ACS decoder
installed in an old Harman Kardon AM/FM stereo
receiver. Two aluminium brackets were used to
suspend the decoder above the tuner board.
A subcarrier decoder
for FM receivers
Many FM stations are now radiating piggyback
signals with their normal stereo transmission.
You can’t decipher these “hidden” signals using
a standard FM receiver but you can by adding
this low-cost ACS decoder.
By JOHN CLARKE
The jargon doesn’t sound very
enlightening but ACS stands for Ancillary Communication Service. This
is a technique whereby a normal FM
broadcast transmitter carries one or
two extra subcarrier signals that ride
“piggyback” along with the normal FM
stereo transmission.
These hidden transmissions have
no affect on standard FM mono and
20 Silicon Chip
stereo receivers. Only the main signal
can be detected by such receivers, so
most people are unaware that ACS
signals are even being broadcast. To
listen to these extra signals, you need
to fit an ACS decoder such as the unit
described here to your FM receiver.
Despite this, you’ve probably already heard ACS broadcasts. Many
department stores and shopping cen-
tres now use this service to provide
background music for their customers.
And the program content is usually
just straight music, with no voiceovers or advertising.
Other ACS services include foreign
language, news and special interest
programs.
Signal transmission
Before we describe how our ACS
decoder works, let’s take a look at
how the ACS signals are added to the
FM signal.
A normal FM stereo transmission
is made up of three components: (1)
an L+R mono signal modulated from
0-15kHz; a stereo pilot tone at 19kHz;
and a multiplexed L-R difference
signal centred on 38kHz. These com-
Fig.1: the ACS signals are produced by
modulating subcarriers centred on 67kHz
& 92kHz. These subcarriers are then mixed
with the normal FM stereo components &
used to modulate the main carrier.
% MODULATION
CARRIER
STEREO
CHANNEL
STEREO
PILOT
0
15
19
67kHz ACS
CHANNEL
23
38
53
59
67
92kHz ACS
CHANNEL
75
84
92
100
FREQUENCY (kHz)
ponents are mixed together and used
to modulate the main carrier out to
53kHz – see Fig.1.
By contrast, the ACS signals are
produced by modulating subcarriers
centred on 67kHz and 92kHz. These
two frequencies are well above the
upper limit of the L-R difference signal to avoid interference. As a further
precaution against interference, the
ACS signal bandwidths are limited to
just 6kHz. They are mixed at low level
with the existing stereo components
before being used to modulate the
main carrier.
ACS decoding
At the receiving end, these ACS
subcarrier signals are ignored by a
standard FM receiver since they fall
well outside the passband. In fact, the
detected 67kHz and 92kHz subcarriers
are effectively removed by the 50µs
de-emphasis filtering. So, to detect
ACS signals, we need to modify the
receiver by fitting an ACS decoder
immediately following the FM de
modulator, before any filtering takes
place.
The ACS decoder described here
can be switched to decode either ACS
subcarrier (ie, either 67kHz or 92kHz).
This is done using a single toggle
switch; there are no other controls
to worry about. The recovered audio
67kHz AND 92kHz
INPUTS FROM
FM
DEMODULATOR
decoder inside a separate case and
run it from a suitable DC plugpack
supply. We’ll have more to say about
the installation later on.
Block diagram
Fig.2 shows the block diagram of
the ACS Decoder. Its input signal is
extracted from the FM demodulator
in the receiver and is fed to two bandpass filter stages centred on the ACS
subcarri
er frequencies. These filters
separate the ACS subcarriers from each
other and from the other components
of the normal FM stereo signal.
S1a selects between the filter outputs, after which the selected sub
carrier is boosted by amplifier stages
IC2a-IC2c. The boosted signal is then
fed into a phase lock loop (PLL) de
modulator to recover the audio.
Immediately following the PLL
stage is a 150µs de-emphasis stage.
This rolls off frequencies above
1061Hz, thereby reducing noise in the
audio signal and compensating for the
150µs boost (pre-emphasis) given to
the audio signal before transmission.
Finally, the recovered audio is fed to
the output via a low pass filter which
removes the original subcarrier plus
any other un
w anted components
above 6kHz.
In summary then, the 67kHz and
92kHz subcarriers are first separated
S1b
67kHZ
BANDPASS
FILTER
IC1a,IC1b
output is fed into an auxiliary input
of an amplifier.
Once fitted, the unit is very easy to
use. All you have to do is tune your
receiver to an FM station and select
the appropriate auxiliary input on the
amplifier. An ACS signal will now be
heard (provided, of course, that the
station is transmitting ACS signals).
If the station is transmitting two ACS
signals, the alternative signal can then
be selected using the toggle switch.
Provided you live in a good signal
area and have a reasonable antenna,
the ACS signal should be quite clean.
But don’t expect it to sound as good
as a regular FM stereo signal. That’s
because of the restricted bandwidth
(6kHz) and the fact that the signal is
mono only. In addition, an ACS signal
has only relatively low deviation, so
you’ll need a strong signal to avoid
hiss.
It should be possible to fit the ACS
Decoder to most FM tuners and receivers, and even to many portable
FM receivers. Basically, there are a
couple of ways you can go about this.
First, if there is sufficient room, the
unit can be fitted inside the receiver
itself and powered from an existing
supply rail. In fact, the prototype was
fitted inside an old Harman Kardon
receiver – see photos.
Alternatively, you could mount the
S1a
6kHz
12dB/OCTAVE
LOWPASS
FILTER
AMPLIFIERS
IC2a-IC2c
PHASE LOCK
LOOP
DEMODULATOR
150us
DE-EMPHASIS
ACS
AUDIO
OUTPUT
92kHz
BANDPASS
FILTER
IC1c,IC1d
Fig.2: block diagram of the ACS decoder. The 67kHz & 92kHz subcarriers are separated out using
bandpass filters & the selected subcarrier then amplified & fed to a PLL demodulator to recover the
audio. Finally, the recovered audio is filtered & fed to the output.
March 1995 21
22 Silicon Chip
DEMODULATED
FM
560pF
INPUT
10k
.0033
.0015
1.1k
9
10
10k
10k
1k
.0047
B
C
VIEWED FROM
BELOW
E
10k
1.1k
13
12
.0033
.0015
VCC/2
I GO
92kHz TWIN TEE FILTERS
560
.0015
1.1k
8
2
3
.0027
VCC/2
67kHz TWIN TEE FILTERS
430
1k
.0047
IC1c
10k
7
.0027
1k
4
IC1a
6 TLO74
11
5
.0027
VCC/2
10k
VCC/2
10
+12V
10k
IC1d
10k
IC1b
560
.0015
1.1k
14
430
.0027
1k
1
.01
10k
S1a
2
4
12
5
0V
+15-30V
PHASE LOCK LOOP
DEMODULATOR
22k
COMP OUT
VCO IN
9
VCO OUT
IC3
4046
7
VCO
16
1
B
150us
DE-EMPHASIS
.015
10k
GND
10
16VW
1k
Q1
BC548
POWER SUPPLY
VR1
10k
10k
11
IC2b
AMPLIFIERS
5
6
100k
10pF
REG1
IN 7812 OUT
10k
10k
10
10
10
35VW
8
DEMOD
IC2a
3 TLO74
2
92kHz
.0015
10k
6
VCO
14
INPUT
3
COMP IN
67kHz
S1b
.0027
VCC/2
220pF
ACS DECODER
92kHz
67kHz
100k
10pF
4.7k
4.7k
E 0.68
C
7
220pF
10
16VW
10
9
VCC/2
+12V
6kHz FILTER
12
13
IC2c
0.1
.0033
3k
VCC/2
.012
6.2k
6.2k
10k
8
4
14
+12V
.01
ACS
AUDIO
OUT
1
11 100
IC2d
100k
100k
10pF
PARTS LIST
1 PC board, code 06303951,
137 x 80mm
1 DPDT toggle switch (S1)
11 PC stakes
1 10kΩ 5mm horizontal trimpot
(VR1)
Semiconductors
2 TL074 quad op amps (IC1,IC2)
1 4046 CMOS phase-lock loop
(IC3)
1 7812 12V regulator (REG1)
1 BC548 NPN transistor (Q1)
This close-up view shows the completed ACS decoder board. It should fit inside
most FM tuners & receivers & can be powered from an existing 15-30V DC
supply rail. Note that the decoder will not interfere with the reception of normal
FM stereo transmissions.
out using bandpass filters. The selected subcarrier is then amplified and fed
to a PLL demodulator to recover the
audio. Finally, the recovered audio is
filtered and fed to the output.
Circuit details
Refer now to Fig.3 for the circuit
details. This can be directly related
back to the block diagram. IC1a & IC1b
form the 67kHz bandpass filter, IC1c &
IC1d form the 92kHz bandpass filter,
IC2a-IC2c are the amplifier stages, IC3
is the PLL demodulator, and IC2d is
the 6kHz low pass filter.
In greater detail, the input signal is
picked off from the FM demodulator
via a 560pF capacitor and coupled
to pin 6 of IC1a via a 10kΩ resistor.
IC1a and IC1b together function as
cascaded twin-T filter stages centred
on 67kHz. In the case of IC1a, the two
1kΩ feedback resistors and the .0047µF
Fig.3 (left): the final circuit is based
on two quad op amps (IC1 & IC2) &
a 4046 PLL (IC3). Twin-T filter stages
IC1a & IC1b form the 67kHz bandpass
filter, while IC1c & IC1d form the
92kHz bandpass filter. The selected
signal is then amplified by IC2a-IC2c
& demodulated by the PLL. Q1 buffers
the demodulated signal, while IC2d
rolls off the response above 6kHz to
reduce noise.
capacitor to ground form one half of
the twin-T filter, while the two .0027µF
capacitors and the 430Ω resistor form
the second half of the filter.
Because the twin-T filter network
has a high impedance at 67kHz, IC1a
essentially functions with a gain
of one at this frequency due to the
10kΩ feedback resistor. At the same
time, frequencies on either side of the
67kHz centre frequency are heavily
attenuated by the filter action. So
IC1a allows the 67kHz subcarrier to
pass through while drastically curtailing frequencies that are outside
the passband.
The output of IC1a appears at pin
7 and is fed to a second twin-T filter
stage based on IC1b. Note that cascaded filter stages have been used here
to ensure adequate attenuation of the
adjacent stereo signals and the ACS
subcarrier at 92kHz. Filter stages IC1c
& IC1d operate in identical fashion to
IC1a & IC1b, except that their passband
is centred on 92kHz.
Switch S1a selects between the two
subcarrier frequencies and feeds the
resulting signal to IC2a via a 220pF
capacitor and a 10kΩ input resistor.
IC2a, IC2b and IC2c each function as
inverting amplifier stages with a gain
of 10 and thus provide an overall
gain of 1000. The 220pF capacitors
at the inputs of IC2a & IC2c roll off
the response below 67kHz, while the
three 10pF feedback capacitors limit
Capacitors
1 10µF 35VW PC electrolytic
4 10µF 16VW PC electrolytic
1 1µF 16VW PC electrolytic
1 0.68µF MKT polyester
1 0.1µF MKT polyester
1 .012µF MKT polyester
2 .01µF MKT polyester
2 .0047µF MKT polyester
3 .0033µF MKT polyester
5 .0027µF MKT polyester
5 .0015µF MKT polyester
1 560pF ceramic or MKT polyester
2 220pF ceramic
3 10pF ceramic
Resistors (0.25W, 1%)
4 100kΩ
4 1.1kΩ
1 22kΩ
5 1kΩ
14 10kΩ
2 560Ω
2 6.2kΩ
2 470Ω
2 4.7kΩ
1 100Ω
1 3kΩ
Miscellaneous
Hook-up wire, solder, mounting
brackets, screws, nuts, etc.
the high frequency response to reduce
noise in the signal.
Demodulation
IC3, a 4046 phase lock loop IC, has
everything we need to decode the FM
signal. It contains two phase comparators, a voltage-controlled oscillator
(VCO) and a source follower.
The signal from IC2c is AC-coupled
to pin 14, after which it is buffered
and fed to a phase comparator. This
compares the incoming frequency
with the VCO frequency at pin 4 and
produces an output at pin 2. This
output is then filtered and applied to
pin 9. It controls the VCO so that it
March 1995 23
6
1
2
3
Fig.4: install the parts on the PC board as shown
here, taking care to ensure that all polarised
parts are correctly oriented. It is a good idea to
use PC stakes at all external wiring points.
1uF
2
3
10k
10k
0.68
.012
Q1
VR1
10k
.01
1k
6.2k
3k
100k
220pF
1.1k
560
1.1k
1.1k
1.1k
560
1 10uF
22k
10uF
remains in lock with the input signal.
The filtered VCO control voltage
represents the phase dif
ference between the incoming signal and the
VCO signal and thus represents the
audio modulation on the subcarrier.
However, rather than extracting the
demodulated audio directly from
pin 9, it is taken from the output of
the internal source follower at pin 10
instead. This ensures that we don’t
load down the VCO control signal and
create further distortion.
6 .0015
10k
.0033
.0033
IC3
4046
10k
10pF
6.2k
4.7k
4.7k
10k
10k
2x.0015
0.1
100
IC2
TLO74
10uF
10k
5
1
1
IC1
TLO74
10k
REG1
.0027 4
10k
560pF
.0033
10uF
100k
1
10k
2x.0015
10uF
35VW
100k
10k
1k
100k
10pF
2x.0027
10k
DEMODULATED
FM INPUT
10pF
.01
.0027
220pF
10k
10k
.0027
430
1k
.0047
1k
1k
430
.0047
ACS
AUDIO
OUT
GND
S1
+15-30V
INPUT
5
GND
4
.015
S1b selects the free-running VCO
frequency by switching in the appropriate capacitor value between pins
6 & 7. When the .0027µF capacitor is
selected, the VCO free-runs at 67kHz.
Alternatively, when the .0015µF capacitor is selected, the VCO free-runs
at 92kHz. VR1 sets the centre frequency and the locking range.
Immediately following the PLL is
the 150µs de-emphasis network. This
network is simply a low-pass filter
and consists of a 10kΩ resistor and a
.015µF capacitor. The filtered signal
is then buffered by emitter-follower
stage Q1 and fed to the 6kHz lowpass filter stage (IC2d). Two 6.2kΩ
resistors, a .0033µF capacitor and a
.012µF capacitor make up the filter
components.
This stage operates with a gain of -1
for frequencies below 6kHz and rolls
off the response at 12dB per octave for
higher frequencies. Its output appears
at pin 14 and is coupled to the output
terminals via a 100Ω resistor and a
RESISTOR COLOUR CODES
❏
No.
❏ 4
❏ 1
❏
14
❏ 2
❏ 2
❏ 1
❏ 4
❏ 5
❏ 2
❏ 2
❏ 1
24 Silicon Chip
Value
100kΩ
22kΩ
10kΩ
6.2kΩ
4.7kΩ
3kΩ
1.1kΩ
1kΩ
560Ω
470Ω
100Ω
4-Band Code (1%)
brown black yellow brown
red red orange brown
brown black orange brown
blue red red brown
yellow violet red brown
orange black red brown
brown brown red brown
brown black red brown
green blue brown brown
yellow violet brown brown
brown black brown brown
5-Band Code (1%)
brown black black orange brown
red red black red brown
brown black black red brown
blue red black brown brown
yellow violet black brown brown
orange black black brown brown
brown brown black brown brown
brown black black brown brown
green blue black black brown
yellow violet black black brown
brown black black black brown
ACS SUBCARRIER SIGNALS PICKED OFF HERE
Fig.5: as with most FM tuners, the Sony ST-JX220A uses two ICs to do most
of its FM processing. These are: (1) an IF amplifier & demodulator IC; & (2) a
following multiplex (MPX) stereo decoder IC. The most convenient point to pick
off the subcarrier signals is at the output of the demodulator (detector) IC.
1µF capacitor. The associated 100kΩ
resistor prevents large offset voltages
from appearing at the output.
Power for the circuit can be derived
from just about any +15-30V rail (normally from inside the receiver). This
is fed to 3-terminal regulator REG1 to
derive a +12V supply rail. In addition,
a half-supply rail (Vcc/2) is derived
via a voltage divider consisting of two
4.7kΩ resistors and this biases all the
non-inverting inputs of the various op
amp stages.
Construction
All of the parts for the ACS Decoder
except switch S1 are installed on a PC
board coded 06303951. Fig.4 shows
the assembly details.
No particular order of assembly
need be followed but we suggest that
you start by installing PC stakes at the
11 external wiring points. The two
wire links can then be installed, followed by the resistors, capacitors and
ICs. Make sure that the ICs are correctly
oriented and use your multimeter to
check each resistor value before installing it, as some of the colours can
be difficult to decipher.
Finally, complete the board assembly by installing VR1, transistor Q1
and REG1. Note that REG1 is mounted
flat against the PC board with its leads
bent at right angles and is secured
using a screw and nut. Don’t bother
wiring up the switch at this stage;
that step comes later, when the unit
is installed inside a receiver.
(check the ICs and the regulator).
Assuming all is well, check that the
regulator output is at +12V. You should
also find this voltage on pin 4 of IC1,
pin 4 of IC2 and pin 16 of IC3. Finally,
check that +6V is present on pins 3, 5,
10 & 12 of both IC1 and IC2.
Initial tests
Installation
Once the board assembly has been
completed, connect your multimeter
in series with the +15V supply input
and apply power. A 12V DC plugpack
will make suitable temporary power
supply, as it will have a no-load output
of about 17V DC and will only be lightly loaded. Check that the quiescent
current is no more than about 25mA
(no input signal).
If it is much more than this, switch
off immediately and locate the source
of the problem before proceeding
The ACS Decoder can be mounted
inside the receiver using suitable
brackets and the toggle switch mount
ed on the rear panel. This done, the
switch can be wired to the PC board
using rainbow cable – see Fig.4. The
power supply connections (+15-30V
& ground) can be run using hook-up
wire.
Ideally, you should have a circuit
diagram of your receiver so that you
can find a suitable supply rail. Important: make sure that the ACS Decoder
and all connecting leads are kept well
away from any mains wiring inside
the receiver. In addition, you should
run a separate earth lead between the
switch body and the metal chassis if
the switch is not earthed via the rear
panel (eg, if the rear panel is plastic).
If you are installing the decoder inside a receiver, the audio output lead
can be internally connected to a spare
pair of line input sockets (eg, aux).
This lead can be run using light-duty
hook-up wire. Note that you will have
to connect the two sockets in parallel,
since the decoder only has a single
mono output.
Alternatively, if the board is mount
ed inside an FM tuner, the decoder’s
output can be run to an additional
RCA socket installed on the rear
CAPACITOR CODES
❏
❏
❏
❏
❏
❏
❏
❏
❏
❏
❏
❏
Value
IEC
EIA
0.68µF
680n
684
0.1µF
100n
104
0.012µF
12n
123
.01µF
10n
103
.0047µF
4n7
472
.0033µF
3n3
332
.0027µF
2n7
272
.0015µF
1n5
152
560pF
560p
561
220pF
220p
221
10pF 10p 10
March 1995 25
Fig.6: this is the full-size
etching pattern for the PC
board. Check your board
carefully for possible
defects before installing
any of the parts.
panel. This audio output can then be
connected via a Y-adapter shielded
cable to the line inputs on your stereo
amplifier.
You now have to find the signal
at the output of the demodulator. In
a stereo tuner, this comes before the
multiplex decoder and treble de-emphasis networks. In a mono tuner,
you must tap into the demodulated
output before de-emphasis has taken
place. After de-emphasis, the ACS
subcarriers will be non-existent as
we’ve already pointed out.
Fig.5 shows a typical FM tuner circuit (Sony ST-JX220A) as an example.
As with most such tuners, it uses two
ICs to do most of its FM processing.
These are: (1) an IF amplifier & detector IC; and (2) a following multiplex
(MPX) stereo decoder IC. The most
convenient point to pick off the sub
carrier signals is at the output (in this
case, pin 6) of the detector IC.
Alternatively, the signal can be
picked up at the input to the multiplex
decoder IC.
A suitable power supply rail for the
decoder can usually be picked up
from the regulator board inside the
receiver.
Testing
The ACS Decoder should initially be
tested with S1 set to 67kHz and VR1 at
mid-position. Apply power and tune
in one of your regular FM stations.
This done, select the ACS decoder
(using the selector switch on the amplifier) and check for the presence of
an ACS signal. If no signal is heard, try
adjusting VR1 until a signal is heard.
Failing this, retune to another station
and try again.
When an ACS station comes up,
adjust VR1 for best signal, then switch
to the 92kHz position and adjust VR1
again so that both ACS signals can be
heard. If no signal is present on 92kHz,
try other stations in turn until you find
one that’s broadcasting ACS signals on
both frequencies.
Copyright
The signal for the prototype ACS decoder was derived by soldering the input
lead directly to the output pin of the demodulator IC in the Harman Kardon
receiver. If you don't have a circuit diagram of your receiver, use a CRO to
determine which pin is the demodulated output. Alternatively, you may have to
test each pin of the demodulator IC on a trial & error basis until an ACS signal
is heard.
26 Silicon Chip
Finally, readers are warned that recording or broadcasting received ACS
programs without proper authorisation may breach copyright. If you have
any doubts about your obligations,
check with the copyright holder. SC
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
Build a 50W/channel
stereo amplifier
Looking to upgrade your system with a
new amplifier? This new stereo amplifier
is easy to build & does not need setting-up
adjustments. Most importantly, it will give
excellent sound quality & up to 50 watts per
channel into 8-ohm loads.
By LEO SIMPSON & BOB FLYNN
Our last integrated stereo amplifier
design was presented in the March &
April 1992 issues of SILICON CHIP but
it is now obsolete because the power
transistors specified are no longer
available. This new design is based on
the 50W per channel stereo amplifier
module presented last month.
While this new amplifier offers very
similar facilities to the unit referred to
above, it is a completely new design
with a much wider chassis and all
32 Silicon Chip
new PC boards. And while the super
sed
ed design had an inbuilt RIAA
preamplifier for phono cartridges, in
the new amplifier the RIAA preamp is
an optional extra board. We took this
approach because many people these
days do not have any vinyl records
or a turntable so they don’t want the
RIAA preamp.
Leaving the RIAA preamplifier out
also has the advantage that you have
an extra pair of line level inputs (ie,
suitable for CD, tuner or other program
source).
The overall design approach to this
amplifier has been middle of the road.
We have not taken the spartan European approach with virtually no controls
except for the volume knob and nor
have we sought to incorporate every
feature found in expensive Japanese
amplifiers. Still, it does have all the
features that most people want and
will use. For example, while it does
include tone controls, it also has a
switch to disable them, to obtain a
completely flat frequency response.
Let us now talk about the features
in some detail.
Features
The new SILICON CHIP 50W Stereo
Amplifier is housed in a low profile
case measuring 435mm wide, 95mm
high and 320mm deep, including
knobs rubber feet and rear projections.
Specifications
Power Output
47W into 8-ohm loads, both channels driven; 57W into 8-ohm loads with
one channel driven.
Frequency Response
High level inputs: within ±1dB from 10Hz to 50kHz
Phono inputs: RIAA/IEC within ±0.5dB from 20Hz to 20kHz.
Total Harmonic Distortion
Typically less than .05% (see graph).
Signal-to-Noise Ratio
High level inputs (CD, Tuner, etc): 99dB unweighted (20Hz to 20kHz) with
respect to rated output (with volume at maximum) with Tone Defeat switch
in or out; 100dB A-weighted under the same conditions.
Phono (moving magnet): 83dB unweighted (20Hz to 20kHz) with respect
to 10mV input signal at 1kHz & rated output with 1kΩ resistive input termination; 88dB A-weighted under the same conditions.
Channel Separation
-78dB at 100Hz; -81dB at 1kHz; & -61dB at 10kHz with respect to rated
output & with undriven channel input loaded with a 1kΩ resistor.
Above: the new SILICON CHIP 50W
per channel amplifier offers all the
facilities expected on a modern stereo
amplifier &, in addition, it has a
separate headphone amplifier.
Input Sensitivity
Phono inputs at 1kHz: 4.3mV
High level inputs: 235mV
Tone Controls
Bass: ±13dB at 50Hz.
Treble: ±13dB at 10kHz
Damping Factor
>56 from 100Hz to 10kHz (for 8Ω loads)
Stability
Unconditional
It has the usual line-up of controls
found on most amplifiers: bass, treble,
balance, input selector, tape monitor
switch, tone defeat switch and volume
control. It also has a stereo/mono
switch, headphone socket and power
switch. Plugging into the headphone
socket disables the main power amplifiers and engages a separate high
quality low power stereo amplifier to
drive the headphones directly. This
now only gives better reproduction
via headphones but it also simplifies
the internal wiring.
Block diagram
Now let’s have a look at the circuit
features which are depicted in the
The new 50W Stereo amplifier uses this 50-watt/channel stereo power module, as described in the previous
issue. It’s based on two monolithic power ICs to give a rugged, compact design that requires no adjustments.
March 1995 33
POWER
AMPLIFIER
IC4
OPTIONAL RIAA
PREAMPLIFIER
IC5
AUX 3/
PHONO
CD
x23
x56
OUT
SOURCE
MONITOR
S2
TONE
S5
TAPE
PREAMPLIFIER
IC1
TUNER
VCR
AUX 1
VOLUME
VR1
SOURCE
S1
AUX 2
TAPE
OUT
TAPE
IN
S6
x4.2
IN
TONE
CONTROLS
IC2
POWER
AMPLIFIER
HEADPHONES
HEADPHONE
AMPLIFIER
IC3
x5.7
MONO
SPEAKER
HEADPHONES
MODE
S3
STEREO
TO OTHER CHANNEL
TO
OTHER
CHANNEL
BALANCE
S4
Fig.1: the circuit features of the new stereo amplifier
are illustrated in this block diagram. To keep things
simple only one channel is shown. Note the separate
amplifier to drive the headphones.
TO OTHER CHANNEL
block diagram of Fig.1. This shows
only one channel, to keep things
simple. All the circuit functions are
duplicated in the second channel.
S1 is the 6-position selector switch
and it feeds the tape output as well
as the Tape Monitor switch S2. S2
selects the signal from the input
selector S1 or from a cassette deck
connected to the Tape In inputs. The
signal then goes to S3, the stereo/
mono switch which shorts the two
channel signals together when in the
mono setting.
Following S3, the signal is fed
to the 11-position balance control
switch S4 and the volume control
potentiometer VR1. The use of a
rotary switch for the balance control
is unusual but there are good reasons
for this approach. In past designs we
have specified a special dual ganged
potentiometer known as an M/N type.
This has half the resistance track in
each channel shorted out to give a
good balance control action and is
the same as used in most domestic
stereo amplifiers.
However, this type of balance control has become difficult to obtain
34 Silicon Chip
and so we initially took a different
approach, using a single linear potentiometer with the ends connected to
the signal in either channel and the
wiper connected to signal earth. This
approach is cheap but does not work
particularly well, for two reasons.
First, it has very little apparent effect
over most of the middle range of the
pot – all the attenuation is cramped
into the extreme ends of rotation.
Second, because the resistance of the
wiper itself is quite high, and this
resistance is common to the signal
path in both channels, the separation
between channels is seriously degraded, to a figure of about 25dB.
Now while -25dB separation between channels is adequate to produce
a convincing stereo effect, it is far
below what the circuit is otherwise
capable of. One approach used by
some amplifier manufacturers is to use
a linear potentiometer with a centre
tap connection. This gets around the
problem of the wiper resistance but
it still has all its control action con
centrated at the extremes of rotation.
In any case, such potentiometers are
also difficult to obtain.
Our approach was to use an 11-position rotary switch with resistors wired
around it. The resistors are arranged
to progressively reduce the gain of the
attenuated channel by about 2dB. So
from the centre position, the gain of
each channel can be varied by -2dB,
-4dB, -6dB, -8dB and then completely
off. This works reasonably well and
has the advantage of giving good channel separation.
Following the volume control, the
signal goes to a non-inverting op amp
stage with a gain of 4.2. From there,
it goes to the unity gain tone control
stage which can be switched out of
circuit by the Tone defeat switch, S5.
After the tone defeat switch, the
signal goes to switch S6 which is part
of the headphone socket. It normally
Fig.2 (right): this diagram shows the
circuit of one channel of the new
amplifier & the power supply which is
common to both channels. The RIAA
preamplifier (not shown) is optional &
can be omitted, giving another pair of
line level inputs.
March 1995 35
E
10k
C
-15V
E
5.6k
B
33pF
C
5.6k
D2
1N914
7(1)
D1
1N914
47k
IC3a
6(2) TLO72
5(3)
TO
S6a
+15V
VIEWED FROM BELOW
B
10k
TAPE
IN
TAPE
OUT
AUX2
AUX1
VCR
TUNER
CD
AUX3/
PHONO
GIO
7915
A
MONO
OTHER
CHANNEL
E
N
240VAC
A
1.6k
F1
1A
CASE
S7
.01
250VAC
OTHER
CHANNEL
1.6k
820W
1.6k
4.7k
91k
91k
4.7k
1.6k
820W
1k
HEADPHONES
OTHER
CHANNEL
STEREO
MODE
S3A
82
K
1k
TAPE
50W STEREO AMPLIFIER
I GO
7815
E
Q2 C
BC327
B
15
15
E
Q1
BC337 C
B
SOURCE
S1a
1k
SOURCE
MONITOR
S2a
OPTIONAL
PHONO PREAMP
T1
1
25V
25V
BALANCE
S4
VOLUME
VR1a
50k LOG
4.7k
6(2)
1k 5(3)
4700
50VW
4700
50VW
BR1
KBPC10-4
11
TO
HEADPHONE
AMPLIFIER
100k
1
15k
7(1)
22k
1
4.7k
2x330
1W
-35V
47
63VW
47
63VW
IN
REG2
7915
GND
GND
OUT
100
16VW
100
16VW
+35V
REG1
2x330
7815
1W
OUT
IN
L1 : 16T 0.5mm DIAMETR
ENAMELLED COPPER WIRE
WOUND ON 10 1W
RESISTOR
100pF
IC1a
LM833
22
BP
22k
TREBLE
VR3a
25k LIN
-15V
GND
8
100
16VW
4
*0.1
5.6
1W
F3
2A
100
16VW
100
16VW
100
16VW
100
16VW
*SEE TEXT
100
63VW
3
100
63VW
10
1W
LED1
3.9k
0.5W
8W
+35V
7(1)
-35V
L1
0.7uH
F2
2A
IC2a
5(3) LM833
6(2)
CONTROL BOARD FILTERING
0.1
0.1
5
0.1
100
16VW
39k
22k
7
IC4
LM3886
1
22k
6.8
S6a BP
0.1
33pF
TONE CONTROLS
S5a
IN
4.7k
22k
OUT
.0047
22
16VW
9
10
AMP
+15V
47
16VW
1k
220pF
1k
100W
PHONES
.0047
22k
BASS
VR2a
100k LIN
.01
Fig.3: this graph shows the frequency response of the tone controls at their
maximum boost & cut settings & also at the flat setting.
AUDIO PRECISION FREQRESP AMPL(dBr) & AMPL(dBr) vs FREQ(Hz)
5.0000
14 JAN 95 20:39:02
5.000
4.0000
4.000
3.0000
3.000
2.0000
2.000
1.0000
1.000
0.0
0.0
-1.000
-1.00
-2.000
-2.00
-3.000
-3.00
-4.000
-4.00
-5.000
-5.00
20
100
1k
10k
50k
Fig.4: the frequency response of the headphone amplifier, with the right channel
dotted.
feeds the audio signal through to the
following power amplifier but when
the headphone jack is inserted, the
signal is diverted to the headphone
amplifier.
Circuit description
The complete circuit diagram,
except for the optional RIAA preamplifier, is shown in Fig.2. The three
36 Silicon Chip
op amps are shown as IC1a, IC2a
and IC3a and each is half of a dual
low noise op amp. The pin numbers
for the other halves which are in the
second channel, IC1b, IC2b and IC3b,
are shown in brackets on the circuit.
For example, the non-inverting (+)
input for IC1a is pin 5 while the
corresponding input for IC1b is pin
3 (shown in brackets).
IC1a is the non-inverting op amp
with a gain of 4.2, as set by the feedback resistors connected to pin 6.
Besides providing gain and a high
impedance load for the volume control pot, IC1a acts as a low impedance
source for the tone control stage, IC2a.
This has the tone controls connected
in the negative feedback network.
When the bass and treble controls
are centred (ie, in their flat settings),
the gain of stage is unity, up to at
least 50kHz.
Winding the bass or treble controls
towards the input side of IC2a (ie,
applying boost) increases the gain for
frequencies above 2kHz for the treble
control and below 300Hz for the bass
control. When the tone controls are
rotated in the opposite direction (applying tone cut), the gain is reduced
above 2kHz and below 300Hz. This
is because the negative feedback has
been increased, giving a reduction in
gain at these frequencies.
The amount of treble boost and cut
provided by IC2a is limited by the
4.7kΩ resistors on either side of the
25kΩ treble pot, VR3a. Similarly the
maximum bass boost and cut is limited
by the 22kΩ resistors on either side of
the bass pot, VR2a. Fig.3 shows the
action of the tone controls at their
maximum boost and cut settings and
also at the flat setting.
Note how S5a, the Tone Defeat
switch, bypasses the tone control circuitry. Its output feeds a 6.8µF bipolar
capacitor which is there to block DC
from the tone control stage from getting into the input of the headphone
amplifier.
Headphone amplifier
Following the 6.8µF capacitor and
headphone switch S6a is the head
This prototype amplifier uses five PC boards, including the optional RIAA
preamplifier which is adjacent to the selector switch. No setting up adjustments
are required for the power amplifiers.
phone amplifier which consists of
op amp IC3a in combina
tion with
transistors Q1 and Q2. The transistors
are there to boost the output current
capability of the TL072 op amp. They
are slightly forward-biased (to keep
crossover distortion to a minimum)
by the two diodes connected between
the bases. Any distortion produced by
the transistors is also minimised by
incorporating them inside the feedback network for the op amp.
The output current of the head
phone amplifier is limited by the
15Ω emitter resistors and the 82Ω
output resistor. This provides short
circuit protection and protects the
headphones against damage in the
unlikely event of the amplifier being
damaged. Fig.4 shows the frequency
response of the headphone amplifier,
with the right channel dotted.
Power amplifiers
As noted above, the power amplifiers are the stereo 50W module
described last month. For the sake of
completeness and for those who did
not see the previous article, we repeat
the circuit description.
IC4 is an LM3886 monolithic power
amplifier module with balanced supply rails and direct coupling to the
loudspeaker load. It is very similar to
the LM3876 50W module featured in
the March 1994 issue of SILICON CHIP.
The input signal which comes via the
headphone switch S6a is coupled via
a 1µF MKT polyester capacitor and
then via an RC network consisting of a
March 1995 37
distortion versus frequency at 30 watts
into 8Ω loads.
Phono preamplifier
Fig.5: total harmonic distortion versus frequency at 30W into 8Ω loads, for both
channels.
1kΩ series resistor and a shunt 220pF
capacitor. This is an RF suppression
capacitor.
The voltage gain of the power amplifier is set 23 by the 22kΩ negative
feedback resistor from pin 3 to pin 9,
in conjunction with the 1kΩ resistor
and 47µF capacitor.
The output from IC4 drives the
loudspeaker via an RL network consisting of a 10Ω resistor in parallel
with an inductance of 0.7µH. This
acts in conjunction with the Zobel
network comprising the 5.6Ω resistor
and 0.1µF capacitor to ensure that the
LEFT
INPUT
amplifier is stable under varying load
conditions.
Power supply
The power supply uses a 50V
centre-tapped 160VA transformer
feeding a bridge rectifier and two
4700µF 50VW capacitors. Posi
tive
and negative 3-terminal regulators fed
by paralleled pairs of 330Ω resistors
provide the ±15V supply rails to the
preamplifier boards (ie, tone control
board and optional RIAA preamplifier). Fig.5 shows another aspect of the
amplifier’s performance: harmonic
+15V
L1
150
100k
47
BP
100k
8
3(5)
IC5a
2(6) LM833
4
100pF
L1 : 4T, ENCU WIRE
ON PHILIPS 4330 030 3218
FERRITE BEAD
16k
IC PIN NUMBERS IN BRACKETS
ARE FOR RIGHT CHANNEL
.0047
390
-15V
1(7) 100
10
BP
LEFT
OUTPUT
1M
200k
.015
+15V
+15V
22
BP
0.1
0V
0.1
RIAA PREAMPLIFIER
(OPTIONAL)
-15V
RIAA/IEC equalisation
-15V
Fig.6: the circuit of the optional RIAA preamplifier is based on an LM833
dual low noise operational amplifier.
38 Silicon Chip
As noted above, this phono preamplifier is optional. The circuit is
depicted in Fig.6 and again, only one
channel is shown. IC5a is one half of
an LM833 low noise op amp. It takes
the low level signal from a moving
magnet cartridge and applies a gain of
56 at the median frequency of 1kHz.
Higher frequencies get less gain while
lower frequencies get considerably
more, as called for in the RIAA equalisation. The preamplifier board is the
same as the universal preamplifier
board presented in the April 1994
issue of SILICON CHIP.
The phono signal is fed directly
from the input socket via inductor L1,
a 150Ω resistor and a 47µF bipolar capacitor to the non-inverting input, pin
3, of IC5a. The inductor, series resis
tor and 100pF shunt capacitor form a
filter circuit to remove RF interference
signals which might be picked up by
the phono leads.
The 100pF capacitor is also important in capacitive loading of the magnetic cartridge. Most moving magnet
(MM) cartridges operate best with
about 200-400pF of shunt capacitance.
The 100pF capacitance in the preamp
input circuit plus the usual 200pF or
so of cable capacitance for the pickup
leads will therefore provide about the
right shunt capacitance.
For its part, the 47µF bipolar cap
acitor is far larger than it needs to be
as far as bass signal coupling is concerned. If we were merely concerned
with maximising the bass signal from
the cartridge, then an input coupling
capacitor of 0.47µF would be quite
adequate. At 20Hz, a capacitor of this
value would have an impedance of
around 15kΩ which is considerably
less than the nominal 50kΩ input
impedance of the preamp.
However, having a large input cap
acitor means that the op amp “sees”
a very low impedance source (ie,
essentially the DC resistance of the
cartridge) at low frequencies and this
helps keep low frequency noise, generated by the input loading resistors,
to a minimum.
The RIAA equalisation is provided by the RC feedback components
between pins 1 and 2 of IC5a. These
PARTS LIST
1 steel case with aluminium front
panel, 435 x 90 x 265mm
1 2-pole, 6-position rotary switch,
Altronics S-3022 (S1
3 2-pole 2-position pushbutton
switches, Altronics S-1410
(S2,S3,S5)
1 single pole 12-position rotary
switch, Altronics S-3021 (S4)
1 SPST 250VAC rocker switch,
Altronics S-3210 (S7)
1 dual-gang 50kΩ log
potentiometer (VR1)
1 dual-gang 100kΩ linear
potentiometer (VR2)
1 dual-gang 25kΩ linear
potentiometer (VR3)
1 PC mounting 6.5mm switching
stereo socket, Altronics P-0076
3 3 x 2-way RCA socket panels,
Altronics P-0213
1 black binding post terminal,
Altronics P-0264
3 22mm diameter black aluminium
knobs, Altronics H-6213
2 30mm diameter black aluminium
knobs, Altronics H-6224
1 3-way mains terminal strip
2 solder lugs
1 toroidal power transformer, 2 x
25V, 160VA
1 M205 panel mount fuse holder
1 2A M205 20mm fuse
8 20mm fuse clips
4 2.5A M205 20mm fuses
2 single sided heatsinks, 72mm
high, Altronics H-0522
2 TA11B IC mounting kits
3 3-way PC terminal blocks,
Altronics P-2035
23 PC pins
7 15mm tapped standoffs
4 3mm x 6mm untapped standoffs
4 4M x 10mm screws
11 3M x 10mm screws
2 3M x 15mm screws
10 3M x 6mm screws
9 3M nuts
6 black No.6 x 10mm self-tapping
screws
1 1-metre length 0.5mm
enamelled copper wire
1 1-metre length twin shielded
audio cable
3 1-metre lengths 32 x 0.2mm
hookup wire (three different
colours)
1 3-core mains cord & moulded
3-pin plug
1 cordgrip grommet (to suit mains
cord)
4 rubber feet
1 6.4mm shaft coupler
1 6.4mm dia. x 144mm long
extension shaft
1 LED bezel
equalisation components provide the
standard time constants of 3180µs
(50Hz), 318µs (500Hz) and 75µs
(2122Hz).
The preamplifier also adds in the
IEC recommendation for a rolloff
below 20Hz (7950µs). This is pro-
vided by the 22µF bipolar capacitor
in series with the 390Ω resistor. The
390Ω resistor sets the maximum AC
gain at very low frequencies while the
22µF capacitor ensures that the gain
for DC is unity. This means that any
input offset voltages are not ampli
PC boards
1 power amplifier board, code
01102951, 247 x 58.5mm
1 input selector board, code
01103951, 132 x 58mm
1 selector switch board, code
01103952, 55 x 37mm
1 tone control board, code
01103953, 277 x 86mm
1 RIAA preamp board (optional),
code 01103954, 76 x 78mm
Semiconductors
2 LM833 operational amplifiers
(IC1,IC2)
1 TLO72 operational amplifier
(IC3)
2 LM3886 audio power amplifiers
(IC4)
4 1N914 signal diodes (D1,D2)
2 BC337 NPN transistors (Q1)
2 BC327 PNP transistors (Q2)
1 KBPC10-04 bridge rectifier
(BR1)
1 LM7815T 3-terminal regulator
(REG1)
1 LM7915T 3-terminal regulator
(REG2)
1 red LED (LED1)
Capacitors
2 4700µF 50VW electrolytics
4 100µF 63VW electrolytics
2 47µF 63VW electrolytics
8 100µF 16VW electrolytics
2 47µF 16VW electrolytics
2 22µF 16VW electrolytics
2 22µF 50VW bipolar electrolytics
2 6.8µF 50VW bipolar
electrolytics
4 1µF 63V MKT polyester
10 0.1µF 63V MKT polyester
1 .01µF 250VAC metallised paper
2 .01µF 63V MKT polyester
4 .0047µF 63V MKT polyester
2 220pF 50V ceramic
2 100pF 50V ceramic
4 33pF 50V ceramic
Resistors (0.25W, 1%)
2 100kΩ
4 1.6kΩ
2 91kΩ
12 1kΩ
2 47kΩ
2 820Ω
2 39kΩ
4 330Ω 1W
12 22kΩ
2 100Ω
2 15kΩ
2 82Ω
4 10kΩ
4 15Ω
4 5.6kΩ
2 10Ω 1W
8 4.7kΩ
2 5.6Ω 1W
1 3.9kΩ 0.5W
Optional RIAA Preamplifier
1 RIAA preamp board, code
01103954, 76 x 78mm
11 PC pins
1 LM833 operational amplifier (IC5)
2 Philips ferrite beads, 4330 030
3218
Capacitors
2 47µF 50VW bipolar electrolytics
2 22µF 50VW bipolar electrolytics
2 10µF 50VW bipolar electrolytics
2 0.1µF 63V MKT polyester
2 .015µF 63V MKT polyester
2 .0047µF 63V MKT polyester
2 100pF 50V ceramic
Resistors (0.25W, 1%)
2 1MΩ
2 390Ω
2 200kΩ
2 150Ω
4 100kΩ
2 100Ω
2 16kΩ
fied, which would inevitably cause
trouble with asymmetrical clipping
and premature overload in the preamplifier.
Next month, we shall continue with
the construction details for the new
SC
50W Stereo Amplifier.
March 1995 39
LIGHTNING
DISTANCE METER
Have you ever wondered just how close that
bolt of lightning was? Well, don’t wonder
about it; check it out with this Lightning
Distance Meter instead. The device uses
common components & measures flash
distances up to 19 kilometres.
By DARREN YATES
There are many situations where it
can be useful to know the distance to
an approaching thunderstorm. Perhaps you’re just the curious type who
likes to keep an eye on the weather or
maybe you have a far more practical
reason for wanting to know, such
as when you’re ploughing a field or
you’re out on the footy oval or golf
course. Being caught out in the open
in the middle of a thunderstorm is not
a pleasant experience.
Of course, you could always abandon the game when the first lightning
flash appears or you could use the old
“1001” rule that you learnt as a kid.
40 Silicon Chip
Whenever you saw a flash of lightning,
you would count 1001, 1002, 1003
and so on, and when you heard the
thunder you divided the last digit by
five to determine how many miles
away the “bolt” was. Armed with this
information, you could then elect to
do a runner when the lightning got too
close for comfort – five miles if you
were chicken or five feet if you were
more adventurous!
Unfortunately, in this metricated
age, most youngsters don’t know
what a mile is! So unless we apply a
metric conversion to the 1001 rule, we
either run the risk of getting zapped
or abandoning a perfectly good game
for nothing.
Alternatively, we could apply a
more scientific approach to the problem. The answer is this Lightning
Distance Meter. With a bit of eye, ear
and hand coordination, you can work
out the distance to a lightning flash
within a kilometre of so.
There’s nothing complicated about
using the unit. Apart from the power
switch, there are just three pushbutton
controls and these are labelled Start,
Reset and Stop. In addition, the front
panel carries a row of LEDs and these
are numbered from 1-10.
The principle of operation is quite
simple. The speed of sound in air is
about 1207km/h, which is equivalent
to 1km every 3 seconds. So all the
circuit does is light each LED in turn
at 3-second intervals when the Start
button is pressed. To use the unit, you
simply press the Start button when you
see the lightning flash and then press
the Stop button when you hear the
thunder. The LED that’s lit then gives
the distance to the flash (eg, if LED 6
is lit, then the distance is 6km).
D1
1N4004
S4
+6V
RESET
S3
680k
IC1
555
2
2.2
16VW
VR1
500k
8
6
1
14
CLK
4
IC2
4017
1
2
1k
6
5
7
6
100k
1k
A
A
K
6
S
C
IC3a
5 4013 2
D
Q
R
4
1k
A
K
13
8
6V
3
9
11
1k
A
A
K
K
8
9
1k
1k
A
A
K
K
CE
5
1
1k
1k
A
A
K
4
10
1k
1k
A
LEDS 1-9
3
7
2
4
100
16VW
15
RST
12
CO
16
3
.01
LED 10
K
K
K
+6V
14
13
Q
IC3b
7
S
R
START
S1
8
STOP
S2
D2
1N4148
.01
10
A
100k
K
100k
LIGHTNING DISTANCE METER
Fig.1: the circuit uses 555 timer IC1 to clock decade counter IC2. IC2's decoded
1-9 outputs go high in turn & drive the indicator LEDs. On the 10th count, the
CO output goes high & this toggles flipflop IC3a to light LED 10. IC3b controls
IC1 to start & stop the count.
If the distance is greater than 10km,
the circuit first counts to 10 in the
usual manner. LED 10 then remains
lit while the circuit cycles through
the first nine LEDs again. In this way,
the circuit can effectively count up to
a maximum value of 19. Thus, if both
LED 4 and LED 10 are alight when the
Stop button is pressed, for example,
the distance to the flash is 14km.
When a count of 20 is reached,
LED 10 goes out and the count starts
all over again from zero (ie, the count
continually cycles). So, for all practical
purposes, the maximum count is 19.
This is not really a problem however,
since it is unlikely that you will be
able to hear individual thunderclaps
at distances greater than 19km.
The Reset button clears the counter
used in the circuit and effectively
“freezes” the circuit so that all LEDs
are off. This reduces the current consumption to a bare minimum and is
useful for maximising battery life if
there is a substantial delay between
each measurement.
However, the circuit is also automatically reset each time the Start button
is pressed. This feature is handy if you
are taking a number of measurements
in quick succession, since you don’t
have to continually press the Reset
switch.
How it works
Refer now to Fig.1 for the circuit
details.
IC1 is a 555 timer which operates as
an astable oscillator. It is wired here
in a somewhat unconventional manner, however. Normally, the timing
capacitor charges from the positive
supply rail via a resistive network and
discharges (via part of that network)
into pin 7. In this circuit though, the
timing capacitor (2.2µF) charges when
IC1’s pin 3 output goes high and discharges when pin 3 goes low.
PARTS LIST
1 PC board, code 08103951,
102 x 54mm
1 plastic case, 130 x 68 x 41mm
3 momentary normally-off
pushbutton switches (S1-S3)
1 SPDT toggle switch (S4)
1 front panel label, 125 x 63mm
4 AA alkaline cells
1 long 4 x AA cell holder
1 500kΩ miniature horizontal
trimpot (VR1)
4 15mm-long spacers
4 3mm x 25mm machine screws
4 3mm hex nuts
Semiconductors
1 NE555 timer (IC1)
1 4017 CMOS decade counter/
decoder (IC2)
1 4013 dual D flipflop (IC3)
1 1N4004 silicon diode (D1)
1 1N4148 signal diode (D2)
5 5mm red LEDs (LED1-5)
5 5mm green LEDs (LED6-10)
Capacitors
1 100µF 16VW electrolytic
1 2.2µF 16VW electrolytic
2 .01µF MKT polyester
Resistors (0.25W, 1%)
1 680kΩ
3 100kΩ
10 1kΩ
Miscellaneous
Light duty hook-up wire, tinned
copper wire for links
March 1995 41
START
S1
POWER
S4
1
STOP
S2
1
3
2
4
.01
IC1
555
680k
100uF
RESET
S3
VR1
IC2
4017
IC3
4013
1
2.2uF
D2
1
D1
LED3
LED5
LED6
LED7
1k
1k
1k
1k
1k
1k
1k
1k
LED4
LED8
LED9
100k
LED1 LED2
1k
1k
100k
100k
1
2
3
4
.01
LED10
6V BATTERY PACK
Fig.2: make sure that all polarised parts, including the LEDs, are correctly
oriented during the PC board assembly. VR1 is used to adjust the 555 timer so
that the circuit counts to 10 in 30 seconds.
The circuit works like this: at
switch-on, pin 3 of IC1 goes high and
the 2.2µF timing capacitor charges
via VR1 and a 680kΩ resistor. When
the capacitor voltage reaches 2/3Vcc
(ie, 2/3 the supply rail voltage), pin
3 switches low and the capaci
tor
discharges until it reaches 1/3Vcc.
At this point, pin 3 switches high
again and so the cycle is repeated
indefinitely.
As a result, IC1 produces a square
wave pulse train at its pin 3 output.
VR1 is adjusted so that oscillator operates at a nominal 0.33Hz, which is
equivalent to one positive going pulse
every 3 seconds.
This signal is used to clock IC2,
which is a 4017 decade counter. Its
decoded 1-9 outputs are normally
low but sequentially switch high in
response to the clocking signal (ie,
Fig.3: this is the full-size etching pattern for the PC board.
42 Silicon Chip
one output goes high at a time for the
duration of each clock cycle). These
outputs, in turn, drive LEDs 1-9 via
1kΩ current limiting resistors.
The tenth LED in the sequence (LED
10) is driven from the CO (carry out)
output of IC2 via flipflop IC3a (4013).
In operation, the CO output goes high
once every 10 clock cycles and this
in turn clocks IC3a which operates
in toggle mode. This ensures that
LED 10 remains lit as the counter
cycles back through again after first
counting to 10.
When power is first applied, both
IC2 and IC3a are reset by virtue of
the 0.01µF capacitor across the Reset
switch (S3). This briefly pulls pin 15
(reset) of IC2 and pin 6 (set) of IC3
high. As a result, outputs 1-9 of IC2
and Q-bar of IC3a are all initially low
and so the LEDs are all off. Only the
decoded ‘0’ output of IC2 is high but,
as this output is unused, this is of no
consequence.
IC3b, along with switches S1 & S2,
provides the start\stop control function. When power is applied, its reset
input (pin 10) is briefly pulled high via
the .01µF capacitor across S2 and this
ensures that the Q output (pin 13) is
initially low. This, in turn, holds pin
4 (reset) of IC1 low and prevents IC1
from operating.
Pressing the Start button (S1) now
pulls the set input of IC3b high and
this toggles pin 13 high and releases
the reset on IC1. IC1 now oscillates
and clocks IC2 at 3-second intervals
to light the LEDs in sequence. The
count continues until the Stop button
is pressed, at which point the Q output of IC3 goes high again and stops
IC1. The count is now effectively
frozen until either the Start button
is pressed again or the Reset button
is pressed.
Diode D2 is necessary to make the
circuit start counting correctly. Without this diode, IC2 would be clocked
by a high going pulse from IC1 as soon
as the Start button was pressed and so
the first LED would light immediately
instead of after the required 3-second
delay.
By including D2, IC2 and IC3 are
reset when the Start button is pressed,
which means that IC2 ignores the
initial high-going pulse from IC1 and
thus counts correctly.
There’s one important point to note
here, though. IC2 and IC3 are held
reset for as long as the Start button is
held down. This means that the circuit will not start counting until the
Start button is released, so it should
only be pressed briefly when you see
a lightning flash.
Power for the circuit comes from a
6V battery (4 x 1.5V AA cells) and this
is applied via power switch S4 and
reverse polarity protection diode D1.
A 100µF capacitor is used to provide
supply decoupling.
Construction
The prototype Lightning Distance
Meter was built on a small PC board
coded 08103951 and is housed in a
plastic utility case. Fig.2 shows the
assembly details.
Before starting construction, check
the board carefully for any shorts or
breaks in the copper tracks by comparing it with the published artwork.
Repair any defects that you do find
(generally, there will be none), then
install PC stakes at the eight external
wiring points.
This done, install the six wire links,
followed by the resistors, diodes,
capacitors and the ICs. Take care to
ensure that the polarised components
are correctly oriented and be sure to
use the correct type numbers for D1
and D2.
Trimpot VR1 can now be installed,
followed by the 10 LEDs. Just load the
LEDs into the board as shown on Fig.2
but don’t solder or trim their leads at
this stage. That step comes later, after
the front panel has been attached.
Take care to ensure that each LED
is correctly oriented – the anode lead
is the longer of the two. We used red
LEDs for LEDs 1-5 and green LEDs for
LEDs 6-10, since we reckoned that any
flashes within 5km were too close for
comfort.
The plastic utility case can now be
drilled to accept the PC board, the four
switches and the LEDs. The first step
is to attach the front panel artwork to
the lid. This can then be used as a template for drilling out the LED mounting
holes. It’s best to drill small pilot holes
first and then carefully enlarge them
using a tapered reamer until the LEDs
are a good fit.
Once this has been done, use the
PC board as a template for marking
out its four mounting holes on the
lid. Drill these holes to 3mm, then
fasten the PC board to the back of the
lid using 15mm spacers and machine
screws and nuts. The 10 LEDs can
This view shows the completed PC board assembly, before it is mounted on the
lid of the case. Note that the final version differs slightly from this prototype (ie,
D2 & the two .01µF capacitors were added after this photo was taken).
The completed PC board is mounted on the lid on 15mm spacers & secured
using machine screws & nuts. Arrange the LEDs so that they just protrude above
the surface of the front panel.
now be pushed into their respective
front panel holes and their leads
soldered. Adjust each LED so that it
just protrudes above the surface of
the front panel.
The front panel can now be used as
a guide for marking out the holes for
the switches. The three pushbutton
switches are mounted on the top of
the case, while the power switch is
mounted on the lefthand side. They
must all be posi
tioned towards the
back of the case so that they clear the
PC board when the lid is fitted.
Once the holes have been drilled,
mount the switches in position, then
March 1995 43
Start
Reset
On
Lightning
Distance Meter
Power
Off
Stop
1
2
3
4
5
6
7
8
9
10
Pressing the Start button again
should now clear the display and
restart the count.
Finally, check the operation
of the Reset button. It should
only be pressed after the Stop
button has been pressed and
should clear the display. Do not
use the Reset button to restart
the count if a count is already
in progress, as this will give
inaccurate results.
Calibration
Kilometres
Assuming that everything
works correctly, the unit can now
be calibrated so that its counts at
Fig.4: this full-size artwork can be used as a drilling template for the front panel. It
the correct rate. As mentioned
should also be used as a guide for marking out the switch mounting positions.
earlier, the sound from a lightning flash travels about 1km in 3
remove the PC board from the lid and on after a brief delay, followed by each seconds. So, to calibrate the unit, simcomplete the wiring. You can use light of the remaining LEDs in turn. Check ply adjust VR1 so that the unit takes
duty hook-up wire for this job.
that the unit counts correctly to 10 30 seconds to count up to 10km. This
and that LED 10 then remains on as will have to be done on a trial and erSmoke test
the count cycles through the first nine ror basis. Rotating VR1 anticlockwise
The test procedure simply involves LEDs again. If any of the LEDs fail to increases the time, while rotating VR1
switching the unit on and checking light, it has probably been installed clockwise reduces it.
Once thus has been done, you can
that everything works correctly. First, the wrong way around.
Now press the Stop button and complete the final assembly and wait
check that all the LEDs are out immediately after switch-on, then press the check that the display “freezes”, with for that next southerly-buster to blow
SC
Start button. LED 1 should now come the current LED(s) remaining on. up.
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1. Power switch
2. LED
3. Graticule illumination
switch
4. Trace rotation
5. Trace focus
6. Trace intensity for B
sweep mode
7. Brightness control for
spot/trace
8. Trace position
9/10/11. Select input
coupling & sensitivity of
CH3
12. Vertical input terminal
for CH3
13. AC-GND-DC switch for
selecting connection mode
14. Vertical input terminal
for CH2
15/22. Fine adjustment of
sensitivity
16/23. Select vertical axis
sensitivity
17/24. Vertical positioning
control
18/25/38. Uncal lamp
19. Internal trigger source
CH1,CH2,CH3,ALT
20. AC-GND-DC switch for
selecting connection mode
21. Vertical input terminal
for CH1
26. Select vertical axis
operation
27. Bezel
28. Blue filter
29. Display selects A & B
sweep mode
30. Selects auto/norm/single
sweep modes
31. Holdoff time adjustment
32/51. Trigger level
adjustment
33/50. Triggering slope
34/49. Select coupling mode
AC/HF REJ/LF REJ/DC
35. Select trigger signal
source Int/Line/Ext/Ext÷10
MACSERVICE PTY LTD
36. Vertical input terminal
for CH4
37. Trigger level LED
39. A time/div & delay time
knob
40. B time/div knob
41. Variable adj of A sweep
rate & x10 mag
42. Ready lamp
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43. Calibration voltage
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44. Horizontal positioning
of trace
45. Fine adjustment
46. Vertical input terminal
for CH5
47. Delay time MULT switch
48. Selects between
continuous & triggered
delay
52. Trace separation
adjustment
53. Ground terminal
SILICON
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SERVICEMAN'S LOG
Doing the rounds with remote control
This month’s notes have turned out to be a
continuation of last month’s. It wasn’t planned
that way; it just happened. As readers will
recall, they were about remote control units &
this month’s notes describe two more faults.
One of last month’s stories was
about some funny goings on with the
infrared LEDs in a particular model
remote control unit (NEC RD-309E).
They would work when the unit was
upside down but not when it was right
way up.
And it wasn’t just a one-off; I had
two with identical symptoms, which
was enough to suggest that it involved
an inher
ent weakness in the LEDs
themselves. Replacing them was all
that was required to cure the fault but
the exact failure mechanism remained
a mystery.
Which was where we left things last
month. But hardly had the presses
begun to roll, than there was another
episode. It was the same model unit
and it came in with a familiar complaint: “it doesn’t work.”
And with very good reason, as I
found when I opened the case. It was
another case of a broken crystal lead,
only this time the break was so close
to the case that there was no chance
of salvaging it. Fortunately, a scrabble
through the junk box produced another such unit from which I was able to
retrieve a perfectly good crystal.
So it all looked like plain sailing.
I fitted the substi
tute crystal, put
everything back together, and gave it a
try. No joy. For a moment I wondered
whether I had tricked myself and fitted
another dud crystal.
But then I remembered the upside
down behaviour. Surely not another
one? But it was; I turned it over and
it worked, and when I turned it back
again it was dead. I could hardly
believe it. I fitted another LED and
that was it; its behaviour was back to
normal.
So there it is – mystery fault number
three. And that means there must be
some inherent fault in those LEDs. I
had hoped to make some attempt to
find out what it is but, as I mentioned
last month, the LEDs involved are
coated with an infrared filter which
excludes visible light and makes them
appear black.
My idea was to try to break one
open, with a minimum of force, in an
effort to preserve the electrodes and,
hopefully, reveal the fault. No such
luck. These things are not hollow, as
I had thought, but solid plastic.
But one final thought. With two
Fig.1: Der Fernbedienungstester RCT 5502 (ie, the remote control tester).
It carries a microphone (marked “US”), an infrared sensor (marked “IR”),
two LEDs (shown on the top of the case), & a 3.5mm socket on one side.
46 Silicon Chip
faults in this last unit, which came
first; which one prompted the customer to call me? We shall never know.
The main event
So much for that little preliminary
bout. The main event this month
concerns a Philips colour TV set, a
63cm model using the KL9A chassis.
This chassis first appeared about 1012 years ago and was used in a whole
range of sets. In many sets, it was
used in its basic form, without any
frills, but in this case it came with the
works: remote control, stereo sound
and Teletext.
The customer’s complaint came
in the form of a phone call along the
now familiar lines, “the remote control
doesn’t work.” So I said, “bring it in
and we’ll test it”.
At this stage, it may help the reader
to follow the story if I describe the test
unit I use for situations like this. It is
a commercial unit of German manufacture and carries the Konig brand
name (type number RCT 5502). As a
matter of interest, the German term for
remote control transmitter appears to
be “Fernbedienung”, so the name of
this device becomes “Fernbedienungs
tester” (I wonder if they play scrabble
in Germany!).
I understand that there is also at
least one locally made unit available.
This is carried by J. V. Tuners, 216
Canterbury Rd, Revesby, NSW 2212.
Phone (02) 774 1154.
The unit I have is basically a remote
control receiver, similar to that used
in TV sets but, for reasons which
will become apparent, is a good deal
simpler.
It is designed for use with both
infrared transmitters and the older
ultrasonic transmitters, being fitted
with both an IR photocell and a small
microphone. It is housed in a small
plastic case about 35mm wide, 25mm
thick and 120mm long. There is an on/
off switch on one side of the case, two
LEDs (one red & one green) on the top,
and a 3.5mm socket on the other side.
The red LED indicates that the power is on, while the green LED indicates
when pulses are being received from
the remote control. The 3.5mm socket
may be used to bring the pulses out
for checking on a frequency counter
or CRO. Power is supplied by a 9V
alkaline battery, while the internal
circuit consists of just four transistors
and a few minor components.
It’s all quite simple really but it
works very well. However, it is not
infallible.
Anyway, the customer brought in
his control unit and I put it through
its paces on the tester. This initially
involves setting up the remote control transmitter and the tester so that
they are about 150mm apart on a flat
surface. The tester is then switched
on and each of the transmitter buttons
pressed in turn. It is important to test
every button because only one or two
may be faulty. Many customers don’t
bother with such subtle points; to them
it is all summed up in the phrase, “it
doesn’t work.”
There were no such problems in this
case. Each button produced a response
from the green LED and I pronounced
the unit OK. Unfortunately, this wasn’t
the good news one might imagine
because it meant that the fault was in
the TV set. This would now have to
be brought in for service.
Fortunately, the customer had a
second set and he duly organised
delivery of the Philips set to the workshop. So, at the first opportunity, I put
it up on the bench for a preliminary
check. And this produced a surprise;
there were no channels programmed
into it.
This was rather strange, particularly
as the customer had not mentioned
it, but I considered that it might be a
byproduct of whatever fault there was
in the remote control section.
Anyway, I programmed the local
channels into it, just to get it working,
and this caused no problems. Nor did
there appear to be any problems with
the set’s overall behaviour; it was
first class. But, as the customer had
indicated, it would not respond to the
remote control.
No circuit
At this point, I fished out my circuit
of the KL9A but very quickly realised
that it was for the basic chassis only;
there was no remote control circuitry
in it. And that was about it for then;
there was little point in wasting time
working blind and so I rang Philips
and placed a manual on order. But I left the set running
on the bench for the rest of
the day, until I shut down
and pulled the main switch
for the night.
Next morning, when I
pushed in the main switch,
everything came up as normal except for the Philips set.
All it produced was snow and
noise. It didn’t take long to
confirm that all the channels
I had programmed into its
memory the day before had
been lost.
Fortunately, the reason
wasn’t hard to find. This set
uses a nicad battery backup
for the memory, designated
as part No. 1675. And since
it was the original, it was not
surprising that it had failed
after about 12 years.
I rang the customer and
explained that I would have
to wait on a manual before I
could fix the remote control
problem. At the same time, I
took the opportunity to point
out the additional problem with the
channel memory system.
He was quite understanding about
any delay caused by the manual. And
when I mentioned the memory loss
his reaction was immediate. “Oh yes,
I forgot to mention that – it’s all right
as long as I leave the power point on
but it loses it if I turn it off”.
Well, that figured; the channels had
been lost when he unplugged the set
to bring it in. But at least I could go
ahead with this problem. In greater
detail, the battery is a 2.4V 110mAh
type, about 7mm in diameter and
30mm long. It was readily available
from one of my regular parts suppliers
and, after fitting it, we had no more
memory problems. With luck, it might
last another 12 years.
I now had to solve the problem
with the remote control. Eventually, the manual arrived and, after
some confusion due to the fact that
it contains two different versions
of the circuit, I was finally able to
tackle the job.
The relevant part of the circuit is
reproduced here – see Fig.2. It shows
the IR receiver (part 1725) and a couple
of voltages and waveforms. I decided
to start by checking the voltages.
The two points involved were 3C1
March 1995 47
Fig.2: the IR receiver circuitry in the Philips KL9A. The incoming pulses from the transmitter are processed by the
IR receiver at extreme left & then fed to the base of a BC548 transistor via a 1µF capacitor. The resulting signal on
the emitter of this transistor in then fed via a 10kΩ resistor to pin 13 of the data processor IC at right.
and 2C1 on the IR receiver. And, in a
moment of carelessness, I neglected to
observe the polarity signs at these two
points, assuming instead that the 5V
marking indicated two separate rails,
each at 5V with respect to chassis.
The habit of measuring all voltages to
chassis is strongly ingrained but it is
not always the right thing to do.
I woke up to this very quickly but,
by a strange twist of fate, both points
measured very close to 5V with respect
to chassis. In practice, of course, the
5V is supposed to be read between
2C1 and 3C1, with 2C1 being at 5V
with respect to chassis and 3C1 being
at 10V with respect to chassis.
Or that was how it was supposed to
be. But 3C1 was not at 10V; instead,
it was almost exactly at 5V, so there
was virtually no voltage between the
two points. By now, having realised
my mistake and analysed the circuit
correctly, I realised that there was
something amiss around 3C1.
The easiest thing to do was to pull
the 3-pin plug to the IR receiver,
whereupon the 3C1 supply line from
the main part of the circuit jumped to
10V. Pushing the plug back in again
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48 Silicon Chip
pulled it back down to around 5V,
which suggested a fault in the IR receiver module.
The IR receiver
I pulled the entire IR receiver out
for a closer look. It is housed in a
small but substantial aluminium box
and consists of a PC board carrying a
16-pin IC, an IR photodiode, a couple
of coils, and a few other components.
I quickly concluded that there was
little point in thinking about repairs.
There was no circuit available and, as
far as I could determine, the IC wasn’t
This photo shows the IR receiver board after it has been slid out of its metal
case. The IR photodiode is on the board at right, while the 3-pin socket is at left.
Note the IR lens on the end of the case.
available as a separate item.
Trying to troubleshoot a problem in
these circumstances can be very risky.
One can waste hours, only to finish
up being unable to repair it anyway.
The only logical answer was a new
receiver.
And that posed a whole new set of
questions. Was a replacement readily
available? What would it cost? And,
most importantly, would the customer
want to incur such cost?
While I was fairly confident that a
replacement would be available, the
cost was another matter. Receivers
for other brands retail from $25 to $50
and I had a gut feeling that the higher
figure would be the place to start from.
I rang the customer and explained
the situation. Naturally, he wanted
some idea as to what it was all going
to cost. I went over the cost of the work
already done, added my estimate of
the receiver price plus labour, and we
came up with a guesstimate of between
$150 and $200. Did he consider it
worthwhile to go this far? Yes, he did
– I should go ahead.
And so I contacted Philips. Yes,
the receiver was avail
able and my
gut feeling was not far out; the retail
price I should charge my customer was
$75. Since this kept the overall cost
within my guesstimate, I went ahead
and ordered it.
It duly arrived and, at the first opportunity, I set about fitting it. This
took no more than a few minutes work
but when I gave it a trial run, it simply
would not respond to the remote unit.
So much for my optimistic “she’ll be
right now mate” attitude! She wasn’t
right at all.
All kinds of horrible possibilities
raced through my mind. Had I fouled
up the receiver installation, which
seemed so straightforward? Was it a
modified receiver design, unsuitable
for a set of this age? Was it a much
more subtle fault, somewhere in the
bowels of the set itself? Was the fault
really in the transmitter, in spite of my
previous tests? And had I invested unnecessarily in a replacement receiver,
which would sit in my stock for years
to come?
When the panic subsided, I decided
that the first two thoughts were the
least likely, so I concentrated on the
possibility of a fault in the set. The
first step was to check the rail voltages
at 2C1 and 3C1. These now measured
5V and 10V respectively, exactly as
marked on the circuit.
Next I turned to the CRO. The circuit
shows a waveform coming out of the
receiver at terminal 1C1. The circuit
depicts square wave pulses with an
amplitude of 5V but, unfortunately,
there is no indication as to the frequency of these pulses, nor is there any
other data on the coding used.
Anyway, this was the first check
point. And on the basis of the limited
information in the manual, everything
appeared to be OK at this point. From
there, the signal goes via a 1µF electro
lytic capacitor to the base of a BC548
transistor. The resulting signal on
the emitter of this transistor is then
fed via a 10kΩ resistor to pin 13 of
the data processor IC, where another
waveform is shown. This is similar
to the first but with a slightly lower
(4V) amplitude.
I traced the signal along this path
and finished up with the correct
waveform at pin 13, as shown on the
circuit. So pulses were coming out of
the remote transmitter, being picked
March 1995 49
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up by the receiver, processed, and
passed to the data processor IC.
So why wouldn’t it work? The most
logical suggestion seemed to be a fault
in the data processor IC, which wasn’t
a very happy thought. From previous
experience, I tipped that it would
be quite expensive and that, in turn,
meant that the cost situation would be
getting out of hand.
But there were other factors to be
considered. How could I be absolutely sure it was that IC? Granted,
the evidence was strong but if I was
wrong, I would be down the drain for
an expensive IC.
What else could it be? One slim
possibility was the trans
mitter, in
spite of the tests I’d already made.
Remember that I said earlier that the
transmitter tester was not infallible.
Its weakness is that it can only confirm that pulses are being transmitted;
it has no way of confirming that they
have the correct coding sequence for
a particular set.
No gambling
So although the risk appeared to
be slight, I wasn’t prepared to gamble
the cost of an IC until I was absolutely
sure that the transmitter was clean.
Ideally, this could be confirmed by
acquiring another transmitter, perhaps
borrowed from a colleague if I was
lucky enough.
But first I decided to have a look
inside the transmitter for any clues
or obvious faults. A general once over
didn’t show up anything obvious,
such as dry joints or obviously faulty
components, and the voltages seemed
to be at least sensible, which was the
best I could do.
Next, I connected the CRO across
the crystal oscillator circuit and
confirmed that this was working
correctly. Its frequency was around
4MHz, which is similar to many other
systems. So it looked as though I had
drawn a blank.
And then the system suddenly came
good. Acting on an impulse, I pressed
one of the control buttons, whereupon
the receiver immediately responded.
I went through the whole range of
control functions and they all worked
perfectly.
The trouble was, I hadn’t a clue as
to why this had happened. I could
only assume that there was faulty
connection in the transmitter somewhere (perhaps the battery contacts),
which had come good as a result of
my prodding and probing. But, try as
I might, I couldn’t recreate the fault.
So I simply went over the board with
a hot iron and resoldered all the joints,
with particular attention to those
around the crystal oscillator circuit. I
didn’t find anything suspicious in the
process and the unit still functioned
in all modes afterwards.
By now, I imagine, some readers are
querying whether I goofed over the
receiver; was it really faulty, or had it
been a transmitter fault all the time?
Well, the same thought occurred
to me and I couldn’t rest until I had
plugged the old receiver back in. No
question; it pulled the 10V rail down
as before and simply wouldn’t work,
so that was the end of that theory.
Finally, after putting the system
through a week’s hard yakka, I returned the set to the customer with a
warning to contact me immediately if
the fault recurred. That all happened
nearly 12 months ago and the system
hasn’t missed a beat since. And what
did it cost? It all added up to $149, so
my initial estimate of $150-200 wasn’t
SC
too far out.
March 1995 51
In this second
article, we give the
details on how to
build this set of wide
range electrostatic
speakers which have
been developed in
Australia. They can
be built using simple
materials & readily
available tools.
By ROB McKINLAY
Wide range electrostatic
loudspeakers; Pt.2
To build these loudspeakers, you
will need the following equipment:
(1) a table or bench with a work surface
of at least 700 x 1400mm, preferably
coated with melamine, Laminex or a
similar material. It must be flat and
able to take heavy weights.
(2) One 1220 x 605mm sheet of 18mm
chipboard or MDF (medium density
fibreboard). This will need to be cut
into three strips, two measuring 240
x 1220mm and one measuring 120 x
1220mm. These are used as the pressure pads when gluing down the air
gap spacers. Subsequently, the MDF
strips will need to be cut down again,
to be used as grid pressure pads.
(3) 70mm disposable foam paint roller covers. One frame and two roller
covers are supplied in the kit. More
may be necessary depending on how
you proceed.
This photo shows one treble and two bass panel matrix
panels laid out with their respective air spacers ready to
be glued. Note the crosses marked on the matrix panels.
52 Silicon Chip
(4) A soldering iron. This is needed to
assemble the EHT supply boards and
make the various connections from the
supply to the panels.
(5) A heat gun such as the unit made
by Black & Decker. This will be used
to tension the film after it has been
applied to the panels. Don’t bother
trying to use a hair drier. They are not
hot enough and deliver too much air.
(6) Digital multimeter with a 200
After glue has been applied to the top of the matrix panels,
the air gap spacers are placed around the periphery, as
shown here.
PLASTIC
MATRIX
AIR-GAP
SPACERS
GRID
(NODE POINTS ONLY
ON ONE HALF
PANEL)
DIAPHRAGM
GRID
AIR-GAP
SPACERS
PLASTIC
MATRIX
AUDIO
CONNECTION
Fig.1: this diagram shows how the plastic matrix panels, air
spacers, perforated steel grids and the central diaphragm are
sandwiched together to make a complete panel. The central
diaphragm is glued to the air spacers of one half panel and,
after tensioning, is painted with a conductive coating.
megohm resistance range, to be
used for checking out the individual
panels.
(7) Tools such as wire cutters/strippers, pliers, screwdrivers, electric
drill and bits.
As noted last month, the kits for
these speakers include all the materials you will need, including adhesives.
The enclosures are not included but
are available fully finished. Having
seen the excellent finish of the enclosures and having in mind their very
reasonable cost ($499 for the pair), few
people would wish to build their own
enclosures from scratch.
Handy hints
The adhesives used in this project
are very strong and durable. There
are no solvents for them that are kind
to your skin. Always wear the gloves
supplied during the gluing operations
and when applying the conductive
coating to the diaphragms.
To ensure a good understanding of
how this project goes together, it is a
good idea to do a “dry run” with one
panel half. Fig.1 shows an exploded
view of the panels which are all the
March 1995 53
After the air gap spacers have been attached, pressure pads are applied while
the adhesive sets. In this case, plate glass sheets are being placed and these will
be weighted down with bricks.
Adhesive is applied to the perforated
grid with the aid of a smaller paint
roller, before the grid is attached to its
matrix panel.
the 10mm disc node points. These are
the half panels that the diaphragm is
attached to.
Plastic support panels
This photo shows the perforated steel grid ready to be glued into the matrix
panel which has air gap spacers glued to it.
same in principle although the central
treble panel is narrower than the two
bass panels.
Essentially, each side of the panel is
a plastic matrix to which air gap supports are glued. Then a perforated steel
grid is fitted into the frame formed by
the air gap supports. Then the plastic
diaphragm is placed over one of the
matrix/grid assembles and attached
with adhesive. It is then ten
sion
ed
with a hot air gun and sprayed with the
conductive layer. Finally, the mating
matrix/grid assembly is attached and
the panel is complete.
The dry run should be as follows.
Place a white plastic support matrix
54 Silicon Chip
on the work surface with the black
crosses facing up. Place two long air
gap spacers on top of the matrix covering the edge square segments. Place a
medium length air gap spacer at each
end on top of the matrix, forming a
rectangle with the two long spacers.
Place a perforated steel grid centrally
within the rectangle with the screw
terminal protruding into the matrix;
ie, facing the work surface. The black
crosses should be visible through the
holes in the grid. This is where the
node points are attached.
This forms the basis on which the
12 half panels are assembled. Note
that only six of these half panels carry
The first operation is to bond the air
gap spacers around the outside section
of each plastic support matrix. Six of
the panels are marked with a series
of crosses running vertically down
the centre line and six have a cross
in each corner. During all assembly
procedures place these faces up on
the work surface.
The white PVC spacers are to be
bonded around the outside section
of the plastic matrix. One side of the
PVC strip will have a clear protective
covering stuck to it; this face is to be
kept up on the assembled half panel.
Before applying adhesive to any
components, check that they fit in their
intended positions. The long spacers
may overhang the matrix slightly but
this excess can be sanded off after
gluing.
It is best to start work on a maximum of three half panels at first,
until you have some experience with
the process. Therefore, you can start
with two bass half panels and one
treble half panel. Place the three half
panels on the work surface with the
black crosses up. Select six long, four
medium and two short air gap spacers.
Lay these on the work surface next to
each other with the non-covered side
facing up. This will allow you to roll
a coat of adhesive, first over the long
spacers, then the medium and short
spacers, in one operation.
Note: it is essential to place a plastic
sheet) under the plastic matrix before
gluing, in case the adhesive runs down
and sticks to the work surface, making
removal of the matrix difficult. The
clear plastic covering on the spacers
will prevent adhesion to the pressure
pad. This covering should be not be
removed until all gluing operations
are finished.
Apply a thin coat of adhesive to the
non-covered side of the spacers with
a roller. Place the spacers around the
matrix outer segment as in Fig.1. It is
important that the outer edge of the
spacers line up with the outer edge of
the support matrix. This will ensure
that the grid has sufficient room to
fit into and be bonded to the support
matrix.
When in position, place a sheet of
chipboard (or plate glass) over the
spacers, making sure not to disturb
them. Place weights on the chipboard
such as 12 bricks, etc. Allow 24 hours
for the adhesive to cure. Repeat this
operation on all panels.
Once the perforated grids have been attached to the matrix panels, MDF
pressure pads ensure they are kept flat while the adhesive cures.
Grid preparation
12 perforated steel grids have been
provided; eight wide (bass) and four
narrow (treble). The grids are supplied in mirror matched pairs. Do not
mix them up. They have been colour
coded to assist in identification. Each
grid has a 3mm screw connection
silver-soldered to it. This screw protrudes through a segment of the plastic
support matrix, enabling the signal
connection to be made.
Before proceeding to the next step,
check that the grid sits in the gap
created by the air gap spacers, without the screw fouling the matrix. If
necessary, carefully use side cutters
to break out the offending piece of
matrix.
Grid bonding
For this operation, you need a piece
of MDF 5-6mm narrower and 5-6mm
shorter than the grid, to enable pres
sure to be applied during bonding.
Cut some polyethylene sheet into
strips that are wider than the grids to
be glued. These will stop the pressure
pad from sticking to the grid. Lay
Once the matrix/grid assembly is
complete, blobs of silicone are applied
to the grid to form nodes for the
diaphragm.
Teflon node buttons are placed onto
the blobs of silicone (see previous
photo) & pressed down using a steel
ruler (see text).
some polyethylene sheet on the work
surface, then lay the plastic matrix on
the sheet with the white PVC spacers
facing up.
Hold the grid vertically in one hand
and roll a light coat of adhesive onto
the side of the grid that is to come into
contact with the plastic matrix; ie, the
side with the threaded portion of the
terminal. Avoid getting adhesive on
the diaphragm side of the grid or onto
the threads of the audio connection
terminal.
Place the grid centrally in the space
created by the PVC spacers so that
the glue contacts the plastic matrix.
Ensure that the audio connection
terminal does not foul the plastic
matrix. Place a strip of polyethylene
sheet over the grid and then the MDF
pressure pad. Place weights on the
MDF to ensure good adhesion to the
matrix.
The polyurethane glue used for the
construction relies on the moisture in
the air to cure. Normal curing occurs in
24 hours. On very dry days the curing
cycle will be longer. If there is any
doubt as to whether the glue is cured,
leave for additional time.
Repeat the above operation for all
the grids, then remove the clear plastic
covering from the air gap spacers.
Diaphragm nodes
Six of the plastic matrix panel
halves are supplied with a series
of black crosses running vertically
March 1995 55
position level to the top of the air gap
spacers, plus a thickness of paper,
they will be level with the air gap
spacer when the backing paper is
removed. The diaphragm will adhere
strongly to the adhesive on the disc,
eliminating diaphragm rattles and the
need for a matching disc on the other
half panel.
This method of construction greatly
reduces the risk of EHT leakage from
the conductive side of the diaphragm
to the grid. Leakage caused by dust collecting on the node points is also eliminated. Allow the silicone adhesive to
cure before attaching diaphragms to
these panels.
This photo shows the foil tape attached to one side of the matrix assembly. It is
then drilled to take a screw connection.
The clear plastic diaphragm is
stretched over the panel and taped
down as shown and the adhesive is
activated by the heat gun.
Once the diaphragm adhesive has
cured, the film is tensioned on the
panel by shrinking it with the heat
gun.
through the centre axis. These crosses
are where the nodes are to be fixed and
should be visible through the grid. If
the centre is not visible, project where
it should be and mark the grid with a
felt pen at this point.
The nodes are made up of small
discs of 2mm thick Teflon attached to
the grids with silicone adhesive. Place
a blob of silicone adhesive about 5mm
in diameter and 4mm high at the centre
of each cross. Place a white Teflon disc
with the backing paper (brown side)
up, gently on top of the blob. Place an
ordinary piece of A4 paper on top of
the long PVC spacer on either side of
the Teflon disc.
Using the edge of a steel rule, press
the disc into the blob of silicone until
the rule is resting on top of both pieces
of paper. The surface of the disc should
be parallel to the surface of the air gap
spacer. Now move up to the next node
position. Repeat this process on all
panel halves which are marked with
the black crosses running down the
centreline (six of them).
The Teflon discs have an adhesive
layer which is covered by backing
paper. As the disc has been set at a
56 Silicon Chip
Installing the foil tape
Each panel has a wire attached to its
diaphragm for the EHT. Some matrix
panels do not have a fully filled-in
section on one side. The side that is
filled in has the foil tape attached to
it. The 150mm long foil tape is placed
on the air gap spacer, running towards
the top of the panel.
From the small roll, tear off about
150-175mm of foil tape. Peel about
50mm of the backing from the foil
and apply the tape at the connection
point first and run it onto the top of
the PVC spacer. The tape needs to be
turned through 90° toward the top of
the half panel.
The easiest way to do this is to fold
the tape over at 90° in the opposite
direction to that which is desired; ie,
fold the tape towards the bottom of the
panel. Peel off some more backing and
fold the tape back on itself towards the
top of the panel. This will make a neat
turn in the tape. Peel off the backing
about 50mm at a time and stick the
remainder of the tape down onto the
air gap spacer.
Drill a 3mm hole through the foil
and matrix at the connection point.
Don’t use too much pressure as the
matrix is fragile. Crimp or solder an
eye connector to 400mm of EHT wire
and fix to the panel connection point
with a screw and nut. It is best if the
terminal is on the inside section of the
matrix. This will allow the channel
section to sit as close as possible to the
matrix. When tightening the screw, be
careful not to tear the foil tape.
Diaphragm installation
It is suggested that the diaphragms
for the narrow treble panel should
be fitted first. This will give some
experience for the more difficult bass
panel. Place the half panel with the
Teflon node points spacer side up
onto the work surface. Make sure that
the clear protective covering on the
air gap spacers has been removed, as
mentioned earlier.
Remove the backing paper from
the Teflon node points. Remove the
clear backing from the supplied diaphragm. “TOP” has been marked on
the diaphragm surface to identify it.
Tear off four pieces of masking tape
about 80mm long and attach them to
each corner of the diaphragm.
With the help of an assistant, hold
the diaphragm taut over the half panel
and lower it onto it. It is important that
the diaphragm overlaps the air gap
spacers on all sides before coming into
contact with the Teflon node points,
as the adhesive bond will be difficult
to break if an error is made.
If an assistant is unavailable, tape
down one end of the diaphragm to the
work surface, keeping the other end off
the panel. Lower the diaphragm down
onto the panel, ensuring there is some
overlap around all edges.
Tape the diaphragm down to the
work surface using more masking
tape. Use tape in the four corners and
at about seven or eight equally spaced
positions along the longest edge.
Tension the diaphragm as much as
possible by pulling on the tape prior
to sticking to the work surface. This
initial tensioning will not affect the
ultimate tension achieved after the
heat shrinking process. It is simply to
make this process easier.
The diaphragm should now be taut
and wrinkle free. The node points
should be visibly contacting the diaphragm all down the centre axis of
the half panel.
Using a heat gun on low setting,
aim the hot air from about 150mm
at an angle of about 45° at the PVC
spacer. Keeping the heat gun moving
at all times along the air gap spacer,
use a small pad of folded tissue to
gently push the heated diaphragm into
contact with the PVC. The heat will
melt the adhesive backing and allow
a strong bond to the PVC spacer.
Follow this procedure all the way
around the perimeter of the panel.
Small wrinkles will occur in the
diaphragm during this procedure.
Don’t worry about them. They will
disappear when the diaphragm is fully
tensioned.
Conductive fluid is applied to the diaphragm film with the aid of a small sponge.
After the diaphragm is stuck to the
panel it will need to be tensioned.
Keeping the heat gun moving at all
times, direct the hot air around the
edges slowly working towards the centre of the panel. Take care not to blow
the diaphragm down onto the grid. If
this does happen it may be released
by gently heating and pushing through
from underneath with a paint brush.
The alternative method is to release
the diaphragm from the PVC spacer
nearest to the stuck down portion
using gentle heat, and lifting the diaphragm clear of the grid. It can then
be re-stuck to the PVC spacer.
The correct tension has been reach
ed when the diaphragm will not
shrink any more. This point can be
determined by passing the gun over
the diaphragm and watching if any
wrinkles appear as heat is applied. If
none do, the diaphragm has reached its
maximum tension. If wrinkles appear
or the diaphragm “sags” when heat is
applied, continue with the shrinking
process.
Applying conductive coating
Note: it is essential that the conductive coating is applied in temperatures
above 20°C. Failure to do so will lead
to a poor surface cure.
After the diaphragms have been tensioned they need to be made conductive. Gently wash down the surface of
the diaphragm with methylated spirit
and a clean tissue. Do this three times
(on the same diaphragm). Ensure that
the diaphragm is dry. The heat gun can
be used for this.
Pour a small amount of the acrylic
conducting solution into a small bowl.
Using a small piece of sponge, lightly
swab the solution over the surface of
the diaphragm. Keep the conductive
coating about 5mm from the internal
edge of the air gap spacers except in
the area that will be contacted by the
foil tape on the other half panel. The
conductive coating should overlap
this air gap spacer by about 10mm
for the length of the foil tape. This is
the only portion of air gap spacer that
should have the conductive coating
overlapping it.
The covering should be light with no
evidence of puddles. Avoid air bubbles
on the surface. If any foreign matter
such as hair sticks to the coating, it
may cause a discharge path for the
bias voltage. Avoid this like the plague.
Do not allow the conductive solution
to spill over the side of the panel as
this may also allow a leakage path for
the EHT. Make sure that the solution
is applied to the diaphragm area that
the foil tape will contact when the
panel halves are assembled. Now put
this panel aside and coat the next.
The solution takes about two to three
hours to cure.
Check the resistivity and continuity with your multimeter. Place the
two probes gently on the diaphragm
surface about 100mm apart. The
resistance reading should be 20 to
100 megohms. Place the probes at
either end of the diaphragm on the
conductive coating. A reading of over
20 megohms should be obtained. The
actual value is not critical. This test
just confirms that the diaphragm is
conductive all over.
When using probes on the diaphragm ensure that it is not punctured.
Next month will give the final assemSC
bly instructions.
March 1995 57
A Look At
The 68000
Microprocessor
RO
UN
DE
DG
E
0
HB
By ELMO JANSZ
The 68000 microprocessor is manufactured
by Motorola & made its debut in about 1979.
It is a 16-bit device & was designed to
supersede the earlier 8-bit 6800. It is widely
used in Apple Macintosh & Atari machines.
Over the years, the amount of hardware and software accessories available for this device has grown rapidly.
From the 68000, a family of devices
has now come into existence such
as the 68010, 68020, 68030 and the
68040. In this article we shall confine
discussion to the 68000.
From this point onwards we shall
refer to the microproces
sor as the
MPU. The 68000 comes in a 64-pin
package which elimi
nates the need
for multi-function pins and simplifies
interfacing with external hardware.
It has a 32-bit internal architecture,
which includes 16 internal general
purpose registers, each 32 bits wide.
Eight of these are data registers and
the rest are address registers.
The data and address registers do
not have dedicated functions such as
an accumulator, which was so with
the 6800. Instructions can be written
58 Silicon Chip
so that operands reside in any of the
data registers or storage locations
in external memory. The MPU can
handle a bit, a byte, a word or a long
word of data.
A bit is one binary digit, a byte is
eight binary digits, a word is 16 binary
digits, and a long word is 32 binary
digits.
The MPU has 23 address lines, giving it access to a very large range of
addresses in external memory. It also
has access to a user/supervisor environment which provides for multipro
cessing and multitasking activities; ie,
the ability to handle more than one
task at a given time.
Interface buses
Fig.1 is a block diagram of the MPU
showing its interface buses. Buses
are groups of pins or lines and these
come under the following headings:
Address, Data, Asynchronous Control,
Processor Status, System Control Bus/
Function Codes, Interrupt Control,
Arbitration Control and Synchronous
Control. Let’s examine each of these
in turn.
The address bus: the MPU has a 23bit address bus. Lines A1 to A23 are
used to address memory and input/
output devices. A0 is not shown as it
is internal to the device and is used to
determine whether the upper or lower byte of a word is to be used when
processing byte size data.
The data bus: labelled D0-D15, this
bus is bidirectional and can be used to
read/write data. Byte size data can be
transferred on either half of the bus,
while word transfers use both halves.
The asynchronous control bus: the
MPU uses asynchronous bus control.
This means that once a bus cycle
(ie, a procedure) is initiated, it is not
completed until a signal is returned
from external memory. Five signals
are available to control address and
data transfers. These are:
(1) Address strobe (AS-bar)
(2) Read/write (R/W-bar)
(3) Upper data strobe (UDS-bar)
(4) Lower data strobe (LDS-bar)
(5) Data transfer acknowledge
(DTACK-bar)
The MPU has to indicate to external
devices when an address is available
and whether a read or write operation is to take place. The AS-bar and
R/W-bar signals perform this activity.
When a valid address is placed on
the address bus, the AS-bar line is
pulsed low.
The R/W-bar indicates whether a
read or a write is to commence. When
the MPU reads data from the data bus,
R/W-bar is pulsed high. When data
is written to memory or to an output
device, R/W-bar is pulsed low. The
asynchronous bus cycle requires external memory to signal the MPU when
the cycle is completed. The DTACKbar input provides this. During a read
cycle a low on DTACK-bar indicates to
the MPU that valid data is on the bus.
The MPU reads, latches the data, and
completes the cycle.
During a write operation, DTACKbar informs the MPU that data has
been written to memory or an output
device. The UDS-bar and the LDS-bar
are called the upper and lower data
strobes respectively, and indicate
whether a byte or word of data is on
the data bus. A low on UDS-bar indicates a data transfer on the upper
eight lines of the data bus. A low on
LDS-bar indicates a transfer on the
eight lower data lines.
Table 1 shows the logic levels possible for each type of data transfer.
Bus function codes: during a bus
cycle, the MPU outputs a 3-bit status
code on FCO, FC1 and FC2. These
are called the bus function codes and
these inform external devices what
type of bus cycle is in progress. They
indicate whether data or program is
being accessed and whether the MPU
is in the user or supervisor state.
The codes are output at the beginning of each read or write cycle and
continue to be valid until the next read
or write cycle commences.
System control bus: this bus is
comprised of the three lines BERR-bar,
HALT-bar and RESET-bar. BERR-bar is
an input to the MPU to inform it that
there is a problem with the current
bus cycle, while the HALT-bar signal
is used to stop the MPU. An external
signal applied to this line stops it at
the completion of the current cycle.
HALT is bidirectional and when an
instruction execution is terminated,
external devices are informed of the
fact using this line. RESET-bar is used
for initialisation with a signal from
ADDRESS
BUS
VCC(2)
A1-A23
ADDRESS/
DATA
GND(2)
CLK
DATA
BUS
D0-D15
FC0
PROCESSOR
STATUS
MC68000
PERIPHERAL
CONTROL
(SYNCHRONOUS
CONTROL)
FC1
FC2
MC68000
MICROPROCESSOR
R/W
UDS
E
LDS
VMA
ASYNCHRONOUS
BUS CONTROL
DTACK
VPA
BR
BG
BERR
SYSTEM
CONTROL
AS
BGACK
RESET
HALT
BUS
ARBITRATION
CONTROL
IPL0
IPL1
IPL2
INTERRUPT
CONTROL
Fig.1: this block diagram of the 68000 MPU shows all the various interface
buses. These fall into various groups & the function of each group is explained
in the text.
external hardware, generally at power
up. It is bidirectional but its output is
software controlled.
Interrupt control bus: this bus is
comprised of three lines, IPLO-bar,
IPL1-bar and IPL2-bar, and is used to
service interrupts from external devices. In an interrupt routine, the MPU
discontinues its current activities
and services an external device. The
external device provides a 3-bit code
on these lines and this is compared
with a mask value in the status register.
Arbitration control bus: this bus is
comprised of the three lines BR-bar,
BG-bar and BGACK-bar. These signals
are used for hand
shaking activities
that control transfer of the MPU’s
system bus between devices. Hand
shaking is the correct communication
between devices so that information
can be smoothly transferred between
them. The device that possesses control of the bus at any time is called the
Bus Master.
Synchronous operation: the MPU
has facilities for transferring data
over the system bus in a synchronous
manner. In a synchronous transfer, no
acknowledgment is required from the
receiving device before the next piece
of information is transmitted. Three
control signals are available for this
function: Enable (E), Valid Peripheral
Address (VPA-bar) and Valid Memory
Address (VMA-bar). They are used
to interface the MPU to much slower
devices.
Enable (E) provides a free-running clock 1/10th of the MPU clock
frequency. For example, it could be
used to interface the 10MHz MPU
Table 1: Logic Levels For Each Type of Data Transfer
UDS-bar
LDS-bar
R/W-bar
0
0
0
Word transferred to memory or I/O
0
1
0
High byte transferred to memory or I/O
1
0
0
Low byte transferred to memory or I/O
1
1
0
Invalid data
0
0
1
Word transferred to MPU
0
1
1
High byte transferred to MPU
1
0
1
Low byte transferred to MPU
1
1
1
Invalid data
Comments
31
16 15
87
16 15
31
0
0
15
87
SYSTEM BYTE
USER BYTE
to a 1MHz external device. VPA-bar
indicates to the MPU that it is to perform a synchronous data transfer over
its asyn
chronous system bus. Valid
Memory Address (VMA-bar) is a signal
produced by the MPU when VPA-bar
goes active. It tells external equipment
that a valid address is present on the
address bus and that the next data
transfer will be synchronised to the
enable (E) line.
Clock input: the block diagram
shows a single clock input labelled
CLK. This signal is externally generated and fed to the MPU at frequencies
between 4MHz and 12.5MHz.
Internal registers
The MPU contains 18 32-bit internal registers as depicted in Fig.2.
Observe that there are eight data
registers, seven address registers, two
stack pointers, a program counter and
a status register.
The status register, unlike the others,
is only 16 bits wide. The eight data registers are labelled D0 - D7 and are each
32 bits wide. The least significant bit
is labelled B0 and the most significant
bit B31. Each can work with a byte, a
word or a long word of information.
This information is generally referred
to as the operand.
Byte data always resides in the
eight least significant bits, words in
the least significant 16 bits and long
words occupy all 32 bits. The size of
the operand is specified in the instruction. Data registers can also be used
as index registers. The value in the
register represents an offset, which
60 Silicon Chip
EIGHT
DATA
REGISTERS
A0
A1
A2
A3
A4
A5
A6
SEVEN
ADDRESS
REGISTERS
A7
TWO STACK
POINTERS
0
USER STACK POINTER
SUPERVISOR STACK POINTER
31
D0
D1
D2
D3
D4
D5
D6
D7
0
Fig.2: the MPU
contains 18 32-bit
internal registers
as depicted here
There are eight data
registers, seven
address registers,
two stack pointers,
a program counter
& a status register.
PROGRAM
COUNTER
STATUS
REGISTER
can be combined with the contents
of another register to point to a data
location. This facility is very useful in
reading blocks of information.
Address registers
The address registers are labelled A0
to A7 and are also 32 bits wide. They
do not store data but rather address
information such as base and pointer
addresses.
There are two stack pointers called
the user stack pointer (USP) and the
supervisor stack pointer (SSP). Only
one of these is active at any time and
for this reason they are shown as a
single register, A7. USP identifies the
top of the stack in the user part of
system memory. This is the section
in memory where return addresses,
(ie, when called upon to temporarily
suspend its normal activities and attend to some other demand) are stored.
Register data and other parameters are
also saved in the stack.
When in the supervisor state the
user stack pointer becomes inactive
and the supervisor stack becomes
active. The address contained in the
supervisor stack points to the top of
a second stack called the supervisor
stack.
The supervisor stack is used for the
same purpose as the user stack but it
is also used by supervisor calls such
as software exceptions, interrupts and
internal exceptions. Exceptions are
similar to interrupts. The procedure
permits the MPU to respond to certain events, external or internal, by
suspending its current activities and
switching to a new program sequence.
At the completion of the routine, the
program is switched back to the point
at which it left off in the main program.
(The return address is stored in the
stack before commencement of the
new program sequence).
The program counter
The program counter points to
the next instruction to be executed.
It is automatically incremented by
two when an instruction is fetched.
Although the PC is shown as composed of 32 bits, only the lower 24 are
used. These can access 16M bytes or
8M words; ie, the address space can
be considered to hold 16M bytes or
8M words. Word addresses are even
and can have values from 00000016
through to FFFFFE16.
Note that 1K = 1024 bytes and 1M
= 1,048,576 bytes.
The status register
The status register is shown in
Fig.3. Two bytes called the User byte
and the System byte are shown. Each
byte consists of a number of flags or
condition codes.
The carry flag, bit 0, is set when an
add operation generates a carry out
or a subtract (or compare) operation
requires a borrow. During shift or rotate operations (ie, the movement of
the bits of a piece of information), it
holds the bit that is rotated or shifted
out of a register or memory location.
The overflow flag is bit 1. If an
arithmetic operation on signed numbers (numbers that are represented
as positive or negative quantities)
produces an incorrect result, then
the overflow flag is set; otherwise it
is cleared.
The zero flag, bit 2, is set when
the result of an operation is zero. A
non-zero result clears the z flag. The
negative flag, bit 3, depends on the
sign bit; ie, the most significant bit of
the result of an arithmetic logic, shift
or rotate operation. If this bit is 1 then
the flag is set; otherwise it is cleared.
The extend flag, bit 4, takes the same
status as the C Flag, resulting from a
shift or rotate operation.
Let us now examine the system byte
of the status register. It contains the bits
that control the operational options of
the MPU and the interrupt mask which
was mentioned above.
Bit 13 is used to distinguish between the user and supervisor states
of operation. A logic 1 in this bit indicates that the MPU is operating in the
supervisor state while a 0 indicates
the user state.
Trace Mode (T)
The T bit (Trace mode) is used to
enable or disable trace (Single Step)
operation. It is active or not by setting
or clearing bit 15. The entire contents
of the Status Register can be read using
software. Un-implemented bits are
read as logic 0. The system byte can
be modified only when the MPU is in
the supervisor state.
Addressing modes
Addressing modes give information
to the programmer on how to generate
an address that identifies the location
of the operand. The operand is the
information being worked upon.
We observed earlier that the MPU
includes eight data registers and eight
address registers.
Data registers are used for storing
usable data. Address registers, on the
other hand, are used to access source
or destination operands residing in
memory. The MPU can address a very
large memory space, 16 megabytes
in fact.
The addressing modes available to
the MPU can be classified under the
following headings:
(1) Immediate
(2) Direct
(3) Absolute
(4) Address Register Indirect
(5) Address Register Indirect with
16-Bit Displacement
(6) Address Register Indirect with
Index and 8-Bit Offset
(7) Address Register Indirect with
Post-Increment
(8) Address Register Indirect with
Pre-Decrement
(9) Program Counter Relative with
16-Bit Displacement
(10) Program Counter Relative with
Index and 8-Bit Offset
Let us examine each of these using
only the MOVE instruction which is
available with all addressing modes.
Immediate: in immediate addressing, the operand is included in the
instruction. For example the operation
“MOVE.W #$AABB,DO” moves the
word $AABB into Data Register D0.
The symbol # indicates that immediate addressing is to be used. The $
sign indicates hex-data. $AABB is the
source operand.
SYSTEM BYTE
15
T
13
S
USER BYTE
8
10
I2 I1 I0
4
X N Z V
0
C
TRACE MODE
SUPERVISOR STATE
INTERRUPT MASK
EXTEND
NEGATIVE
CONDITION
CODES
ZERO
OVERFLOW
CARRY
Fig.3: the status register. Two bytes called the user byte & the system
byte are shown. Each byte consists of a number of flags or condition
codes.
For dealing only with bytes of data,
a special form of immediate addressing
called Quick Immediate addressing is
available.
The instruction “MOVEQ #AA,D0”
uses this form of immediate addressing
to move the byte $AA into D0.
Direct: Direct addressing is used
only when one of the data or address
registers contain the operand. If the
register specified by the instruction is
the data register, the addressing mode
used is called Data Register direct. On
the other hand, if the address register
is specified, it is called Address Register direct. Consider the instruction
“MOVE.W AO,DO”. The Move.W
portion indicates that the word in A0
is to be moved into D0. A0 contains
the source operand and D0 has the
destination operand.
The source operand uses address
register direct addressing, while the
destination operand uses data register
direct addressing. Both operands do
not reside in external memory.
Absolute: in the absolute addressing mode, the effective address of the
operand is included in the instruction. There are two forms of absolute
addressing, called absolute short and
absolute long. Both forms are used to
access operands residing in external
memory.
If absolute short addressing is used,
a 16-bit address must be included as
the second word of the instruction.
This is the storage location of the
operand in memory. Consider the
instruction: “MOVE.L $2345,D0”. It
indicates that the long word commenc
ing at address location $2345 is to be
moved into the data register D0.
The MPU does a sign extension
based on the most significant bit of
the absolute short address to give a
32-bit address. (Remember only 24
bits are used as the address bus is 24
bits wide).
$2345 = 0010 0011 0100 0101
The most significant bit is 0. Extending it gives:
0000 0000 0010 0011 0100 0101
ie, the required address is $002345.
Absolute short addressing generates
an address corresponding to the first
and last 32K bytes of the MPU’s address space. Absolute long addressing
permits the use of a 32-bit number as
the data address.
The instruction “MOVE.L $02345,
D0” has the same effect as the previous
one, with the exception that the absolute address is specified with more
than four digits. The source operand
is now encoded by the assembler as
an absolute long address using 32 bits
instead of 16. Again, only 24 bits are
actually used.
The operand can now reside anywhere within the address space associated with the MPU.
Address register indirect: in this
form of addressing one of the address
registers contains the address of the
source or destination operand. As an
example, in the instruction “MOVE.L
(AO), D0”, A0 contains the address
of the source operand and must be
enclosed in brackets. D0 is the destination operand.
Execution of the instruction causes
the long word at the address location
pointed to by the contents of A0 to be
copied into D0.
Address Register Indirect With
16-Bit Displacement: this address
ing mode uses a sign extended 16-bit
displacement, which is added onto
the contents of the address register to
March 1995 61
generate the address of the operand.
Consider the instruction “MOVE.W
10 (AO), D0”. 1010 is the 16-bit displacement. Since the displacement
is 16 bits wide, the operand must be
within +32K bytes of the memory
contents pointed to by the address
register.
In Address Register Indirect addressing, the address of the operand is
determined by adding the contents of
an internal register and the signed 8-bit
offset to the contents of the address
register. The internal register serves
as the index.
For example, in the instruction
“MOVE.W 12(A0, D0), D1” 1210 is
the offset, A0 the address register and
D0 the index register. These quantities
are added to determine the address of
the operand.
Address Register Indirect With
Post-Increment: this addressing mode
is similar to address register indirect
addressing.
However, with post-increment, after
the address is used, the contents of
the address register are incremented
by one, two or four depend
ing on
whether a byte, a word or a long word
was accessed. Consider the instruction
“MOVE.W #AABB,(A0)+”. We observe
that the operand is to be placed in the
address location pointed to by the
address register. After the operation,
the address register is automatically
incremented by 2, since the operand
is a word.
Address Register Indirect with
Pre-Decrement: is similar to address
register indirect with Post-Increment,
except that the address register is
first decremented by one, two or four
depending on whether a byte, word
or long word is involved. Consider
the instruction “MOVE.W #AABB,
-(A0)”. The address register is first dec
remented by 2 since a word is involved
and the word $AABB is moved into
the address indicated by the address
register.
Program Counter Relative with
16-Bit Displacement: in this mode,
a displacement is used to indicate to
the program counter how many bytes
the data to be accessed is located away
from its current position. When the
instruction is executed, the MPU sign
extends the 16-bit displacement to 32
bits and then adds it to the updated
value of the program counter.
Consider the instruction “MOVE.L
Loc (PC), D0” which moves the long
word starting at memory location with
label Loc into D0.
To do this the assembler calculates
the number of bytes the updated value
of the program counter is away from
the address with label Loc. This value
is expressed as a signed 16-bit binary
number and is added onto the current
value of the program counter. Since 16
bits are used the operand lies within
+32K bytes of the updated value of the
program counter.
Program Counter Relative with Index and 8-Bit Offset: this is similar to
the addressing mode examined above
except that both an index and an offset
are used. The contents of an index
register – any of the data or address
registers, together with a signed 8-bit
offset – are added to the updated value
of the program counter to determine
the address of the operand.
Now consider the instruction
“MOVE.W 6(Pc, D0), D1”. 610 is the
8-bit offset and D0 represents the
index. Both values are added to the
updated value of the program counter
to obtain the address of the operand.
Once located the operand is loaded
SC
into D1.
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Phone (02) 979 5644 Fax: (02) 979 6503.
REMOTE CONTROL
BY BOB YOUNG
Building a complete remote
control system for models; Pt.3
This month, we describe the construction of
the Mk.22 receiver board. The top of the board
accommodates the coils, a ceramic resonator &
crystal holder, while the underside is packed
with surface mount components.
D1 C4 ANT2
Q1
C3
R1
R9
E
OUTPUT
+4.8V
C16
TB1
L4
CF1
L3
R11
R3
C12
Q2
Q5
Q6
L6
Q4
R13
C8
R2
C6
C1
R4
C2
C14
C9
C5
This is quite a delicate little PC
board to make. Minimum track spacing
is .016-inch, minimum track width is
XTAL1
C10
C11
R12
C15
R5
C13
Q3
R10
C7
Construction
R6
R7
R8
ANT1
ers. The decoder layout (to follow next
month) allows the utmost in flexibility to overcome the problems of non
standardisation of the servo plugs. The
decoder also features heavy filtering to
help minimise the problems of inter
ference on long servo leads.
The physical layout is that used in
all Silvertone receivers since 1969
and both the receiver and decoder
PC boards may be used as direct replacements for earlier modules back
to Mk.7. The Mk.22 is better in regard
to mechanical robustness, receiver
OUTPUT
The receiver will be supplied as a
full kit, as an assembled and tested PC
board, or as a fully assembled receiver
with decoder included. In all cases a
PC board is supplied but for the those
wishing to do their own PC boards, I
have just one few tip which is “don’t
bother. After all, it took many refinements of the basic layout before I was
completely happy.”
However, a little background won’t
hurt. The Mk.22 is designed essentially as an AM receiver replacement for
all brands of commercial R/C receiv-
sensitivity and electric motor noise
immunity. The physical layout provides the smallest frontal area, with
the PC boards mounted at right angles
to the direction of travel of the model.
This minimises component damage
in crashes. The case is very robust,
being heavy gauge aluminium, and
this also provides improved noise
immunity.
The two-board arrangement also
allows the receiver to be used separately, free of the clutter of an existing
decoder. Note that the board is double
sided, with the ground plane on the
top. The holes are plated through, so
there’s no need to solder the throughhole components on both sides.
L1
L2
L4
D2
Fig.1: the layout of the surface mount components,
shown 50% larger than actual size. Note that the
components are numbered to match those on the
circuit published in last month’s issue.
Fig.2: the through-hole components, such as the coils
and crystal holder, shown 50% larger than actual
size. Note that the coils are numbered to match those
on the circuit published in last month’s issue.
March 1995 63
Fig.3: repeated from last month, this scope photo shows
a typical output waveform at the collector of transistor
Q6. Note that the number of spikes will depend on the
control settings of the transmitter.
.012-inch and minimum component
spacing is .020-inch. I have tried to
keep the number of components to
a minimum and the spacing as wide
as possible but on a board this size
spacing will always be tight. Check
the etched PC board for shorts, particularly where two tracks go under
one component.
Now set the PC board groundplane
down on a clean sheet of white paper
and commence to place the surface
mount components. The paper is for
contrast when you drop a component.
You will not find it on a dirty bench.
Do not leave discarded components
lying around on the bench where you
are working, especially unmarked
capacitors. You have been warned.
Keep that sheet of paper clear of all
items except the component value you
are working with at the time. I would
suggest that before going further, you
re-read the column on the hand assembly of surface mount PC boards in the
January 1995 issue.
The layout of the surface mount
components is depicted in Fig.1,
shown 50% larger than actual size.
The through-hole components, such as
the coils and crystal holder, are shown
in Fig.2, again 50% larger than actual
size. Note that the diagrams show
the components numbered to match
those on the circuit published in last
month’s issue.
Begin by aligning the PC board with
the single SOT23 pad for D2 closest
to your soldering hand. Proceed to
tin one pad only in each component
64 Silicon Chip
This larger-than-life size photo shows the completed
receiver assembly. Note the socket for the plug-in crystal.
The resistors, capacitors & transistors are surface-mounted
on the other side of the board.
set. The best pad to tin is that closest
to your soldering hand. Once one pad
in every component set is tinned, you
may commence component placement. To mount each component,
simply pick it up with the tweezers,
heat the tinned pad and slide it into
position, taking care to obtain correct
alignment on the centre of the pads.
Now, while the component is still
warm, solder the other leg(s).
There is no set order of assembly
but it is a good idea to place all of one
value at a time. I usually start with the
semiconductors. One good tip is keep
your components in a little plastic
tray. The lid of a small pill bottle is
ideal, but make sure it is white. Tip
all of the components (one type only)
into the lid.
Most components, if they are
marked at all, are only labelled on one
side and you should mount them with
the marking visible, so that servicing
is easier later. Now when you want to
turn a component over you just tap the
lid gently on the workbench and the
components will do a little dance and
some of them will turn over. Mount
those that present the markings up and
then just keep tapping the lid until all
components are placed.
When all the surface mount devices
are mounted, begin mounting the components on the topside of the board,
as shown in Fig.2.
Finally, solder one metre of hook-up
wire to Antenna 2 (ANT 2). Plug in the
receiver crystal and you now have a
finished receiver. It takes me approxi-
mately an hour to assemble a receiver
with conventional components or 45
minutes for the surface mount version.
A surface mount assembly machine
will do the same job in approximately
one minute!
There is one point to note in regard
to TB1, the 4-pin header. This may be
mounted or left out completely. In the
latter case simply insert the wires from
the decoder directly into the holes.
You may wonder why there are two
pins connected together. The spare
pin can be very useful for tuning the
receiver. Even if the header pins are
not mounted, solder a short piece of
wire into the spare hole as a tuning
point to hook oscilloscope and meter
leads onto.
Alternatively, if a remote antenna
is used, these two pins may be separated and the spare pin used as an
antenna connection. In this case, join
Antenna 1 to the spare pin on TB1
with a jumper.
Testing & tuning
Conduct one final visual inspection
to ensure all connections are complete.
Check for shorts and then switch your
multi
meter to its lowest resistance
range and check across the power
connections for a direct short.
Wind the slugs in RF coils L5 &
L6 well in towards the bottom of the
formers and set the oscillator slug flush
with the top of the coil. You must use
a plastic alignment tool for this job;
don’t use a small screwdriver as it is
too easy to damage the slugs.
Begin with the routine DC checks.
Hook up a 4.8V nicad pack to the appropriate pins on TB1. If the header
pins have been installed, then the pin
layout is directly compatible with a J.R
or Futaba battery pack connector and
the battery pack may be plugged directly into this connector. Check to ensure
that the DC conditions are correct on
each stage. The decoupled power rail
after Q5 will be about +4.1V when
supplied directly from the battery
and approximately 0.2V lower when
supplied from the decoder which has
its own decoupling.
The oscillator coil tuning is not
critical and the oscillator should be
running with the slug in the coil flush
with the top of the coil former. If an
oscilloscope and frequency counter
are at hand, then check the waveform
and frequency of the oscillator.
The waveform should be near sinusoidal, approximately 1.5V volts
peak-peak in amplitude and if Showa
crystals are used, almost on frequency. The tolerance on these crystals
is ±0.005% and thus a variation of
±1.5kHz is acceptable. C7 and C10
may be adjusted to trim the frequency
if other brands of crystals are used
and they are not close enough to the
designated frequency.
If all is well at this point, hook up
a meter to ground (Black) and pin 4
on TB1 (red lead). It is a good idea to
put a 4.7kΩ resistor in each meter lead
to provide isolation for the receiver.
Hook the scope to the meter side of
these leads. Apply power and the
meter should read approximately 3.9V
and steady. The scope trace should be
a straight line. You are now ready to
tune the RF and IF stages. This will be
achieved by tuning for the maximum
no further gains are to be had. At this
point the receiver is tuned.
A word of warning: do not run
commercial transmitters for too long
with the antenna collapsed as this may
damage the output transistors.
If you have a scope, check the output
waveshape at Q6 and compare it with
the photo of Fig.3. All being well, it
should be comparable. You now have
a going receiver ready for connection
to a decoder.
Troubleshooting
The finished receiver & decoder are
shoe-horned into a very compact
folded aluminium case. This easily
comes apart for good access to the two
boards inside.
dip in the collector voltage of Q6.
Turn on the transmitter or signal
generator and set the output to maximum or fully extend the transmitter
antenna. A dip should be noticeable
on the meter with the RF signal present. You may have to almost touch
the transmitter and receiver antennas.
These may be touched together as
long as the Rx antenna is insulated.
Beginning with coil L5, tune the slug
for maximum dip (minimum volts) at
the collector of Q6. Move then to L6,
L4, L2 and L1. By this time the voltage
at Q6 should be almost zero.
Now reduce the signal level, move
the transmitter away or collapse the
antenna and retune with the smallest
comfortably detectable signal (about
0.5V). From here on, all tuning must
be done with the lowest level of signal
possible, otherwise the AGC action
will affect the tuning on the IF coils.
Continue to cycle through the coils,
reducing signal and retuning until
Provided you have used the components supplied in the kit, most of
your problems will be assembly faults.
Check for dry joints and shorts or
missing or unsoldered components.
A scope is very handy at this point.
Begin by checking the rail voltages
and then move on to the oscillator and
check the DC voltages at the transistor.
If the oscillator is running, the base
voltage will be lower than the emitter
voltage.
Next, check the voltages around
transistors Q1, Q2 and Q4. The base
voltage will be approximately 0.6V
higher than the emitter voltage (eg,
base +1.1V, emitter +0.35V). The collectors will sit at the decoupled supply
voltage, +4.1V. The base of Q6 will be
+0.6V and the collector with no signal
approximately +3.9V.
If all of the DC conditions are OK,
from here on it is routine RF servicing, using a signal generator (Tx) and
oscilloscope and stage by stage debugging. If all else fails, send it back to
father (yours truly) and he will either
repair it or replace the module at a
nominal fee. Details of kit availability and prices will be given in next
SC
month’s issue.
Protect your valuable issues with these
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.
They hold up to 14 issues & will look great on your bookshelf.
★ High quality with heavy board covers
★ Each binder holds up to 14 issues
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March 1995 65
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
An IR illuminator for
cameras & night viewers
What ever would you use an infrared (IR)
illuminator for? To see in the infrared region,
that’s what for. More precisely, an IR illuminator
can be used with CCD video cameras & with IR
night viewers such as the model described in the
September 1994 issue of SILICON CHIP.
By BRANCO JUSTIC
This IR illuminator provides an
output of up to 1.4 watts at 880
nanometres. Most CCD cameras will
respond, to some extent at least, to
infrared light. The CCD modules themselves are quite responsive to infrared
light but many cameras include an
infrared filter. This is done so that
pictures taken in low light conditions
do not have unnatural highlights (to
our eyes) due to the pickup of infrared
light.
There are two easy ways to check the
IR response of your CCD video camera.
First, set it up in a darkened room and
then use a torch with red cellophane
over the glass. The camera should
then produce a useable picture of the
room. Second, try the same thing but
with illumination now provided by
the infrared remote control for your
TV, VCR or other appliance. This is
also a good way of checking that your
IR remote control is working.
Applications
Now that we have established that
CCD cameras can work with IR light,
why would you want to do it? The
most important appli
cation is for
security. You could light a building,
room, or a yard with infrared light and
any miscreant would have no way of
knowing that his actions were being
monitored by a video camera.
You could also use an IR illuminator
and CCD video camera for watching
wildlife. Perhaps you have possums or
other nocturnal visitors in your backyard or at your campsite. Now you can
video them without any disturbance
to their behaviour.
March 1995 69
D1
MR856
L1
200uH
0.47
5
4
PARTS LIST
+26.5-29.5V
+9-12V
100k
100
47
47
A
1
100
16VW
IC1
LM2577
2
4.3k
1.5k
1k
0V
K
A
LED40
LED20
K
LED41
K
A
VR1
1k
A
LED21
K
3
0.47
47
A
LED1
2 PC boards (see text)
1 200µH inductor (L1)
1 1kΩ pot (VR1)
A
LED60
K
K
CIRCULAR PCB
1
5
A
K
INFRA-RED ILLUMINATOR
Fig.1: the circuit uses a switched mode power supply based on IC1 to step up
the battery voltage to 26.5-29.5V. This rail then drives an array of 60 IR LEDs
via 47Ω current limiting resistors.
Another application is for monitoring patients in sickrooms or in hospital. They can then be permanently
watched without having their sleep
disturbed.
Some CCD camera modules intended for security applications come
with inbuilt IR LEDs for illumination
but generally they would only be
sufficient for close-up work. The IR
illuminator to be described here is
much brighter.
It is also an ideal IR source for most
first generation IR night viewers. For
example, just one single fibre optic
tube from the three stage viewer design published in the September 1994
issue of SILICON CHIP would produce
good results when illuminated with
this IR source.
One experiment involved combining the unit with a CCD camera
supplied by Oatley Electronics. This
setup provided good vision on a monitor of a vehicle parked about 50 metres
away in very low ambient light.
The circuit
As you can see from the circuit
diagram of Fig.1, the illuminator is
basically a closely packed array of 60
IR LEDs. There are three series strings
of 20 LEDs fed via a 47Ω resistor
The power supply section employs
a switched mode power supply which
is used to step up the voltage of the
battery to a regulated output voltage
adjustable over a range of about
26.5-30V. The battery voltage can be
9-12V without any need to change
the circuit.
An economical way of obtaining
a 12V battery for this unit would be
to connect two 6V lantern batteries
in series. These can be obtained for
around $4 each, or less.
Each IR LED drops a voltage of
approximately 1.33V when it is conducting, thus each string of 20 LEDs
requires a minimum of 26.6V. The
Semiconductors
1 LM2577T-ADJ step-up voltage
regulator (IC1)
1 MR856 or PL01 fast recovery
diode (D1)
60 IR383 880nm IR diodes
(LED1-60)
Capacitors
2 100µF 35VW electrolytic
2 0.47µF 50V monolythic
Resistors (0.25W 5%)
1 100kΩ
1 1kΩ
1 4.3kΩ
3 47Ω 1W
1 1.5kΩ
Where to buy a kit
The complete kit for this project,
including the two PC boards is
priced at $60 plus $4 for postage
& packing. The LEDs are available
separately at 10 for $9.00.The kit is
available from Oatley Electronics,
PO Box 89, Oatley, NSW 2223.
Phone (02) 579 4985 or fax (02)
570 7910.
current in each string is equal to (Vo26.6)/47Ω. The current in each string
is, therefore, adjustable from about 8
to 72mA. Since there are three strings,
the maximum total power delivered by
the step-up inverter is approximately
6.5W.
The voltage regulator employs a
National Semiconductor LM2577T.
This device can be used to step up
input voltages in the range of 3.5-40V
to output voltages up to 60V.
The IR LEDs used in this project
(IR383) have a very high quantum
efficiency. They are specified as having an output of 30mW <at> 100mA at a
wavelength of 880 nanometres. The
maximum continuous current for
these is 100mA but they can be pulsed
at currents up to 1.2A. The diodes supplied in the kit have a radiation angle
of 12° but they are also available in a
60° version (IR333).
Construction
This view shows the final version of the
IR Illuminator. Note the small heatsink
attached to IC1.
70 Silicon Chip
Two PC boards are required for this
project. There is a small board for the
step-up circuit and one for the 60-LED
array. The photos accompanying this
LED1-60
100uF
0V
0.47 0.47
200uH
+9-12V
D1
100k
IC1
LM2577
(ON HEATSINK)
1.5k
Fig.2: install the parts on
the two PC boards as shown
in this wiring diagram. The
200µH inductor is supplied
ready-wound.
100uF
A
A
A
A
A
A
A
A
A
A
A
A
47
A
A
A
A
A
47
A
A
A
A
A
47
1k
4.3k
A
A
A
A
A
A
A
A
A
A
A
A
A
A
A
A
A
VR1
article show the two boards neatly
mount
ed in a short length of PVC
tubing but while this is quite an attractive package, we found it doesn’t
work well in practice because both
the LM2577T switching regulator and
the LEDs themselves dissipate quite a
respectable amount of heat.
However, provided the regulator
is fitted with a small heatsink and is
not mounted in the same housing as
the LEDs, the circuit will function
satisfactorily.
On the other hand, if the whole unit
is packed into a short length of tubing
as shown, and no heatsink is fitted, the
current drawn from the battery will
gradually rise and the regulator’s temperature will rise to the point where it
switches itself off. So you have been
warned – don’t pack it tightly into a
small space and make sure both the
regulator and the LEDs are reasonably
well ventilated.
Assembly of the boards is quite
straightforward. Install all the components on the regulator board first. Note
that a 100µF electrolytic capacitor
must be connected across the battery
inputs to the board. This capacitor is
not shown on the
screen print overlay
on this board alA
though it is shown
on Fig.2.
A
A
When the reguA
A
A
lator board is complete, power it up
A
A
A
and check the DC
A
A
A
output voltage. The
voltage should be
A
A
A
able to be varied
from about 29.3V to
A
A
A
26.6V. The LM2577
A
A
IC runs at close to
50kHz and if you
A
are able to examine
the switching waveform on an oscilloscope, you will find
that the duty cycle
varies depending
on the input voltage
and the setting of
the pot, VR1.
Now assemble the LED board and
make sure you connect each LED in the
right way around. The longer lead on
each LED is the cathode, marked “K”
on the PC board.
When complete, connect both PC
boards together and power up. Unfortunately, you can’t immediately
tell whether the LEDs are emitting
but after a short while you can easily
tell –they radiate heat! As a final
check, fire up your video camera
in a completely dark room – it will
show the illuminator lighting it up
SC
brightly.
The prototype PC boards were built into a short length of PVC tubing but note that this will lead to overheating
problems unless the unit is used only in brief bursts (see text). A heatsink should also be fitted to IC1.
March 1995 71
COMPUTER BITS
BY DARREN YATES
Record real-time video with
the Video Blaster FS200
Creative Labs have released the second version
of their popular video package. We take a look
at the improvements which include real-time
video recording & playback.
These days with movies such as
Jurassic Park, as much work is done
on the computer (in this case Silicon
Graphics) as there is on the actual set.
While these computer systems can
cost beyond the million dollar mark,
Creative Labs, the makers of the Sound
Blaster, have made some big improvements in their graphics package, the
Video Blaster.
The original version (see our review
in the April 1994 issue) could display
real-time video on screen but the only
manipulation you could do was to grab
a frame and edit it or save it to disc.
The FS200 provides a pretty dramatic improvement by allowing you to
record and replay full-motion video
at up to 30 frames per second – not at
full VGA resolution but good enough
to make watching video on your PC
worthwhile.
What you’ll need
As you can imagine, capturing video signals is a pretty time consuming
task so don’t expect an XT to do the
job. In fact, you’ll need a minimum of
an 386SX-25 (25MHz) processor with
4Mb of RAM and at least 4Mb of spare
The Video Blaster FS200 lets you display full-motion video in a moveable
window. It comes bundled with a comprehensive range of software, including
Aldus PhotoStyler & Aldus Gallery Effects so that you can edit captured video.
72 Silicon Chip
hard disc space. The manual quotes
2Mb but by the time you’ve installed
the Video Blaster software, as well as
the Microsoft Video for Windows software, plus some space to work with,
you’ll need at least 4Mb.
The Video Blaster software itself
only allows capturing of a video frame
for editing but it does allow you to do
some special effects with a live video
feed such as chroma keying and rotation. To record and replay full motion
video, you’ll need to install the Video
for Windows software. Here, the user’s
guide suggests a minimum of a 386
processor and 2Mb of RAM, or 4Mb
of RAM if you wish to capture video.
As with most software, the more RAM
you have, the faster it will run.
Both packages require a VGA card
with at least 16-colours and 640 x 480
pixels resolution. You’ll also need a
CD-ROM drive to access the video
images located on the CD-ROM that
accompanies the package. Microsoft
suggest also that you have at least
100Mb of hard disc space free to store
your captured video and your drive
will need a write speed of at least
320Kb/second.
Any of the Sound Blaster audio
cards can also be used to record and
replay audio with your video as well.
Note that you’ll need this just to get the
audio/video signals into your computer. You’ll need the TVCoder to export
the video to your VCR if you wish to
store it on tape. If you use one of the
16-bit stereo sound cards, then you’ll
need a hifi VCR to record the sound
at the same quality.
Video accelerator card
One aspect that is a little disappointing is the fact that to get full
Software
The software for both packages
comes in both DOS and Wind
ows
versions. Also bundled in with the
FS200 are a couple of Aldus packages – a special edition of PhotoStyler
and the first volume of Gallery Effects. Both of these are designed for
single-frame editing and for creating
special effects.
PhotoStyler allows you to alter the
screen image by removing unwanted
objects from a picture as well as allowing you to convert a captured image to
CYMK colours.
You can also produce colour separations if need be. One of the more
stunning effects is the ability to cut out
a portion of an image and paste it directly onto another, called “merging”.
This is similar to an effect that can be
done with Windows Paintbrush but
with much greater control.
Gallery Effects allows you to change
the texture of a captured image. Some
of the textures you can use are chrome,
emboss, mosaic, watercolour and spatter. These can give your images a more
artificial, “painted” look.
System requirements for these
packages are the same as for the Video
Blaster except for hard disc space.
The Gallery Effects manual suggest
that a scanned 8 x 10-inch image
can require up to 7Mb of space so we
recommend that you have at least a
200Mb drive if you wish to use this
for serious work.
Overall, the Video Blaster FS200
system is a very desirable improvement over the original version but
you’ll need to have a few extras such
as the video accelerator card and others mentioned previously to get the
maximum benefit.
The package comes complete with
a video card, software and manuals,
plus connection cables for your PC
and video equipment. At $599, it has
to be one of the cheapest solutions for
editing full frame rate video. For further information, contact your nearest
SC
Rod Irving Electronics store.
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
❏
Floppy Index (incl. file viewer): $A7
❏
Notes & Errata (incl. file viewer): $A7
❏
Alphanumeric LCD Demo Board Software (May 1993): $A7
❏
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
Disc size required: ❏ 3.5-inch disc
❏ 5.25-inch disc
TOTAL $A
Enclosed is my cheque/money order for $A__________ or please debit my
❏
Bankcard
❏
Visa Card
❏
MasterCard
Card No.
Signature_______________________________ Card expiry date______/______
Name ___________________________________________________________
PLEASE PRINT
Street ___________________________________________________________
Suburb/town ________________________________ Postcode______________
Send your order to: SILICON CHIP, PO Box 139, Collaroy, NSW 2097; or fax your
order to (02) 9979 6503; or ring (02) 9979 5644 and quote your credit card number
(Bankcard, Visa Card or MasterCard).
✂
motion replay on your VGA screen,
you need a video accelerator card.
The only place I saw this mentioned
was at the beginning of Chapter 2 of
the Video for Windows user manual.
I would have thought that this was a
pretty crucial point considering that
the major selling point of the FS200
is its full motion record and replay.
March 1995 73
VINTAGE RADIO
By JOHN HILL
The inaugural vintage radio swap meet
This month, we begin by taking a look at the
Inaugural Vintage Radio Swap Meet. We then
review a new & interesting book on crystal sets
by Australian author, Bob Young.
Swap meets are common these days
and one of the biggest and longest
running is the Bendigo Swap Meet,
which is held annually in mid-Nov
ember. While the Bendigo Swap Meet
is pre-dominantly a vintage car meeting, the Historical Radio Society of
Australia (HRSA) has a site there each
year and encourages members who
wish to sell their wares to come along.
Dick Howarth is a Bendigo radio
collector who has somewhat more
go than most. He has just organised
Australia's first Vintage Radio Swap
Meet which was held on 23rd October
1994 at the Glenroy Technical School
Assembly Hall in Melbourne.
The meet was not confined to
vintage radio. It was more of a vintage sound affair and included phonographs and some amateur radio
equipment as well, although most of
the items offered were vintage radio
receivers.
Dick is a relative newcomer to ra
dio collecting. He is a fairly impatient
type who wants his repairs done yes
terday, works on his radio cabinets
until 2am, and is prepared to travel
interstate on the off-chance of finding
an interesting old radio. He always
seems to be thinking about vintage
radio and he probably dreams vintage
radio as well.
Anyway, things weren't happening
fast enough for Dick and he felt that
more could be done to promote interest
in vintage radio. A radio swap meet
seemed like a good idea and he set
the wheels in motion some six months
before the actual meeting. Dick always
does what he says he is going to do
and he is prepared to put his money
where his mouth is.
The highly successful Inaugural
Vintage Radio Swap Meet was a good
example of Dick Howarth doing what
he said he would do. What's more,
the meet was well organised, properly
run, and a credit to Dick and his wife
Raeleene, who put as much work into
the day as anyone.
The HRSA were approached and
they added their support to the project.
Some of the Melbourne members arranged a display of vintage equipment
which was neatly laid out on the stage
of the hall. Dick added to the stage display by including some of his console
radios. Only a console with turned legs
will attract Dick's attention and his
radios are really first class. Dick does
his own cabinet refurbishing and few,
if any, could do a better job.
Unwanted items
HRSA President Bruce DeLacy with some of the HRSA receivers on display.
These are, from left: a Dutch Philips multi-band radio, a mid-1930s Radiolette, a
Healing mantel model, a Little Nipper all transistor radio, and the top of a late
1930s Airzone console.
74 Silicon Chip
Unfortunately, driving to Melbourne
is something I loathe and will do just
about anything to avoid. But as Glen
roy is on the right side of Melbourne
for me, I decided to take a site at the
meet to help off-load some of my unwanted bits and pieces, and to support
Dick's venture.
Apart from being a profitable day,
the swap allowed me to catch up with
some old friends and meet a few new
ones. My wife and I took turns at our
site while the other walked around,
looking and talking. I suspect I may
have scored the better deal there, as
I knew a lot more people to talk to.
This site had a large range of early radios, radiograms & phonographs. The STC
console radio (centre) was priced at $645.
Author Bob Young spent more than
12 months on his book “Crystal Sets
‘n’ Such”. The book is a remarkably
informative publication & should
be of interest to most vintage radio
enthusiasts.
Pride of place on this table was taken by a fully-restored Edison "Fireside"
cylindrical phonograph. Immediately behind it are an Airzone mantel radio
& a Celestion loudspeaker. According to some old avertisements, the tone of a
Celestion loudspeaker improved with age!
The difference in prices from site to
site was considerable and one example
was lightning arresters. Mine were
priced at $5 while those at another
site were $15. Neither of us sold any!
Items for sale
As the accompanying photographs
show, there were a lot more items for
sale apart from lightning arresters.
There was an impressive array of
vin
tage equipment and just about
everyone who came to the meet went
away with something they wanted or
could use.
At the end of the day, my trading
table was just about bare. Four 807
valves, two 1950s mantel receivers,
two books, a valve tester and the
lightning arresters were the only things
left. If prices are realistic, just about
any item will sell. In most instances,
people were happy to pay the marked
price.· Only a few haggled for a better
deal.
Looking back on the day, I'm glad I
decided to take a site at the swap meet.
Fortunately, this year's site hold
ers
have first preference for next year and
I have already indicated my intention
to be there.
One different aspect to the swap
meet was the launching of a new book.
As mentioned in my October 1994
column, Bob Young (no, not Remote
Control's Bob Young) has been writing
a book on crystal sets and now it has
finally reached completion.
It was my pleasure to help launch
the book at the swap meet. Of course,
this is a difficult task when one is presented with the book only a couple of
hours beforehand, with no time to read
it. I'm sure that the ink was still wet!
Fortunately, I had previously read
some of the earlier chapters and had a
good idea of the direction Bob's book
was heading.
In my opinion, “Crystal Sets ‘n’
Such” is a brilliant piece of work!
It is in all probability the first really
com
plete work on crystal sets that
has been written and it should be of
interest to any vintage radio enthusiast, whether he is a new recruit or
someone who thinks he knows it all.
There is something in it for just about
everyone. A number of the early chapters are interesting from a historical
viewpoint alone.
Keep it simple
The secret to good technical writing
March 1995 75
is to keep things as elementary as
possible and never assume that your
reader knows everything about the
subject being covered. If this basic
rule is ignored, then the text may be
come quite meaningless to many read
ers and they will soon lose interest
and look for something else to read.
That's not the case with “Crystal Sets
‘n’ Such”. Every concept presented to
the reader is carefully explained in
simple terms, along with the appropriate illustrations, charts, diagrams
and analogies. It is a very informative
book and is directed at those with an
interest in radio and particularly those
who like to dabble around building
their own receivers.
Pick a meter, any meter – there's lots to choose from amongst this collection! As
far as a vintage radio enthusiast is concerned, these's no such thing as a digital
meter.
Just about every site had vintage radios on display. In the front row here,
from left, are two Philips receivers and a Mullard, while in the back row are a
Breville, an Aristone, a "don't know", and a Stromberg-Carlson.
This RCA Model 60 cabinet (circa 1928) was refurbished by Dick Howarth. It
was just about a total wreck before he started and has been restored to "betterthan-new" condition.
76 Silicon Chip
Crystal detectors
The chapter on crystal detectors is
interesting and delves into the many
and varied types that have been used
over the years. A comparison between
the various detectors is very well
dealt with. This comparison is not
done using a headphone performance
test but on an oscilloscope screen.
There are also instructions for setting
up similar tests if you wish to do so
yourself.
This book on crystal sets is a whole
new approach to building these sim
ple receivers and the theories and
practices involved.
“Crystal Sets ‘n’ Such” includes, as
one would expect, a wide range of crystal set circuits. These cover everything
from basic single-coil types to several
three-coil sets which are quite elaborate affairs for a supposedly simple
radio receiver. When a crystal set ends
up with half a dozen or more controls
(which all interact with each other), it
is starting to get fairly complicated - for
a crystal set, that is!
I was particularly pleased to see my
“Classic Crystal Set” (Vintage Radio,
September 1994) amongst the more
complex designs (circuit number 7).
It is a very good performer – not that I
can lay claim to its good design.
The chapter on coil winding is also
well covered. The “Q” factor of a tuned
circuit makes interesting reading
when it is presented simply with explanations and appropriate diagrams.
Although a mathematical formula is
given relating to the Q factor, complex
calculations do not enter into the text
of the book to any great extent. But the
odd formula is there for those who may
require them.
RESURRECTION
RADIO
VALVE EQUIPMENT SPECIALISTS
Repairs – Restoration – Sales
for RADIO & AUDIO Equipment
S
VE
L
VA
These three consoles are from Dick Howarth’s collection. They are, from left, a
1932 AWA 55E, a 1932 Raycophone, and a 1934 Airzone. Dick mostly collects
console receivers with legs.
BOUGHT
SOLD
TRADED
Send SSAE for Catalogue
Visit our Showroom at
242 Chapel Street (PO Box
2029) PRAHRAN, VIC 3181
Tel: (03) 9510 4486; Fax (03) 9529 5639
Silicon Chip Binders
This table carried an old Palec valve tester and what appears to be an early
Stromberg-Carlson communications receiver.
A “Resonant Circuit Component
Value Calculator” is also included in
the book and this could be of some
assistance when coil winding. The
calculator is a chart with three scales:
(1) inductance in microhenries; (2)
frequency in kilohertz; and (3) capacitance in picofarads. By placing a
straight edge through any two known
quantities, the unknown value can be
read off the third scale.
Perhaps the most refreshing aspect
of “Crystal Sets ‘n’ Such” is the way in
which it is written. Bob Young’s sense
of humour really shows through and
his book is a fun thing to read. He has
a way of expressing himself that is, at
times, quite light-hearted, which is one
of the best ways there is of getting a
message across.
“Crystal Sets ‘n’ Such” is a good
book. It covers the subject well, I
enjoyed reading it and I learnt from it
too! It is available from: Mr R. Young,
RMB 1561, Benalla, 3673. Phone (057)
68 2418. Fax (057) 68 2508.’’The cost
is $19.95, including postage.
Yes, the Inaugural Vintage Radio
Swap Meet (including the book
launch) was a great day and was enjoyed by all who attended. I for one
will be there again next year for what
will, no doubt, be an even bigger and
SC
better event.
These beautifully-made binders will
protect your copies of SILICON CHIP.
They are made from a distinctive
2-tone green vinyl & will look great
on your bookshelf.
Price: $A11.95 plus $3 p&p each
(NZ $8 p&p). Send your order to:
Silicon Chip Publications
PO Box 139
Collaroy Beach 2097
Or fax (02) 979 6503; or ring (02)
979 5644 & quote your credit card
number.
March 1995 77
NICS
O
R
T
2223
LEC
7910
y, NSW
EY E
OATLBox 89, Oa8t5leFax (02) 5s7a0 C a rd
KITS & BITS
i
9
PO
579 4 r C a rd , V e & fax
)
2
0
(
n
e
e
Phon rd , M a s t with pho orders:
a
d
c
ed
B a n k x accepte most mix 0. Orders
$3; 50 x 72 x 3mm: $3. LINE GENERATING
e
r
1
OPTIC: makes a line out of a laser beam:
& Am . P & P fo (airmail) $
s
$5. LASER DIODE COLLIMATING LENS:
order 4-$10; NZ world.net
$4. PORRO 90 deg. PRISM: makes a
$
<at>
.
y
t
e
s
l
t
u
rainbow from white light: $10. PRECISION ROTATING
a
A
AIL: o
MIRROR ASSEMBLY: as used in levelling equipment,
by EM
needs small motor/belt, plus a laser beam, will draw a
HIGH INTENSITY RED LEDs
550-1000mCd <at> 20mA, 100mA max, 5mm housing:
10 for $4, or 100 for $30.
LOW COST IR ILLUMINATOR
Employs 42 high output 880nM IR LEDs (30mW
<at> 100mA ea.) & a seven transistor adjustable
constant current driver circuit. Designed to be
powered from 10-14V DC, current depends on
power level setting: 5 - 600mA. The compact
PCB is designed to replace the lid on a standard
small 82 x 53 x 28mm plastic box. Good for
illuminating IR responsive CCD cameras, IR
& passive night viewers & medical use. The
complete kit even includes the plastic box & is
priced at a low:
$40
MINIATURE FM TRANSMITTER
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: 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". $32.
COLOUR MONITORS
Used but guaranteed 12" colour computer
monitors:
$40
REEL TO REEL TAPES
New studio quality 13cm-5" “Agfa” (German) 1/4" reel to
reel tapes in original box, 180m-600ft: $8 ea.
ARGON HEADS
These low voltage air cooled Argon Ion Laser Heads
are priced according to their hours of operation. They
produce a bright BLUE BEAM (488nM) and a power
output in the 10-100mW range - depending on the
tube current. The head includes power meter circuitry,
and starting circuitry. We provide a simple circuit for
the supply. Limited supplies at a fraction of their real
cost: $300 - $500.
AC MOTOR
Small but very powerful GEARED AC motor. 1
RPM/60Hz/24V/5watt. We supply a circuit diagram
that shows how to power this motor from 12V
DC: Variable speed/full power (bridge output).
Bargain priced: $9
PCB and all on-board components kit for the 12V
driver kit will be available late in May:
$8
OPTICS
BEAM SPLITTER for 633nM: $45. PRECISION FRONT
SURFACE ALUMINIUM MIRRORS 200 x 15 x 3mm:
78 Silicon Chip
line right around a room (360 deg.) with a laser beam:
$45. LARGE LENS: out of a night viewer, can easily be
pulled apart: $18. ARGON MIRRORS: high reflector
and output coupler used to make an Argon tube: $50.
POWER SUPPLIES
Used but very clean non standard computer power
supplies, enclosed in metal casing with perforated
ends for air circulation, built in fan, IEC input
connector and OFF-ON switch, “flying” DC output
leads, overall dimensions: 87 x 130 x 328mm,
110-220V input, +5V/8A, +12V/3A, and -12V/0.25A
DC outputs. BARGAIN PRICED:
$18 ea. or 4 for $60.
Used IEC lead with Australian plug $2.50 extra.
TWO STEPPER MOTORS PLUS A DRIVER KIT
This kit will drive two stepper motors: 4, 5, 6 or 8-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.
MAINS LASER SPECIAL
Includes a compact potted US made power supply
which can be powered from 110/220-240V AC,
a 2-3mW He-Ne tube, a ballast resistor and
instructions. The power supply requires 4-6V <at>
2mA DC enable to run. Brand new components.
Giveaway price:
$65
27MHz TRANSMITTERS
These new Australian made transmitters are assembled
(PCB and components) and tested. They are Xtal locked
on 26.995 MHz and were originally intended for transmitting digital information. Their discrete component
design employs many components, including 5 transistors and 8 inductors: circuit provided. A heatsink is
provided for the output device. Power output depends
on supply voltage and varies from 100mW to a few
watts, when operated from 3-12V DC. These are sold
for parts/experimentation/educational purposes, and
should not be connected to an antenna as licensing
may be required: $7 ea. or 4 for $20.
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
CD MECHANISMS
Used compact disc player mechanisms. Include IR
laser diode, optics, small conventional DC motor, gears,
stepping motor, magnets etc. Great for model railway
hobbyists: The motor/gear assembly produces a linear
movement of approx. 60mm. The whole assembly is
priced at less than the value of the collimating lens,
which is easy to remove: $6. We also have some similar CD assemblies that have linear motors. Used CD
mechanisms with linear motors: $4.
IMAGE INTENSIFIER TUBES
Used but in excellent condition second generation image intensifier tubes. Can be used
to make a small and very sensitive scope that
can produce high resolution pictures in very
low illumination. US made tubes that produce
superior results!
$650
We should have a complete kit of parts for a small
scope available at the time of the publication of
this advertisement: “Ring”.
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.
IR REMOTE SWITCH KIT
Consists of a PCB and all on board components
kit for an IR receiver with a toggle output, and a
brand new commercial ready made slimline IR
remote control transmitter, which was designed
for a CD player. Simply press any button on the IR
transmitter to toggle the output on the receiver.
The system has up to 20M range and will also work
from most other IR remote controls! Receiver uses
an IC “front end”, has a toggle output, operates
from 8-15V DC, and will drive a relay. Transmitter
operates from two “AAA” batteries (not supplied).
Unbelievable pricing:
$18
For the slimline IR remote control transmitter
and a kit for the IR receiver. Suitable 12V/8A
relay with 4kV isolation: $3, 12V DC plugpack:
$10.
PRINTER MECHANISMS
Brand new Epson dot matrix printer mechanisms: overall
dimensions are 150 x 105 x 70mm. These are complete
units and contain many useful parts: 12V DC motor
(50mm long - 30mm diam.) with built in tachometer,
gears, solenoid, magnet, reed switch, dot matrix print
head etc.: $12.
VISIBLE LASER DIODE MODULES
Industrial quality 5mW/670nM laser diode modules.
Overall dimensions: 11mm diameter by 40mm long.
Have APC driver built in and need approximately 50mA
from 3-6V supply. $60.
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
3.4A Peltier effect semiconductor, two thermal cutout
switches, and a 12V DC fan for a total price of: $35.
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.
12V-4.5A Peltier device only: $25.
DOT MATRIX LCDs
Brand new Hitachi LM215 400 x 128 dot matrix
Liquid Crystal Displays in an attractive housing. These have driver ICs fitted but require an
external controller. Effective display size is 65
x 235mm. Available at less than 10% of their
real value:
$25 ea. or 3 for $60
VISIBLE LASER DIODE KIT
A 5mW/670nM visible laser diode plus a collimating
lens, plus a housing, plus an APC driver kit (Sept. 94
EA) UNBELIEVABLE PRICE: $35. The same kit is also
available with a 3mW/650nM laser diode: $60.
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.
$215 CCD VIDEO SECURITY SYSTEM
Monochrome CCD Camera which is totally assembled on a small PCB and includes an auto iris
lens. It can work with illumination of as little as
0.1Lux and it is IR responsive. This new model
camera is about half the size of the unit we previously supplied. It is slightly bigger than a box of
matches! Can be used in total darkness with Infra
Red illumination. NEW LOW PRICE:
$180
With every camera purchased we can supply an
used but tested and guaranteed 12V DC operated
Green computer monitor. We can also supply a
simple kit to convert these monitors to accept
the signal from the CCD camera: monitor $25,
conversion kit $10.
A COMPLETE 12V CCD VIDEO SECURITY
SYSTEM FOR $215!!
LOW COST 1-2 CHANNEL UHF REMOTE CONTROL
A single channel 304MHz UHF remote control with over
half a 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.
is available: suits 12-24V batteries, 0.1-16A panels,
$27. Also available is a simple and efficient shunt
regulator kit, $5.
BLEMISHED 3 STAGE TUBES
We have accumulated a good number of 40mm
three stage fibre optically coupled 3 stage image
intensifiers that have minor blemishes: similar to
above but three tubes are supplied already bonded
together: extremely high gain!! Each of these tubes
will be supplied with the power supply components
only. See SC Sept. 94.
$200
For the 3 stage 40mm tube, supply kit. We can also
supply the full SC Sept. 94 Magazine: $5
TDA ICs/TRANSFORMERS
We have a limited stock of some 20 Watt TDA1520 HI-FI
quality monolythic 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
monolythic HI-FI amplifier ICs, two PCBs to suit, circuit
diagram/layout. Some additional components and a
heatsink are required.
RUBY LASER HEADS
These complete and functional heads include a
flash tube, mirrors, and 4" ruby rod! Produce a
high intensity visible red beam! We should have
suitable circuits - components to drive these
available. Dangerous units with restricted sales.
Limited quantity.
$695
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
INCREDIBLE PRICES:
COMPLETE 1 CHANNEL TX-RX KIT: $30
COMPLETE 2 CHANNEL TX-RX KIT: $36
ADDITIONAL TRANSMITTERS: $10
We can also supply a 240V-12V/4A-5V/4A switched
mode power supply to suit for $30.
FIBRE OPTIC TUBES
Originally designed for bicycles, but these suit
any moving vehicle that has a rotating wheel!
A nine function computer with speed, average
speed, maximum speed, distance, odometer,
timer, scan, freeze frame memory, and a clock.
Its microprocessor based circuitry can be adapted
to work with almost any wheel diameter. Simply
divide the wheel diameter in millimetres by
6.8232, and program the resultant figure into
the computer.
We have a good supply of some tubes that may have a
blemish which is not in the central viewing area! These
produce a very high resolution image but would require
IR illumination: !!ON SPECIAL!! $50 for a blemished
25 or 40mm (specify preference) image intensifier
tube and supply kit. Matching good quality eyepiece
lens only, $2 extra! That’s almost a complete night
viewer kit for: $52.
12V-2.5 WATT SOLAR PANEL KITS
These US made amophorous 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:
$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
VEHICLE COMPUTERS
$29.90
$70. SWITCHED MODE POWER SUPPLIES: mains in
(240V), new assembled units with 12V-4A and 5V-4A
DC outputs: $32. ELECTRIC FENCE KIT: PCB and
components, includes prewound transformer: $40.
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 nonferrous 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 EXTENSION
LEADS: 2M long, IEC plug at one end, IEC socket at
other end: $5. MOTOR SPECIAL: these permanent
magnet 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. 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. MODULAR TELEPHONE CABLES:
4 way modular curled cable with plugs fitted at each
end, also an 4M long 8way modular flat cable with
plugs fitted at each end, one of each for: $2. 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: ON SPECIAL
$15. 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: $20. 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.2: high quality - high
stability, suit radiomicrophones 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.1: 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.
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. 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. SUPERCAPS: 0.047F/5.5V capacitors: 5 for $2.
PCB MOUNTED SWITCHES: 90 deg. 3A-250V, SPDT: 4
for $2. 3-INCH CONE TWEETERS: sealed back dynamic
8-ohm tweeters: $5 ea. CASED TRANSFORMERS:
230V-11.7V 300mA AC-AC transformers in small
plastic case with separate input and leads, each is
over 2 metres long: $6.
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: SC DEC 93: 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 12V DC supply-plugpack:
MORE ITEMS AND KITS
Poll our (02) 579 3955 or (02) 579 3983 fax
numbers for instructions on how to obtain our
Item and Kit lists. MANY MORE ITEMS AND
KITS THAN ARE LISTED HERE!! You can also
ask for a copy of these to be sent out with
your next order.
March 1995 79
AMATEUR RADIO
BY DARREN YATES
Simple 2-transistor CW filter
If you’re having trouble picking CW signals out
of the mud, then try this handy little circuit. It’s
a 2-transistor CW filter & it’s just the shot for
beefing up those buried signals.
Deciphering CW signals on a noisy
band can often be quite difficult, particularly for novice operators with
only basic equipment. Fortunately,
there are various techniques that can
be used to “clean-up” the signal.
By far the most common technique
is to employ a CW filter. A CW (or
continuous wave) transmission, as
used for Morse code, is essentially an
interrupted carrier; ie, the carrier is
switched on and off by the Morse key.
When you tune your receiver, you tune
it close enough to the incoming carrier
to give an audible beat.
Most people tune their receiver to
give a beat somewhere below 1kHz.
This is particularly the case where you
have a noisy signal; a lower audible
frequency can be somewhat easier to
distinguish from the noise and this
is where this CW filter comes in. It is
essentially a notch filter set at 750Hz
which effec
tively attenuates noise
either side of this frequency and thus
greatly improves signal reception.
In use, you tune the receiver so that
the audible beat is right on 750Hz, at
which point the modulated carrier will
stand out well above the noise.
AUDIO PRECISION FREQRESP AMPL(dBr) vs FREQ(Hz)
50.000
11 JAN 95 01:27:07
40.000
30.000
20.000
10.000
0.0
The circuit itself uses just two
transistors and a handful of passive
components. It is built on a PC board
measuring just 46 x 36mm, which
should be small enough to fit inside
most re
ceivers. The power supply
requirements are a 9-12V DC at just a
few milliamps and this can easily be
derived from an existing supply rail.
Fig.1 shows the frequency response
of the filter, as measured on an Audio
Precision audio test set. As can be seen,
it effectively provides around 40dB of
gain at 750Hz.
Circuit details
Refer now to Fig.2 for the circuit
details of the CW Filter. It is basically
a 2-transistor amplifier with a twin-T
filter in the feedback path.
In greater detail, transistors Q1 and
Q2 make up a DC feedback pair, with
negative feedback applied from Q2’s
collector to Q1’s emitter via the twin-T
filter network. The input signal is applied via a 0.1µF capacitor to Q1’s base,
while the 120kΩ and 150kΩ resistors
set the bias for this stage.
The 330Ω resistor and series 1µF
capacitor roll off the low-frequency
response of this first stage, to make
the overall filtering more effective.
The resulting amplified output on Q1’s
collector is then fed directly into base
of PNP transistor Q2. Note the 33kΩ
load resistor on Q1’s collector. This
is not strictly necessary but has been
included since it significantly reduces
distortion.
Finally, the amplified signal on Q2’s
collector is coupled to the output via
a 10µF capacitor.
Twin-T filter
-10.00
10
100
1k
10k
20k
Fig.1: the frequency response of the filter. The passband is centred on 750Hz.
80 Silicon Chip
Six components are used in the
twin-T filter network: two 2.2kΩ
resistors, a 1.1kΩ resistor, two 0.1µF
capacitors and a 0.22µF capacitor. Its
+9-12V
120k
0.1
CW
SIGNAL
IN
C
B
Q1
BC548
E
150k
B
E
Q2
BC558
B
33k
10
E 16VW
C
2.2k
10
16VW
2.2k
330
0.1
1
63VW
0.22
0.1
1.1k
OUTPUT
SIGNAL
10k
0V
1k
Fig.2: Q1 & Q2
make up a DC
feedback pair,
with negative
feedback
applied from
Q2’s collector
to Q1’s emitter
via a twin-T
filter network.
PARTS LIST
1 PC board, code 06104951,
46 x 36mm
6 PC stakes
Semiconductors
1 BC548 NPN transistor (Q1)
1 BC558 PNP transistor (Q2)
Capacitors
2 10µF 16VW electrolytic
1 1µF 16VW electrolytic
1 0.22µF MKT polyester
3 0.1µF MKT polyester
C
VIEWED FROM
BELOW
ACTIVE FILTER FOR CW RECEPTION
notch frequency is determined by the
formula F= 1/(2πRC).
Since the impedance of the twin-T
network is a maximum at this frequency (in this case, 750Hz), this
corresponds to minimum negative
feedback and the maximum gain. Note
that because the circuit has considerable gain at the notch frequency, the
input signal needs to be below 20mV
in order to prevent clipping at the
output. If you have too much signal,
just wind back the volume control or
use a resistive attenuator to reduce
the input level.
Construction
10uF
2.2k
10uF
330
10k
1k
0.22
1.1k
0.1
Q1
2.2k
0.1
CW
SIGNAL
INPUT
GND
colours can be difficult to decipher. Be
sure to install the electrolytic capacitors with the correct polarity.
Finally, complete the assembly by
installing the two transistors.
The finished PC board can be mounted inside the receiver or installed in a
plastic case and run off batteries or a
DC plugpack. If you elect to mount the
unit separately, then you will need to
fit an on/off switch.
The filter can be driven from the
volume control, from the headphone
output, or from the “record” output
of most receivers. In fact, by using the
record output, which allows the loudspeaker to operate in normal fashion, it
is possible to compare the filtered and
unfiltered signals. You will be amazed
at the difference.
Finally, note that careful tuning of
the receiver will be necessary to ensure that the beat frequency is centred
within the narrow filter passband. This
is not as difficult as it sounds and is
SC
readily done by ear.
The PC board is small enough to fit
inside most receivers.
Begin construction by installing PC
stakes at the external wiring points,
then install the resistors and capacitors. Table 1 lists the resistor colour
codes but it is also a good idea to check
them on your multimeter, as some
+9-12V
0.1
Q2
33k
120k
150k
All the components for the CW
filter are installed a PC board coded
06104951. Fig.3 shows the details.
Resistors (0.25W, 1%)
1 150kΩ
2 2.2kΩ
1 120kΩ
1 1.1kΩ
1 33kΩ
1 1kΩ
1 10kΩ
1 330Ω
1uF
SIGNAL
OUTPUT
GND
0V
Fig.3 (left) shows how the parts are installed on the PC board while Fig.4 (right)
shows the full-size etching pattern.
TABLE 1: RESISTOR COLOUR CODES
❏
No.
❏ 1
❏ 1
❏ 1
❏ 1
❏ 2
❏ 1
❏ 1
❏ 1
Value
150kΩ
120kΩ
33kΩ
10kΩ
2.2kΩ
1.1kΩ
1kΩ
330Ω
4-Band Code (1%)
brown green yellow brown
brown red yellow brown
orange orange orange brown
brown black orange brown
red red red brown
brown brown red brown
brown black red brown
orange orange brown brown
5-Band Code (1%)
brown green black orange brown
brown red black orange brown
orange orange black red brown
brown black black red brown
red red black brown brown
brown brown black brown brown
brown black black brown brown
orange orange black black brown
March 1995 81
PRODUCT SHOWCASE
NAD 513 carousel
compact disc changer
CD changers have been around for
some time, in permutations such as
magazine, carousel or internal storage systems, each with their specific
ad
vantages and disadvantages, but
almost always with a capacity of five
discs. After careful market research,
NAD found that most people do not
need to play more than two or three
CDs after one another, as the total playing time of three CDs can be as much
as 3 hours and 45 minutes.
With this in mind, NAD engineers
developed the model 513. By employing the carousel principle and limiting
the number of discs it can hold to
three, the end result is a CD changer
with the performance and price of
single disc CD player.
Like other NAD CD players, the
513 uses a single-bit MASH circuit,
while balanced filtering removes ultrasonic byproducts of the decoding
process without affecting the audio
performance.
Despite its simplicity, the NAD
513 offers all the facilities normally
associated with carousel CD changers
- two discs may be changed while the
third is playing; the remote control
allows changing discs and selecting
tracks without having to touch the
front panel, the programming facility
for 32 tracks over three discs makes
Cordless infrared
headphones
Instrumentation
catalog
National Instruments has an
nounced its new 584 page catalog
which describes more than 900
software and hardware products.
The 1995 catalog is colour-coded
into five sections: software, GPIB/
serial interfaces, data acquisition,
VXI/MXI and customer education.
The first four sections feature
com
p rehensive tutorials, complete with application examples,
to help readers learn more about
IEEE 488.2, SCPI, plug-in data
acquisition (DAQ) systems, signal
conditioning accessories, VXI and
MXI. Complete ordering, pricing
and warranty information is also
included.
Expanded sections are included
on how to choose hardware and
software for IEEE 488, plug-in DAQ,
serial and VXIbus products. Also
82 Silicon Chip
track selection a breeze; and with the
Random function engaged, all tracks
from all three discs will be played
without repetition.
NAD products are available from
authorised NAD dealers across Aus
tralia. For further information please
contact Marantz Australia on (02)
742 8322.
new to the 1995 catalog are separate
listings of instrument driv
ers by
industrial I/0 and test and measurement categories.
To request copies of the free
catalog or for product information,
contact National Instruments Aus
tralia, PO Box 466, Ringwood, Vic
3134. Phone (03) 879 9422 or fax
(03) 879 9179.
Amber Technology has announced
the Beyer IRS890 & IRS790 cordless
infrared headphones which combine
freedom of movement with audio per
formance normally only associated
with wired headphones.
Position Vacant
Electronics Designer
Silicon Chip, Australia’s dynamic electronics magazine, is
looking for an electronics project
designer to work for us. The
successful applicant will have a
good knowledge of electronics and
computers and should be able to
program in Basic. Good writing
skills are desirable. If you think
you could be that person, apply
in writing to the Publisher, Silicon
Chip Publications, PO Box 139,
Collaroy, NSW 2097; or fax your
application to (02) 976 6503.
The system comprises three components – the IRH890 cordless headphone, featuring comfortable, soft ear
cushions, automatic level control,
individual channel volume controls,
switchable to stereo, mono-left or mono-right, and powered via 2 x 1.5V AA
cells; the IS890 infrared transmitter;
and the LG890 power supply.
Additional pairs of IRH890 headphones may be operated simultaneously from the same transmitter,
while coverage in other rooms can
be obtained with the addition of the
ISS890 slave transmitter.
The system has a claimed frequency response of 18Hz to 24kHz with
a maximum SPL of 1 l0dB and has
a recommended retail price of $579.
The IRS 790 offers similar features and
pro
vides 20Hz to 23kHz frequency
response with 116dB SPL capability.
It has a recommended retail price of
$499.
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.
New catalog from All
Electronics Components
All Electronic Components
has announced
their first catalog listing their
full range.
As the catalog
shows, they are
strong in semi
conductors and
have a comprehensive range of
passive components as well.
The catalog has a $2 cover charge bit
is available free to readers of Silicon
Chip provided they send a couple of 45
cent stamps with their request.
For your copy, contact All Electronic
Components, 118-122 Lonsdale Street,
Melbourne, Vic 3000. Phone (03) 662
3506 or fax (03) 663 3822.
Combination CD-ROM
& hard disc
Teac Corporation of Japan has
released a combination fast CDROM
drive and integrated hard disc. Three
models are available: 250Mb, 360Mb
and 540Mb.
The CD-ROM drive is a quad
speed AT interface drive with a
fast access time of 195ms and a
sustained data transfer rate of 600Kb
per second. It will read both 12cm
and 8cm discs of CD-DA, CD-ROM
Mode-1, XA Mode-2 (Form-1, Form2) formats and is multi-session Photo-CD compatible. The AT interface
is compat
ible with SoundBlaster
sound cards.
The hard disc has an IDE inter
face, requires only 5V, is lockable
and changeable. The Combo Drive
SATELLITE
SUPPLIES
Aussat systems
from under $850
SATELLITE RECEIVERS FROM .$280
LNB’s Ku FROM ..............................$229
LNB’s C FROM .................................$330
FEEDHORNS Ku BAND FROM ......$45
FEEDHORNS C.BAND FROM .........$95
DISHES 60m to 3.7m FROM ...........$130
LOTS OF OTHER ITEMS
FROM COAXIAL CABLE,
DECODERS, ANGLE
METERS, IN-LINE COAX
AMPS, PAY-TV DECODER
FOR JAPANESE, NTSC TO
PAL TRANSCODERS, E-PAL
DECODERS, PLUS MANY
MORE
For a free catalogue, fill in & mail
or fax this coupon.
✍
Please send me a free catalog
on your satellite systems.
is supplied with an interface card
for the CD-ROM plus data and
sound cables, device driver, user’s
manuals, mounting screws and
configuration software for the hard
disc drive.
For more information please contact Rick Stanford at Southend Data
Storage on (02) 541 1006.
Name:____________________________
Street:____________________________
Suburb:_________________________
P/code________Phone_____________
L&M Satellite Supplies
33-35 Wickham Rd, Moorabin 3189
Ph (03) 553 1763; Fax (03) 532 2957
March 1995 83
SILICON CHIP
BOOK SHOP
Newnes Guide
to Satellite TV
336 pages, in paperback at $49.95.
Installation, Reception & Repair.
By Derek J. Stephenson. First
published 1991, reprinted 1994
(3rd edition).
This is a practical guide on the
installation and servicing of
satellite television equipment. The
coverage of the subject is extensive, without excessive theory or
mathematics. 371 pages, in hard
cover at $55.95.
Servicing Personal
Computers
By Michael Tooley. First pub
lished 1985. 4th edition 1994.
Computers are prone to failure
from a number of common causes
& some that are not so common.
This book sets out the principles
& practice of computer servicing
(including disc drives, printers &
monitors), describes some of the
latest software diagnostic routines
& includes program listings. 387
pages in hard cover at $59.95.
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
for engineers and technicians to
bring themselves up to date. The
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
understand digital audio, you need
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
electronics has come into its own,
particularly in the areas of traction
and electric vehicles. F. F. Mazda
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
phenomena, material & components, electronic design, and
applications. The sixth edition has
been expanded to include chapters
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hardware & software design,
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This timely book strips away the
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These two new digital storage oscilloscopes from
Tektronix are right at the leading edge of technology.
The TDS 784A at left, has a bandwidth of 1GHz &
4-gigasamples/second maximum sampling rate. The
TDS 744A at right operates at real-time speeds up to
500MHz & with a maximum sample rate of 2Gs/s. Both
have liquid crystal shutters to provide colour displays
& have an unsurpassed ability to catch & display rare
glitches in signal waveforms.
Tektronix TDS 784A
TruCapture oscilloscope
Tektronix has really taken the bit in its teeth
over the last few years in developing the art of
digital storage oscilloscopes. Now it has taken another big step forward with its TDS 784A
& TDS 744A scopes which can display up to
400,000 acquisitions per second. This is a huge
improvement over previous digital scopes.
By LEO SIMPSON
While digital scopes have come a
long way over the last few years, they
still have drawbacks in the way they
display signal waveforms. Partly this
is due to the sampling system which
shows the waveform as a series of dots.
On a signal which has superimposed
noise, the resultant waveform can be
quite jagged and quite different from
what would be displayed on a conven-
tional analog oscilloscope. The truth
is that the both oscilloscopes show
the waveforms differently and both
conceal information.
Actually, a major shortcoming of
digital storage oscilloscopes (DSOs)
has been the small fraction of time
they spend capturing waveforms. This
is quite different from the impression that you get when the display is
updated at 60 times per second. For
example, if the DSO is set at an appro
priate sweep speed to display a 10MHz
clock signal, each refreshed display
will show about five clock signals
or half a microsecond (500ns). This
means that in 60 displayed waveforms,
only 30 microseconds of signal will be
acquired by the scope in one second.
This is 30 parts per million or just
.003% of real time. So while things
appear to happening rapidly on the
screen, in reality the scope is sitting
there doing nothing most of the time
and many “events” could occur which
are just not captured.
Analog scopes do a lot better in
terms of their “display refresh” rate; ie,
the number of times the screen display
is updated. The best analog scopes can
refresh the display at several hundred
times a second (at a sweep speed of
higher than 1µs/div) but then they also
have trouble displaying rare events;
March 1995 85
Displaying a 3MHz signal of a Tektronix 2465 analog scope shows a waveform
which is clean and apparently free of any glitches.
The same 3MHz signal displayed on a Tektronix 2467B, one of the world’s
fastest analog scopes which has an enhanced CRT. Here a glitch is apparent in
the form of a “runt” pulse (about half the full height), although the reproduction
of this photo may not show this.
the writing speed of the phosphor
used in cathode ray tubes (CRTs) is too
slow for single glitches to be observed
by the user, even if a viewing hood is
employed.
The only way to see very fast glitch86 Silicon Chip
es buried in a repetitive signal with an
analog scope is use one that includes
an electron multiplying plate between
the deflection plates and the phosphor
of the CRT. Examples of such scopes
are the Tektronix 2467B and 7104 but
these are expensive scopes indeed.
Of course, some high-end digital
scopes can be programmed to find
glitches in repetitive signals but you
have to know what you are looking
for in order to do the programming.
And since the digital scope spends
so little time actually acquiring the
signal, you might have to wait a long
time before the glitch actually is found,
if at all. And while analog scopes can
be better at finding glitches, you have
to spend unconscionably long times
glued to the screen in order to actually
see them.
Sometime in the future, digital
scopes must equal the glitch finding
ability of the best analog scopes but
according to theory, this would require
a display system capable of several
thousand full screen acquisitions per
second.
The instrument would then have to
rasterise these acquisitions at nearly
200 million pixels per second (compare that to today’s VGA screens at
about 55 million pixels per second.
1024 x 768 x 70). In addition, the data
move:gient between the ac
quisition
system and the display would need
to be around 200 megabytes per second. Now while these parameters are
technically feasible, there is no digital
scope available today which comes
within cooee of them.
All of which leads up to how Tektronix has gone about achieving the
desired result by taking another approach – changing the architecture of
the digital scope. Briefly, these changes
are as follows. first, the rasterisation
capability of the display system is
duplicated in the acquisition system,
next, the rasteriser is allowed to use a
portion of the high speed acquisition
memory to build display images; and
third, the acqui
sition hardware is
allowed to start acquisitions without
the intervention of the instrument’s
firmware and to calculate its own
trigger positions.
This new architecture is used in the
Tektronix TDS700A TruCapture digital
scopes in a mode called “InstaVu” acquisition. When this mode is enabled,
the data moved from the acquisition
system is a complete rasterised image
of many triggered acquisitions of the
input signal.
By the way, perhaps we should briefly explain the term rasterisation as it
pertains to digital scopes. It refers to
the display system. In a conventional
analog scope, the input signal is applied directly to the deflection plates of
the CRT and so the signal on the screen
is an “analogue” of the input; it is also
a vector display with the electron beam
tracing out the signal on the screen in
response to the deflection voltages on
the plates.
A raster signal, by contrast, is the
same as a computer video display; the
electron beam scans the whole screen
at rates similar to a computer VGA display and the beam is modulated on and
off by the video signal to produce the
individual pixels (picture elements).
In essence, the DSO converts the input
signal to digital data and stores it in
high speed video memory.
Getting back to the plot, we talked
about moving a complete rasterised
image from the acquisition system
to the display. Transferring this 500
x 256 pixel map requires a lot more
data to be transferred between the two
systems but the raster is only moved at
the refresh rate of the scope’s display
and contains information from tens
of thousands of acquisitions. Doing it
this way makes the data transfer rate
manageable and in fact, it equates to
417Kb/sec.
Tektronix has had to develop a considerable range of new semiconductor
hardware to achieve its new architecture and among these is a new kind
of demultiplexer which integrates
360,000 transistors into a CMOS IC
with 304 pins. It dissipates about 2.5
watts when running at full speed.
Normally, the only function of this IC
would be to demultiplex (ie, switch)
data from the analog to digital converter and store it in a high speed static
RAM. One third of this new demultiplexer is devoted to that job. The remainder is split between a high speed
rasteriser and a digital signal processor
(DSP). The DSP is included for, among
other things, mathematical algorithms
and trigger position calculations.
We could discuss this new technology at greater length but none of
it really means much until you see
the results. To this end, four screen
photos are included with this article,
showing how different scopes behave
when displaying a 3MHz waveform
with buried glitches. Briefly, all but
the best analog scopes never reveal
the glitches and nor does the Tektronix
544A colour digital scope (reviewed
in Silicon Chip, November 1993) but
the TDS784A and TDS744A, with
On a Tektronix TDS 544 digital colour scope, the 3MHz signal results in a
waveform which is similar to that shown on the Tektronix 2465 analog scope.
Note that it has been sampled at a rate of 500 megasample/second.
Finally, this is the 3MHz signal depicted on a Tektronix TDS 784A digital colour
scope in InstaVu mode. Here the runt signal is clearly visible, made doubly by
the colour display (although not reproduced in this B&W photo). Note that the
acquisition rate is also 500Ms/s, the same as for the TDS 544A, but the number
of acquisitions is a great deal more (75,896 versus 1156).
their extremely high sampling rates
and high acquisition rates, do reveal
the glitches and do so even more
dramatically with the aid of a colour
screen. Most impressive.
For more information and prices
on these new digital oscilloscopes,
contact Tektronix Australia Pty Ltd,
80 Waterloo Road, North Ryde NSW
2113. Phone (02) 888 7066.
SC
March 1995 87
Silicon Chip
Universal Stereo Preamplifier; Load Protection Switch For
Power Supplies; A Speed Alarm For Your Car; 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.
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.
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.
April 1989: Auxiliary Brake Light Flasher; What You Need
to Know About Capacitors; 32-Band Graphic Equaliser, Pt.2;
LED Message Board, Pt.2.
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.
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 Capacitors.
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.
July 1989: Exhaust Gas Monitor (Uses TGS812 Gas Sensor);
Extension For The Touch-Lamp Dimmer; Experimental Mains
Hum Sniffers; Compact Ultrasonic Car Alarm.
September 1989: 2-Chip Portable AM Stereo Radio (Uses
MC13024 and TX7376P) Pt.1; High Or Low Fluid Level
Detector; Simple DTMF 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.
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.
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.
March 1990: 6/12V Charger For Sealed Lead-Acid Batteries;
Delay Unit For Automatic Antennas; Workout Timer For
Aerobics Classes; 16-Channel Mixing Desk, Pt.2; Using The
UC3906 SLA Battery Charger IC.
April 1990: Dual Tracking ±50V Power Supply; Voice-Operated Switch (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 Receivers
From The 1920s.
June 1990: Multi-Sector Home Burglar Alarm; Low-Noise
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 Telephone; 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 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; Low-Cost Sinewave
Oscillator; Fast Charger For Nicad Batteries, Pt.2; How To
Design Amplifier Output Stages; Tasmania's Hydroelectric
Power System.
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v
March 1991: Remote Controller For Garage Doors, Pt.1;
Transistor Beta Tester Mk.2; Build A Synthesised AM Stereo
Tuner, Pt.2; Multi-Purpose I/O Board For PC-Compatibles;
Universal Wideband RF Preamplifier For Amateur Radio
& 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.
Miniature 1.5V To 9V DC Converter; Dummy Load Box For
Large Audio Amplifiers; Internal Combustion Engines For
Model Aircraft; Troubleshooting Vintage Radio Receivers.
& Efficient 12-240VAC 200W Inverter; Single Chip 0.5W
Audio Amplifier; 3A 40V Adjustable Power Supply; Electronic
Engine Management, Pt.5; Airbags – How They Work.
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.
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.
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.
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.
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.
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.
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.
August 1991: Build A Digital Tachometer; Masthead Amplifier
For TV & FM; PC Voice Recorder; Tuning In To Satellite TV,
Pt.3; Step-By-Step Vintage Radio Repairs.
March 1993: Build A Solar Charger For 12V Batteries;
Alarm-Triggered Security Camera; Low-Cost Audio Mixer
for Camcorders;A 24-Hour Sidereal Clock For Astronomers.
September 1991: Studio 3-55L 3-Way Loudspeaker System;
Digital Altimeter For Gliders & Ultralights, Pt.1; The Basics
Of A/D & D/A Conversion; Windows 3 Swapfiles, Program
Groups & Icons.
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.
October 1991: Build A Talking Voltmeter For Your PC, Pt.1;
SteamSound Simulator For Model Railways Mk.II; Magnetic Field Strength Meter; Digital Altimeter For Gliders &
Ultralights, Pt.2; Getting To Know The Windows PIF Editor.
May 1993: Nicad Cell Discharger; Build The Woofer Stopper;
Remote Volume Control For Hifi Systems, Pt.1; Alphanumeric LCD Demonstration Board; The Microsoft Windows
Sound System.
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.
June 1993: Windows-Based Digital Logic Analyser, Pt.1;
Build An AM Radio Trainer, Pt.1; Remote Control For The
Woofer Stopper; Digital Voltmeter For Cars; Remote Volume
Control For Hifi Systems, Pt.2
December 1991: TV Transmitter For VCRs With UHF Modulators; Infrared Light Beam Relay; Solid-State 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
Directories; Valve Substitution In Vintage Radios.
April 1992: IR 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; Low-Cost 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 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; 60-LED Brake
Light Array; A Microprocessor-Based Sidereal Clock; The
Southern Cross Z80-based Computer; A Look At Satellites
& Their Orbits.
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 Micro
controller – 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; Low-Cost 25W Amplifier
Module; Peripherals For The Southern Cross Computer; Build
A 1-Chip Melody Generator; Electronic Engine Management,
Pt.3; Index To Volume 6.
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.
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.
August 1992: Build An Automatic SLA Battery Charger;
February 1994: 90-Second Message Recorder; Compact
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.
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
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.
August 1994: High-Power Dimmer For Incandescent
Lights; Microprocessor-Controlled Morse Keyer; Dual
Diversity Tuner For FM Microphones, Pt.1; Build a Nicad
Zapper; Simple Crystal Checker; Electronic Engine Management, Pt.11.
September 1994: Automatic Discharger For Nicad Battery
Packs; MiniVox Voice Operated Relay; Image Intensified
Night Viewer; AM Radio For Aircraft Weather Beacons; Dual
Diversity Tuner For FM Microphones, Pt.2; Electronic Engine
Management, Pt.12.
October 1994: Dolby Surround Sound – How It Works;
Dual Rail Variable Power Supply (±1.25V to ±15V); Talking
Headlight Reminder; Electronic Ballast For Fluorescent
Lights; Temperature Controlled Soldering Station; Electronic
Engine Management, Pt.13.
November 1994: Dry Cell Battery Rejuvenator; A Novel
Alphanumeric Clock; 80-Metre DSB Amateur Transmitter;
Twin-Cell Nicad Discharger (See May 1993); Anti-Lock
Braking Systems: How They Work; How To Plot Patterns
Direct To PC Boards.
December 1994: Dolby Pro-Logic Surround Sound Decoder,
Pt.1; Easy-To-Build Car Burglar Alarm; Three-Spot Low
Distortion Sinewave Oscillator; Clifford – A Pesky Electronic
Cricket; Cruise Control – How It Works; Remote Control
System for Models, Pt.1; Index to Vol.7.
January 1995: Build A Sun Tracker For Solar Panels;
Battery Saver For Torches; Dolby Pro-Logic Surround
Sound Decoder, Pt.2; Dual Channel UHF Remote Control;
Stereo Microphone Preamplifier; The Latest Trends In Car
Sound; Pt1.
February 1995: 50-Watt/Channel Stereo Amplifier
Module; Digital Effects Unit For Musicians; 6-Channel
Thermometer With LCD Readout; Wide Range Electrostatic Loudspeakers , Pt.1; Oil Change Timer For Cars;
The Latest Trends In Car Sound; Pt2; Remote Control
System For Models, Pt.2.
PLEASE NOTE: all issues from November 1987 to August
1988, plus October 1988, November 1988, December
1988, January, February, March and 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 (includes.
p&p). When supplying photostat articles or back copies,
we automatically supply any relevant notes & errata at
no extra charge.
March 1995 89
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.
Modification to
coolant level alarm
I am about to build the Coolant
Level Alarm, as described in the June
1994 issue of SILICON CHIP. Could you
please advise me how I can modify
this circuit to replace the rather fragile 8Ω mini loudspeaker with a piezo
transducer as marketed by Dick Smith
Electronics (Cat L-7022)? (L. A., Winn
ellie, NT).
• You can connect the piezo transducer directly in place of the loudspeaker. If you wish, you can also
omit the series 47Ω resistor and
2.2µF capacitor but in practice they
will make negligible difference to the
sound output.
Fast charger
for six cells
I have seen the “Fast Charger for
Nicad Batteries” in the May 1994 issue. As I do a fair amount of wedding
photography, I could use a charger as
presented as my flash batteries will
sometimes become exhausted before I
Questions on weather
beacon radio
I am constructing the Long
Wave AM Receiver for aircraft
weather beacons, as published
in the September 1994 issue. Is it
possible that IC1 on the overlay
diagram, page 56, should be a
YS414 type, not a ZN414 as in
the parts list?
The problem that I have is that
when moving VC1 full travel both
ways I can only pick up 612kHz
(radio station). I have checked VC1
with a capacitance meter and it is
OK. The 10mm ferrite rod came out
of an old radio and is a little longer
than 85mm. Is this length critical?
Perhaps you can help me with
this problem? (D. C., Bris
bane,
Qld).
90 Silicon Chip
am finished, and being able to recharge
one of them in less than an hour would
solve the problem.
Alas, my Metz 45CT5 flash uses a
battery holder containing not four but
six AA nicad cells which can only be
accessed for charging at their 7.2V
output terminals. Is it possible to modify the charger circuitry to charge six
720mA.h cells in series? There would
appear to be enough supply volts (12V)
as the cells need 9V to push 950mA
through them. Your help would be
greatly appreciated.
Incidentally, I bought six of the new
metal hydride rechargeable batteries
and when charging at the 5-hr rate
(360mA) as quoted on their information sheet, one of them exploded. I
could easily have been blinded if I had
been near it at the time.
The company replaced the cells and
the $50 battery holder and I tried again
at 100mA. No explosion, but they all
had different amp-hour and short circuit capabilities and my flash took 20
seconds to build up where it normally
takes eight seconds with fully charged
batteries! So I went back to nicads – a
•
The YS414 and ZN414 are
equivalent devices so you should
not have a problem there. Both
are shown on the circuit diagram,
by the way. Indeed the circuit is
apparently working, even though
you can only pick up 612kHz. This
frequency should be tuned when
the capacitance of the tuning gang
is towards the minimum.
If this is so, your circuit is
working correctly and it is then a
question of how far away you are
from the nearest LF beacon. If you
cannot receive signals indoors, try
it outside, especially if you are in a
weak signal area and the building
you are in is of reinforced concrete
or steel construction or has aluminium sarking in the roof.
The length of rod is not critical –
in fact, the longer the better.
great disappointment. (N. W., Peak
hurst, NSW).
• It is possible to use the Fast Charger
without modification to charge six
nicad cells but there are a number
of constraints. First, the end-point
voltage of a 6-cell pack will be around
10.2V. This, combined with a maximum switching duty cycle of 78% for
the TEA1100, means that the circuit
will fully charge the batteries only if
the input voltage is above 13V. Ideally,
it should be about 14-15V DC. This
could be obtained from a 1-amp DC
plugpack with a nominal rating of
12V or more.
Alternatively, you could elect to
charge two or three cells at a time,
provided you can remove them from
the battery pack.
Component tester
for oscilloscope
I refer to an Altronics advertisement in December 1989 for a Labtech
20MHz CRO which shows that it has
the capability to display component
test status patterns. Is it possible that
there are circuits available as an “addon” to old CROs that would allow one
to test capacitors and zeners? (B. S.,
Burwood, Vic).
• We have not published anything on
this topic to date and shall put it on
our list of projects to be considered.
Sending audio signals
along the AC mains
Have you ever thought about designing a converter and asso
ciated
receiver-amplifier along the lines of
a mains connected intercom? The
converter feeds stereo signals into
the house wiring and speakers can
be plugged in anywhere in the house.
Your comments on such a system,
please. (W. J., Tranmere, SA).
• There is no reason why stereo signals could not be sent via mains AC
wiring using an FM carrier and stereo
multiplex encoding. Funnily enough,
shortly after your letter arrived one
D1-D4
4x1N4001
A
240VAC
FROM
SECURITY
LAMP
IN
12V
N
Buzzer for infrared
security light
I have an infrared sensor on my
house with a spotlight to detect any
visitors and turn on the light. This
light can be set for seconds or minutes at a time. What I would like
to do is attach a buzzer that would
sound for only one or two seconds
each time the detection field was
broken and then not sound again
until the light had turned off and
then on again.
I imagine this would be possiof our contributors sent in a design
along these lines. We hope to publish
it within the next few months.
Electronic ballast
coil confusion
Being a circuit junky, I had a
butcher’s at the Electronic Ballast
for Fluorescent Lights in the October
1994 issue. John Clarke has once again
delivered an interesting circuit that
is sophisticated but straightforward,
without unnecessary complexity. The
power factor correction is a good idea
and I can tell that the MC34262P needs
closer study. Thanks for bringing it to
my notice.
Unfortunately, there is some confusion over the connection of L1 and
L2. On page 45 you say that “L1 & L2
are wound onto a common toroid in
antiphase so that the inductor works
to elim
i nate common mode high
frequency signals without saturation
from the line current”. Figs. 7 & 8 show
the inductors wound and connected
this way. This is quite reasonable and
is exactly how such inductors are
used in most commercially available
mains filters.
However, the circuit diagram (Fig.6,
page 45) and the front cover show the
inductors connected such that the load
current in each inductor adds; ie, they
are in phase. As such the inductors
220
25VW
7812
OUT
GND
+12V
2.2M
7
470k
4
IC1
555
6
2
2.2M
1
8
3
D5
1 1N4001
BUZZER
0.1
ble to do: a unit that would plug
into the light socket and operate
through a step-down transformer
to run a timer circuit of some type
and a buzzer. I have the experience to construct such a project
but not the knowledge to design
the needed equipment. Hoping
you can come up with a possible
will not reduce common mode signals
(noise) and in some circum
stances
saturation may occur, reducing the effective inductance and hence reducing
their effectiveness.
As you are aware, the phasings of
windings on a toroidal core is determined by which way they pass through
the hole. For a common mode choke,
the wires to the mains must come
from the same side of the toroid, and
naturally the wires to the load must
come from the other side of the toroid.
The direction that the windings take
around the toroid is irrelevant except
to parasitic components.
It is probably the extra series inductance that the differential mode
connection adds that causes the flat
topping on the 240V waveform (see
oscillograph, top of page 51). This is
quite similar to the waveform seen
at the secondary of a mains power
transformer driving a full wave bridge
rectifier with filter capacitors, the
leakage inductance of the transformer
being the cause in that case.
But there is a twist. With L1 and
L2 connected as shown in the circuit
diagram, they will reduce any differential mode noise (ie between active
and neutral) that may be present.
Considering the circuit generates
moderate levels of high frequency
power, this may not be such a bad
thing as long as L1 and L2 do not
circuit to do this job. (A. F., Seaton, SA)
• It should be possible to achieve
your purpose with the circuit
shown here. Essentially, it is based
on a 555 monostable timer (IC1)
and this operates a buzzer for two
seconds each time the light comes
on.
saturate. In some two-stage mains
filters this connection is used along
with inductors connected to reduce
common mode noise.
At this point you probably expect
me to give the solution but this is
not a simple thing to do. Noise on
the mains can have differential and
common mode components and, as I
have stated, the inductors can be connected to block one or the other, but
not both simultaneously. The answer
to which connection is best depends,
to some extent, on the installation; ie,
the wiring, the nature and sensitivity
of appliances connected to the mains,
etc, over which we have no control.
I think that probably the best way
to go is to connect it in the common
mode. This should eliminate the
possibility of saturation in the ferrite
and maximise the useful inductance.
Besides, the filter capacitors should
reduce the high frequency differential mode noise and the power factor
correction should take care of the harmonic garbage that would otherwise
be generated by the rectifier and filter
capacitor combination.
I am glad to see that you have made
a serious effort to design a quiet and
efficient circuit. It is much better to
have noise stopped at its source than
to have to deal with it everywhere else.
(P. D., Sydney, NSW).
• The phase of the windings for L1
March 1995 91
More light on power
factor controller
Could you please elaborate a
little more on the operation of the
power factor controller circuit,
Fig.4, page 44 of your October 1994
edition. What I want to know is at
what point is the switching of Q1
affecting the 400V output given
that, according to your diagram,
Q1 is switched on and off over the
full half cycle. It seems a bit much
to step, say, 50V coming from the
bridge rectifier to over 400V at that
point in the half cycle, or is using
R1 & Lx as a load sufficient to cause
Iav to be in phase with Vin regardless of the tube current?
Also, your parts list for that
project describes the 1N5062 as a
transient protected diode. What do
you mean by this? (G. F., Nairne,
SA).
• The boost converter comprising
IC1, Q1, Lx, Dx and C2 begins to operate from a relatively low voltage
within the AC waveform, as shown
in Fig.4 on page 44. Typically, it
starts at around 50V.
While it may seem impossible
for the converter to boost the
voltage from 50V to 400V, it is the
and L2 is not very clear in the front
cover photo. However, we can assure
you that the windings in the prototype
are as per Fig.7 and a better photograph
of the actual winding directions can
be seen on page 52. Yes, we concede
that the circuit diagram phase dots
are incorrect.
The flat topping of the mains is due
to the supply that we obtain here in
Warriewood. This flat topping can
also be seen in the oscilloscope photographs for the High-Power Dimmer
for Incandescent Lamps, as published
in August 1994 (see page 32 and the
caption referring to flat topping).
Input capacitor
wrongly polarised
After seeing your 25W amplifier
design in the December 1993 issue, I
purchased two of these modules as I
was constructing an amplifier at the
time. I also took the tone control section from the circuit for your Studio
92 Silicon Chip
rate of change of current through
Lx which develops the voltage
into C2 rather than some form of
transformer action. Consequently,
it is possible to boost the voltage
to very high values.
Note that the current drawn by
the power factor circuit is also
sinusoidal and follows the input
voltage waveform. This is shown in
the top waveform on page 51. The
current flow is forced this way by
the multiplier which sets the current through R1. This depends on
the phase of the incoming voltage
at pin 3 of IC1.
The transient protected diode is
also called a controlled avalanche
type. It refers to the diode’s perfor
mance when in the breakdown
region of its V1 curve. Once in
this region, where reverse voltage
is sufficient to force the diode into
breakdown, a normal diode will
possibly fail since its impedance
suddenly drops to a low value to
allow a high current flow.
Transient protected diodes, on
the other hand, have a soft breakdown characteristic, so that when
breakdown does occur, the impedance remains relatively high. This
prevents damage to the diode.
Twin Fifty Amplifier (March & April
1992) to complete the project as an
amplifier to power a pair of scratchbuilt 40-watt 3-way speakers.
Upon testing of the amplifier modules I was initially delighted with the
performance. However, after attaching
them to a pair of different speakers
having a higher sensitivity, I noticed
that a substantial amount of noise
appeared at the output when any input (including a direct ground, 50kΩ
pot or preamp output via latter) was
connected to the input of the module.
I constructed the single supply
version of the project and was quite
certain that the kits were constructed
perfectly, and indeed the fault showed
up in both modules. Extensive testing
using different power supplies and
checking things with the CRO yielded
nothing so I looked to the 1µF input capacitor. It seemed suspect and a quick
multimeter measurement showed that
it did not sit at half supply voltage as
expected from the 22kΩ divider net-
work. I substituted the nearest thing
I had, a 0.47µF greencap and had
immediate success. Why?
The answer was extremely simple.
The electro had been shown with incorrect polarity on the parts layout on
page 34! It is shown correctly in the
circuit diagram. On the same topic, I
believe the input capacitor on the dual
supply version should be a bipolar or
other non-polarised type. The completed project now sounds superb,
and the tone controls are excellent
as well – in my opinion better than
the five-plus band graphic equalisers
found commonly on middle of the
range equipment today.
Secondly, also on the topic of audio
amplifiers, I need to build an amplifier for my car stereo. Its signal will
have to be derived from the unit’s
speaker outputs and I will provide
tone controls to try and extract some
reasonable audio from my $45/pair
speakers. I looked at a few different
amplifier designs, including that
mentioned above, but 13.8V operation
did not suit any.
However, I then remembered your
data page on the LM383 in the March
1991 issue. It (Fig.5, page 39) shows
two of these devices connected in
bridge mode, which can supposedly deliver 16 watts into 4Ω; perfect
for my application. It supposedly
achieves this by the fact that bridged
amplifiers effectively “see” only half
the speaker impedance; as you again
mention replying to G. F. on page 92
of the November 1994 issue.
My knowledge of bridge amplifier
theory is virtually non-existent but
I don’t believe in any case that an
amplifier can deliver a peak-peak output greater than its DC power supply
voltage. In this case, with a 14V DC
supply rail, the output power into 4Ω
amounts to a little over 6W; although
if the speaker impedance is taken as
2Ω this value changes to double that.
Is this theory correct? If so, how
does this circuit deliver 16W? Otherwise could you recommend a source
of suitable ferrite components to be
used in a voltage step-up circuit to
power a pair of 25W modules? A
30W continuous power rating would
be ample to power two of these with
normal music.
I have seen your DC-DC converter
kit but this is far too expensive and
overkill for the power my car speakers
can handle. Are there any other ways
of getting reasonable power from car
battery voltage into 4Ω loads?
Still on audio topics, I would like
to express my annoyance at the PMPO
marketing terms used by reputable
audio equipment manufacturers to
sell hifi equipment. Words like 400W
PMPO are a common sight on cheap
midi systems which don’t even draw
more than 50W or so from the mains.
In fact, looking at the amplifiers and
drivers in these systems, they don’t
look like they can deliver more than
10-15W RMS per channel. I am quite
sure there is no mathematical basis for
these figures and they simply make it
hard to choose an amplifier with the
power you require.
I am pleased to say, however, that
quality Japanese brands such as Sony
and JVC do use correct RMS terminology and believable figures. Surely the
use of such meaningless figures should
be prohibited by Australian standards.
Similar situations apply with car
speakers; the $45 speakers I mentioned
above are marked “80 watts maximum
music power” though they are sold
as 40W speakers and in practice they
don’t like much volume through a true
20W RMS good quality amplifier. (S.
Longer fade for
diesel horn
I always enjoy the magazine and
the model railway projects. The
whistle and horn described in the
July 1994 issue have a very good
tone but the diesel horn needs to
have a longer fade as the air bleeds
off and the horn trumpet continues
to “ring” in the prototype. If you
could change that, it would be
perfect. Any suggestions?
A very impressive digital controlled throttle was demonstrated
at the October 1994 Liverpool
model railway exhibition with
AC on the track permanently and
locos addressed by the controller.
This seems the way of the future.
Do you see it as a viable project?
Finally, I must say how much I
like your circuit diagrams, compared with those tiny computer
generated symbols of some other
magazines. (T. B., Kogarah, NSW).
• It is possible to increase the fade
time by using a bigger capacitor
for the 22µF capacitor at the base
J., Surrey Downs, SA).
• You are right about the input coupling capacitor’s polarity and, ideally,
the input capacitor for the balanced
supply version should be a bipolar
type.
The LM383 can deliver around 1112W in bridge mode since its output
swing is doubled and it “sees” a 2Ω
load. The figure of 16W is only possible at the higher supply voltage of 20V.
We don’t have any simple answers to
your need for power amplifiers run
from 13.8V DC; a big inverter is the
only way.
We agree with you about the absurdity of amplifiers with PMPO figures. To
our knowledge, an Australian stand
ard for hifi equipment has never been
promulgated although our publisher
spent a good deal of time in the 1970s
sitting on a standards committee for
that purpose. Since so little hifi equipment is manufactured in this country,
there seems little point in having a
local standard anyway.
Car speakers are rated with nonsensical figures and even those that
do have high ratings are often quite
inefficient so that the overall loudness
and dynamic range is not marvellous.
of Q2. Try 100µF or larger. Alternatively, try connecting a 100kΩ
or larger resistor in series with
diode D1.
We are familiar with the train
control you mention which was
featured at the October model
railway exhibition. Generally
called “Command Control”, these
systems enable realistic control of
a large number of locomotives on a
layout, without the need for block
switching and so on. The drawback
is that they are quite expensive
and require a control receiver to
be installed in every locomotive,
together with a changeover switch
if it is desired to run the loco on
other layouts with conventional
controllers.
Thanks for the compliment on
our circuit diagrams. They are actually generated on a CAD system
but our draughtsman, Bob Flynn,
has spent a considerable amount
of time to produce a library of
symbols which look very similar
to those used when our diagrams
were hand-drawn.
Notes & Errata
25W Amplifier Module, Dec. 1993: the
wiring diagram for the single supply
version (Fig.3) shows the 1µF input
capacitor installed the wrong way
around; the circuit diagram is correct.
Also the 1µF input capacitor for the
dual supply version should be a bipolar electrolytic or other non-polarised
capacitor such as an MKT polyester.
Multi-Channel Remote Control, May
1994: the Vcc (supply line) to a number
of ICs (IC4, IC6, IC8, IC9, IC10 & IC11)
is open circuit on the PC board, as
supplied by the author. This presents
a problem when using the outputs for
latched operation.
To correct the error, wire a link from
pin 7 of IC2 to the pin of C7 (.0047µF)
which is closest to the outside edge of
the PC board. A corrected PC pattern
is available if necessary.
Some codes may not operate correctly due to the thresholds being quite
critical on IC12a. This causes the rate
pin (RB) of IC1 to pulse erratically and
therefore IC1 is not able to receive a
valid code. To correct this problem,
replace R5 with a trimpot and adjust
it so that the voltage on pin 6 of IC12b
is halfway between the voltage at pin
5 when transmitting a valid code with
link SW13 (on the transmitter board)
in and when transmitting a valid code
with link SW13 out.
The author has experimented with
this and, with a supply rail of 6.39V,
the value for R5 worked out at 6.8kΩ.
The voltages on pin 5 varied between
2V and 3V and so the threshold was
set for 2.5V.
50-watt Stereo Amplifier Module,
Feb. 1995: the parts list should show
2 x 22µF 16VW electrolytic capacitors
(not 4). In addition, 2 x 47µF 16VW
electrolytic capacitors should be added to the list.
Digital Effects Unit, Feb. 1995: The
parts list should show 19 330Ω resistors rather than one. On the circuit
(Fig.2), the 3.3kΩ resistor shown at the
input to the modulation filter should
be 22kΩ. An extra 3.3kΩ resistor
should be included between the positive side of the 100µF capacitor and
the junction of the 1.8kΩ and 22kΩ
resistors.
Finally, the two 56pF capacitors
shown on the PC board overlay (Fig.3)
should each be 560pF, while the unmarked electrolytic capacitor at top
right should be labelled 10µF.
SC
March 1995 93
MARKET CENTRE
Cash in your surplus gear. Advertise it here in Silicon Chip.
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FOR SALE
Advertising rates for this page: Classified ads: $10.00 for up to 12 words plus 50
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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.
HD 64000 DEVELOPMENT SYSTEM.
All plug-ins, emulation pods, ASM, C
and Xcompilers, software and very
full documentation for 64000 systems,
Z80 NSC800, 80xx, 68xxx, $2.5k. P. L.
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ASIAN ELECTRONICS repairs and service data. Phone Phil 2pm-5pm Mon-Fri
(03) 773 3997.
LEARN MICROCONTROLLER programming with our Motorola 68HC
705K1 & P9 Kits. All code fully commented, provided on floppy disk. Introduction to the K1 (reviewed in Everyday
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P9). DIY Electronics, phone/fax: (058)
62 1915.
PELTIER EFFECT solid state modules
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FAX/SSTV “MFAX” Multipur pose
IBM PC plug-in card for Satellite Fax
WEAFAX and SSTV. Compatible with
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Enclosed is my cheque/money order for $__________ or please debit my
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94 Silicon Chip
RCS Radio Pty Ltd is the only company that manufactures and sells every
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RADIOTRON DESIGNERS HANDBOOK, 4th edition (Langford-Smith)
approx. 1500pp. Best book EVER
about valves and radio design. Good
condition, considering 40 years old,
$100 each. Broken back, otherwise
complete, $80. Plus post * pack (within
Australia) $10 each. Also Paleo VCT,
valve tester, signal generator, valves,
other old radio books, offers? Hurley,
POB 245/R, Blackburn, Vic 3130. Tel/
Fax (03) 889 6337.
A $2 COIN (or stamps) for Don’s New
Menu Driven Promo Disk. Covers all
Short Form Kits. COM1: driven 18 I/O
$70, LPT1: driven 64 I/O $38, Z80 Dev
$38+, PIC16C5x/71/84 Universal PCB
$23, Basic Stamps $63. Don McKenzie,
29 Ellesmere Crescent, Tullamarine
3043. Phone (03) 338 6286.
TINY VIDEO CAMERAS $10 off! This
month from $189. Previous buyers get
DOUBLE $20 off.
MATCHBOX SIZE PCB MODULES
MEMORY & DRIVES
PRICES AT APRIL, 1995
SIMM (all 70ns)
Parity/No Parity
1Mb 30-pin
$64/58
4Mb 30-pin $200/200
2Mb 72-pin $148/135
4Mb 72-pin $258/228
8Mb 72-pin
$515/470
16Mb 72-pin
$780/690
32Mb 72-pin $1560/1380
Parallax “BASIC STAMP”: 8
I/O pins and proto
typing area.
Program it with a PC, 33 simple
instructions. Development kit
includes one “BASIC STAMP”
($270). Extra modules ($79.85).
Chipset and Resonator to make
your own $30.25. STAMP Stretch
er 16 I/O 1 A/D $91.96. Serial
input LCD display $102.85.
Scarce components needed for
Application notes now in stock.
Small items XPress post $5, kit
$8. Send four 45c stamps for
details. Parallax Distributor and
technical support in Australia.
MicroZed Computers
PO Box 634 (296 Cook’s Rd),
ARMIDALE 2350
V (067) 722 777 F (067) 728 987
Credit cards accepted.
MAC
8Mb P’BOOK
CO-PROCESSORS
387S/DX to 40
$405
$90
LASER PRINTER HP
with 2Mb
$200
DRAM DIP
1Mb x 1
70ns DIP $7.80
256 x 4
70ns DIP $7.80
256 x 16
70ns SOJ $48.00
IBM PS.2
THINKPAD
L40/N33
8Mb
4Mb
$655
$275
TOSHIBA
3100SX
2100/50
4Mb
8Mb
$255
$585
SUN
SPARC 5
32Mb
SPARC 10/20 64Mb
$1780
$3696
DRIVES – SEAGATE
545Mb 14ms 3yr wty $335
1052Mb 9ms 5yr wty $550
COMPAQ
2148Mb 9ms 5yr wty $1470
CONTURA 8Mb
$550
Sales tax 21%. Overnight delivery. Credit cards welcome.
Ring for latest prices. We buy & trade RAM.
1st Floor, 100 Yarrara Rd, PO Box 382, Pennant Hills, 2120.
Tel: (02) 980 6988
Fax: (02) 980 6991
•
PELHAM
ELECTROSTATIC
LOUDSPEAKERS
• 3-Panel Full Range Design.
Available in kit form or fully assembled.
Locally designed & manufactured.
•
For information brochure,
Phone (09) 397 6212 Fax (09) 496 1546
Or write to: E. R. AUDIO,
119 BROOKTON HWY, ROLEYSTONE,
WESTERN AUSTRALIA 6111.
N.S.W. Ph. (02) 804 6859
S.A. Ph. (08) 332 6513
TAS. Ph. (002) 31 2403
SILICON CHIP FLOPPY INDEX
WITH FILE VIEWER
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.
Price $7.00 each + $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.
March 1995 95
Microprocessor For
Digital Effects Unit
Microprocessor For
Stereo Preamplifier
Advertising Index
Now available from SILICON CHIP:
the 68HC705-C8P pre-programmed
micro
pro
cessor IC for the Digital
Effects Unit described in this issue.
Price: $45 + $6 p+p
Payment by cheque, money order or
credit card to: Silicon Chip Publica
tions, PO Box 139, Collaroy, NSW
2097. Phone (02) 979 5644; Fax (02)
979 6503.
Now back in stock: the 68HC705-C8P
pre-programmed microprocessor for
the Infrared Remote Controlled Stereo
Preamplifier (SILICON CHIP, Sept.Oct. 1993). This device also suits the
Remote Volume Control published in
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.
Altronics ................................ 66-68
from 32 x 32 x 23mm with lens. 16 types.
Optional lenses, C lens mounts, cases
& technical manuals.
ALLTHINGS Ph/Fax (09) 349 9413.
VALVES: all types for radio, audio and
industrial use. For sale and wanted to
buy. SSAE for list. Electronic Valve and
Tube Company, PO Box 381, Chad
stone, Vic 3148. Fax (03) 571 1160. Ph
(018) 557 380.
MicaSOFT Electronics and Computing
tutor program, written in UK, ideal for
TAFE, schools or individual use. Now
available in Australia. Send 4 x 45c
stamps for demo disk (tell us what size)
MicroZed Computers, PO Box 634,
Armidale 2350.
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.
C COMPILERS: everything you need
to develop C and ASM software for
68HC08, 6809, 68HC11, 68HC16,
8051/52, 8080/85, 8086 or 8096:
$150.00 each. Macro Cross Assemblers
Av-Comm.....................................49
Dick Smith Electronics........... 12-15
E.R. Audio....................................95
Greg Ball Electronics...................95
Instant PCBs................................95
Jaycar .........................................45
L&M Video...................................83
for these CPUs + 6800/01/03/05 and
6502: $150 for the set. Debug monitors:
$75 for 6 CPUs. All compilers, XASMs
and monitors: $550. 8051/52 or 80C320
simulator (fast): $75. Demo disk: $5.
Network Software: use serial, parallel,
Arcnet or Ethernet to share files and
printers on your PCs. DOS and Windows
compatible. $105 per network. All prices
+ postage. GRANTRONICS, PO Box
275, Wentworthville 2145. Ph/Fax (02)
631 1236.
Macservice...............................3,44
BINARY CLOCK – OCTOBER 1993:
complete documentation supplied,
includes introduction to binary, how it
works, PLD source listings, conversion
tables. Kit with PC board and all components $75 plus $5 p&p. Optional Z frame
stand (includes spacers and chassis DC
connector) $25 plus $5 P7P. Available
from Prototype Electronics, 1/29 Stewart
St, Paramatta, NSW 2124. Phone (02)
890 2960; Fax (02) 630 3148. Pay by
cheque, money order, credit card.
SC Railway Projects Book.......OBC
PRINTED CIRCUIT BOARDS for the
hobbyist. For service & enquiries contact: T. A. Mowles (08) 326 5590.
MicroZed Computers...................95
Oatley Electronics.................. 78-79
Pelham.........................................95
RCS Radio ..................................94
Resurrection Radio .....................77
Rod Irving Electronics .......... 27-31
Silicon Chip Back Issues....... 88-89
Silicon Chip Binders....................62
Silicon Chip Bookshop.................67
Silicon Chip Software..................73
Silicon Chip Wallchart................IBC
Tektronix....................................IFC
Yuga Enterprise...........................95
_________________________________
PC Boards
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 31, or phone or fax your order to:
Silicon Chip Publications, PO Box
139, Collaroy Beach, 2097. Phone
(02) 979 5644. Fax: (02) 979 6503.
96 Silicon Chip
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.
Order by phone or fax from SILICON CHIP - or use the handy order form inside
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