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Items relevant to "Low-Cost Colour Video Fader":
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GHOST BUSTING FOR TV SETS NOW FEASIBLE
$4.50 AUGUST 1993
NZ $5.50
INCL
GST
REGISTERED BY AUSTRALIA POST – PUBLICATION NO. NBP9047
SERVICING — VINTAGE RADIO — COMPUTERS — AMATEUR RADIO — PROJECTS TO BUILD
Z80-BASED SINGLE
BOARD COMPUTER
Build A Super Bright
60-LED Brake Light Array
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which is now out of date and the advertiser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
Vol.6, No.8; August 1993
FEATURES
FORGET THOSE
MESSY edits on
your VCR. This
project smoothly
fades any composite PAL video
signal to black & can also wipe
left or right across the screen for
special effects. Details page 18.
4 Ghost-Busting for TV Sets Now Feasible
New system from Philips cleans up the signal
6 The Keck Optical Telescope, Pt.2 by Bob Symes
The world’s biggest optical telescope
PROJECTS TO BUILD
18 Low-Cost Colour Video Fader by Darren Yates
Fades to black or wipes left or right across the screen
30 A Microprocessor-Based Sidereal Clock by John Western
THIS STAR CLOCK is micro
processor controlled & has two
6-digit displays which show
sidereal time & either local or
universal time. See page 30.
Shows sidereal time plus local or universal time
56 Build A 60-LED Brake Light Array by Leo Simpson
The LEDs light from the centre outwards
82 The Southern Cross Computer by Peter Crowcroft & Craig Jones
A single-board Z80-based computer for the 1990s
SPECIAL COLUMNS
40 Serviceman’s Log by the TV Serviceman
Little things can be big time wasters
53 Remote Control by Bob Young
Unmanned aircraft – Israel leads the way
YOU’VE SEEN THOSE fancy
brake light arrays on late-model
sports cars & now you can build
one for your car. It uses 60 highbrightness LEDs that light from
the centre outwards. Construction
starts on page 56.
62 Vintage Radio by John Hill
How to deal with block capacitors
72 Amateur Radio by James Morris, VK2GVA
A look at satellites & their orbits
DEPARTMENTS
2
28
75
79
Publisher’s Letter
Circuit Notebook
Order Form
Product Showcase
90
92
95
96
Back Issues
Ask Silicon Chip
Market Centre
Advertising Index
THIS SINGLE-BOARD Z80-based
computer is designed for the
1990s generation of students. It
comes with a fully commented
monitor & is designed to teach
microprocessor & microcontroller
programming techniques.
August 1993 1
Publisher & Editor-in-Chief
Leo Simpson, B.Bus.
Editor
Greg Swain, B.Sc.(Hons.)
Technical Staff
John Clarke, B.E.(Elec.)
Robert Flynn
Darren Yates, B.Sc.
Reader Services
Ann Jenkinson
Sharon Macdonald
Marketing Manager
Sharon Lightner
Phone (02) 979 5644
Mobile phone (018) 28 5532
Regular Contributors
Brendan Akhurst
Garry Cratt, VK2YBX
Marque Crozman, VK2ZLZ
John Hill
Jim Lawler, MTETIA
Bryan Maher, M.E., B.Sc.
Philip Watson, MIREE, VK2ZPW
Jim Yalden, VK2YGY
Bob Young
Photography
Stuart Bryce
SILICON CHIP is published 12 times
a year by Silicon Chip Publications
Pty Ltd. A.C.N. 003 205 490. All
material copyright ©. No part of
this publication may be reproduced
without the written consent of the
publisher.
Printing: Macquarie Print, Dubbo,
NSW.
Distribution: Network Distribution
Company.
Subscription rates: $42 per year
in Australia. For overseas rates, see
the subscription page in this issue.
Editorial & advertising offices:
Unit 1a/77-79 Bassett Street, Mona
Vale, NSW 2103. Postal address:
PO Box 139, Collaroy Beach, NSW
2097. Phone (02) 979 5644. Fax
(02) 979 6503.
PUBLISHER'S LETTER
Pay TV will
boost optical
fibre technology
Since I wrote about the "Pay
TV Farce" back in the August
1992 issue, the story has had
more twists and turns than
any fiction writer could have
dreamed up. The big players
missed out on getting a satellite TV licence while two unknowns, Ucom and Hi-Vision,
got the prizes. Now that the Australian Broadcasting Authority has approved
the licences, there remains the matter of about $400 million to be paid.
However, the satellite TV licences may yet turn out to be the "booby
prizes" if the Packer/Murdoch/Telecom pay TV consortium looks seriously
at the other way open to it – optical fibre transmission and what it terms
"Asymmetric Digital Subscriber Lines". While we don't know exactly what
Telecom is planning, it is an obvious move. Having lost its monopoly on
telephone traffic and having been told by the Federal Government to go out
and behave like a commercial corporation, it is starting to do just that, to
the consternation of some politicians within the Government. Not only has
it aligned itself Packer and News Corporation in the Pay TV consortium, it
has also taken the unprecedented step of taking a shareholding in the Seven
TV network. This last step is of particular significance because of the Seven
Networks' experiment in interactive television in Adelaide.
Let's just crystal-ball on how the Packer/Murdoch/Telecom Pay TV system
might work and remember it will probably be interactive. Therefore, the
subscriber could use his set to dial up the exchange and select whatever
program he wants or switch between any of dozens of programs. This would
be no problem for the optical fibre system, especially since only one video
program would need to be sent from the exchange to the subscriber at any
one time. Think about it? A choice of maybe dozens of programs, always
with high signal quality and with no need for a dish on the roof. Satellite
pay TV is unlikely to be able to offer the same range of choice. So really, at
some stage in the next decade, a satellite TV licence could just be a millstone
around a company's neck.
Remember also that the optical fibre system will probably also support
video telephones and data services of all sorts – education, banking, shopping, TAB, you-name-it. When you think of the huge potential of an optical
fibre network, it could well be that Telecom is quite happily contemplating
its prosperous future. And why shouldn't it? After all, it was told to go out
and play with the big boys and that's what it is doing.
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
Ghost-busting for
TV sets now feasible
However much we might like watching TV,
a great many viewers are plagued by ghost
reception. This is caused by signals which have
travelled by reflection rather than the direct
path. A number of ghost cancelling circuits have
been mooted over the last 10 years but none has
come to fruition. Now Philips has succeeded
where others have failed.
At the recent National Association
of Broadcasters (NAB) Conference in
Las Vegas, Philips Research Laboratories demonstrated the world’s first
prototype TV receivers with built-in
ghost cancellation circuitry.
The demonstration consisted of live
Ghost-Cancelling Refer
ence (GCR)
signals beamed to the convention
centre by five local TV stations. At
the convention centre, delegates compared heavily ghosted pictures with
specially prepared large screen TVs incorporating Philips ghost cancellation
technology, on which there was not the
slightest hint of a ghost.
4 Silicon Chip
At the heart of the system is a special
Ghost Cancellation Reference signal
which the broadcasters transmit in
a hidden portion of the TV field. By
the time the GCR signal reaches a
receiving antenna, it has undergone
the same ghost distortions as the tele
vision picture.
The received analog signal is then
changed into digital form using an
inexpensive 8-bit converter. Once
the signal is in digital form, it can be
easily manipulated. The signal is then
compared to the original GCR signal.
Based upon this analysis, settings are
made for a ghost cancelling filter. The
filtered signal, with ghosts removed,
is then converted back to analog for
normal viewing.
This whole process is done electronically and the processing speed
is what makes the Philips system so
effective. The ghost cancelling filter
chip is produced by Philips, as are the
mathematical algorithms and processing software that control the system.
This system has out-performed all others in trials to win the “ghostbuster”
title, and has an internal clock speed
of 57MHz.
The USA’s Federal Communication
Commission (FCC) has approved use
of the Philips ghost cancelling signal
by TV broadcasters, effective from 30th
June, 1993. The immediate objective
at the Philips Briarcliffe Laboratories
is to reduce the power supply require
ments and make the chips sufficiently
cost effective for mainstream production.
Helen Freeman, Philips TV and
video product marketing manager in
Australia, says that we can expect the
“ghostbusting” option to be available
SC
in TV sets from 1995.
8MM VIDEO CASSETES
These 120-minute 8mm metal oxide video cassettes
were recorded on once for a commercial application
and then bulk erased. They are in new condition but
don’t have the record protect tabs fitted. The hole
in the upper right corner will have to be taped over.
$9 Ea. or 5 for $38
LARGE NIGHT VIEWERS
One of a kind! A very large complete viewer for
long range observation. Based on a 3-stage fibre
optically coupled 40mm first generation image
intensifier, with a low light 200mm objective mirror
lens. Designed for tripod mounting. Probably the
highest gain-resolution night viewer ever made.
ONE ONLY at an incredible price of:
$3990
BINOCULAR EHT POWER SUPPLY
This low current EHT power supply was originally
used to power the IR binoculars advertised elsewhere in this listing. It is powered by a single 1.5V
“C” cell and produces a negative voltage output
of approximately 12kV. Can be used for powering
prefocussed IR tubes etc.
$20
IR BINOCULARS
High quality helmet mount, ex-military binocular
viewer. Self-powered by one 1.5V “C” size battery.
Focus adjustable from 1 metre to infinity. Requires
IR illumination. Original carry case provided. Limited
stocks, ON SPECIAL AT:
$500
IR FILTERS
A high quality military grade, deep infrared filter.
Used to filter the IR spectrum from medium-high
powered spotlights. Its glass construction makes
it capable of withstanding high temperatures.
Approx. 130mm diameter and 6mm thick. For use
with IR viewers and IR responsive CCD cameras:
ON SPECIAL
$45
12V OPERATED LASERS WITH KIT
SUPPLY
Save by making your own laser inverter kit. This
combination includes a new HeNe visible red laser
tube and one of our 12V Universal Laser Power
Supply MkIII kits. This inverter is easy to construct
as the transformer is assembled. The supply powers
HeNe tubes with powers of 0.2-15mW.
$130 with 1mW TUBE
$180 with 5mW TUBE
$280 with 10mW TUBE
MAINS OPERATED LASER
Supplied with a new visible red HeNe laser tube with
its matching encapsulated (240V) supply.
$179 with 1mW TUBE
$240 with 5mW TUBE
$390 with 10mW TUBE
GREEN LASER HEADS
We have a limited quantity of some brand new
2mW+ laser heads that produce a brillant green
output beam. Because of the relative response of the
human eye, these appear about as bright as 5-8mW
red helium neon tubes. Approximately 500mm long
by 40mm diameter, with very low divergence. Priced
at a small fraction of their real value
$599
A 12V universal laser inverter kit is provided for
free with each head.
ARGON HEADS
These low-voltage air-cooled Argon lon 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. Depends
on the tube current. The head includes power meter
circuitry, and starting circuitry. We provide a simple
circuit for the supply and can provide some of the
major components for this supply. Limited supplies
at a fraction of their real cost.
$450-$800
ARGON OPTIC SETS
If you intend to make an Argon laser tube, the
most expensive parts you will need are the two
mirrors contained in this ARGON LASER OPTIC
SET. Includes one high reflector and one output
coupler at a fraction of their real value. LIMITED
SUPPLY
$200 for the two Argon LASER mirrors.
LASER POINTER
Improve and enhance all your presentations. Not
a kit but a complete commercial 5mW/670nm pen
sized pointer at ONLY:
$149
LARGE LENSES
Two pairs of these new precision ground AR coated
lenses were originally used to make up one large
symmetrical lens for use in IBM equipment. Made
in Japan by TOMINON. The larger lens has a
diameter of 80mm and weighs 0.5kg. Experimenters
delight at only:
$15 for the pair.
EHT GENERATOR KIT
A low cost EHT generator kit for experimenting
with HT-EHT voltages: DANGER – HIGH VOLTAGE! The kit also doubles as a very inexpensive
power supply for laser tubes: See EL-CHEAPO
LASER. Powered from a 12V DC supply, the EHT
generator delivers a pulsed DC output with peak
output voltage of approximately 11kV. By adding
a capacitor (.001uF/15kV $4), the kit will deliver
an 11kV DC output. By using two of the lower
voltage taps available on the transformer, it is
possible to obtain other voltages: 400V and 1300V
by simply adding a suitable diode and a capacitor:
200mA - 3kV diode and 0.01uF 5kV capacitor: $3
extra for the pair.
Possible uses include EHT experiments, replacement supplies in servicing (Old radios/CRO’s),
plasma balls etc. The EHT generator kit now includes
the PCB and is priced at a low:
$23
LED DISPLAYS
National Seminconductor 7-segment common
cathode 12 digit multiplexed LED displays with 12
decimal points. Overall size is 60 x 18mm and pinout
diagram is provided.
2.50 Ea. or 5 for $10
BATTERIES
Brand new industrial grade PANASONIC 12V-6.5AHr
sealed gel batteries at a reduced price.Yes, 6.5 AHr
batteries for use in alarms, solar lighting systems,
etc. Dimensions: 100 x 954 x 65mm. Weight of one
battery is 2.2kG. The SPECIAL price?
$38
PIR DETECTORS
What are the expensive parts in a passive movement dector as per EA May 89? A high quality dual
element PIR sensor, plus a fresnel lens, plus a white
filter. We include these and a copy of PIR movement
detector circuit diagram for:
$9
MASTHEAD AMPLIFIER KIT
Based on an IC with 20dB of gain, a bandwidth of
2GHz and a noise figure of 2.8dB, this amplifier kit
outperforms most other similar ICs and is priced
at a fraction of their cost. The cost of the complete
kit of parts for the masthead amplifier PCB and
components and the power and signal combiner
PCB and components is AN INCREDIBLE:
$18
For more information see a novel and extremely
popular antenna design which employs this amplifier: MIRACLE TV ANTENNA - EA May 1992: Box,
balun, and wire for this antenna: $5 extra
SODIUM VAPOUR LAMPS
Brand new 140W low pressure sodium vapour
lamps. Overall length 520mm, 65mm diameter, GEC
type SO1/H. We supply data for a very similar lamp
(135W). CLEARANCE AT:
lenses: two plastic and one glass. The basis of
a high quality magnifier, or projection system?
Experimenters’ delight!
$30
CRYSTAL OSCILLATOR MODULES
These small TTL Quartz Crystal Oscillators are hermetically sealed. Similar to units used in computers.
Operate from 5V and draw approximately 30mA.
TTL logic level clock output. Available in 4MHz,
4.032MHz, 5.0688MHz, 20MHz, 20.2752MHz,
24.74MHz, 40MHz and 50MHz.
$7 Ea. or 5 for $25
FLUORESCENT BACKLIGHT
These are new units supplied in their original
packing. They were an option for backlighting Citizen
LCD colour TVs. The screen glows a brilliant white
colour when the unit is powered by a 6V battery.
Draws approximately 50mA. The screen and the
inverter PCB can be separated. Effective screen
size is 38 x 50mm.
$12
MAINS FILTER BARGAIN
For two displays - one yellow green and one
silver grey.
SOME DIFFERENT COMPONENTS
1000pF/15kV disc ceramic capacitors ..............$5
20kV PIV - 5mA Av/1A Pk fast diodes .........$1.50
3kV PIV - 300mA / 30A Pk fast diodes ........... 60c
0.01uF /5kV disc ceramic capacitors ...........$1.80
680pF / 3kV disc ceramic capacitors .............. 30c
Who said that power MOSFETS are expensive??
MTP3055 N-channel MOSFETS as used in many
SC projects ............................$2 Ea. or 10 for $15
MTP2955 P-channel MOSFETS (complementary
to MTP3055) ..........................$2 Ea. or 10 for $15
BUZ11 N-channel MOSFETS $3 Ea. or 10 for $25
Brief DATA and application sheet for above MOSFETS free with any of their purchases (ask)
Flexible DECIMAL KEYPADS with PCB connectors
to suit ...........................................................$1.50
1-inch CRO TUBES with basic X-Y monitor circuit
CLEARANCE <at>..............................................$20
Schottky Barrier diodes 30V PIV - 1A/25A Pk. 45c
100 LED BARGRAPH DISPLAY
Note that we also have some IEC extension leads
that are two metres long at $4 Ea.
Yes 100 LEDs plus IC control circuitry, all surface
mounted on a long strip of PCB. SIMPLE - a 4-bit
binary code selects which one out of the 10 LED
groups will be on, whilst another 4-bit binary code
selects which one of each group of 10 LEDs will
be ON. Latching inputs are also provided. We
include a circuit and a connecting diagram. VERY
LIMITED QUANTITY
WEATHER TRANSMITTERS
FM TRANSMITTER KIT - MKll
A complete mains filter employing two inductors
and three capacitors fitted in a shielded metal IEC
socket. We include a 40 joule varistor with each filter.
$5
These brand new units were originally intended
to monitor weather conditions at high altitudes:
attached to balloons. Contain a transmitter (12GHz?) humidity sensor, temperature sensor,
barometric altitude sensor, and a 24V battery which
is activated by submersing in water. The precision
all mechanical altitude sensor appears similar
to a barometer and has a mechanical encoder
and is supplied with calibration chart. Great for
experimentation.
$16 Ea.
SOLAR CHARGER
Use it to charge and or maintain batteries on BOATS,
for solar LIGHTING, solar powered ELECTRIC
FENCES etc. Make your own 12V 4 Watt solar
panel. We provide four 6V 1-Watt solar panels with
terminating clips, and a PCB and components
kit for a 12V battery charging regulator and a
three LED charging indicator: see March 93 SC.
Incredible value!
$42
6.5Ahr. PANASONIC gel Battery $35, ELECTRIC
FENCE PCB and all onboard components kit $40.
See SC April 93.
$7Ea.
This low cost FM transmitter features pre-emphasis, high audio sensitivity as it can easily pick
up normal conversation in a large room, a range
of well over 100 metres, etc. It also has excellent
frequency stability. The resultant frequency shift
due to waving the antenna away and close to a
human body and/or changing the supply voltage
by +/-1V at 9V will not produce more than 30kHz
deviation at 100MHz! That represents a frequency
deviation of less than 0.03%, which simply means
that the frequency stays within the tuned position
on the receiver.
Specifications: tuning range: 88-101MHz, supply
voltage 6-12V, current consumption <at>9V 3.5mA,
pre-emphasis 50µs or 75µs, frequency response
40Hz to greater than 15kHz, S/N ratio greater than
60dB, sensitivity for full deviation 20mV, frequency
stability (see notes) 0.03%, PCB dimensions
1-inch x 1.7inch.
Construction is easy and no coil winding is necessary. The coil is preassembled in a shielded metal
can. The double sided, solder masked and screened
PCB also makes for easy construction. The kit
includes a PCB and all the on-board components,
an electret microphone, and a 9V battery clip:
$11 Ea. or 3 for $30
LARGE LCD DISPLAY MODULE - HITACHI
These are Hitachi LM215XB, 400 x 128 dot displays.
Some are silver grey and some are yellow green
reflective types. These were removed from unused
laptop computers. We sold out of similar displays that
were brand new at $39 each but are offering these
units at about half price. VERY LIMITED STOCK.
$40
OATLEY ELECTRONICS
$15 Ea.
PO Box 89, Oatley, NSW 2223
STEPPER MOTORS
Phone (02) 579 4985. Fax (02) 570 7910
$12
MAJOR CARDS ACCEPTED WITH
PHONE & FAX ORDERS
These are brand new units. Main body has a diameter of 58mm and a height of 25mm. Will operate
from 5V, has 7.5deg. steps, coil resistance of 6.6
ohms, and it is a 2-phase type. Six wires. ONLY:
PROJECTION LENS
Brand new large precison projection lens which
was originally intended for big screen TV projection systems. Will project images at close proximity
onto walls and screens and it has adjustable
focussing. Main body has a diameter of 117mm
and is 107mm long. The whole assembly can
be easily unscrewed to obtain three very large
P & P FOR MOST MIXED ORDERS
AUSTRALIA: $6; NZ (Air Mail): $10
August 1993 5
KECK OBSERVATORY
The world’s biggest
optical telescope; Pt.2
Last month, we gave the background to the site
selection and segmented design of the 9.84-metre
Keck Telescope. The guiding force for the project
was Jerry Nelson who had the job of promoting
the concept & convincing enough people to give
financial grants to allow it to proceed.
By BOB SYMES
Ultimately, he was successful in
convincing the astronomers and accountants that the challenge could
be met, and the problems overcome.
Armed with a $US70 million grant
from the W. M. Keck Foundation, Nelson and his collaborators set to work.
The California Institute of Technology
and the University of California made
up the difference in the projected cost
of $US94 million.
These two institutions will run the
telescope through the California As6 Silicon Chip
sociation for Research in Astronomy
(CARA), an association inaugurated
specifically for this purpose. Through
CARA, they will allocate the major part
of observing time, though the University of Hawaii will receive 10% of the
time as co-ordinator of the science
reserve atop Mauna Kea.
On September 12th, 1985, the
ground-breaking ceremony took place
on the summit and the dome and associated complex was completed in
October 1988. The tube and supporting
structure was contracted out to the
civil engineering firm of Schwartz and
Hautmont of Tarragona, Spain and was
also completed in 1988. It was erected
on the summit in 1989.
Understandably, the mirrors caused
the major headaches. At every step of
the way problems arose and had to be
overcome.
Since multiple mirrors, when used
together, cause optical diffraction
effects if they remain as individual
round segments, it was necessary to
construct hexagonal segments that
nestle into each other to minimise the
effect. Under certain circumstances,
such as when two telescopes are used
as an optical interferometer, it is these
very diffraction effects that are used to
extract information about the object
under study, but when the telescope is
used on its own, the diffraction spikes
can hide details that might otherwise
be observed.
A further effect of diffraction is
that contrast is reduced, thus further
hiding subtle detail. Squares, triangles and hexagons are the only shape
of mirror that can nestle together in
this fashion. From the point of view
of wasted material and keeping the
shape as nearly round as possible to
make figuring easier, a hexagon shape
was chosen.
And this is where the problems began. Normally, a mirror is ground and
polished in its final (usually circular)
shape. But a new technique, known
as stressed mirror polishing, was to
be attempted. In this method, the
polishing table has a series of suction
pads and rams which distort the blank
before polishing begins. The mirror
is then polished to a spherical figure,
and when it is released from the table,
the correct hyperboloidal figure would
be obtained.
Terry Mast, the University of
California optician who over
s aw
most of the design and construction
of the mirrors, determined that the
correct shape would not be realised
unless the blanks were polished in
the round and then cut to hexagons,
rather than the other way around.
The danger was that when cut, internal stresses in the blank would
be released, thus throwing out the
carefully created profile.
Less of a problem, but still requiring
careful attention, was that since each
of the 36 mirror segments has one of
six possible different surface profiles,
dependent on where it will be in the
final mosaic, the radial position of
the hexagonal sides had to be in exact
relationship to the figure.
Optics fabrication
Itek Optical Systems of Lexington,
Massachusetts was chosen to fabricate
the optics, as they had much experience in satellite optical systems. The
first six segments were to be delivered
by late 1987 and the following 36
(which included six spares – one for
each position) were to be made available within two years. However, by
late 1987, work was still being done
on the first segment and by mid- 1988
the second was giving trouble.
The feared stress-relief distortions
had materialised and each segment
had to be individually touched up under computer control, optically tested
using a laser interferometer, and then
touched up again, until the residual
errors were within the ability of the
This diagram shows the
location of the 36 segment
primary mirror, the
secondary (2) and tertiary
(3) mirrors and the Nasmyth
(4) & Cassegrain (5) foci. The
tertiary mirror is required
for the Nasmyth focus but is
removed to allow light to pass
through a hole in the primary
mirror to the Cassegrain focus.
warping harness on the tele
scope
mirror mount to correct.
As a result of this delay, in 1989
CARA contracted another optical
laboratory, Tinsley Laboratory of
Richmond, California, to take over
the construction of half the mirror
segments. Work was under way by
February.
Both the Tinsley and Itek blanks
were “hexagonised” at the Itek works,
and by mid-1989 two segments per
month were being produced between
the two contractors. By this time, it
had been decided to forego the computer controlled zonal refiguring, since
this was proving too slow, and it was
hoped that the warping harness could
cope with the now greater residual
aberrations. In fact, the after hexing
deformations have been reported to
be as great as 1 micron.
The warping harness is a series
of adjustable springs on the support
structure of each mirror. There are
30 such springs for each segment and
when correctly set, they can reduce
the residual aberration by a factor of
up to 15.
At least the delivery was easy, unlike the delivery of the great primary
of the 5-metre Hale telescope which
made a slow journey from the Corning
Glass works in New York to the west
cost on a specially constructed flatbed railcar. By contrast, the mirror
segments for the Keck were shipped
from Lexington, Mas
sachusetts to
Honolulu by Federal Express! They
were then sent by barge to Hilo on the
windward side of the Big Island and
by truck to the summit. The relatively
low weight of each segment made
this method quite feasible, something
that couldn’t be said of the massive
Hale mirror.
In common with most observatories,
there is a re-aluminising facility in the
building, so that the mirrors do not
need to leave the mountain when the
reflecting surfaces need to be refur
bished. In fact, they were delivered
from the mainland uncoated and were
aluminised just prior to installation.
Each mirror is housed in a complex
support that includes adjustable pads,
feedback sensors and actuators, as well
as the preset warping components. The
requirement is that every segment is
supported in such a way that all act
together to form one 10-metre mirror.
Each segment be in perfect collimation
with all the rest in the mirror support
framework and must be able to correct for the inevitable tube flexure of
a structure as large as this when the
August 1993 7
movement is in the order of 1mm, in
increments of 0.004 microns. The position actuator consists of a precision
ground screw of 1mm pitch. Shaft
encoders allow the screw to be turned
in increments of one ten-thousandth of
a revolution. This 1mm per revolution
displacement is further reduced by a
factor of 24 by a ratio-reducing hydrau
lic bellows unit.
Capacitive feedback sensors
This view, taken from within the tubular structure of the telescope, shows all
the mirror segments in place. In all, some 36 hexagonal segments are used to
create the primary mirror.
telescope is slewed from one part of
the sky to another.
Flexure of the tube has been estimated to be in the order of 0.5mm as
the telescope is pointed in different
directions, and this flexure has to be
reduced by a factor of 10,000 in order
to maintain the perfect collimation
required to give the sub arc-second
images that the site is capable of producing. The actuators are also capable
of detecting and correcting thermal
changes in the mirror and support
structure.
Mirror support system
In order to provide this required
collimation, the mirror support system
comprises passive and active support.
The passive support is made up of a
stainless steel hub and disc (the flex
disc), which sits in a circular cutout
in the rear of the mirror and prevents
the mirror moving laterally from its
assigned posi
tion. Support for the
mass of each mirror is by means of
three “whiffletrees” evenly spaced
about the mirror, and about two thirds
8 Silicon Chip
of the way out from the centre – at the
radial centre of mass of the segment.
Each whiffletree contains a further
12 floating supports, giving a total of
36 floating supports per segment. The
principal is similar to the technique
used by thousands of amateurs for
their home-made telescopes, only
mechanically far more complex and,
of course, on a completely different
scale. Effectively, each mirror segment
is able to tilt or shift to counteract the
previously discussed errors.
By the way, the word “whiffletree”
comes from the days of stagecoaches,
where the whiffletree was the pivoting
wooden cross-arm attached to the drag
spar. By pivoting, it compensated for
any uneven pull by the horses on either
side of the spar.
Each mirror segment, thus being
able to move freely within its lateral
confinement, allows the active control
system to tilt or move it toward or away
from the focus in order to maintain
collimation. Each segment has three
position actuators associated with
it, one on each whiffletree. The total
Feedback for the actuators is supplied by temperature com
pensated
displacement sensors, consisting
of parallel plates mounted on each
mirror, with a third plate, called
the paddle, attached to the adjacent
mirror, placed between the first two.
The change in capacitance induced
by any relative shift between the two
mirrors is detected and the resulting
corrective commands are sent to the
position actuators.
Each internal segment has 12 sensors attached to it and each peripheral
segment has six or eight, depending on
whether it is a corner or side segment.
The sensitivity of this system is such
that displacements of the order of
0.001 microns can be detected. Jerry
Nelson states that there are actually
63 more sensors than are required
to define the mirror shape, so there
is sufficient redundancy to keep the
telescope functioning to specification
even if there are some sensor failures,
assuming those failures are randomly
distributed around the various mirrors.
This also gives the ability to switch
out a (faulty) sensor that is returning
readings that are substantially different from its neighbours, whilst still
allowing the telescope to operate normally. This is similar to the multiple
sensor “democratic” systems used on
aircraft computer controls. He further
comments that a great advantage of
the active control chosen is that it
relies on no external source to define
its parameters. When the telescope is
switched on, it corrects itself and is
ready for work.
This can be done at any time, day
or night, or even with the dome slit
closed. Thus, engineering calibration
or work can be carried out when ever
it is convenient. This contrasts with
some active systems, where a star or
artificial equivalent has to be viewed
and its image analysed before the
appropriate commands can be issued
to the correcting mechanism. False
incoming data, such as air-column or
dome turbulence that scatters the incoming star image, is therefore entirely
eliminated.
The information received from the
168 sensors, the correc
tive calculations and the correction commands
to the 108 actuators are handled by
12 microcomputers under the overall command of a DEC Micro-VAX.
Corrections are performed every half
second, with a 10-second settling
time required after a major slew of
the telescope. One of the computers is
dedicated to maintaining a log of all
readings and subsequent actions, so
that if anything goes wrong, its data
can be analysed to isolate the problem.
An example would be where a wire
or actuator rod breaks. The computer
would sense an alignment problem,
send a corrective command, and fail
to see a response from the displacement sensors. Obviously a runaway
condition is then likely. Whilst such
conditions can be trapped by the software, by keeping an activity log, the
actual source of the problem can be
quickly identified.
Secondary mirrors
There are two interchangeable secondary mirrors that result in overall
focal ratios of f/15 and f/25. The f/15
secondary is 1.45 metres in diameter
and is intended for work in the visible
spectrum. The f/25 secondary is 51cm
in diameter and is designed for observation in the infrared region.
The f/15 secondary mirror was
ground and polished at the Lick
Observatory optical laboratories in
Santa Cruz, California, under the
guidance of master optician David
Hilyard and astronom
e r Joseph
Miller, who described it as the most
difficult grinding job they had ever
undertaken. The mirror is made of
Zerodur, is hyperboloidal in figure
and, because of the very small focal
ratio of the optics, is highly convex
(the radius of curvature is only 4.7
metres). As a result, special flexible
polishing laps had to be devised, and
progress constantly monitored with a
laser profilometer, which could detect
aberrations of the order of λ\2. After
final figuring, testing by more elaborate optical methods indicated a figure
of better than λ\15.
The finished mirror was shipped to
Hawaii on July 19th, 1991. The optical
Great care must be taken in polishing & figuring the mirror blanks & this is
done before they are hexagonised. Here an optical technician uses a laser
profilometer to check a mirror blank.
combination of the f/1.75 primary
and the secondary yield a final f/15
focus. This secondary will be used for
observations at visible wavelengths.
A further complication that occurred
during the polishing of this mirror was
its disturbance on the polishing table
during the San Francisco earthquake
in October 1989. Luckily no damage
was sustained and re-alignment was
successfully carried out.
The f/25 secondary is made of nickel-plated beryllium. It was figured at
the Lawrence Livermore National
Laboratory near San Francisco, tested
and finally plated with gold. It will
be used exclusively for work in the
infrared spectrum and has the ability
to be used as a “chopper”, mechanically moving to alternately provide a
view of the object being studied and
the background sky. In this way, sky
readings can be subtracted from “object + sky” readings to give an “object
only” output from the detectors.
Each secondary mirror is housed
in its own secondary support which
can be placed interchangeably forward of the prime focus as required.
Both supports have the same external
August 1993 9
This photo shows the complex support structure of the main mirror. Each
mirror segment is monitored & adjusted by the computer control system twice
every second.
shape as the main mirror mosaic to
minimise the effects of diffraction
and also to minimise the central obstruction. They block only 9% of the
incoming light.
Both secondaries will deliver their
light to either the Cassegrain focus
behind the primary mirror – the central hexagon being left out to provide
access to this focus – or via a flat ter-
tiary mirror placed in line with the
mechanical axis, and at 45 degrees to
the light path, to a focus at one of six
locations around the telescope. Two of
these locations pass through the axis
bearings to two Nasmyth platforms,
where bulky or heavy equipment can
be accommodated without affecting
the fine mechani
cal balance of the
system. The other four are for lighter
Table 1: Telescope Facilities on Mauna Kea
Facility
Size
Primary Use
University of Hawaii 24-inch Telescope #1
0.61m
Optical
University of Hawaii 24-inch Telescope #2
0.61m
Optical
University of Hawaii 88-inch Telescope
2.24m
Optical/Infrared
NASA Infrared Telescope Facility
3.0m
Infrared
Canada-France-Hawaii Telescope
3.6m
Optical/Infrared
United Kingdom Infrared Telescope
3.8m
Infrared
Carltech Sub-Millimetre Observatory
10.4m
Millimetre/sub-millimetre
James Clerk Maxwell Telescope
15m
Millimetre/sub-millimetre
W. M. Keck Telescope
10m
Optical/Infrared
Table 2: Facilities Planned Or Under Construction
Facility
Size
Primary Use
Second keck Telescope
10m
Optical/Infrared
VLBA Facility
Subaru Telescope
US-Canada-UK National Optical Telescope
Radio
8.3m
Optical/Infrared
8m
Optical/Infrared
Smithsonian 6-Antenna Array
Galileo National Telescope
10 Silicon Chip
Radio
3.5m
Optical/Infrared
instruments that can safely ride in the
tube itself.
In addition to standard observatory
instrumentation, five major instruments are being built specifically
for use on the Keck telescope to take
advantage of its unique capabilities.
They are:
(1). The Low-Resolution Imaging
Spectrograph (LRIS), a collimated array of four 2048 x 2048 CCDs imaging
an area of 6 by 8 arc-minutes at prime
focus. Used in the 0.4-1.0µm region of
the spectrum, its angular resolution is
0.15 arc-seconds.
(2). The High Resolution Echelle
Mosaic Spectrograph (HIRES). This
is similar in construction to the low
resolution spectrograph but the spectral resolution is 10 times higher and
it works in the 0.3-1.0µm region.
(3). The Long Wavelength Spectro
graph (LWS), a 96 x 96 BIB (Bumped
Indium Bond) array used in the
8-20µm region.
(4). The Near Infra-Red Camera
(NIRC). Covering the 1-5µm spectrum,
it uses a 256 x 256 indium antinomide
array with an angular resolution of
0.15 arc-seconds. It was developed
at Caltech.
(5). The Long Wavelength Infrared
Camera (LWIC) for use in the 8-14µm
spectrum. It uses a 20 x 64 BIB array
from Hughes and, depending on wavelength, the angular resolution is 0.08
to 0.32 arc-seconds.
On November 7th, 1991, the telescope was officially dedicated at a
ceremony at the summit. At this stage,
only nine mirrors were in place but
already the first official observation
and concept-proving run had been
made. The first image obtained was
a CCD image of the galaxy NGC 1232
(Arp 41) in Eridanus.
The results were as encouraging as
the design and construction team had
hoped, fully vindicating the optimism
they had shown in this radical new
telescope. The image showed detail
that had not been previously seen from
ground based telescopes, and was a
portent of what was to come once all
segments were in place and the telescope fully commissioned.
Although the warping harnesses
had not yet been fully adjusted, and
seeing was less than perfect, Airy
disc star images were obtained with
diameters of 0.61 arc-seconds at the
50% energy level, and 80% of the
light fell in a circle 1.6 arc-seconds
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August 1993 11
Table 3: W. M. Keck Telescope Specifications
Optical Design: Ritchey-Chretien
Primary Mirror
Secondary Mirror (f/25)
Effective aperture
8.2m
Figure
Convex hyperboloid
Maximum diameter
10.95m
Shape
Circular
Light-collecting area
75-76 sq.m
Diameter
0.51m
Limiting magnitude
±28
Radius of curvature
1.82m
Figure
Concave hyperboloid
Distance from primary
16.6m
Number of segments
36
Focus behind primary
4.54m
Radius of curvature
35m
Equivalent focal length
250m (f/25)
Focal ratio
1.75
Gap between segments
3mm
Site
Mauna Kea, HI
Total weight of glass
14.7 tonnes
Longitude
West 155 deg 28 min 3 sec
Position actuators
108 - 3 per segment
Latitude
North 19 deg 49 min 6 sec
Whiffletrees
108 - 3 per segment
Elevation of dome
4150m
Displacement sensors
168 - 6-12 per segment
Dome height
31m
Active-control
0.5 second cycle
Dome width
37m
Setting time after siew
10 seconds
Dome moving weight
635 tonnes
Dome air exchange
5 minute cycle
Observatory
Individual Segments
Number of aspheric types
6
Telescope mounting
Altazimuth
Number of each type
6
Max. telescope height
24.6m
Spares of each type on hand
1
Telescope moving weight
270 tonnes
Focal length tolerance
0.2mm
Project cost
$US94 million
Shape
Hexagonal
Construction time
7 years
Greatest diameter
1.8m
Project headquarters
Kamuela, HI
Thickness
75mm
Glass type
Schott Zerodur
Mean annual temperature
0°C
Mass
400kg
Average wind velocity
25km/h
Clear night per year
250
Environmental
Secondary Mirror (f/15)
Figure
Convex hyperboloid
Average relative humidity
Less than 10%
Shape
Circular
Sub-arc-second seeing
Greater than 50% of time
Diameter
1.45m
Radius of curvature
4.73m
Distance from primary
15.41m
Focus behind primary
2.5m
Equivalent focal length
150m (f/15)
across. These images were obtained
at the prime focus since the secondary
and tertiary mirrors had not yet been
installed. After these test images, the
nine mirror segments, already greater
in light collecting capacity than the
5- metre Hale telescope on Mount
Palomar, were removed for safety so
that work could continue on the as yet
unfinished support structure.
At this same November ceremony,
12 Silicon Chip
the ground was turned for a second,
identical telescope, the Keck II. If all
goes according to schedule, Keck II is
expected to be operational some time
in 1996. In October 1991, the Schott
Glassworks began delivery of the first
of the 42 1.9 metre blanks required for
the Keck II.
Used alone, the second telescope
will double the available observing
time. Just as important, the two tele
scopes, 85 metres apart, can potentially be used as an optical interferometer,
giving a light grasp equal to a single
14.1-metre mirror but with the resolving power of a mirror 85 metres in
diameter. In practice, however, this
theoretical resolving limit is unlikely
to be achieved but confidence has been
expressed that a resolution of better
than 0.01 arc-seconds is feasible. The
light collecting area of the two mir-
An optical technician monitors a diamond-edged circular saw as it cuts a
mirror blank to a hexagon. Thirty six of these hexagonal segments are used
in the Keck mirror & the gaps between them are less than 3mm.
rors will be greater than the world’s
current 10 largest optical telescopes
combined!
By early 1992, when 18 of the segments were in place, the telescope
already ranked as the largest optical
reflector. Work had been slowed
down by a snowstorm in November,
hampering access to the summit and
progress once there, but finally, on
April 14th, 1992, the last of the 36
segments was lowered into position.
Designer Jerry Nelson, project manager Jerry Smith, facilities manager
Ron Laub and Don Hall from CARA
were all present for the final mirror
positioning, the culmination of a 15year dream.
Although the telescope is officially
completed, shake-down engineering
tests, alignment, tracking and ironing
out the bugs inevitable in a project of
this size are continuing before it is
finally commissioned. The same can
be said of the fine tuning required to
optimise the new instruments to the
telescope.
This is expected to take about a year
and will be under the watchful eye of
operations director Peter Gillingham,
recently moved to Mauna Kea from
the Anglo-Australian Observatory at
Coonabarrabran, NSW. Most of the
problems encountered earlier in the
telescope pointing software seem to
have been solved but further work is
required to iron out troubles in the
segment active control computer.
From concept to completion, the
Keck telescope has taken nearly two
decades to come to fruition, during
which time many valuable technological lessons have been learned.
Its commissioning will have lasting
implications for astronomy. New horizons have been opened up to keep
researchers and theoretical astro
physicists occupied for years.
It also comes at a time when new
and exciting data is being returned
from the orbiting Hubble Space Tele
scope. Both telescopes have the same
limiting magnitude of about 28 but
they can work independently or in
concert to push the frontier of knowledge forward an order of magnitude
from anything that has gone before.
Hubble’s great strength is its superb
location; Keck’s is its massive light
collecting power. And Keck does it
at 1/16th the construction and operational costs!
Hard on the heels of the now proven
design concepts comes confirmation
that other telescopes of this kind are
to follow – from the US, Japan and
Europe. This is perhaps the greatest
contribution of its designers, builders
and the telescope itself – the heralding
SC
of a new era.
Acknowledgments
“Sky & Telescope” magazine;
CARA; Caltech; Itek Optical Systems; Summit & facility support
staff - especially Andy Pera
la,
Jerry Smith and Mary Beth Murrill.
August 1993 13
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
By DARREN & GARY YATES
Low-cost
colour video fader
Forget those messy edits on your VCR! This
project uses readily available components
& smoothly fades any composite PAL video
signal to black level to enhance your home
movies. It can also wipe left or right across
the screen for special effects.
Let’s face it – editing home movies
is not easy. Have you ever tried to
get your VCR to do a clean edit from
one scene to the next? It’s virtually
impossible unless you have one of the
top-of-the-line models.
Often, the only result you get is the
brief flash of a “snowy” screen as you
cut from one scene to the next. It not
only looks unprofessional and messy
but is annoying to look at as well.
This Colour Video Fader solves
that problem. It accepts any colour or
black-and-white composite PAL video
18 Silicon Chip
signal and can fade it smoothly down
to a black screen and back up again.
This makes it easy to fade one scene
to black, set your camcorder for the
next scene and then bring that scene
up from black to full brightness again.
Result – a professional transition from
one scene to the next.
Since no movie is complete these
days without some special FX (movie
lingo for “effects”), we’ve also added a
screen wipe facility. This allows you
to wipe the screen to black from leftto-right or from right-to-left. Again,
once the screen is black, you can make
your cut, move on to the next scene
and wipe the video back on again by
turning the control in the other direc
tion. What could be easier?
In addition to these features, the
Colour Video Fader also features an
external control input. This input is
for a future project that will allow you
to wipe a scene to black in over 50
different ways; eg, from top to bottom,
diagonally, disappearing squares, and
so on. This optional add-on project
will be described in SILICON CHIP in
a few month’s time.
By now you’re probably thinking,
“OK, so what expensive chips have
been used?” Well, we haven’t used
any. The circuit uses just two common
CMOS ICs, a few transistors and a
handful of other components.
Fading video signals
Before we dive straight into the
circuitry, let’s take a look at a typical
Colour burst signal
Immediately following the sync
pulse is the colour burst signal, which
is nominally 10 cycles of 4.43MHz
sinewave. This signal provides a
phase reference so that your TV can
decode the colour (or “chrominance”)
information in the video signal. (Note:
this signal does not appear in blackand-white TV systems).
Both of these signals are vital to
your TV set. If the horizontal sync
pulse disappears, your TV picture
will start to tear horizontally and the
picture will break up. And if the colour
burst signal disappears, then so will
the colour from your TV screen. No
amount of knob-twiddling on the front
of your TV will help if either of these
two signals has disappeared.
One signal that doesn’t appear in
Fig.1 but which is also vitally important is the field (or vertical) sync pulse.
This occurs once every 20ms and has a
250µs duration. It synchronises the TV
to the field rate – each time a vertical
sync pulse is received, the set begins
BLUE
RED
MAGENTA
GREEN
CYAN
WHITE
100%
YELLOW
video signal – one that we would like
to fade down to black.
To fade down the audio level, you
simply reduce the amplitude of the
audio signal and that’s about it. But
that’s not the case for a composite
video signal.
Fig.1 shows a typical PAL composite video signal from a colour bar
pattern generator. This waveform represents just one of the 625 horizontal
lines on the TV screen and has three
main features: (1) a line sync pulse;
(2) a colour burst signal; and (3) the
picture information (luminance &
chrominance).
The line sync (synchronisation)
pulse is used to signal the start of a
new line on the screen. This pulse
lasts for 5µs and occurs once for every
line. Since there are 625 lines on the
screen and they are updated 25 times
per second, the sync pulse frequency
is 15.625kHz (more commonly called
the horizontal line frequency).
In a colour TV receiver, the 625
lines are interlaced into two groups
or fields, each containing 312.5 lines.
Thus, one field consists of lines 1, 3,
5, 7, etc, while the other field consists
of lines 2, 4, 6, 8, etc. Each field is displayed alternately at a 50Hz rate and
this virtually eliminates the flicker
that would otherwise be apparent at
a 25Hz rate.
30%
BLACK
VIDEO SIGNAL
10-CYCLE
COLOUR
BURST
0%
LINE SYNC
PULSE
Fig.1: a typical PAL composite video signal from a colour bar pattern generator.
This waveform represents just one of the 625 horizontal lines on the TV screen
and has three main features: (1) a line sync pulse; (2) a 10-cycle colour burst
signal; and (3) the picture (or video) information.
scanning a new field.
The video component of the waveform follows the colour burst signal
and it is this that determines what
appears on the screen. In the case of the
waveform shown in Fig.1, the result
will be a set of vertical colour bars,
starting with white on the lefthand
side of the screen and going through
yellow, cyan, green, magenta, red, blue
and finally black on the righthand side.
The sync pulses ensure that all the
horizontal lines match up so that the
bars are vertically aligned.
If we reduce the video section of
the signal in amplitude, we reduce
the “brightness” of the display and
we can fade all the way to black.
However, we must leave the sync
pulse and colour burst signals at
their original amplitude otherwise
the picture will lose sync and colour
during the fade.
In practice, what we have to do is
reduce the amplitude of one part of the
waveform (the video information) and
keep the rest the same (sync pulse and
colour burst). This may sound difficult
but in the end it is fairly simple due
to the repetitive nature of a composite
video waveform.
The trick is to first extract the sync
pulse and colour burst signals from
the waveform, play around with the
video information that remains, and
then mix the sync pulse and colour
burst signals back in.
Block diagram
Block diagram Fig.2 shows the
basics of the circuit. As shown, the
incoming video signals are fed into a
The Colour Video Fader can smoothly fade a video signal from full brightness to
black & back up again, or can wipe left-to-right or right-to-left across the screen
as shown on the facing page. It uses only low cost parts.
August 1993 19
INPUT
VIDE0 +
SYNC
MIXER
Q2,Q3
Q1
SYNC +
COLOUR
BURST
ENABLE
IC1c
DC
CLAMPING
VIDEO
ENABLE
FADER
IC2a,IC1a
IC1b
VR1
VIDEO
BUFFER
VIDEO
AMPLIFIER
SYNC + CB ONLY
+10dB
Q4,Q5
VIDEO
ONLY
SYNC +
WIPE
GENERATOR
IC2b,IC2d,IC1d
D1,D2
buffer stage, after which the signal is
fed three ways:
(1). to a DC clamping stage (IC2a &
IC1a). This clamps the bottom of the
video signal to a steady DC voltage
regardless of the video amplitude. In
this case, it’s the bottom of the sync
pulses; ie, the level corresponding to
0% in Fig.1.
(2). to the sync and colour burst enable
circuitry (IC1c); and
(3). to the video enable circuitry.
The job of the sync and colour
burst enable circuitry is to allow just
the sync and colour burst signals to
pass through to the final mixer stage.
It blocks out all other video signals.
Conversely, the video enable circuit
only allows the picture information
to pass through and rejects the sync
and colour burst signals.
Once the composite video signal
has had the sync and colour burst
components stripped from it, it can
be manipulated in the fader stage (ie,
faded up or down). The signal is then
fed to the mixer stage which mixes the
sync and colour burst signals back in
to produce the modified composite
PAL signal. This signal is then fed to
your VCR.
At this stage, we haven’t mentioned
the sync and wipe generator circuit.
This part of the circuit is a bit more
SYNC +
COLOUR
BURST
ENABLE
IC1c
DC
CLAMPING
IC2a,IC1a
TO
MIXER
SYNC
SEPARATOR
TO
MIXER
VIA
FADER
VIDEO
ENABLE
IC2a
IC1b
D1,D2
IC1d
COLOUR
BURST
PULSE
GENERATOR
IC2b
VARIABLE
WIPE PULSE
MONOSTABLE
IC2d
EXTERNAL
INPUT
DRIVE
Fig.3: this expanded block diagram shows the sync & wipe generator
circuitry in greater detail. The output from the colour burst gating pulse
generator (IC2b) is used to trigger a variable wipe pulse monostable
(IC2d). Its output is ANDed with the pulses to the sync & colour burst
enable circuitry via diodes D1 and D2 & fed to the video enable switch.
20 Silicon Chip
OUTPUT
Fig.2: block diagram of
the Colour Video Fader.
The incoming composite
video signal is stripped
of sync & colour burst
signals before being
applied to the fader
section (VR1). After
fading, the sync & colour
burst signals are mixed
back in & the resulting
signal amplified to make
up for losses in the
circuit chain.
in
volved and needs another block
diagram to explain fully – see Fig.3.
The first thing to notice is that the
incoming signal from the video buffer
doesn’t go directly to the DC clamp but
via a sync separator. This separates
out the horizontal and vertical sync
pulses and generates positive-going
pulses which switch in the DC clamping circuit.
The output of the sync separator is
also fed to a colour burst gating pulse
generator (IC2b). This produces negative-going pulses about 7µs in length,
which cover the length of the colour
burst. The sync separator and colour
burst pulse generator outputs are then
ORed together and the resulting signal
fed to the sync and colour burst enable
circuitry. Thus, the sync and colour
burst enable circuit allows only the
colour burst and the sync signals to
pass through to the mixer.
The output from the colour burst
gating pulse generator is also used to
trigger a variable wipe pulse monostable (IC2d), which produces variable-length pulses. These pulses are
then ANDed with the pulses to the
sync and colour burst enable circuitry
via diodes D1 and D2 and fed to the
video enable switch. The outputs of
both enable circuits are then fed into
the video mixer as before.
Circuit diagram
Let’s now take a look at the complete circuit – see Fig.4. All the major
circuit elements depicted in the two
block diagrams can be directly related
to this diagram.
As shown, the incoming video
signal is AC-coupled to the base of
transistor Q1 via a 0.1µF capacitor.
The 82Ω resistor connecting the input
+5V
Q2
BC548
B
10k
VIDEO
IN
Q1
BC558
0.1
C
E
B
C
82
IC1b
4066
E
1.2k
1.2k
10k
C
B
14
3
Q4
BC548
4
470
1.5k
5
Q5
BC548
B
E 1.2k
FADE
VR1 1.5k
10k
0.1
Q6
BC558
B
6.8k
2.2k
C
E
100
680
IC1a
E
C
100
16VW
2.2k
150
VIDEO
OUT
470
1
13
100
16VW
+5V
1M
2
VR3
20k
1.2k
10
16VW
+5V
IC2a
4070
1
3
IC1c
1k
10
Q3
BC548
6.8k
B
11
2
47pF
12
C
E
10k
470
+5V
4.7k
75k
100pF
13
5
IC2b
6
6
4
270pF
EXTERNAL
INPUT
+5V
L TO R
EXTERNAL
WIPE
S1
IC2c
D1
1N914
B
4.7k
11
E
C
VIEWED FROM
BELOW
7
I GO
7
9
4.7k
100k
12
IC1d 8
14
SET BLACK LEVEL
MAY NEED ADJUSTMENT
8
WIPE
VR2
500k
LIN
D2
1N914
IC2d
10
D3
1N4004
9
9VDC
300mA
PLUG-PACK
100
16VW
IN
7805
GND
OUT
100
16VW
+5V
0.1
0.1
5.6k
R TO L
COLOUR VIDEO FADER
Fig.4: the various elements in the circuit diagram can be directly related to the
two block diagrams. IC2a functions as a sync separator, its output switching
high for the duration of each sync pulse. The video signal (minus the sync &
colour burst signals) passes through IC1b & is faded by VR1. The signal is then
buffered by Q4 & mixed with the sync & colour burst signals from IC1c & Q3.
to ground provides the correct terminating impedance so that “ghost” or
reflected signals do not occur.
Transistors Q1 & Q2 form the
buffer stage. Because a PNP/NPN
arrangement is used, the required
level of input impedance has been
achieved with negligible voltage difference between the base of Q1 and
the emitter of Q2. This is important
for the correct functioning of the DC
clamping circuitry.
From the emitter of Q2, the signal
path is split three ways, as mentioned
before. First, it goes to IC2a via a lowpass filter consisting of a 1kΩ resistor
and a 47pF capacitor. This reduces the
amplitude of the colour burst signal
so that it doesn’t cause IC2a to false
trigger. IC2a is an exclusive-OR gate
and is used here as a very high gain
ampli
fier/comparator. By tying one
input to the supply rail, we have also
made it work as an inverter.
IC2a and CMOS analog switch IC1a
together form the DC clamping circuit.
Q2’s emitter is set to +2.7V by virtue
of the bias voltage applied to the base
of Q1. A video signal applied to the
base of Q1 will swing high and low
but each time a sync pulse arrives it
will cause IC2a to switch its output
high. This will cause CMOS switch
IC1a to close and thus “clamp” the
bottom of the sync pulse to +2.7V.
This happens for every sync pulse
that arrives at the base of Q1. Thus,
the incoming video signal at the base
of Q1 (and therefore at the emitter of
Q2) can only swing between +2.7V
and +3.7V (approx.).
At the same time, IC2a effectively
August 1993 21
10-CYCLE
COLOUR
BURST
BLUE
RED
LINE SYNC
PULSE
MAGENTA
GREEN
CYAN
YELLOW
WHITE
100%
30%
BLACK
0%
+5V
PIN 3
IC2a
0V
PIN 4
IC2b
produce the wipe pulse. IC2d triggers
on the rising edge of the pulse from
IC2b, as shown in Fig.5, and its output
pulse length is set by VR2. By varying
VR2, we can vary the pulse length from
almost zero to 64µs (ie, the length of a
screen line).
Because IC2d is triggered once for
every line, we can thus create the effect
of a wipe from one side of the screen
to the other.
In order to eliminate sync and colour burst signals from the video signal
we wish to modify, IC2c is used to
invert the signal at pin 8 of IC1d. Its
output at pin 11 is then ANDed with
the wipe control signal at pin 10 of
IC2d, using diodes D1 and D2, and the
resulting output applied to the control
input of IC1b.
Typical waveforms
PIN 8
IC1d
PIN 10
IC2d
WITH
PIN 8 = GND
PIN 11
IC2c
PIN 5
IC1b
Fig.5: this diagram shows the waveforms produced at various points in the sync
& wipe control circuitry. The width of the screen wipe is controlled by the pulse
width on pin 10 of IC2d & this in turn is set by VR2.
functions as a sync separator, its output switching high for the duration of
each sync pulse. These sync pulses
are used to trigger the colour burst
monostable, made from IC2b.
IC2b is triggered by the falling edge
of the sync pulse appearing at pin 3
of IC2a, so that the colour burst pulse
follows the sync pulse. This monostable produces a brief negative-going
pulse about 7µs long, as set by the
RC time constant on its pin 5 input
– see Fig.5.
The colour burst pulses are applied
to the control input (pin 6) of IC1d,
while the sync pulses are applied to
pin 9. Its output (pin 8) is high for the
combined duration of the sync and
colour burst pulses, and is low while
ever video information is present.
22 Silicon Chip
The output at pin 8 is used to control
IC1c which is another CMOS switch.
Thus, by feeding in the control signal
from IC1d, only the sync and colour
burst signals pass through IC1c, while
the picture information is eliminated
(ie, the video is blanked).
The output from the colour burst
gating pulse monostable (IC2b) is also
used to trigger monostable IC2d to
CAPACITOR CODES
❏
❏
❏
❏
❏
Value
0.1µF
220pF
100pF
47pF
IEC Code
100n
220p
100p
47p
EIA Code
104
221
101
47
Fig.5 shows the results of these
machinations. The waveform applied to pin 5 of IC1b begins with a
low-going pulse that covers the sync
pulse and colour burst signals. This
is then followed by a variable length
positive-going pulse that is controlled
by VR2. As a result, IC1b blanks out
all of the sync pulse and colour burst
signals and only passes video information while the output of the diode
AND gate is high.
Thus, if VR2 is set so that each
positive pulse covers only half the
line length, then only that half of the
picture will be shown while the other
half of the screen will be blacked out.
In other words, the amount of picture
shown is determined by the length
of the positive pulse and this can be
continuously varied using VR2.
Switch S1 controls the wipe direction. If pin 8 of IC2d is pulled high,
then the black is wiped from left to
right (L-R). Conversely, if pin 8 is
pulled low, the black is wiped from
right to left (R-L).
S1 also makes another interesting
effect possible. If the WIPE potenti
ometer (VR2) is turned fully in one
direction, the picture can be instantaneously flicked on or off using S1. This
facility is much more versatile than
it may first appear at first sight, as it
allows us to create a myriad of wipes
including diamonds, centre-splits, diagonal wipes and more using a plug-in
external controller.
At this stage, we have produced
the wipe function by modifying the
control signal to pin 5 of IC1b. What
POWER
SOCKET
EXTERNAL
INPUT
VIDEO
IN
VIDEO
OUT
11
10
4.7k
1.5k
1.2k
0.1
10k
6.8k
5.6k
7
6
100uF
680
Q6
150
9
10
4
100uF
470
5
2
3
▼
S1
remains of the video signal is now
fed to a resistive divider network that
includes 10kΩ potentiometer VR1.
This is the FADE control and it allows
the picture to be smoothly varied from
full brightness at one extreme to full
Q3
8
SEE TEXT
Above: view inside the completed prototype. Keep the
wiring neat & tidy & use PC stakes to terminate all wiring
connections to the PC board.
Fig.6 (right): be careful when installing the transistors on
the PC board, as both NPN & PNP types are used. The 7805
3-terminal regulator is mounted with its metal tab towards
the adjacent 10µF capacitor.
470W
100uF
0.1
100uF
5
270pF
75k
6
7
8
Q5
2.2k
10uF
7805
D3
4
1
4.7k
0.1
VR3
IC2
4070
100pF
10k
100
1k
2.2k
Q4
6.8k
IC1
4066
1
47pF
11
1.2k
1M
82
470
Q2
D1
1.5k
1.2k
0.1
1
2 100k
3
D2
10k
4.7k
1k
Q1
9
black at the other extreme.
The video signal from VR1’s wiper
is fed to buffer stage Q4, after which
it is mixed with the sync and colour
burst information coming from IC1c
and buffer stage Q3. The combined
1
VR1
VR2
composite video signal is then fed to
transistors Q5 and Q6 which together
act as a wide bandwidth amplifier
with a gain of about 3.2. This gain
compensates for any losses in the
buffer stages and CMOS switches and
RESISTOR COLOUR CODES
❏
No.
❏ 1
❏ 1
❏ 1
❏ 1
❏ 1
❏ 4
❏ 2
❏ 1
❏ 3
❏ 1
❏ 2
❏ 2
❏ 3
❏ 1
❏ 3
❏ 1
❏ 1
❏ 1
Value
1MΩ
100kΩ
75kΩ
22kΩ
12kΩ
10kΩ
6.8kΩ
5.6kΩ
4.7kΩ
2.2kΩ
1.5kΩ
1.2kΩ
1kΩ
680Ω
470Ω
220Ω
150Ω
82Ω
4-Band Code (1%)
brown black green brown
brown black yellow brown
violet green orange brown
red red orange brown
brown red orange brown
brown black orange brown
blue grey red brown
green blue red brown
yellow violet red brown
red red red brown
brown green red brown
brown red red brown
brown black red brown
blue grey brown brown
yellow violet brown brown
red red brown brown
brown green brown brown
grey red black brown
5-Band Code (1%)
brown black black yellow brown
brown black black orange brown
violet green black red brown
red red black red brown
brown red black red brown
brown black black red brown
blue grey black brown brown
green blue black brown brown
yellow violet black brown brown
red red black brown brown
brown green black brown brown
brown red black brown brown
brown black black brown brown
blue grey black black brown
yellow violet black black brown
red red black black brown
brown green black black brown
grey red black gold brown
August 1993 23
is set by the 2.2kΩ and 680Ω resistors.
The result is that the overall peak
amplitude of the video signal is the
same at the output as at the input
(provided that the signal has not been
faded). This video output can then be
fed into your VCR which provides the
output termination.
Power for the Colour Video Fader is
derived from a 9V DC plugpack supply.
PARTS LIST
1 PC board, code 02107931,
103 x 57mm
1 plastic case, 130 x 68 x 41mm
2 self-adhesive labels
1 single-pole 3-position toggle
switch
3 panel-mount RCA sockets
1 2.5mm chassis-mount DC
power socket
1 10kΩ linear pot. (VR1)
1 500kΩ linear pot. (VR2)
2 knobs to suit
15 PC stakes
4 rubber feet
Semiconductors
1 4066 quad analog switch (IC1)
1 4070 quad 2-input OR gate
(IC2)
2 BC558 PNP transistors (Q1,Q6)
4 BC548 NPN transistors
(Q2-Q5)
2 1N914 signal diodes (D1,D2)
1 1N4004 silicon diode (D3)
1 7805 3-terminal regulator
Capacitors
4 100µF PC-mount electrolytic
1 10µF PC-mount electrolytic
4 0.1µF MKT polyester
1 220pF MKT polyester
1 100pF ceramic
1 47pF ceramic
Make sure that all polarised parts are correctly oriented when installing them
on the PC board. Pin 1 of each IC is adjacent to a notch or dot at one end of the
plastic body.
Diode D3 provides reverse polarity
protection, while a 7805 3-terminal
regulator is used to derive a regulated
+5V supply rail for the circuit. The
100µF and 0.1µF capacitors fitted to
the input and output terminal of the
regulator provide filtering and supply
decoupling.
Construction
If you’ve had trouble following the
circuit, don’t worry – construction is a
cinch. That’s because most of the parts
are mounted on a single PC board (code
02107931) and the external wiring is
straightforward. Fig.6 shows the parts
layout on the PC board.
Begin the assembly by installing PC
stakes at all external wiring points,
then install the wire links and resistors. The accompanying table shows
the resistor colour codes but it’s also
a good idea to check them on a digital
multimeter just to make sure (the colours on some resistors can be difficult
to decipher). Note that two of the resistors are installed end-on (near IC2)
to conserve board space.
Once the resistors are in, the remaining parts can be installed on the
board. These include the transistors,
diodes, capacitors, the two ICs and the
3-terminal regulator. Be sure to install
the correct part at each location and
make sure that all polarised parts are
correctly oriented. In particular, make
sure that you don’t get the transistors
mixed up, as both NPN and PNP types
are used in the circuit.
Take care also with the orientation
of the 3-terminal regular. It should be
installed with its metal tab towards
the centre of the board. This done, the
completed board should be carefully
checked for missed solder joints and
solder splashes. A little time spent
Resistors (0.25W, 1%)
1 1MΩ
1 2.2kΩ
1 100kΩ
2 1.5kΩ
1 75kΩ
2 1.2kΩ
1 22kΩ
3 1kΩ
1 12kΩ
1 680Ω
4 10kΩ
3 470Ω
2 6.8kΩ
1 220Ω
1 5.6kΩ
1 150Ω
3 4.7kΩ
1 82Ω
Miscellaneous
Light-duty hook-up wire, tinned
copper wire for links, machine
screws & nuts.
24 Silicon Chip
Fig.7: check your etched PC board against this full-size artwork before
mounting any of the parts.
COLOUR
VIDEO FADER
L➙R
EXT.
R➙L
WIPE
DIRECTION
FADE
WIPE
+
VIDEO OUT
VIDEO IN
EXTERNAL
INPUT
9VDC
IN
Fig.8: these full-size artworks can be used as drilling templates for the case.
checking at this stage can save a lot
of frustration later on.
The assembled PC board is housed
inside a standard plastic case measuring 130 x 68 x 41mm. This will have to
be drilled to accept the PC board and
the various hardware items. Before
drilling, attach the front and side panel
labels to the case so that they can be
used as drilling templates.
The various hardware items can
now be installed in the case and the
wiring completed as shown in Fig.6.
The connections to the front panel
components are run using light-duty
hook-up wire, while the power and
RCA socket connections are run using
light-duty figure-8 cable.
Once all of the connections have
been made, the PC board can be
secured to the bottom of the case
using machine screws and nuts, with
additional nuts used as spacers. Complete the construction by fitting four
self-adhesive rubber feet to the bottom
of the case.
is correct, check the current consumption by connecting your multimeter
in series with the positive supply rail
between the DC power socket and the
PC board – you should get a reading
of about 50-60mA.
Now for the big test – you’ll need
either two VCRs or a camcorder and a
VCR. The Colour Video Fader is wired
into circuit as follows:
(1). Connect the VIDEO OUT from
the camcorder (or one of the VCRs) to
the VIDEO IN of the Colour Video
Fader.
(2). Connect a lead from the VIDEO
OUT of the Colour Video Fader to
the VIDEO IN on your VCR (note:
if you are using two VCRs, this
connection goes to the VIDEO IN
of the second machine).
(3). Set your camcorder or first
VCR to either view a scene or replay an existing tape. The second
VCR should be set to AUX IN or
AU and the TV connected to its
RF OUT socket.
(4). Rotate the FADE and WIPE controls fully clockwise, and set the
WIPE DIRECTION switch to R-L.
This sets the fader to maximum
luminance and the wipe function
to show a full picture (note: if the
screen is black, flick the switch
to the L-R position. If the picture
now appears, the switch is upside
down).
The FADE and WIPE controls
can now be varied to check
that they operate correctly. If
everything is OK, set the FADE
control to full brightness and set
the WIPE control for half-picture/
half black. This done, flick the switch
to its alternate setting and check that
the picture and black areas of the
screen are immediately transposed.
Finally, most camcorders and VCRs
have RCA sockets for their video and
audio outputs but some older model
VCRs have a BNC socket for their
VIDEO OUT connection. If your VCR
has a BNC socket, then it’s simply a
matter of purchasing a BNC plug-toSC
RCA socket converter.
Testing
To test the unit, first apply power
and check for +5V on pin 14 of both
ICs. If the reading is 0V, check the
plugpack polarity – it’s probably reversed. Assuming that the supply rail
The external input accepts signals from an external control unit to create a
myriad of fancy wipes. This external controller will appear in a future issue.
August 1993 25
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.
Low-cost
isolation amplifier
It is often necessary to
provide electrical isolation
between one part of a circuit
and another either simply to
AC
INPUT
remove earthing problems or
because one part of the circuit is at a different voltage
potential to the other. This
is a common requirement in
switchmode power supplies,
public address systems and
when connecting transducers
to industrial equipment.
This circuit will accept a
signal of ±1V and provide
the same signal (inverted) at the
output with 0.01% linearity and
7500VAC isolation. Bandwidth is
about 100kHz.
The circuit is based on the IL300
linear optocoupler (IC3). This IC
comprises one infrared LED and two
photodiodes. One photodiode is on the
isolated side of the package and the
second photodiode is on the non-isolated side. The two photodiodes are
manufactured to match within 0.01%
linearity so that the output can closely
match the signal applied at the input
LED.
Feedback is applied using the
second photodiode to monitor the received light from the LED. This means
that the signal across the isolated photodiode is almost the same as the signal
across the diode in the feedback path.
IC1 receives the applied signal
which is divided by two so that the
resulting signal is ±0.5V peak-to-peak.
IC1 is biased on due to diode D1 which
applies -0.7V to the inverting input at
pin 2. The resulting output at pin 6 of
IC1 powers the LED in IC3 via a 100Ω
resistor. Since the LED is always biased
on with no signal applied, a negative
signal can be applied to IC1 without
the LED turning off.
The feedback from the non-isolated
photodiode connects to the inverting
input of IC1. The second and isolated
photodiode at pins 6 and 5 of IC3
28 Silicon Chip
+15V
22pF
IC3
IL300
+12V
3
27k
27k
2
IC1
LF351
4
6
100
2
5
220pF
+1.4V
1
10
33k
10
D1
IN4148
15k
7
3
-12V
-0.7V
+15V
6
4
7
3
56k
15k
D2
1N4148
3
6
IC2
LF351
4
AC
OUTPUT
-15V
D3
1N4148
-12V
INPUT
connects to op amp IC2. A +1.4V
bias voltage set by diodes D2 and D3
offsets the bias initially produced by
the biased LED. The 56kΩ resistor
across the negative feedback path of
IC2 converts the current output from
the photodiode to a voltage.
Note that to obtain the required
voltage isolation, the power supplies
for IC1 and the non-isolated side of
IC3 must be completely separate from
Low distortion
oscillator
Here is a low distortion oscillator
which uses only a single variable
resistor to change the frequency
over a 3:1 range. Thus the circuit
has an advantage over the Wien
bridge oscillator where two elements have to be changed to alter
the frequency.
IC1a functions as a unity gain
inverting amplifier which is fed
from the output of IC1b. IC1b is
connected as a notch filter with
capacitors C1 & C2 and resistors
R1, R2 & R3 forming a “T” filter
section across the feedback and
output terminals of the op amp. To
maintain oscillation, a feedback signal from IC1a is applied to the filter
ISOLATED OUTPUT
the power for IC2 and the isolated
side of IC3. You can use batteries or
separate transformer power supplies to
obtain this isolation. When designing
a PC board, make sure that there are
no tracks run down the centre of IC3
and maintain adequate separation
between the isolated and non-isolated
PC tracks.
John Clarke,
SILICON CHIP.
via a 100kΩ resistor. The inverted
sinewave signal at the output of
IC1a is clipped to 7V peak to peak
using zener diodes ZD1 and ZD2.
This sets the sinewave output level.
Assuming C1 = C2, the frequency of
oscillation is set by the equation: F
= 1/2πC1√R3.(R1+R2).
If C1 & C2 are 560pF, the frequency can be set to any value between
4.7kHz and 15.6kHz. Other values
of C1 can be selected to provide
different frequency ranges. The
maximum oscillation frequency is
limited to about 20kHz using the
LF353 or TL072 op amps. The lowest operating frequency is limited
only by the capacitor size. Distortion of the sine wave is about 0.3%.
John Clarke,
SILICON CHIP.
+5V
100k
.01
100k
+5V
4.7k
4
Q1
BC548
3
V1
2xBAW62
1M
D1
2
D2
10k
1
IC1a
TLO74
11
6
IC1b
5
7
.01
IC2a
74C14
1
16
14
6
2
3
5
7
J
CK
Q
10k
1
4027
KR
S
-5V
INPUTS
IC3a
4
TO DIGITAL
MULTIMETER
7
100k
.01
100k
+5V
+5V
12
V2
2xBAW62
1M
D3
13
D4
10k
14
IC1d
IC1c
10
8
0.1
11
11
IC2f
13
12
13
13
10
10
J
CK
R
IC3b
Q
KS
9
Phase adapter for
digital multimeters
I am often required to construct
a Bode plot for a particular circuit,
requiring a log-magnitude and phase
response. Finding the gain is usually
pretty simple but the measurement
of phase can often be difficult. The
circuit presented here measures the
phase difference between two signals,
and displays the result in degrees on
a digital multimeter.
Essentially, the circuit consists of
two analog to digital converters, whose
output is “mixed” in a T-type flipflop.
The advantage of this technique over
the more usual XOR gate, is that both
the magnitude of the phase and its
sign (either leading or lagging) can be
measured. When one signal is leading
the other, the relevant flipflop will be
toggling, whilst the other output will
be high. Swapping the inputs reverses
this process.
Each input is attenuated and
clipped before being buffered and
amplified by 10 (IC1), then converted
into a digital signal by Schmitt inverters IC2a & IC2f. The operation of
the circuit is fairly self-explanatory,
with the multimeter measuring the
average value of the digital waveform
appearing between the outputs of the
flipflops (IC3a & IC3b).
In practice, the multimeter is set
to the 2mA range, so a reading of
say, +0.163 would correspond to a
10k
R3
330k
10k
+15V
2
3
7
6
IC1a
4
4.7k
-15V
C1
TL072
LF353
4.7k
C2
R1
10k
100k
R2
1k
ZD1
6.8V
ZD2
6.8V
5
220k
15 10k
Q2
BC548
8
phase measurement of +163°. Measurement of phase difference using an
oscilloscope is usually accurate to
around ±5° whereas this adapter can
display to ±1°. Note that this is the
phase resolution and is not a claim
for accuracy which will depend on
calibration.
In order to utilise the adapter, it
must be calibrated. To do this, first
set VR1 to its maximum resistance
and adjust VR2 so that the multimeter
reads the desired value (as calculated
from an oscilloscope). This done, swap
the input probes and adjust VR1 for
the same magnitude but different sign;
eg, if the first reading was adjusted to
+0.045, then adjust VR1 for a display
of -0.045mA. It should be noted here
that a phase difference of ±180° will
actually produce a reading of 0.000
because of the combination technique
used with the flipflop.
The prototype circuit was constructed on Veroboard and powered from a
9V battery driving a 555 charge-pump
oscillator to provide the -5V rail.
Banana plugs spaced at 19mm were
used to provide an easy interface to
the multimeter.
Steven Merrifield,
Heidelberg, Vic. ($30)
Handy hint
6
IC1b
VR1
10k
12
9
VR2
10k
7
SINE
OUTPUT
This low distortion sinewave oscillator uses notch filter IC1b to
drive unity gain inverting amplifier IC1a. Capacitors C1 & C2 &
resistors R1, R2 & R3 form a “T” filter section across the feedback
& output terminals of IC1b.
Quite often, projects and alarms
use pulsating piezo beepers. Elaborate
circuits can be built just to pulse the
beeper or, if you want, you can use a
pulsing beeper. Try connecting a continuous tone beeper in series with a
flashing LED – it works.
R. Barham,
Cairns, Qld. ($5)
August 1993 29
A microprocessor
based sidereal clock
Are you an amateur astronomer who needs to
know the position of the stars in the sky? If so,
you need a sidereal clock. This microprocessor
controlled clock has two 6-digit displays which
show sidereal time & local or universal time.
By JOHN WESTERN
A sidereal clock measures time
relative to the stars as opposed to a
normal clock which measures time
relative to the Sun. A star’s position
relative to the Earth is measured in
sidereal days. A sidereal day is the
time taken for the Earth to spin once
on its axis relative to the stars. This
is about four minutes shorter than a
solar day. The ratio, as listed in “The
Astronomical Almanac” is a factor
of 1.00273790934, accurate to 12
decimal places.
This clock has two displays: the
left-hand display indi
cates sidereal
time while the right-hand display can
display universal or local time. Each
mode is referenced to a common temperature controlled crystal oscillator.
30 Silicon Chip
Five keys on the front panel give
universal/local time selection, display
brightness, time setting and regulation
(ie, setting the long-term accuracy of
the clock). The clock can be set to
provide a tone on the minute for either
universal or sidereal time.
Circuit description
The circuit is based on a Z80C
microprocessor running at 4MHz,
together with a 6116 RAM, a 27C32
EPROM, an 82C55 PIO chip, two 7447
display drivers and 12 7-segment LED
displays as the other major components – see Fig.1 & Fig.2. The circuit
is divided among three PC boards,
one for the CPU, one for the 12-digit
display and one for the temperature
controlled oscillator – see Fig.3.
The CPU board (Fig.1) provides the
functions of a frequency divider, a
power-off detector, a reset circuit, an
address decoder and the power supply.
A 4020 14-stage binary counter, U6,
divides the 4MHz clock by 29 (512)
to give a frequency of 7812.5Hz. This
is then used to interrupt the Z80C on
its NMI input (pin 17, U1). The correct universal time is determined by
counting to a figure close to 7813 for
each second that passes.
Reference divider numbers
In fact, the division process is a little
more complex because if the clock is
to keep accurate time for a long period,
the precise division factor can only
be determined by trial and error over
a period which may span weeks or
months. This design allows the user
to actually program in the division
numbers.
There are four division numbers
for universal time and these are designated as U1, U2, U3 and U4. U1 is
the division number used at the end
of each second; U2 is used at the last
second of each minute; U3 is used at
the last second of each hour; and U4
is used for the last second of each 24hour day. In this fashion, a change in
the value of U4 will allow the accuracy
of the clock to be altered by one part
in 675 million.
The sidereal division factors are
designated as S1, S2, S3 and S4 and
these are used in the same way as the
division factors for universal time. To
keep track of sidereal time, the clock
simply subtracts the value S1 from U1,
S2 from U2 and so on. The numbers are
calculated from the measured timing
error using the Basic program accompanying this article. The measured
timing error is calculated by reference
to a precise clock such as Telecom’s
time service or Radio VNG.
Ultimately, the reference numbers
are stored in RAM when they are fed
via the keypad buttons on the front
panel. The stored program in the
EPROM then uses these numbers for
correct time keeping.
Supply monitoring
U7E, a Schmitt inverter, is used to
monitor the +12V supply and whenever this is present, its output at pin
10 is low. When the +12V supply is
removed, such as when the clock is in
transit or not being used, pin 10 of U7E
pulls PC3 of the 82C55 high (pin 17,
U2). The Z80C then sets all the ports of
the 82C55 to the input condition and
this prevents current being sourced to
the display board from the stand-by
battery BT1.
Thus, the oscillator and CPU boards
keep functioning but the display board
is effectively disabled. Even so, the
time for which the stand-by battery
can keep the clock going is limited to
a few hours at most. This is because
the current drawn by the oscillator
heater is fairly substantial at around
250 milliamps.
U5 is a 74HC138 3-to-8 line decoder. It monitors the A12, A13 & A14
address lines which are used to select
memory blocks of 4096 bytes. The
EPROM is located at address 0000H,
the RAM at address 1000H, the 82C55
at address 2000H and the keyboard
beeper at address 3000H.
The power-on reset circuit is based
on Schmitt inverter stages U7a and
U7b. When power is first applied, C1
charges to +5V via R1. Schmitt trigger
inverter U7a detects the transition
from low to high on pin 1. Its output
at pin 2 then goes low and resets the
This view inside the completed prototype shows how the CPU board, display
board & the oscillator (inside small box) fit together inside the case. Note that
the piezo buzzer is mounted on the solder side of the display board, while 5V
regulator U8 is heatsinked to the rear panel.
The display board accommodates two groups of LED displays plus the five
pushbutton switches. One group of displays show sidereal time, while the other
group shows either local or UTC time.
82C55 (U2) and the 4020 (U6). At the
same time, U7b inverts this signal to
reset the Z80C (U1).
Clock signal
The 4MHz clock signal for the CPU
board is generated on the oscillator
board and appears on pin 5 of JP3.
Inverter U7d buffers and squares up
the signal which is then applied to the
Z80C and the 4020.
Power for the clock can be supplied from a 12V battery or a 12V 1A
DC plugpack. Diode D1 protects the
circuitry from reverse polarity while
zener diode D5 prevents voltage spikes
from interfering with or damaging the
circuit. The 12VDC is then applied
to +5V regulators U8 and U9. They
provide separate +5V supplies to the
display and CPU boards. If the +12V
supply is not present, diodes D2
and D3 allow the CPU and oscillator
boards to continue functioning from
the battery.
Ports PA0-PA5 and PB0-PB7 on the
82C55 peripheral interface are config
ured as outputs and they drive the
7447 7-segment decoder drivers (U1
& U2) on the display board.
Ports PC0-PC3 are configured as
inputs to monitor the power-off detector (PC3) and the keyboard matrix
(PC0-PC2) on the front panel. Ports
PC4-PC7 are configured as outputs;
PC4 and PC5 drive the keyboard matrix
August 1993 31
PARTS LIST
CPU board
1 L-shaped double-sided PC
board
1 9V battery & snap connector
(BT1)
1 14-pin IC socket
2 16-pin IC sockets
1 24-pin IC socket
1 28-pin IC socket
2 40-pin IC sockets (see text)
Semiconductors
1 Z80C microprocessor (U1)
1 82C55 programmable interface
(U2)
1 6116 static RAM (U3)
1 27C32 or 27C64 programmed
EPROM (U4)
1 74HC138 decoder (U5)
1 4020 14-stage binary counter
(U6)
1 74HC14 hex Schmitt trigger (U7)
2 7805 3-terminal regulator (U8,
U9)
1 1N5404 rectifier diode (D1)
2 1N4001 rectifier diodes (D2,D3)
1 1N4733 5V zener diode (D4)
1 1N4746 18V zener diode (D5)
Capacitors
1 220µF 25VW electrolytic
1 100µF 25VW electrolytic
2 1µF 25VW electrolytic
6 0.1µF 63VW monolithic ceramic
Resistors (1%, 0.25W)
1 22kΩ
1 5.1kΩ
8 10kΩ
1 330Ω
Oscillator PC board
1 PC board,
1 4MHz crystal
1 1mH inductor
1 brass block (see Fig.7)
Semiconductors
1 LM358 dual op amp (U1)
1 LM334 current source (U2)
1 78L05 3-terminal regulator (U3)
and PC7 indicates whether the righthand display is showing universal or
local time.
Display board
The display board accommodates
the 12 7-segment displays, the key32 Silicon Chip
2 2N5485 N-channel FETs (Q1,Q2)
1 TIP31 NPN transistor (Q3)
Capacitors
2 0.1µF 63VW monolithic ceramic
1 68pF ceramic
2 27pF ceramic
Resistors (1%, 0.25W)
1 10MΩ
3 10kΩ
1 1MΩ
1 8.2kΩ
2 100kΩ
1 1kΩ
1 18kΩ
1 220Ω
Display board
1 double-sided PC board
1 piezo beeper (Tandy Cat. 273065)
5 panel switches (E.S.Ruben Cat
RF19 3.14001.006)
Semiconductors
12 TIL312 common anode LED
displays (DIS1 to DIS12)
2 7447 decoder/drivers (U1,U2)
1 555 timer (U3)
10 BC548 NPN transistors
(Q1,Q3,Q5,Q7,Q9,Q11,
Q13-Q16)
6 BC337 NPN transistors
(Q2,Q4,Q6,Q8,Q10,Q12)
2 1N4148 signal diodes (D1,D2)
Capacitors
1 10µF 35VW tantalum
2 0.47µF 16VW electrolytic
3 0.1µF 63VW monolithic
Resistors
6 10kΩ
6 4.7kΩ
1 3.9kΩ
16 27Ω
Miscellaneous
1 3AG 1A slow blow fuse
1 in-line 3AG fuseholder
1 can Electrolube nickel screening
paint (DSE N-11138)
2 RF suppression beads (DSE
R-5425)
board switch matrix, a beeper, a pulse
detector and driv
ers for the heater
on indicator and the universal/local
indicator – see Fig.2.
The displays are multiplexed two at
a time. The Z80 feeds a BCD number
via the 82C55 to the two 7447 decoder
Fig.1 (right): the CPU board is based
on a Z80C microprocessor (U1)
running at 4MHz, together with a
6116 RAM (U3), a 27C32 EPROM
(U4) & an 82C55 PIO chip (U2). It acts
as a frequency divider, a power-off
detector, a reset circuit & an address
decoder.
drivers, U1 & U2. The appropriate digits (say DIS1 & DIS7) are then enabled
by turning on one of the six Darlington
pairs (Q1 & Q2). The process is then
repeated for the other five pairs of
digits. The brightness of the display
is changed by reducing the on time
for each digit, via the Z80C.
The keyboard matrix is scanned by
taking ports PC4 or PC5 low and then
reading the condition of ports PC0PC2. If one of the switches has been
pressed, then one of ports PC0-PC2
will be low. Switch debouncing is
achieved via the software. Each time
a key is pressed, the beeper sounds.
A CPU write or read to any address in
the range 3000h-3FFFh causes pin 12
of U5 (74C138) to go low momentarily
and trigger 555 timer U3, which drives
the piezoelectric beeper.
The decimal points of displays DIS7
and DIS12 are used as indicators.
The decimal point of DIS7 indicates
when the oscillator heater is on. This
decimal point is driven by transistor
Q13 which is turned on by the “heater
output” (HO) line from the oscillator
board.
The decimal point of DIS12 indicates whether universal or local time
is being displayed on the right-hand
6-digit display. This same decimal
point also has the function of indicating that the power has been off. If
the power goes off, the decimal point
begins flashing. It is driven by transistor Q14 which is turned on by the PC7
line from the 82C55.
Diodes D13 and D14, together with
transistors Q15 and Q16, form a missing pulse detector. This is used to disable the displays if the microprocessor
stops running normally. This prevents
a particular display from being provided with a continuous high current.
The pulse detector monitors the 5V
pulses on the O1 line from the CPU
board. With pulses normally present,
Q15 will be on and Q16 will be off so
that pin 4 on each of the 7447 decoder/
drivers will be high. If the pulses on
+5V FROM U8
JP2
VCC
R5
330
9
R3
10k
R4
10k
16
8
16
10
CLK
U6
4020
25
U7c
74HC14
12
Q9
14
5
8
R1
22k
NMI
11
U7a
U7b
2
1
4
3
26
RESET
30
C1
100
A2
33
C8
0.1
C9
0.1
39
HO 4
40
GND 3
1
+9V 2
2
+12V 1
32
D3
31
D4
30
D5
29
D6
28
D7
27
A12
A11
RD
A13
WR
D3
PC4
D4
PC2
D5
PC1
D6
PC0
D7
A0
PA5
A1
8
D3
PB7
7
D4
PB6
9
D5
PB5
10 D6
PA2
13 D7
PA1
PA0
21
5
22
36
17
A14
PB1
RD
PB0
WR
PB2
PC3
RST CS
29
35
PB3
6
R9
10k
13 VCC
R10
10k
12 VCC
11 TO
10
10 LO
9 HO
12
8 S5
13
7 S4
16
6 S3
15
5 S2
14
4 S1
3 GND
U2
82C55
PB4
D7
A10
PC5
12 D2
D6
A9
D2
PA3
D5
A8
4
D2
D1
15 D1
D4
A7
3
33
PC7
PA4
D3
A6
37
38
D1
D0
14 D0
D2
A5
36
JP3
TO OSCILLATOR
4MHz 5
D1
A4
35
C10
0.1
D0
A3
34
VCC
34
A1 8
U1
Z80C
A1
32
D0
A0 9
AO
31
C7
0.1
WAIT
BUSRQ
17
R8
10k
26
11
7
RST
VCC
6
24
INT
CLK
6
U7d
R2
10k
2 GND
39
1 O6
JP1
40
1
13 O5
12 04
22
11 1C
25
10 8C
24
9 4C
23
8 2C
2
7 O3
3
6 O2
4
5 O1
19
4 2D
18
3 1D
20
2 4D
21
1 8D
TO
DISPLAY
7
C2
0.1
VCC
+5V
D3
1N4001
IN
BT1
9V
U9
7805
GND
OUT
C5
1
D2
1N4001
JP4
+5V
TO JP2
D1
1N5404
IN
+12V 1
0V 2
R11
10k
D5
1N4733
C6
220
U8
7805
GND
OUT
C4
1
U7e
11
R12
4.7k
VCC
VCC
24
24
A0
8
A1
7
A2
6
A3
5
A4
4
A5
3
A6
2
A7
1
A8
23
A9
22
A10
19
WE
A0
A1
D0
A2
D1
A3
D2
A4
D3
U3
6116
A5
D4
A6
D5
A7
D6
A8
D7
A9
OE
A10
CE
10
21
D0
9
10 D1
D1
10
11 D2
D2
11
13 D3
D3
13
14 D4
D4
14
15 D5
D5
15
16 D6
D6
16
17 D7
D7
17
9
D4
1N4733
D0
A1
D0
A2
D1
A3
D2
D3
U4
27C32
D4
A4
A5
A6
D5
A7
D6
A8
D7
20
A9
18
A10
OE/
VPP
12
C11
0.1
A0
20
A11
8
A0
7
A1
6
A2
5
A3
4
A4
3
A5
2
A6
1
A7
23
A8
22
A9
19
A10
21
A11
CE
18
12
VCC
R6
10k
6
I GO
A12
1
A13
2
A14
3
16
G1
Y1
A
B
C
U5
74HC138
G2A G2B
SIDEREAL CLOCK - CPU
4
5
Y2
Y0
Y3
14
13
15
12
8
August 1993 33
34 Silicon Chip
C2
0.1
1
2
6
2D
4D
8D
6
8C
O6 1
8D 1
4D 2
1D 3
2D 4
O1 5
O2 6
O3 7
2C 8
4C 9
8C 10
1C 11
O4 12
O1
2
4C
GND 2
FROM CPU
BOARD
JP1
O5 13
1
2C
GND 3
D1
1N4148
C5
0.5
4
7
1C
S1 4
5
4
7
1D
5
3
S2 5
C4
0.1
3
VCC
C3
0.1
S3 6
S4 7
S5 8
HO 9
LO 10
TO 11
VCC 12
FROM CPU
BOARD
JP2
VCC 13
VCC
C
1
R21
10k
HO
C6
0.5
D2
1N4148
G
BI/RBO
E
D
F
8
U2
7447
C
B
A
8
4
2
1
RBI
LT
16
8
F
G
8
BI/RBO
E
4
E
C
R7-13
7x 27
E
C
7
8
10
13
1
6
R28
10k
E
E
C
VIEWED FROM
BELOW
B
E
Q16
BC548 C
B
DIS7
TIL312
HEATER ON
LED DRIVER
R22
27W
11
2
7
8
10
13
1
SW1
11
2
7
8
10
13
1
S1
Q4
BC337
B
11
E
C
11
R29
10k
O2
Q3
BC548
B
2
14
DIS1
TIL312
14
E
C
R2
4.7k
2
7
8
10
13
1
B
Q2
BC337
Q15
R27 BC548 C
10k B
VCC
B
Q13
BC548
14
15
9
10
11
12
R14-20
13 7x 27
VCC
14
15
9
10
11
12
13
VCC
Q1
BC548
B
D
B
RBI
2
A
LT
U1
7447
16
O1
R1
4.7k
O3
SW3
1
14
E
C
DIS3
TIL312
Q6
BC337
B
11
2
7
8
10
13
1
DIS9
TIL312
14
SIDEREAL DISPLAY
11
2
7
8
10
13
E
C
S3
S4
SW4
UNIVERSAL/LOCAL DISPLAY
B
Q5
BC548
SW5
O4
R4
4.7k
S5
Q7
BC548
B
SIDEREAL CLOCK - DISPLAY
SW2
S2
DIS8
TIL312
14
DIS2
TIL312
14
E
C
R3
4.7k
11
2
7
8
10
13
1
11
2
7
8
10
13
1
E
C
TO
14
E
C
R25
10k
DIS10
TIL312
14
DIS4
TIL312
Q8
BC337
B
O5
R5
4.7k
C1
10
R26
3.9k
LO
6
7
11
2
7
8
10
13
1
11
2
7
8
10
13
1
E
Q9
BC548 C
B
KEYBOARD
BEEPER
2
U3
LM555
4
DIS11
TIL312
DIS5
TIL312
Q10
BC337
B
1
8
14
14
E
C
3
VCC
VCC
R23
10k
O6
R6
4.7k
1
E
C
PIEZO
BEEPER
R24
27
Q14
BC548
B
11
2
7
8
10
13
1
11
2
7
8
10
13
Q11
BC548
B
E
C
6
14
14
E
C
UNIVERSAL/
LOCAL LED
DRIVER
DIS12
TIL312
DIS6
TIL312
Q12
BC337
B
JP1
TO CPU
BOARD
1 +9V
OUT
R7
10M
R3
8.2k
R6
10k
R
U2
LM334
R1
220
2
1
U1a
LM358N
5
8
6
R4
18k
R8
390
7
U1b
3 +12V
4 HEAT ON IND
5 4MHz OUTPUT
3
R5
10k
R2
10k
C4
0.1
2 GND
IN
U3
78L05
GND
Q3
TIP31
B
SEE
TEXT
4
C
E
U2, Q3 AND Y1 ATTACHED TO BRASS BLOCK
OUT
L1
C1 1mH
27pF
Y1
4MHz
Q1
2N5485
G
R9
1M
R12
100k
C3
27pF
D
S
C2
68pF
R10
100k
C5
0.1
Q2
2N5485
G
U4
78L05
GND
Fig.3: the crystal
oscillator circuit. Crystal
Y1 & transistor Q1 form
a Pierce oscillator which
operates at 4MHz, while
FET Q2 buffers the
4MHz signal to the CPU
board. U2 is an LM334
adjustable current source
& functions here as a
temperature sensor. It is
monitored by U1a & U1b
& these in turn control
Q3. When Q3 is on, it
dissipates several watts
to heat the interior of a
small plastic utility box
which houses the oscilla
tor board.
IN
D
TIP31
S
R11
1k
78L05
LM334
I G O
R
VIEWED FROM BELOW
2N5485
G S D
B CE
SIDEREAL CLOCK - OSCILLATOR
O1 are missing, Q15 will turn off, Q16
will turn on and the displays will be
disabled.
Oscillator board
The oscillator PC board features a
4MHz crystal oscillator and a temperature controller – see Fig.3. Crystal
Y1 and transistor Q1 form a Pierce
oscillator. FET Q2 buffers the 4MHz
signal to the CPU board.
U2 is an LM334 adjustable current
source connected as a temperature
sensor. It causes a voltage drop,
proportional to the Absolute temperature, to be developed across
R2. This resistor is connected to the
inverting input of op amp U1a which
is connected as a comparator. Pin 3
of U1a is connected to a reference
voltage divider across the 5V supply
and this effectively sets the operating
temperature of the circuit.
Fig.2 (left): the display circuit is
controlled by the CPU board & uses
two 7447 display drivers (U1 & U2)
plus 12 7-segment LED readouts. U3
drives a piezo beeper to provide the
keypad beep function.
When pin 3 is more positive than
pin 2, the output (pin 1) of U1a goes
high. This output is buffered by U1b
and is used to drive transistor Q3.
This transistor is connected across
the +12V supply and functions as
the heater in the circuit. When the
transistor is on, it dissipates several
watts to heat the interior of a small
plastic utility box which houses the
oscillator board.
As the temperature inside the box
rises, the voltage at pin 2 of U1a increases to the point where it is more
positive than pin 3. This causes pin 1
(and thus pin 7 of U1b) to go low and
therefore transistor Q3 is turned off.
The circuit then cools down to the
point where the transistor is switched
on again.
Q3, Y1 and U2 are all attached to a
brass block which is maintained at a
constant temperature of 70°C. Pin 7 of
U1b is also routed to the display board
to light up a “heater on” indicator, as
mentioned above.
Construction
The three PC boards should be
assembled and then linked together
–see Figs.4-6. The CPU and display
boards are double-sided but without
plated through holes. This means that
any holes in the board not associated
with components should have pinthroughs installed and these should
be soldered on both sides of the board.
You can use tinned copper wire for all
pin-throughs.
Once the pin-throughs have been
installed, the IC sockets can be
inserted. They provide additional
pin-throughs for the board so their
pins must be soldered on both the
component and solder sides. The
use of machined pin or wire wrap IC
sockets is recommended because the
pins on these are longer than normal,
allowing soldering on both sides of
the board. Sockets which are too close
to each other to allow soldering on
the component side will need to be
split into two halves and installed
separately. There are no sockets used
on the display board.
Once the IC sockets have been installed, the other components should
be added. All components must be
soldered on both sides of the board
except the displays which are only
soldered on the copper side. The
piezoelectric buzzer is mounted on
the solder side of the display board
(see photo).
August 1993 35
U9 7805
D2
D1
R5
C11
JP3
C5
R4
+12V
R2
+9V
R11
GND
R12
D4
HO
U1
Z80C
CLK
R3
1
C8
U5 74HC138
1
U3
6116
C9
R6
1
U6 4020
1
U4
27C32/27C64
C7
U7 74HC14
R9
R8
1
1
R1
C10
R10
U2
82C55
C1
1
JP1
JP2
Fig.4: this diagram shows how the parts are installed on the CPU board. Note
that pin throughs must be installed at all vacant hole positions, while all
components & IC sockets must be soldered on both sides of the board.
R15
R19
R20
R16
R17
R18
D2
U1 7447
R29
1
Q9
R5
1
1
Q10
The correct operation of all functions should be established by using
them as described below.
In normal mode, the SELECT key
Q11
R6
1
1
Operation
Q12
Q14
1
R27
R28
SW1
SW2
SW3
SW4
SW5
R23
R26
C3
C1
JP1
36 Silicon Chip
Q13
R21
R24
C6
D1
Q16 Q15
C4
1
D11 TIL312
R14
Q8
D10 TIL312
1
Q7
D9 TIL312
1
R4
D8 TIL312
1
Q6
D7 TIL312
1
D6 TIL312
D2 TIL312
D1 TIL312
1
Q5
R3
C5
1
C2
1
Q4
D5 TIL312
1
R8
R12
R13
R9
R11
R10
Q3
R2
D3 TIL312
R7
Q2
D4 TIL312
Q1
R1
functioning. The oscillator board can
now be placed in a standard plastic
box measuring 28 x 54 x 83mm (DSE
H-2855 or equivalent). The board is insulated by surrounding it with pieces
of 10mm thick polystyrene.
The three boards can now be linked
together. The connec
tions between
the CPU and display boards can be of
tinned copper wire, with every second
link insulated.
The connections between the CPU
and oscillator boards should be made
with about 80mm of insulated wire.
Note that the pin numbers for each
wire differ on each board. The boards
are installed in a standard plastic instrument case measuring 200 x 65 x
U2 7447
The brass block (see Fig.7) on the
oscillator board should be installed
at the same time as the components.
Transistor Q3 is screwed to the block
while the crystal and temperature
sensor are held in place using strips of
metal as clamps. Heatsink compound
should be used to ensure a good thermal bond to the brass block.
The heater current must be set before the three boards are connected
together. Apply +12V to the oscillator
board and measure the current drain.
Choose a value of R8 which gives
a supply current of about 250mA.
Monitor this current until it drops
to a low value. This indicates that
the temperature control circuitry is
160mm (DSE H-2505 or equivalent).
You will need to make several cutouts
in the front panel for the two 6-digit
displays and the five pushbutton
switches. You will also need two small
pieces of red transparent plastic and
these are glued behind the dis
play
cutouts.
A 1A slow-blow fuse should be installed in series with the +12V supply
line. The fuseholder can be an in-line
type or mounted on the rear panel.
The whole assembly can now be
fitted in the case. Voltage regulator U8
should be heatsinked to the rear panel
using a piece of aluminium plate bent
into an L shape. The display board
can be fixed to the front panel using
the holes either side of the switches.
The spacing between the board and
the front panel is determined by the
height of the switches and displays.
Appropriate spacers need to be used
to provide this clearance. The CPU
board can be fixed in place using the
mounting holes provided in each corner of the board.
Once the three boards have been
installed, power can be applied. If
all is working correctly, the beeper
should sound and the display should
show all eights (lamp test mode). The
SELECT switch can now be pressed to
acknowledge that a reset condition has
occurred. The right and left displays
should now indicate time in hours,
minutes and seconds. The battery
should not be installed until the operation of all functions is verified, as the
CPU can not be reset with the battery
in circuit. To reset the CPU, turn the
power off for 10 seconds.
R22
D5
D3
D12 TIL312
JP4
BT1
9V
C4
U8
7805
U3 555
C2
GND
+12V
C6
JP2
R25
BEEPER
Fig.5: the parts
layout on the display
board. As with the
CPU board, the parts
must be soldered
on both sides of the
board & pin-throughs
installed at vacant
hole locations.
switches between universal and local
time for the right-hand display. The
decimal point on digit six of the righthand display lights up to indicate that
universal time is selected.
The BRIGHT key changes the display
brightness through five levels. The
DISPLAY key switches the right and
left-hand displays on or off. The SET
TIME key starts and stops the set time
mode of operation. The SET REF key
starts and stops the set reference mode
of operation.
In “Set Time” mode, the SELECT
key selects the digits which are to be
set. The + key will then increment
the hours or minutes that are flashing.
When the seconds are flashing, the +
key will zero them. The seconds on
universal/local time can only be set
in universal mode.
The TONE key enables the buzzer to
sound and indicate the occurrence of
each minute that passes. To indicate
sidereal minutes, the tone key must
be pressed when any sidereal digit is
flashing and vice versa for universal/
local. To stop the tone function, press
the TONE key again.
The BATTERY key causes the display to indicate the length of time that
the battery has been used. If the power
has been off and the decimal point is
flashing, pressing the battery key will
terminate flash mode. When a new
battery is installed, the “-” key can be
used to zero this display.
In “Set Reference” mode, the SELECT key selects the reference number
to be changed. The left-hand display
will cycle through an indication of
U1-U4 or S1-S4 when the SELECT key
is operated. The + and - keys are then
used to adjust the particular reference
number chosen.
This close up view shows the oscillator board in its case, with the cover &
insulation removed. The power transistor (Q3), constant current source (U2) &
crystal are attached to a brass block near the centre of the board.
its accuracy against an accurate time
signal such as Telecom’s time service or radio station VNG on one of
the following frequencies: 2.5MHz,
5MHz, 8.638MHz, 12.984MHz and
16MHz. The error obtained after 24
hours needs to be recorded and entered into a PC running the program
STARTIME.BAS. The program will
calculate and display new values for
U1-U4 and S1-S4.
These updated reference values
should be entered into the clock using
the set reference mode. This process of
adjustment may have to be performed
a number of times, with the accuracy
being checked over longer periods.
The sidereal time is referenced to
Where to buy the kit
Readers can buy a short form kit
of this project from the author. The
kit comprises the three PC boards,
a programmed EPROM and the
five keypad switches for the display board. The kit is priced at $95
plus $5 for postage and packing,
anywhere in Australia. The author
can also provide a repair service
on completed sidereal clock kits
for $60 plus the cost of any parts
replaced.
Payment can be made via
cheque or money order to John
Western, 81 Giles Ave, Padbury
WA 6025. Phone (09) 401 2733.
6
14
Time setting
5
2.6
Set the universal time and check
R3
C2
R12
Q2
R10
R11
+9V
C4
GND
R7
R4
R6
R5
R2
R1
B
+12V
1
U2
L1
C3
BRASS BLOCK
C1
Q1
R8
15
U3
R9
B
HO
U1
LM358
U4
Y1
C5
Q3
A
A
+12V HARD WIRED TO Q3
JP1
CLK
Fig.6: the parts layout for the oscillator
PC board. Keep all component leads
short & note that R8 must be chosen to
give a supply current of about 250mA
– see text.
3.5
20
27
2.5
5
HOLES A = COMPONENT MOUNTING TAPPED M2.5
B = BLOCK MOUNTING TAPPED M2
MATERIAL: BRASS
DIMENSIONS IN MILLIMETRES
Fig.7: this diagram shows the dimensions of the brass block.
August 1993 37
10 ‘*********************************************************
20 ‘* STARTIME.BAS by JOHN WESTERN 12/06/91 This program
*
30 ‘* calculates new values for the sidereal clock reference
*
40 ‘* numbers. The error in seconds/day and the values of U1-U4
*
50 ‘* are entered by the user.
*
60 ‘*********************************************************
70 DEFDBL A-Z
80 CLS:PRINT “
SIDEREAL CLOCK CALCULATION PROGRAM”
90 ‘
100 ‘ GET CURRENT VALUES OF U1-U4
110 INPUT “Enter current value of U1”; U1 ‘get current values
120 INPUT “Enter current value of U2”; U2
130 INPUT “Enter current value of U3”; U3
140 INPUT “Enter current value of U4”; U4
150 ‘
160 ‘CALCULATE TOTAL NUMBER OF PULSES PER DAY
170 PCD = (U1 * 59 * 60 * 24) + (U2 * 59 * 24) + (U3 * 23) + U4
180 ‘
190 ‘GET ERROR FROM USER
200 INPUT “enter number of seconds per day error”;TIMERR
210 WHILE ANSWER$ <> “f” AND ANSWER$ <> “F” AND ANSWER$ <>
“s” AND ANSWER$ <> “S”
220 INPUT “Is clock fast or slow? (F/S)”; ANSWER$
230 WEND
240 ‘
250 ‘CALCULATE PULSE DIFFERENCE FOR EACH REFERENCE VALUE
260 PD = (TIMERR / 86400!) * PCD
270 IF PD >= 84960! THEN PPS= INT(PD/84960!):PD = PD - (PPS * 84960!)
280 IF PD >= 1416 THEN PPM = INT(PD/1416):PD = PD - (PPM * 1416)
290 IF PD >= 23 THEN PPH = INT(PD/23): PD = PD - (PPH * 23)
300 IF PD >= 1 THEN PPD = INT (PD)
310 ‘
320 ‘CALCULATE AND DISPLAY NEW VALUES OF U1-U4
330 IF ANSWER$ = “f” OR ANSWER$ = “F” THEN GOSUB 2010
ELSE GOSUB 1010
340 PRINT
350 PRINT “New U1 =”; U1
360 PRINT “New U2 =”; U2
370 PRINT “New U3 =”; U3
380 PRINT “New U4 =”; U4
390 ‘
400 ‘ CALCULATE AND DISPLAY NEW VALUES OF S1-S4
410 PCD = (U1 * 59 * 60 * 24) + (U2 * 59 * 24) + (U3 * 23) + U4
420 SIDCNT = PCD / 1.00273791#:PULSDIF = PCD - SIDCNT
430 S1 = INT(PULSDIF / 84960!): PULSDIF = PULSDIF - (S1 * 84960!)
440 S2 = INT(PULSDIF / 1416): PULSDIF = PULSDIF - (S2 * 1416)
450 S3 = INT(PULSDIF / 23): PULSDIF = PULSDIF - (S3 * 23)
460 S4 = INT(PULSDIF)
470 PRINT “S1 =”; S1
480 PRINT “S2 =”; S2
490 PRINT “S3 =”; S3
500 PRINT “S4 =”; S4
510 END
1000 ‘ ROUTINE TO CALCULATE NEW VALUE OF U1-U4 FOR CLOCK SLOW
1010 U1 = U1 - INT(PPS)
1020 U2 = U2 - INT(PPM)
1030 U3 = U3 - INT(PPH)
1040 U4 = U4 - INT(PPD)
1050 RETURN
2000 ‘ ROUTINE TO CALCULATE NEW VALUES OF U1-U4 FOR CLOCK FAST
2010 U1 = U1 + INT(PPS)
2020 U2 = U2 + INT(PPM)
2030 U3 = U3 + INT(PPH)
2040 U4 = U4 + INT(PPD)
2050 RETURN
38 Silicon Chip
Fig.8: this full-size artwork can be used as a marking
template for the front panel.
universal time and should be correct once universal
time is adjusted. In the event that the sidereal time is
not accurate, the values S1-S4 allow it to be adjusted.
The sidereal time should now be set following normal
astronomical procedures.
The prototype clock has been operating for two years
with universal time giving an error of less than one
SC
second per month.
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Card No.
August 1993 39
SERVICEMAN'S LOG
Little things can be big time wasters
Frustration & annoyance is the theme of this
month’s notes. It’s about the many & varied
things that can contrive to slow the job & which
collectively can add up to a lot of wasted time.
As most readers will appreciate,
most faults that turn up on the service
bench are fairly routine. Generally,
they are faults that have been seen
before in the same model set or faults
which, by their very nature, can be
recognised in any set.
These are the ones that provide the
bread and butter – and a smidgin of
jam occasionally. The real stinkers –
the ones that call for a lot of patience
and electronic detective work – may
make it into these notes but seldom
earn much income.
In between these two extremes are
those which, in spite of being relatively straightforward in a technical
sense, can be quite frustrating – often
for all kinds of silly reasons. This is
one such story and it has a very silly
twist in the tail.
It is about a Panasonic model 2970V
TV set, a 73cm model with stereo
40 Silicon Chip
sound. This set is fitted with the M15D
chassis which has been very reliable.
Incidently, the “D” in this type number indicates a “dead” chassis; ie,
one which is isolated from the mains.
There is also an M15L model, the “L”
signifying a live chassis.
This set is only about three years
old but it had been used for only
part of that time. The owner had
just moved into a new home and the
set has been in storage for about 15
months while he and his family were
living in smaller temporary accommodation. Obviously, the storage period
may have had something to do with
the problem.
The owner was typically vague
about the nature of the fault, saying
only that the set was still working
but that there was something funny
about the picture. This was confirmed
when I set it up on the bench. Yes, the
set was working and, yes, there was
something funny about the picture; it
was suffering from severe pincushion
in the east-west mode; ie, it bowed
inwards on each side.
This was one of the first frustrations, because it is quite a rare fault
these days. Worse still, it was one I
had never encountered before in this
model chassis. I wasn’t quite sure
where to start.
Another frustration involved the
complexity of the service manual.
While the material in it is very well
presented, the circuit and other data
are spread over many sheets, making it
difficult if the circuit has to be traced
from one sheet to another. On the other
hand, it is much better than having the
circuit reduced so much that essential
detail is lost.
Getting back to the fault, the pincushion circuitry is on a separate
board – designated the K board – and
this same module is used in several
models. Initially, I was unable to find
the circuit and wasted a lot of time
searching for it. I eventually ran it
to earth in the section for the M15L
chassis (of course – where else would
it be?). It is reproduced herewith and
at least I don’t have to apologise for
the quality.
But this only moved me on to the
next stage of frustration. The circuit
did not carry any waveforms or even
any voltages on the transistors. I did
eventually track down the voltage
data – on yet another sheet – but not
before I had wasted more time trying
to rationalise the voltages as I found
them. I also searched through the manual for any explanation as to how the
pincushion circuit functioned, but in
vain – I was on my own.
So, all in all, I wasted a good deal
of time before I even started.
The K board
The K board is about 150mm long
by 100mm wide and slides vertically
between two rails mounted on the
right-hand side of the cabinet (as seen
from the back). It connects to the rest of
the set via two plug and socket assemblies, K1 and K2, on leads long enough
to allow the board to be removed and
worked on while still in circuit. This,
at least, was a plus.
Pin 1 of K2 connects to the 113V
main HT rail, while pin 2 carries
vertical pulses. These were traced
back to a network connected to pin
2 of IC401, the vertical output chip.
Pin 3 has no connection and pin 4
goes to chassis.
Plug K1 connects directly to the
horizontal scan coils via pin 1 (H-) and
pin 3 (H+). Pin 4 connects to chassis.
The horizontal amplitude here is quite
substantial.
The lower part of the circuit shows
three transistors: Q701, Q702 and
Q703. Q703 is the first one in the chain
and is fed with vertical pulses from pin
2 of plug K2. The output from Q703, at
its collector, goes via the pincushion
Fig.1: the K-board (pincushion) circuitry for the Panasonic TC-2970V. Vertical
pulses come in on pin 2 of plug K2 & are fed to the base of Q703 (lower right).
Q703 drives the pincushion control, the output of which then drives Q702 &
Q701. Finally, Q701’s output is coupled to the horizontal scan coil circuitry to
provide the necessary pincushion correction. Note the absence of waveforms
and transistor voltages.
control to the base of Q702 which, in
turn, drives Q701.
Q701 is a power transistor (TO66 package) and is mounted on a
heatsink. Its output is coupled into
the horizontal scan coil circuitry to
provide the necessary pincushion
correction.
Waveform checks
I tried checking various waveforms,
hoping I might find an obvious dis
crepency, but without success. The
vertical pulses appeared to be making
their way through the chain OK but,
without any waveforms for reference,
I had no way of knowing whether the
amplitude and waveform shape were
correct at every stage. The only hint
was that the gain of Q703 was not what
I would have expected from a superficial assessment of its configuration.
But then, I couldn’t be sure.
Also shown in this part of the
circuit is width control R708 (5kΩ)
and pincushion control R710 (20kΩ).
I tried adjusting the width control
and this behaved as expected; it varied the width and nothing else. But
when I tried the pincushion control,
August 1993 41
circuit. But no, it was spot on value.
Next, I lifted C707 and measured it.
It was down to around 700µF, which
made it bad enough to need replacing,
even if it wasn’t the main fault. And it
wasn’t, because a new one made little
difference.
My next stop was C708 (47µF) and
this was where I struck oil; it was
extremely leaky, which could easily
account for the weird voltages and
the failure of the pincushion circuit. And it did, because a new one
immediately cured the pincushion
problem.
Having located the fault, I checked
the voltages again, more or less as a
matter of routine. I didn’t refer to the
manual list this time, having memorised the values well enough – I
thought – to satisfy such a check. And
so it seemed; I measured 1.85V on the
emitter, 2.5V on the base, and 9.3V on
the collector, near enough to the figures
I recalled from the manual.
SERVICEMAN'S LOG – CTD
The final twist
it behaved in a less logical fashion; it
also changed the width and nothing
else! That suggested that the fault was
in this section of the circuit.
Transistor checks
My next step, was to check all
three transistors but, as far as I could
determine, all were OK. I had not at
this stage unearthed any voltage data
for these transistors but I made a few
voltage measurements anyway, hoping
that they might provide a clue.
And they did, in a way. The voltages
on Q701 and Q702 at least seemed
reasonable, by rule-of-thumb guess
timation. But Q703 was another
matter; unless it was being used in
a very unusual way, I couldn’t make
any sense of it. I measured 17V on the
collector, 17V plus on the emitter and
17V on the base. But, while this didn’t
make much sense, it did remind me
of the apparent low gain of this stage.
But what should the voltages be?
I found them listed quite by chance
when, as so often happens, I was
42 Silicon Chip
searching the manual for something
else. At a quick glance I registered that
those for Q703 were not only nothing
like the values I had measured but
seemed to be much more reasonable.
All of which simply confirmed my
idea that whatever was wrong was in
the immediate vicinity of Q703, the
transistor itself having already been
cleared.
There aren’t many components directly associated with Q703. I started
with R712, thinking it might be open
COMMON TEST POINT VOLTAGES
E
B
C
Q701
0.025
0.62
13.8
Q702
11.9
11.3
0.62
Q703
1.85
9.3
2.5
Q802
0
0.01
16.5
Fig.2: this is the relevant portion of
the transistor voltage table from the
Panasonic TC-2970V manual. The
collector & base voltages shown for
Q703 are transposed.
And so, after a routine check and
adjustment, the set was duly returned
to the customer, putting an end to my
time-wasting frustrations. Or so I imagined. My final frustration came as a
nasty twist when I later took a second
look at the voltage table in the manual.
It was then I suddenly realised that
the voltages were not listed as I had
recalled them. Oh, the values were correct but not the transistor connections.
The manual listed them as 1.85V on
the emitter, 9.3V on the base and 2.5V
on the collector.
I did a double take on that. Those
figures did not make sense and, had
I been more observant, I would have
realised this when I first saw the table.
Instead, I read them as I imagined
they would be, rather than as they
were.
The point about these figures is
that – apart from anything else – they
imply a base-emitter voltage of around
7.5V – an impossible condition according to my understanding of solid
state theory. When I went to (solid
state) school, the maximum voltage
which could normally be developed
across such a junction would not
exceed 0.7V, and would be more like
0.65V in practice.
So what had gone wrong. My immediate reaction was to suspect that the
figures in the manual were a mistake;
that they had been wrongly set out
Fig.3: this diagram shows the front-end circuitry for the High Energy Ignition
System, as published in the May 1988 issue of SILICON CHIP. The constructor’s
problems were at the very front of the circuit.
with the base and collector values
transposed. I spent a lot of time, on
and off, thinking about the problem
and the longer I thought about it, the
more convinced I became that the
manual was wrong. Note particularly
that, if we transpose the base and collector values as given in the manual,
we then have 0.65V across the base/
emitter junction, exactly according to
the rules.
Finally, at the first opportunity, I
rang my colleague in the Panasonic
service department and put the problem to him. It didn’t take him long
to fetch the manual and look up the
circuit and chart. His reply was brief,
to the point: “Ah yes, a typo” (typographical error).
Anyway, that was the end of story
as far as the various problems and
frustrations were concerned, But I
do suggest that anyone who is likely
to be dealing with the M15 chassis,
or the manual, make a note of the
mistake.
Finally, I do have some other
comments on the fault itself. While
electrolytic capacitor failures are not
unusual, I was surprised that one as
large as C708 should deteriorate to this
extent in only a few years. The fact
that the set was stored for so long may
have been a factor, although it should
not have been.
And what about C707? This, I think,
might have been a victim. Rated at only
6.3VW, it had about 17V applied across
it while ever the fault was present. The
wonder is that it didn’t break down
completely.
In addition, there is another electrolytic capacitor in this part of the circuit
– C716 (10µF 50VW). This was also
checked and was found to be down to
about 5µF. It was replaced along with
C707 and C708.
While on the subject of electrolytics,
I find that if one reads lower than its
rated capacitance, by even a small
amount, it is time to replace it. New
capacitors invariably measure higher
than their marked value. If they drop
below that figure, they are generally
on the way out.
Kit projects
To change the scene, but still on the
subject of frustrating situations, I am
reproducing a letter from a reader, Mr
R. S. of North Melbourne, Victoria. It is
not a servicing story in the usual sense,
nor was it a particularly profound exercise, but it is an excellent example
of the problems which can arise from
the supposedly simple job of building
a kit project.
Assuming a well-designed project
and a properly prepared kit, it is reasonable to expect that it will work at
first switch-on (provided, of course,
that the kit has been correctly assembled).
But it doesn’t always happen that
way. And when it doesn’t, kit builders
react in a variety of ways. Some simply
regard the design as a bomb, curse the
designer, and chuck the whole thing
in the garbage bin.
Some strip it down and rebuild it;
a time wasting and usually futile procedure. One enthusiast, in the days
of build-your-own TV sets, stripped
down and rebuilt a complete 17-inch
TV set, in an attempt to cure a relatively simple fault – the picture was
transposed left to right.
More enlightened souls, like our
reader, assume that the design is capable of working and that its failure must
be due to a construction fault –which
is usually the case. They then set about
finding it in a methodical way. Just
how simple some of these faults can
be is shown in this example. Here’s
how he tells it.
The night before Christmas
Some months ago, my son-in-law
to be raised the question of fitting an
electronic ignition system to his motor
vehicle. Because I had built a number
of CDI (Capacitor Discharge Ignition)
and TAI (Transistor Assisted Ignition)
units, I was consid
ered a suitable
consultant.
Although very pleased with the
performance of all units tested, I have
never been able to detect either an
increase in fuel economy or engine
power. Perhaps this is because I always
cleaned and adjusted the ignition system on a regular basis – about every
3000km.
What I have noticed is that the
electronic systems require virtually
no manitenance or adjustment, unless
I disassemble the distributor for some
other purpose.
Since CDI is currently out and TAI
is in, the choice was simple. I did
not experience any crossfire with
CDI but the inverter squeal could be
objectionable.
My last TAI circuit is dated at 1982
but the “High Energy Ignition System”
unit produced by SILICON CHIP in
May, 1988 was available in kit form.
And, as his training was in the field of
electronics, a kit was purchased and
he assembled the unit.
A few days before his initiation to
son-in-law, he invited me to install
the TAI in the vehicle, as he knew
that I would be more familiar with the
automotive side of things (self-trained
also). However, I put this off while he
August 1993 43
SERVICEMAN'S LOG – CTD
was being moulded into married life
during the next two weeks and I waited
for his return.
A telephone call was subsequently received on December 23rd and
arrangements were made to perform
the change over on the night before
Christmas. He had already mounted
the box in the engine bay and all that
should have been necessary was for
me to find a suitable 12V supply and
make the appropriate connections to
the ignition system.
This particular vehicle incorporates
the ballast resistance in the loom but I
was able to find a suitable power supply connection at the fuse panel and
run a wire to the unit. Laying out the
wiring to the coil in a secure fashion
came next. Suitable checking took
place and I felt that we were ready for
the all-important smoke test.
Switching the ignition to the run
position produced no problems but
switching to the start position failed
to produce any fire in the engine.
This enabled me to demonstrate how
easy it was to revert to the old faithful
44 Silicon Chip
Kettering system, if it was required.
We had begun the work in the open
and in dry conditions, but by now a
light rain had become a heavy downpour and daylight had vanished, so we
called it a night. No smart comments
about Melbourne’s weather thanks; we
aren’t overjoyed either!
The next day, my daughter rang
and invited me to lunch with the
family. No great arm twisting was
necessary, as it would give me the
opportunity for further fault finding.
After a pleasant meal, off came the
lid and the investigation began. I was
expecting to find a fault with D5 but
it still behaved as a diode and was
oriented correctly.
Transposed resistors
The resistors were checked next and
it was found that the 22kΩ resistor to
the input (pin 5) of IC1 was 2.2kΩ. A
search was made for a suitable resistor
and we were able to find two 10kΩ
units. My son-in-law has a very limited
stock of components, as electronics is
not his hobby.
I was concerned that the additional
current through the zener diode in
IC1 might be too much for it. A re-test
took place but the engine did not start.
At this point, it was not noticed that
the 22kΩ resistor which should have
wired into the input of IC1 had been
placed in the collector circuit of Q2.
In other words, the 2.2kΩ and 22kΩ
resistors had been transposed.
The unit was removed from the
vehicle and, because there was the
possibility of serious damage to IC1,
I decided to take the unit with me for
further testing and repair. The 22kΩ
resis
tor problem was corrected the
next day. I then proved that Q1 was
intact and with the aid of a spare coil
connected, produced a spark when
the output of IC1 was taken to chassis
using a jumper lead.
Since waveforms were going to be
traced, the CRO was fired up. This was
an overkill, as will be seen. The action
of the points opening and closing was
mimicked by connecting a flying lead
to the power supply chassis. This
produced a step at the 47Ω resistor,
as was expected.
Unfortunately, when the CRO probe
was transferred to the other side of diode D5, the pulse vanished. On turning
the board over to the track side, it came
to my attention that there were more
tracks and holes than were necessary
for this project (as a last resort read the
text fully). The constructor had placed
the anode lead of D5 into the next hole
up the board.
Once this correction had been made,
a pulse could be traced to pin 7 of IC1.
By now reconnecting the test coil and
spark plug, I was able to view a nice
healthy spark. When installed the next
day, the system worked perfectly.
The constructor did emphasise that
he had performed “high reliability
hand soldering” techniques as his
employer instructs. And to his credit
the soldering could not be faulted.
But my warped sense of humour
considers that suitable connectivity
is required before conductivity can
take place.
Fair enough, R. S. and thanks for
the story. It emphasises one very important point – the difference between
field servicing, where a device originally worked but has now failed, and
production line servicing, where the
device has never worked. Production
line servicing is a completely different
SC
ballgame.
SILICON
CHIP
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SILICON
CHIP
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CHIP
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has requested that the page be removed to
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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:
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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:
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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:
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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:
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SILICON
CHIP
If you are seeing a blank page here, it is
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which is now out of date and the advertiser
has requested that the page be removed to
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Please feel free to visit the advertiser’s website:
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REMOTE CONTROL
BY BOB YOUNG
Unmanned aircraft – Israel
leads the way
UMAs have developed over many years from
craft that have showed promise to devices which
are important in the modern defence arsenal,
as shown by their extensive use in the Gulf War.
However, the country which has really shown
the way has been Israel with its Mastiff & Scout
aircraft.
This month, we will look at some
of the more exotic modern UMA systems but first a few observations. I am
forever amazed at the reader reaction
to each monthly column and to some
extent my own views of each column.
Columns that I am happy with often
pass unnoticed or even attract adverse
comment. On the other hand, some
that I am not happy with, despite my
best efforts, can attract a favourable
reaction.
By far the most persistent cause of
headaches is the choice of topic. When
I settled upon the subject of UMAs
for a purely electronics magazine,
I did so with some trepidation and
they were difficult columns to write. I
had to spend weeks in the NSW State
Library researching the subject, bringing my knowledge of the subject up
to date.
It appears that my fears on this series
of articles were unfounded for they
have attracted possibly the most reader
reaction of all of the columns I have
written to date, with the exception of
the speed controller articles.
This is not to say that all readers
agree with what I have written, so
here are a few comments from readers
who felt moved to communicate their
The IAI Scout is a notable Israeli UMA that began operational flying with the
IDF in 1981. Its wingspan is 4.96 metres, maximum take-off weight is 159kg &
its maximum speed is 176km/h. The endurance time is quoted as seven hours.
interest. My thanks to them and all
of the others who wrote or otherwise
commented on the articles.
First, Tony Mott of Blackburn,
Victoria sent me a very interesting
extract from the book “German Aircraft” by J. R. Smith and Antony Kay.
It gives the most detailed description
of the Mistel (Mistletoe) composite
aircraft (mentioned last month) that
I have yet encountered. Tony pointed out that according to Smith and
Kay, not only did I get the name of
this project wrong but I also gave
incorrect details of the operation of
this intriguing unit. What can I say,
except “OOPS!”
Contrary to what I stated in the
June 1993 issue, the upper fighter
unit of the pair was the mother ship
and the larger, lower (bomber) unit
was the disposable missile. Here is a
classic example of not checking the
facts. The details, sadly, came from
my own (faulty) memory. Despite all
the research I did, the one thing I did
not refresh my memory on was wrong.
Whilst on the subject of the Mistel
project, Smith and Kay give some very
interesting details of this and similar
weapons. They claim the earliest
use of a guided UMA in combat was
when the Italians launched a Savoia
Mar
c hetti S.M.79 bomber packed
with explosives and fitted with radio
control against British warships off
the Algerian coast on the 13th August,
1942. This aircraft was set on course
by the pilot who then bailed out but
the mission failed due to a radio malfunction.
Further to my comments on the improvements in warhead design in the
June 1993 issue, the Mistel was fitted
August 1993 53
The IAI Helstar from Israel is one of the most notable UMAs flying. It has twin
co-axial rotors some two metres in diameter & its maximum take-off weight is
500kg. It can stay airborne for six hours & has a maximum speed of 185km/h.
with a 3500kg hollow charge warhead
made up of 1725kg of high explosive
and a 1000kg steel core. This core
had a theoretical armour penetration
of 7.5 metres. In actual tests, it burst
through some 18.5 metres of concrete,
a staggering result.
As stated previously, men have an
absolute genius for designing ways to
kill each other.
The thing that really impressed me
in regard to the Mistel was just how
advanced the German technology was
in those days. The original Mistel was
aimed at the target and launched,
under control of the autopilot, at the
target. This left much to be desired as
regards accuracy and a proposal was
put forward to fit a wire guidance
system similar to that designed for the
Henschel Hs 293D. In this system, television cameras in the bomber relayed
pictures back to the fighter.
Wire guidance was used very successfully in many early missiles. It is
easy to see where the inspiration for
the smart bomb, used to such great
effect in Iraq, came from.
Wallace Beasley of Hillbank, SA sent
in a fascinating tale he picked up on
the rumour mill whilst working for
the RAF at Lympne as a young lad.
Several British fighter pilots were al
leged to have been arrested because
54 Silicon Chip
they planned to fly to Spain in their
Hawker Fury fighters to fight against
Franco in the Spanish civil war. Not
only that, but it was rumoured that
they had managed to get hold of a
Queen Bee complete with ground
control equipment and had planned to
load it with explosives and use it as a
guided missile against some strategic
target. As primitive as all of the foregoing appeared, they were to spawn
a deadly breed of UMAs and guided
missiles in a very short space of time.
All of this reminds me of Charles
Fort and his theory on the steam engine. Fort held that when it came time
to invent the steam engine it would
appear spontaneously around the
world. This certainly seems to have
been the case with UMAs.
New breed UMAs
Returning now to the Middle East
and the 1990s, we come face to face
with the new and very deadly breed
of UMAs.
As stated previously, the Israelis
now hold the dominant position in
the design and supply of UMAs, so
we will have a quick look at some of
these and their uses.
The leading Israeli UMA company is
Israeli Aircraft Industries (IAI), which
absorbed the Tadiran UAV division in
1984. Tadiran developed the Mastiff
series of UAVs and Mastiff III was
Israel’s first generation production
mini-UAV. Mastiff is now fairly primitive by modern standards but it served
Israel well for almost a decade.
The experience gained from this
UMA and its evaluation by the USMC
led directly to the US Navy requirement for Pioneer, more of which later.
Mastiff does not have a preprogramm
ed opera
tion option and is purely
operator controlled. It is due to be
re
placed by the new IAI Searcher.
Mastiffs were bought by the US Navy
in 1984-85.
Mastiff has a wing span of 4.25 metres and weighs in at 138kg at take-off.
Its maximum speed with a 16.4kW
(22hp) engine is 186km/h, while its
operational ceiling is 4480 metres
(14,700ft).
In 1976, IAI started development of
the Scout and in 1981 Scout II began
operational flying with the Israeli
Defence Forces. Scout is slightly larger than the Mastiff but has the same
basic appearance.
Most IAI UMAs feature a short fuselage fitted with a pusher propeller.
The wing is shoulder mounted on this
pod. The tailplane is mounted on twin
booms which attach to the wing. All
are fitted with a tricycle non-retractable undercarriage – very basic stuff
by modelling standards. The pusher
propeller leaves the nose free for TV
cameras and other sensors, and keeps
the aircraft and camera lenses free from
exhaust waste.
Scout has a wingspan of 4.96 metres and maximum take-off weight is
159kg. Its speed with a 16.4kW motor
is 176km/h (95 knots) and the ceiling
is 15,000 feet. The endurance of the
Scout is quoted as seven hours. Takeoff is via a truck-mounted catapult
(standard), but wheeled take-off is
also an option.
The Scout has been the Israeli Defence Force’s mainstay UMA since
1982 when it was introduced over
the Beka Valley with some outstanding results in defence suppression
missions. Scout has the option of
being able to switch between pre-programmed and operator-controlled
flight. This allows the uplink (the
radio control channel from ground
to aircraft) to remain silent during
most of the mission except for any
unforeseen events which need operator intervention.
The sensors fitted vary and include
a daylight TV camera, FLIR and laser
rangefinder/target designator. Recovery is by net in standard configuration
but wheeled landings are an option.
Scout has been exported to Singapore,
South Africa and Switzerland and,
like Mastiff, will be replaced by the
Searcher.
Interestingly enough, both Switzerland (IAI joint venture) and South
Africa have since developed their
own versions of the Scout, both a
little larger but with the same basic
layout. However, the 6-metre South
African Seeker is far and away the
more elegant looking vehicle. It has a
very interesting “return to base” mode
in the event of the primary or backup UHF control links being broken
or jammed.
The Swiss Ranger has a parachute
recovery for peace-time emergencies
or, for normal operations, a wheeled
or skid undercarriage which can be
used in conjunction with an arrester
cable.
Pioneer
In 1985, the US Navy purchased
the first of nine Pioneer units from
IAI. Developed by IAI and produced
as a joint IAI/AAI venture, Pioneer
is derived from the earlier Scout and
maintains the same basic layout. Its
wingspan is 5.11 metres and maximum
take-off weight is 200kg. Power is by a
Sachs SF 350 2-cylinder, 2-stroke engine rated at 21kW. The service ceiling
battleships Missouri and Wisconsin.
Pioneer flew more than 500 missions during Desert Storm, totalling
in excess of 1700 hours. Its missions
included mine-hunting, naval OTH
(over the horizon) targeting and route
recon
naissance for AH-64 helicopters, as well as the more commonplace
overland surveillance and target
location.
Sensor options include TV, FLIR,
EW/ECM, decoy, communica
tions
relay and laser rangefinder/designator.
The guidance system is either pre-programmed or it can be flown by an operator. Recovery is either by wheeled
undercarriage with an arrester or, on
ship, by net.
Since 1986, IAI has developed a
stream of more and more advanc
ed UMAs including Ranger, Impact,
Searcher (wingspan 7.22 metres, speed
204km/h, ceiling 7620 metres), Hunter
and the very interesting Helstar. Helstar (Heliborne Loitering System with
Thermal imager and Radar) is an unmanned maritime helicopter featuring
twin co-axial rotors some two metres
in diameter (not much larger than the
usual model helicopter). Designed to
operate from Israeli naval corvettes
and other missile carrying boats, the
Helstar take-off weight is a staggering
500kg. It is fitted with an Allison 250C20B turboshaft engine rated at 313kW
(420hp) and can stay airborne for six
hours. Its maximum speed is over
185km/h (100 knots) and the mission
radius is 185km.
Pioneer flew more than 500 missions during
Desert Storm. Its missions included minehunting, naval over the horizon targeting &
overland surveillance & target location.
is 4575 metres (15,000ft), while the
endurance is six hours. It is launched
using wheels, catapult or rocket boost
along a rail.
The EI-Op TV or FLIR camera is
carried in a ventral turret and EW
(electronic warfare), decoy or other
payloads are optional. The USN and
USMC now have nine Pioneer units,
each comprising up to eight air vehicles. Six of these were deployed
before and during the Desert Storm
operations, with two operated from the
I have chosen to devote some considerable time in describing the IAI aircraft for one simple reason. In essence,
they are little more than typical model
aircraft, yet they form the nucleus of
the practical UMA movement. Here
are front-line miniature aircraft, the
likes of which can be found on model
flying fields anywhere in the world.
This really is no accident as many
of the designers are active modellers
who spend their weekends on model
flying fields.
Of course, UMAs are much more
sophisticated and expensive than
model airplanes.
Teledyne UMAs
Two other UMAs of interest before
we close for this month are the Teledyne Ryan Model 410 and the Teledyne Ryan Scarab/BQM-145A.
The Model 410 is large enough
(9.55 metres wingspan) to carry fullsized payloads but looks for all the
world like a grown-up IAI twin boom
UMA. It was designed for long-range
or long-endurance missions and was
first flown on 27th May, 1988 with an
on-board check pilot under a tear-drop
canopy. Here the circle is complete,
for we finally have what is little more
than a man-carrying model aircraft.
The Model 410 has a take-off weight
of 816.5kg and the 119kW (160hp) flat
4-cylinder Lycoming engine pushes
it along at 322km/h (174 knots). Its
maximum endurance is 22 hours, the
service ceiling is 30,000 feet and the
range is 2300km.
Here is the ultimate modeller’s toy
– just hop in and fly to the field, then
whip out your transmitter and have
a nice day of R/C flying. At the end
of the day with your Model 410, you
could then stow the Tx, change back to
manual control, hop in and fly home.
What a way to go!
For the ultra-sophisticated, we have
the Teledyne Ryan Scarab BQM-145A.
It has a wingspan of 3.35 metres, a
length 6.15 metres and weighs in at
1077kg. Fitted with a Teledyne CAE
373-8C turbojet engine rated at 970lb
thrust, the Scarab can nip along at a
handy 851km/h (459 knots). Its mission radius is 966km, while the service
ceiling is 43,000ft.
The Scarab was designed primarily
for Egypt in the mid-1980s as a groundlaunched reconnaissance UMA and
56 were subse
quently delivered. It
is launched by booster rocket from a
truck-mounted “zero length” rail and
recovery is by parachute or airbag
landing.
Here we have left the model movement far behind and on this note we
leave this most fascinating field of
human endeavour.
Acknowledgement
My thanks to Bill Herbert, Flynn,
ACT for the photo of the Jindivik aircraft featured in the May 1993 issue
SC
of SILICON CHIP.
August 1993 55
By LEO SIMPSON
BUILD
You’ve seen those late-model Japanese sports cars with a
row of pinpoint red lights in the spoiler. They look snazzy
& they draw immediate attention to the brakes being
applied. Now you can have one for your car.
This Brake Light Array uses 60
high-brightness light emitting diodes
and a few other components. The
LEDs are installed on two narrow PC
boards and they are driven so that
they light up from the centre of the
array and spread out till all LEDs are
alight. This takes place in a fraction
of a second and looks even more
eye-catching than the brake light
arrays on Japanese cars.
The Brake Light Array, or BLA for
short, is housed in a thin aluminium
channel which is 500mm wide. It can
be mounted on the parcel shelf of your
car and power can be taken from one
of the brake lights.
The total current drain of the BLA
is about 260mA which is minuscule
compared to the current of several
amps drawn by your existing brake
lights. In fact, the BLA is so bright
for such a small current that it seems
likely that brake lights in the future
will not use incandescent lamps – they
will use high-brightness LEDs.
56 Silicon Chip
Interestingly, because the circuit
has a regulated supply voltage, the
brightness of the Brake Light Array
will always be constant, regardless of
any variations in the battery voltage.
Flasher circuitry
Now have a look at the circuitry of
the BLA – see Fig.1. This looks fairly
complicated considering that it merely
lights up a bunch of LEDs. However,
the circuit could be used for other
purposes and so can be made to flash
several times in succession before the
LEDs stay on permanently, until the
power is removed.
Power for the circuit comes from
one of the brake lights. The positive
supply (+12V) is fed through a 500mA
in-line fuse and then to a 2.2Ω resistor
and 15V zener diode which protects
the circuit from any high voltage transients which could come, for example,
from door solenoids or motors.
The +12V supply is regulated to
+8V by a 7808 3-terminal regulator
which feeds all the circuitry. IC2,
an LM3914 dot/bar display driver,
is the heart of the circuit. It drives
30 LEDs in 10 groups of three and
each group of three LEDs is in series
with its particular output from the
LM3914. The LM3914 is operated in
bar mode (pin 9 connected high) and
the current through each set of three
LEDs is set at 10mA by the 1.2kΩ
resistor at pin 7.
Normally, an LM3914 is used to
A 60-LED BRAKE
LIGHT ARRAY
FOR YOUR CAR
drive a bargraph display of LEDs in
response to a signal voltage applied
to its pin 5; the more signal, the more
LEDs light up. And so it is in this
design. The signal voltage is applied
to pin 5 via transistor Q3 which is
connected as an emitter follower. Its
base signal comes from the emitter
of Q1, a unijunction transistor. Q1 is
connected as a relaxation oscillator to
produce a sawtooth waveform at its
emitter. What happens is that the 22µF
capacitor at the emitter is charged up
to about +5V via the 10kΩ resistor
and 100kΩ trimpot, VR1. Each time
the capacitor reaches the threshold
voltage of around +5V, the unijunction
(Q1) discharges the capacitor and the
cycle begins again. So Q1 is the source
of signal voltage applied to pin 5 of
IC2 via Q3.
If we neglected the effect of Q2 and
IC1, the action of the circuit presented
so far would be to repeatedly light
up the full row of LEDs. Clearly, this
would be no good for brake light
use as it would send the drivers of
following cars mad (as well as being
illegal). This is where IC1 comes into
the picture.
Each time Q1 discharges the 22µF
capacitor at its emitter, it produces a
brief positive pulse at its base 1 (B1)
terminal. This pulse is amplified,
inverted by transistor Q2 and fed to
the clock input of IC1, a 4017 decade
counter. With the aid of a link on the
PC board from its pin 13 (enable) input,
IC1 can be made to count any number
of pulses up to six whereupon it will
stop counting and its selected output
will go high. This selected output is
fed via diode D1 to the emitter of Q3
and to pin 5 of IC2. This stops Q3 from
responding to the sawtooth signal from
the emitter of Q1. Thus, IC1 will turn
all LEDs on until power is removed
from the circuit.
Master & slave circuit
The description so far tells how
LEDs 1-30 are driven. LEDs 31-60 are
driven by IC3, another LM3914 which
is “slaved” to the signal from the emitter of Q3. Thus, IC3 is forced to mimic
Below: this close-up view shows the
master board of the LED Brake Light
Array. It carries 30 high-brightness
LEDs, while the slave board carries
another 30 LEDs.
August 1993 57
58 Silicon Chip
B
4.7k
Q3
BC548
E
10k
100k
VR1
22
16VW
C
100W
B1
3
1k
MODE
6 RHI
9
Q1
2N2646
E
B2
8.2k
+V1
1
B
K
K
A
K
A
A
K
K
A
K
A
A
K
K
A
K
A
A
K
K
A
K
A
A
1.2k
E
C
REF
OUT
7
CLK
16
2
Q1
4
2
Q2
IC1
4017 Q3 7
15
10
15
RST
Q4
1
Q5
5
Q6
EN
8
13
14
14
5.6k
RLO
4
LED1LED30
K
K
A
K
A
A
BRAKE-LIGHT ARRAY
100k
0.1
REF
ADJ
8
IC2
LM3914
18 17 16 15 14 13 12 11 10
10k
Q2
BC548
SIG
5
K
K
A
K
A
A
6
5
4
3
2
1
K
K
A
K
A
A
SELECT
SWEEPS
K
K
A
K
A
D1
1N914
A
K
K
A
K
A
A
8.2k
CHASSIS
+12V
FROM
BRAKE
LIGHTS
K
K
A
K
A
A
6
9
F1
500mA
+V2
ZD1
15V
E
2. 2
RHI
MODE
3
B
1
K
K
A
K
A
A
K
K
A
K
A
A
K
K
A
K
A
A
C
22
16VW
1.2k
REF
OUT
7
B2
IN
5.6k
E
B1
REG1
7808
GND
REF
ADJ
8
IC3
LM3914
22
16VW
OUT
RLO
4
I GO
+8V
2
18 17 16 15 14 13 12 11 10
K
K
A
K
A
A
VIEWED FROM BELOW
SIG
5
K
K
A
K
A
A
22
16VW
K
K
A
K
A
+V1
LED31LED60
A
K
K
A
K
A
A
IN
K
K
A
K
A
REG2
7808
GND
A
22
16VW
OUT
K
K
A
K
A
A
+8V
+V2
K
K
A
K
A
A
CHASSIS
500mA
IN-LINE FUSE
+12V FROM BRAKE LIGHTS
ZD1
VR1
REG1
10k
22uF
Q1
22uF
100
1k
10k
Q2
Q3
8.2k
4.7k
1.2k
5.6k
D1
1
IC2 LM3914
100k
COMMON
0.1
22uF
2. 2
IC1 4017
1
2 3 4 5 6
SWEEP
LED1-LED30
K
A
22uF
REG2
8.2k
1.2k
5.6k
1
IC3 LM3914
22uF
LED31-LED60
K
A
everything done by IC2 in driving its
LEDs. IC3 and its 30 LEDs are fed by
their own regulator (REG2).
Note that we do not recommend that
this circuit be set up to provide more
than one sweep of the LEDs before
they turn on fully. Multiple sweeps
of the LEDs will be quite distracting
to following drivers and is illegal in
Australia, as far as we know.
Construction
As noted above, the LED Brake
Light Array is built on two narrow PC
boards which each measure 230 x
27mm. These boards are supplied
with a full component overlay so
assembly is quite straightforward.
One board has LEDs 1-30 on it and
it becomes the “master” while the
second board accommodates IC3 and
LEDs 31-60 and is the “slave”. We
suggest you build the master board
first and get it going before doing the
slave board.
Assemble the small components
such as links, diodes and resistors and
capacitors first, then the transistors
and in
tegrated circuits. The highbrightness LEDs come last.
▲
LED polarity trap
Fig.1 (left): the circuit uses two
LM3914 dot/bar display drivers which
respond to the ramp voltage generated
at the emitter of unijunction transistor
Q1. Decade counter IC1 controls the
number of times that the LEDs are
swept before they come on fully.
You will need to use care in assembling the LEDs so that they are all lined
up – if even one is not lined up with
the others it will stick out like a sore
thumb. The way to line them up is to
install each LED so that its leads are
just long enough so that they can lie flat
on the top surface of the board, with
the LED body butted up to the edge of
Fig.2: install the parts on the two
PC boards as shown in this wiring
diagram. Note that the leads used to
connect the boards together must be
long enough to allow the boards to be
mounted end-to-end.
the board – the accompanying photos
show the general idea.
Before we leave the LEDs, there is a
big trap to watch. We normally show
a pinout diagram on the circuit which
shows the LED polarity. The normal
convention is that the longer lead is the
anode and the lead adjacent to a flat
on the side of the lens is the cathode.
However, it is not always the case and
it could be most frustrating to assemble
30 LEDs onto the board and find that
they are all the wrong way around.
In particular, the LEDs supplied with
this project kit will be the reverse of
normal convention – the shorter lead
will be the anode. To be sure that you
assemble them correctly, check at
least one LED with a 9V battery and
RESISTOR COLOUR CODE
❏
❏
❏
❏
❏
❏
❏
❏
❏
❏
No.
1
2
2
2
1
2
1
1
1
Value
100kΩ
10kΩ
8.2kΩ
5.6kΩ
4.7kΩ
1.2kΩ
1kΩ
100Ω
2.2Ω
4-Band Code (1%)
brown black yellow brown
brown black orange
grey red red brown
green blue red brown
yellow violet red brown
brown red red brown
brown black red brown
brown black brown brown
red red gold gold (5%)
5-Band Code (1%)
brown black black orange brown
brown brown black black red brown
grey red black brown brown
green blue black brown brown
yellow violet black brown brown
brown red black brown brown
brown black black brown brown
brown black black black brown
not applicable
August 1993 59
These two views show how the master & slave boards are mounted end-to-end so that the LEDs form
a single bargraph. This version used a channel made from two angle aluminium sections.
a 4.7kΩ limiting resistor. You have
been warned.
Finally, fit the short link adjacent to
the 4017 which selects the number of
sweeps at six; ie, install a link connect
ing “common” to “6”.
After having checked your work
carefully, connect a DC power supply
set to 12V. The row of LEDs should
sweep towards the regulator end of
the board six times before all flick on
and stay on until power is removed.
You can change the rate at which the
LEDs sweep by adjusting trimpot VR1.
We suggest you set it for a sweep rate
of several times a second. This then
completes your work on the master
PC board.
Now you can assemble the slave PC
board. As can be seen from the photos
and the wiring diagram of Fig.2, the
slave board has quite a few components omitted. To be specific, those
omitted are the 2.2Ω resistor and zener
The slave board is mounted upside
down on the aluminium channel, so
that the LEDs light from the centre
outwards. Ignore the resistor shown
tacked on the back of this prototype
board – the final version has the
resistor mounted on the component
side (see Fig.2).
60 Silicon Chip
diode at the input to the regulator,
transistors Q1, Q2 & Q3, IC1, diode
D1 and all of the associated resistors
except for the 4.7kΩ and 1.2kΩ values
associated with the LM3914.
Begin the slave board assembly by
installing the two resistors, the two
wire links, the two 22µF capacitors
and the 3-terminal regulator, then
install the LM3914 and the 30 LEDs.
To complete the slave board, you will
need to run three insulated wires from
it to the master board. These include
the common ground wire (0V) and a
wire from the input terminal of the
3-terminal regulator on the master
board to the input of the regulator on
the slave board.
Finally, a lead must be run from
the emitter of transistor Q3 on the
master board to the same position on
the slave board; ie, the emitter pad of
Q3. This is the control signal wire for
the slave board.
Now check all your work carefully
again and apply 12V DC once more.
The LEDs on both boards should now
sweep towards the regulator six times
in identical fashion before flicking on
permanently.
Now we strongly suggest that the
BLA be set for only on sweep of the
LEDs before they come on permanently. To accomplish this, remove the link
between pins 13 and 5 of IC1 that was
installed previously and connect a
short link underneath the master PC
board between pins 2 and 13 of IC1.
This done, apply power again and
check that the LEDs make one sweep
and then flick on fully. Finally, set the
rate at which the LEDs sweep on by
adjusting trimpot VR1.
Mounting the boards
To make up the Brake Light Array,
the two assembled PC boards must be
positioned end-to-end with the regulators on the outermost ends. Mounted
in this way, the resulting display will
start in the centre of the two boards
and spread out to the ends until all
LEDs are alight.
We had two prototypes of the BLA.
One had the PC boards mounted in
an aluminium channel measuring 40
x 25 x 500mm long. The boards were
glued together and then secured in
the channel with small blocks of foam
plastic. The channel was mounted on
a short upright made from metal towel
rail fittings. The whole assembly was
then sprayed with flat black enamel.
The second prototype BLA used
a channel made from two angle aluminium sections measuring 25 x 50
x 500mm and secured together with
self-tapping screws. The boards were
mounted end-on on the bottom section using suitable screws, spacers,
Protect your valuable issues
Silicon Chip Binders
PARTS LIST
1 aluminium channel, 500mm
wide (see text)
2 PC boards, 230 x 27mm
1 in-line 3AG fuseholder
1 500mA 3AG fuse
1 100kΩ trimpot (VR1)
Semiconductors
60 5mm high brightness red LEDs
(LED1-60)
2 7808 8V 3-terminal regulators
(REG1,REG2)
1 4017 CMOS decade counter
(IC1)
2 LM3914 dot/bar LED drivers
(IC2, IC3)
1 2N2646 unijunction transistor
(Q1)
2 BC548 NPN transistors (Q2,Q3)
1 15V 1W zener diode (ZD1)
1 1N914, 1N4148 silicon diode
(D1)
Resistors (0.25W, 1%)
1 100kΩ
2 1.2kΩ
2 10kΩ
1 1kΩ
2 8.2kΩ
1 100Ω
2 5.6kΩ
1 2.2Ω 0.5W
1 4.7kΩ
★ High quality
★ Hold up to 14 issues
Miscellaneous
Aluminium channel mounting hard
ware, hook-up wire, screws, nuts,
spacers, washers.
★ 80mm internal width
Where to buy the kit
A kit for this project with all parts
except the metalwork is available
from Oatley Electronics, PO Box
89, Oatley, NSW 2223. Phone (02)
579 4985 or fax (02) 570 7910. The
kit price is $65 plus $3 for postage
& packing.
Note: copyright of the PC artwork
for this project is retained by Oatley
Electronics.
Price: $A11.95 plus $3 p&p each
(NZ $6 p&p). Send your order to:
★ SILICON CHIP logo printed in
gold-coloured lettering on spine
& cover
Silicon Chip Publications
PO Box 139
Collaroy Beach 2097
Or fax (02) 979 6503; or ring (02)
979 5644 & quote your credit card
number.
Use this handy form
➦
Capacitors
5 22µF 16VW electrolytic
1 0.1µF monolithic
These beautifully-made binders
will protect your copies of SILICON
CHIP. They feature heavy-board
covers & are made from a dis
tinctive 2-tone green vinyl. They
hold up to 14 issues & will look
great on your bookshelf.
Enclosed is my cheque/money order for
nuts and washers. A similar support
assembly was made from towel rail
fittings and again the whole assembly
was sprayed with flat black enamel.
The assembled BLA can be mounted
on the parcel shelf of your car, as close
to the rear glass as possible. You will
then need to make a connection to the
chassis for the 0V supply line and to
one of the brake light wires to pick up
the +12V supply. This can most conveniently be done using a “Contact”
connector. This connector is simply
wrapped around and new wire and
the wire to the brake light and then
the connector is squeezed to make a
safe and insulated connection. These
connectors are available in a pack of
four for $1.50 from Jaycar Electronics
(Cat. HP-1206).
Points to note
Two important notes about the connection to the brake light:
(1). Make sure you make the connection to the stop light filament line, not
the tail light; and
(2). Don’t forget to fit a 500mA inline fuse to the +12V line, as specified
SC
on the circuit diagram.
$________ or please debit my
❏ Bankcard ❏ Visa ❏ Mastercard
Card No:
______________________________
Card Expiry Date ____/____
Signature ________________________
Name ___________________________
Address__________________________
__________________ P/code_______
August 1993 61
VINTAGE RADIO
By JOHN HILL
How to deal with block capacitors
As a young lad, I saw quite a few radio sets
come and go from my bedroom. Each one
was the ultimate receiver – that is, until
something better replaced it.
My first sets were a couple of crystal
sets which served me well for many
years. Following these were the regenerative receivers: several 1-valvers, a
2-valver and even a 2-valve shortwave
set with plug-in coils. I spent a fair
amount of my time building receivers
and listening to them. There is nothing
quite like the satisfaction of making
something that actually works. Looking back, I have very fond memories
of those bygone days.
After the home-made battery sets
had run their course, I spent up big
and bought a mains-powered set – my
first big purchase. It was only half a set
really, just a chassis and speaker that
I bought from a kid at school for 30
shillings. Unfortunately, my memory
is not good enough to recall all of the
details and I wish now that I could
remember them more clearly.
The set involved was a 4-valve regenerative detector type receiver. I still
have the single gang tuning capacitor,
so that aspect of it is fairly clear in my
mind. There was no dial, just a knob
fitted to the tuner shaft. It took a steady
hand to tune it to stations at the high
frequency end of the dial.
I distinctly remember that one of the
valves was very large, blue in colour
and extremely hot when it was working. I would just about bet a week’s
This tuning capacitor is all that remains of the author’s
first mains-powered receiver. The set used large block
capacitors for smoothing the high tension rail – common
practice prior to the advent of the electrolytic capacitor.
62 Silicon Chip
wages that it was an E406. A couple
of other valves were silvery looking
5-pin triodes and there must have been
an old 280 rectifier or the like in the
line-up as well.
The chassis was a metallic bronze
colour which seemed to be pretty
classy at the time. No doubt, it was just
one of those cheapies that were made
in the early depression years.
Block capacitors
This old AC receiver had two
volume controls (one being the reaction control), a feature that was
not uncommon in those days. It also
had two large pressed steel covers
mounted on top of the chassis and
these housed the power transformer
and block capacitors. It was that can
full of capacitors that finally caused
the demise of my pride and joy and
the set was eventually cannibalised
for spare parts.
This block capacitor contains three separate 0.5µF
capacitors & their capacitance is clearly marked on the
side. In this instance, each capacitor is separate & none is
connected internally to the case.
VINTAGE
RADIO
We are moving in February 1994
MORE SPACE! MORE STOCK!
Radios, Valves, Books, Vintage Parts
BOUGHT – SOLD – TRADED
Block capacitors were usually housed in large metal cans. The “Chanex” can at
left houses three 0.5µF capacitors, while to its right are a 4µF capacitor (middle)
and two 1µF capacitors. Chanex capacitors were made in Australia.
Send SSAE For Our Catalogue
WANTED: Valves, Radios, etc.
Purchased for CASH
RESURRECTION
RADIO
Call in to our NEW showroom at:
242 Chapel Street (PO Box 2029),
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Phone: (03) 5104486; Fax (03) 529 5639
EXCITING CAREER
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FOR THE ELECTRONIC
COMPONENTS INDUSTRY
This old block capacitor has suffered a terminal internal disorder. No doubt
something like this happened to many block capacitors when the paper
dielectric broke down and allowed them to short circuit.
Many early sets used block capacitors. These units were nothing more
than paper capacitors in metal cans
instead of the cardboard tubes that
were to become the norm in later years.
Although the term “block capacitor”
strictly refers to metal-cased paper
capacitors of quite large size, the comments made in this article include all
metal-cased paper capacitors, even the
smaller sizes.
AC-operated receivers required
much larger capacitors than any battery set had needed up until that time.
Mica capacitors of relatively small
sizes were adequate for battery sets but
this situation changed with the advent
of mains-powered radios.
Initially, paper capacitors were used
in the high tension filter instead of
the electrolytics that were to become
common a few years later. A pair of
4µF paper capacitors did a reasonable
job of smoothing out the mains hum
when used in conjunction with a
loudspeaker field coil (the latter acting
as a choke).
Unfortunately a pair of 4µF paper
capacitors take up a sizable amount
of space. It was common practice at
this stage of receiver development to
place all the big bulky capacitors in
a large pressed steel can instead of
having them situated throughout the
circuit as would be the case a few years
down the track.
When hot wax, smoke and ominous rumbling sounds poured forth
Location: Chatswood, Sydney, NSW
Sales: Territory NSW and Qld.
Altronics Distributors of Perth, Western
Australia have a position for a dynamic
young person for their Sydney Office.
Applicants should be conversant in general purpose electronics and be familiar
with common electronic components.
Formal qualifications in Sales and/or
Management would be an advantage.
A current drivers' licence and a reliable
vehicle is required.
The successful applicant will be appointed initially as Assistant Sales Manager
with a view to promotion to the position
of Manager NSW and Qld in approximately 12 months.
This is an exciting and rewarding career
in Electronics.
Apply to Colin Fobister, Sydney Office.
Phone: (02) 417 8938; Fax: (02) 417 2670.
August 1993 63
This view shows the contents of a typical block capacitor.
This one contained five individual units which could
only be connected as a single unit into the circuit. The
can formed a common chassis connection for all five
capacitors.
from my old regenerative’s capacitor
box, it appeared as though the end
had come. Knowing what I know
now, I guess it wouldn’t have been
a difficult problem to repair but as a
14-year old, it seemed like the end of
the world. What a terrible feeling to
see 30 shillings self-destruct before
your eyes.
At a rough guess, I would say that
the input capacitor on the high tension
filter developed a short circuit. This
is not an unknown happening, even
with electrolytics, and a sure sign of
this problem is the rectifier anodes
glowing red.
Block capacitors are no different
to any other old paper capacitor and
require exactly the same treatment.
The difference in size between a 4µF block capacitor and a
couple of modern 22µF 450V electrolytics is illustrated by
this photograph. Fitting modern capacitors into an old can
is easy as far as space is concerned but getting the cans
apart without wrecking them can be another matter.
That’s right! Discard them completely
and replace with modern equivalents
whether they be polyester or electrolytic. There is no room in any of my
receivers for leaky, troublesome 60year old paper capacitors.
Early paper capacitors were made in
two types: inductive and non-inductive. The inductive type was suitable
only for some applications and could
not be used if the capacitor was required to pass RF signals.
Rolled foil capacitors were made
non-inductive by a very simple trick.
The metal foils were made slightly
wider than the paper dielectric and
offset slightly relative to each other,
so that each protruded from one end
of the roll. A connection was then
Despite its age (at least 60 years), this capacitor still registers it true capacitance
on the meter. How it would perform with 250V across it is quite another matter.
64 Silicon Chip
made to each foil by means of a rivet
which connected all the turns of the
foil together.
Block capacitors vary greatly in size.
Some are relatively small in size and
capacity while others, as previously
discussed, are quite large. Many of the
larger capacitors are not singular in
construction but have multiple units
inside them. In fact, they can have as
many as four or five separate capacitors
in the one casing.
Some electrolytic capacitors were
also built into metal cans, usually in
pairs. In other instances, they were
packaged in cardboard containers.
Common problems
There is a reasonable possibility
of encountering block capacitors in
any mains-powered radio from the
late 1920s to the end of the 1930s. A
1939 German SABA receiver I worked
on recently used quite a large block
capacitor.
One problem frequently encountered when replacing block capacitors
is that, in some instances, there are
no identifying markings on the can
to indicate the capacity or the voltage rating of the capacitor. Some are
clearly marked but others are not. This
can be a problem at times but usually
a solution can be found.
Often, particularly where quite large
capacitances are involved, it doesn’t
make a great deal of difference if the
replacement capacitor is half or double
that of the original value.
I have cut 0.5µF capacitors out of
circuit while a receiver is working
only to find that their removal makes
no apparent difference to the set’s operation. In this case, virtually any size
replacement capacitor would work
OK. On the other hand, capacitors
from some parts of the circuit need to
be of a particular capacitance or fairly
close to it.
Usually however, the capacitance is
not critical and a ballpark value will
work just as well. A substitution box
can be a great help when replacing
capacitors of unknown value.
One way out of the unknown value
dilemma is to measure the old capacitor with a capacitance meter. Although
an ancient paper capacitor may be
leaky, it will usually register its value
with reasonable accuracy on a capac
itance meter. A capacitance meter tests
a capacitor at a potential of only a few
volts and any leakage at those levels
is usually only slight. It can behave
quite differently when 250V is applied
to it, however.
If a capacitor fails the meter test, its
value can often be guesstimated by its
physical size.
The capacitance meter can also
be very handy when replacing those
larger blocks which contain four or
five separate capaci
tors. If the capacitance value of each unit can be
determined, then their substitution
is much easier.
Multiple block capacitors come in
two types: some have a number of different leads coming from them, while
others have connection lugs at the top.
With the first type, each wire connects
to one contact of an internal capacitor,
while all the other contacts share a
common connection to the inside of
the can. In other words, bolting the
can to the chassis effectively grounds
one side of all the capacitors.
Thus, if there are four wires coming from the can, then there are four
capacitors in the block and the can is
the chassis connection.
The other type does not have an internal common connection to the can
and individual units can be connected
singularly or in parallel as required;
eg, the 1.5µF block capacitor shown in
one of the photographs can be wired
into the circuit as a single 1.5µF capacitor, as three 0.5µF capacitors, or
as two capacitors with values of 1µF
and 0.5µF.
When replacing block capacitors,
there is no reason why the new capacitors cannot be placed inside the old
These two block capacitors have values of 4µF (left) & 6µF. Block capacitors
were very large by today’s standards & they took up a considerable amount of
space.
Many early tubular paper capacitors carried the inscription “non inductive”
to distinguish them from earlier inductive types. They used an extended foil
construction similar to that used for modern paper & polyester capacitors.
can if so desired. Sometimes, however,
this is easier said than done because
the can may prove difficult to open
without wrecking it.
In my old 3-valve Seyon, the 280
rectifier originally teamed up with
two 1µF paper capacitors which
were used in the high tension filter.
Unfortunately, such a small amount
of ca
pacitance does not do the job
particularly well and the hum level
is quite objectionable.
When restoring the set, the original
Philips capacitors showed considerable leakage when tested and they
were replaced with modern 1µF
350V electrolytics. Being relatively
inexperienced in valve radio repairs
at the time, it never occurred to me to
increase the capacitance. There was
plenty of room inside the cans to accommodate larger units which would
have greatly reduced the mains hum.
In summary then, block capacitors
should not present any real problems
for vintage radio repairers. They are
simply paper capacitors that should
be replaced if a restoration is to be
effective and reliable. Whether or not
the original can is used to house the
replacement capacitors is entirely up
SC
to each individual restorer.
August 1993 65
SILICON
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Rod Irving Electronics Pty Ltd
SILICON
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has requested that the page be removed to
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Rod Irving Electronics Pty Ltd
SILICON
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which is now out of date and the advertiser
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Rod Irving Electronics Pty Ltd
SILICON
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which is now out of date and the advertiser
has requested that the page be removed to
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AMATEUR RADIO
BY JAMES MORRIS, VK2GVA
A look at satellites & their orbits
Amateurs are in the privileged position of
having access to experimental satellites which
provide a range of technical & operational
challenges. This month’s article discusses some
of the basics of satellite orbits.
The laws of planetary motion were
first described by Kepler and Newton
in the 17th century and they also apply to the motion of satellites around
the Earth. Kepler’s first law states that
the orbit of a satellite is an ellipse
(Fig.1a). The satellite’s closest point of
approach is called the perigee, while
the apogee is the orbital point furthest
from the Earth. The shape of the ellipse
is determined by the semi-major axis
(a) and the eccentricity (e). When the
eccentricity is zero, the shape of the
orbit is circular.
Kepler’s second law states that
equal areas are swept out in equal
times by the satellite’s radius to the
Earth, so that the satellite’s velocity
as seen from the Earth will vary, being maximum at the perigee (Fig.1b).
For circular orbits, the velocity of the
satellite is constant.
Kepler’s third law describes the way
in which there is a fixed relationship
between a satellite’s height and its
orbital period, with smaller orbits
containing faster moving satellites –
see Fig.1c.
Kepler’s laws, in conjunction with
Newton’s laws, can be used to fully
describe the orbit of a satellite around
the Earth, resulting in a mathematical
model with six constant terms. These
constants are called orbital or Kepler
ian elements.
The inclination of an orbit is the
angle between the orbital and equatorial planes (Fig.2a). When a satellite moves in the same direction as
72 Silicon Chip
the Earth’s rotation, it is said to be
in a prograde orbit. Satellites which
follow retrograde orbits move in the
opposing direction (Fig.2b). The most
commonly used orbit is geostationary,
where the satellite moves at the same
speed as the Earth’s rotation, and has
an inclination of 0 degrees.
A geostationary satellite appears at a
fixed location in the sky, so that it can
provide a continuous communications
link between ground stations within
its “footprint”. The use of satellites
in geostationary orbit for global communications was envis
aged by the
scientist Arthur C. Clarke in 1945. His
calculations, based on Kepler’s laws,
showed that geostationary satellites
would orbit the equator at a height of
approximately 35,786km. This unique
orbit is known as the Clarke belt, and
contains many satellites which are
“parked” in “slots” above the equator.
The Optus series of satellites are located in the assigned slots: 156°, 160°
and 164° east.
Recently, there have been proposals
made by amateur groups to establish
geostationary communications links
with the development of the Phase
IV series amateur satellites. This new
generation of Hamsats could provide
some very interesting possibilities for
long distance voice, packet and image
communication.
Polar orbiting satellites pass over the
north and south polar regions (Fig.2b).
The NOAA weather satellites follow
polar orbits which are also sun-syn-
chronous, passing over the same
points at the same local times each
day. This allows the same areas of the
Earth to be imaged under reasonably
consistent lighting conditions.
The footprint of a sun synchronous
polar orbit satellite overlaps itself
during successive passes. SARSATS
(search and rescue satellites), which
often share a common space platform
with weather satellites, utilise this
footprint overlapping to obtain accurate readings for the position of ELT
(emergency locator transmitter) and
EPIRB (emergency position indicating
radio beacon) devices.
A rather specialised orbit is used
by the Russian Molniya satellites,
which are inclined at approximately
64°. Their orbits are optimised to
provide telecommunications for areas
located at high northern latitudes,
as geostationary satellites cannot be
seen from locations above 81° north or
south. Molniyan orbits are also highly
eccentric, and remain within view
of targeted regions for many hours;
a specific appli
c ation of Kepler’s
second law.
Low Earth orbits
Low Earth orbit satellites (LEOS)
follow fast, almost circular orbits and
are relatively inexpensive to implement (approximately 1/20th the cost
of geostationary). LEOS orbits are used
extensively by small satellites which
gather atmospheric and other scientific
data. Many amateur satellites make use
of near-polar low Earth orbits with an
inclination of greater than 80°.
Amateur LEOS are able to rapidly
upload and download information
around the world, making them ideal
vehicles for packet BBS (bulletin board
systems), which have been used for
primary international communications during disasters. The excellent
MAJOR AXIS, A
ORBIT
SATELLITE
EARTH
PERIGEE
APOGEE
SEMI-MINOR
AXIS, b
MINOR AXIS, B
world-wide coverage and low cost of LEOS also provides a
strong commercial potential. Currently, there are a number
of proposals for global personal communications on the
corporate drawing boards.
A disadvantage of LEOS is the amount of tracking required at the ground, as they tend to move rather quickly.
This is partially offset by the fact that the satellites are
closer to the Earth, with the associated increase in signal
strengths. Lower gain antennas may be used, which often
have broader directional characteristics and less critical
aiming requirements.
Orbital perturbations
The Earth has a slight bulge at the equator and a
flattening of the poles; its true shape is as an oblate
spheroid. This complicates the determination of satellite motion, as Kepler’s laws assume the Earth to be
perfectly spherical.
The Earth’s mass is not evenly distributed, producing
minor variations in the gravitational forces acting on its
satellites. The difference in gravity experienced at two
points in an orbit produces a ‘gravity gradient’ or slope.
A satellite will be more attracted to one of these points,
and accelerate towards it.
Geostationary satellites are attracted towards the positions of 75° E or 105° W, and require regular ‘station
keeping’ to prevent their inevitable slide towards what
are commonly referred to as satellite graveyards (orbital
points situated between gravitational ‘bulges’).
A recent example of this effect occurred in 1992, when
two ARABSAT series spacecraft suddenly ran out of station keeping fuel. They began to drift along the Clarke belt
towards 75° E and although still otherwise operational,
were eventually powered down to prevent interference
to other satellites.
The gravitational fields of the sun and moon significantly affect geostationary satellites, by inclining their orbits
away from the equator. The LEOS are less affected, due
to the increased effect of the Earth’s gravitational field at
close range. Again, station keeping is required to correct
the orbit of satellites affected, by the firing of onboard
thrusters in the opposite direction of the drift.
At heights of below approximately 1000km, satellites
are affected by atmospheric drag, which serves to reduce
the eccentricity and apogee height of their orbits. Atmospheric drag can be a particular problem for low Earth
orbiting satellites.
Attitude
The orientation of a satellite in its orbit with respect
to the Earth is its attitude, which is maintained through
attitude control. This differs from station keeping in that
the shape of the orbit is not of prime concern. Attitude
control is used for local stabilisation.
To simplify the stabilisation of satellites in low orbits, the
gravitational field of the Earth is utilised. After launch, the
spacecraft gradually aligns itself vertically with the Earth,
so that the antennas are pointing in the desired direction.
During this time, amateurs monitoring the satellite’s beacon may notice periodic fading as the satellite ‘oscillates’
around the stable attitude. This effectively modulates the
beacon, an effect used to help determine the status of the
satellite in the initial orbit stage.
SEMI-MAJOR AXIS, a
2
a b
a
ECCENTRICITY OF ORBIT, e =
2
PERIGEE HEIGHT = a(1 - e) 6378km
APOGEE HEIGHT = a(1 + e) 6378km
(a)
SATELLITE NEAR
PERIGEE
V2
A2
T2
A1
PERIGEE
T1
APOGEE
V1
SATELLITE
NEAR
APOGEE
EARTH
ORBIT
(b)
PERIOD ~= 105 MINUTES
HEIGHT =
1000km
r
V ~=
26000km/h
EARTH
r=
6378km
LOW
ORBIT
HIGH
ORBIT
HEIGHT = 35786km
VELOCITY ~= 11000km
PERIOD = 24 HOURS
(c)
Fig:1: this diagram illustrates Kepler’s Laws of
planetary motion which also describe the orbits of
satellites around the Earth. Note that at apogee the
satellite is travelling at its slowest speed.
Geostationary satellites, which generally carry telecom
munications and broadcasting, are too far from the Earth
for gravitational torque stabilisation to be efficient. These
satellites are stabilised by two basic methods. An entire
satellite may be set spinning, in the manner of a gyroscope.
The antennas must then either have circular symmetrical
radiation patterns, or be placed upon a non spinning
(despun) platform.
Alternatively, internal stabilisers may be used, in the
form of momentum wheels, which provide the necessary overall stabilising torque. Satellites which use this
August 1993 73
N
The point directly
underneath the satORBITAL
PLANE
ellite at the Earth’s
SATELLITE
surface is called the
sub satellite point
(SSP).
Radio frequenEQUATORIAL
cies
received at the
PLANE
EARTH
i°
ground appear to
vary from high to low
i° = INCLINATION
during the satellite’s
pass overhead, due to
the effect of Doppler
(a)
shift (Doppler shift
is a phenomenon
N
associated with the
POLAR ORBIT
behaviour of waves
HEIGHT ~= 1000km
propa gated from a
moving transmitter).
The nominal freORBIT
quency of a particular
beacon or transponder (transponders are
HEIGHT 35786km
EQUATOR
devices which, upon
receiving signals,
5F 8 180 o
164 o
automatically issue
160 o
responses) is given
156 o
for the TCA, when
the Doppler shift is
B2P
113 o
zero.
(b)
In the case of satFig.2a illustrates the inclination of a satellite orbit,
ellite AO-21, with a
while Fig.2b shows the geostationary orbits of the
Optus satellites at around 160°E, the Intelsat 5F8
nominal downlink
satellite at 180°E & the Palapa B2P satellite at 113°E.
of 145.987MHz (FM
voice), the received
method are called three-axis or body frequency may vary from approximatestabilised.
ly 145.990MHz at AOS to 145.984MHz
To correct for errors in spacecraft at LOS. The effect of Doppler shift
attitude, a variety of techniques are is greater for passes which are more
used, such as firing thrusters, accel- directly overhead.
erating the momentum wheels, and
AO-21 is a LEOS with a near polar
employing reaction wheels to absorb orbit of 83° inclination. Apogee and
the effects of disrupting forces.
perigee heights are 1000km and 958km
respectively. The orbital period is
Tracking
about 105 minutes, and a good pass
Tracking a satellite involves locating may last for 20 minutes.
The FM voice transponder uses an
its position in orbit and determining
its motion. This information is referred experimental digital processing systo the Earth’s motion, so as to provide tem which is used to regenerate weak
pointing coordinates (look angles) for or distorted signals. The downlink
a station’s antenna system. Times at frequency, as mentioned, is approxiwhich the satellite will be visible to mately 145.987MHz.
the station are calculated, and the
A beacon on 145.822MHz (CW) is
feasibility of communications with quite useful for tracking, even with
the satellite during these times are an FM receiver. Due to the relatively
evaluated.
wideband nature of the FM signal, it is
The time at which a satellite appears not necessary to use an expensive mulover the radio horizon, and beacons timode rig to tune in. Try 145.990MHz
or other transmissions are received, as a starting frequency on which to
is known as the acquisition of signal monitor the satellite.
(AOS). The time of closest approach
Some handheld transceivers can
(TCA) and loss of signal (LOS) then be tuned in 5kHz and 12.5kHz steps,
describe the completion of the pass. giving a series of three frequencies
74 Silicon Chip
(145.990MHz, 145.9875MHz and
145.985MHz) to track Doppler shift.
Receive antenna requirements
for this satellite are minimal and a
¼-wave ground plane should give
good results.
The uplink frequency for this transponder is 435.016MHz, making it
“mode B” in hamsat terminology. The
uplink requirements are a little more
involved. Power levels in the range
of 25W are considered the minimum
useful level, although AO-21 has been
worked with a dual band hand-held
(WA5ZIB/KB8KVY).
By using a predictive tracking program, it would be possible to determine the best time to listen out for the
satellite, although it is also possible to
just tune in and wait.
After the first pass, add 105 minutes
to the AOS to give an indication of
when the next pass might be (given
that the satellite will be in view at the
next pass). For those with a computer,
a tracking program is essential for
detailed orbital analysis and more
advanced satellite experimentation.
These programs require a set of
up-to-date Keplerian ele
ments for
each satellite being studied, which
are available from bulletin boards in
a standard format.
Further information
Amateur satellite information is
available from AMSAT Australia. Their
HF net meets on Sundays at 1000z
(UTC). Net frequencies are 7.064MHz
and 3.685MHz, depending on conditions. AMSAT Australia is at GPO
Box 2141, Adelaide 5001. Public domain satellite tracking programs and
NASA-issued Keplerian elements are
available from the Satcom Australia
BBS on (02) 905 0849.
References
(1). The Inclined Orbit Satellite Tracking Guidebook, M. Long & J. Keating,
MLE Inc, 1993 (available from AvComm Pty Ltd, PO Box 225, Balgow
lah, NSW 2093).
(2). Satellite Communications Systems, G. Maral & M. Bousquet, John
Wiley & Sons, 1986.
(3). Satellite Communications, T. Pratt
& C. Bostian, John Wiley & Sons, 1986.
(4). Advanced Electronic Communications Systems, W. Tomasi, Prentice
Hall, 1987.
(5). Satellite Communications, D.
SC
Roddy, Prentice Hall, 1989.
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CHIP
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more than likely that it contained advertising
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PRODUCT SHOWCASE
Acorn’s 16-bit
PocketBook
If you’re always on
the move but still need
information at your
finger tips without the
bulk of a portable PC,
then take a look at the
new PocketBook from
Acorn Computers. It
measures just 63 x 43
x 6mm and runs off
two ‘AA’ cells or an
optional 9VAC 150mA
plugpack. It’s small
enough to fit inside
your coat pocket yet
powerful enough to
handle a wide range of tasks.
The PocketBook comes with several
software packages built-in including
word-processor, spelling checker,
spreadsheet, clock with alarm, scientific calculator and database. Any of
these can be selected by using eight
softkeys which form part of a graphical user interface similar to Microsoft
Windows. It uses a CMOS variant of
the 8086 running at 3.54MHz and also
includes optional internal hard disc
storage and 256Kb of main memory.
Designed with students at school
and university in mind, the Acorn
PocketBook is aimed at bringing the
world of computers closer to students
who can not only do their homework
and assignments at home but down
load them with an optional serial link
to other Acorn 32-bit micros at school.
Low cost
pH meter
This low cost pH meter is not
much larger than a bulky felt-tip
pen. It has a small liquid crystal
display and comes with a buffer
solution for calibration. Using it is
simple. Pull the protective cap off
the bottom of the unit and switch
it on. Dip it in the solution to be
measured and stir gently for a few
seconds. Then read the LCD, turn
the unit off and replace the protective cap. Calibration is done with
the supplied buffer solution and
adjustment is via a small screwdriver which is supplied.
The unit will read pH from
0-14.0 with resolution of ±0.2pH.
It uses four 1.4V mercury batteries
(675H or equivalent) and battery
life is estimated at 1000 hours.
The serial link can transfer data at a
fast 1.54Mbits/second. It’s also suitable for professionals who need access
to numbers and data without the bulk
of even a laptop PC.
The unit has a 58-key softkey QWERTY keyboard, an 8-line x 40- character
LCD and a back-up battery to retain
data when you change the main batteries. You can also install solid-state
drives on which you can save your
files using the menu button on the
keyboard, which brings up a menu
system similar to Windows.
Files are saved in MS-DOS format
with directories and 2-part filenames,
allowing users familiar with PCs to
be quickly up and running. You can
also print out files with the optional
Centronics parallel printer interface
and include information such as page
set-up and fonts.
The PocketBook comes with two
well-produced and comprehen
sive
manuals and retails for $695. For
schools, the deal is $599 which is a
great price for what essentially is a
computer, not a pocket organiser. If
you’d like more information on the
Acorn PocketBook or other Acorn
products, call Peter Revell at Acorn
Computer Australia on Melbourne
(03) 419-3033.
Surface mount
transistors for radios
The unit will have wide application in pH measurement
of swimming pools, aquariums,
water quality, aquaculture and so
on. The unit is available from all
Dick Smith Electronics stores and
is priced at $129.00 (Cat. Q-1403).
These new SOT-323 and SOD-323
surface mount transistors and diodes
are only 1.25mm wide and between
1.7mm and 2mm in length. Siemens
is the first company in Europe to supply tuner diodes of this design. The
components are also available on 8mm
tape for series equipment production.
August 1993 79
For further information, contact
Mark Walsh, Siemens Ltd, Electronic
Components Department, 544 Church
St, Richmond, Vic 3121. Phone (03)
420 7345.
Weatherproof
loudspeakers
Pictured above are a pair of weatherproof loudspeakers which are made
in Australia. The enclosure is based
on a very strong aluminium extrusion
which is finished in powder-coat
enamel, while the end-caps are made
of Luran UV-resistant plastic. The
speaker grille is made from steel mesh
that is also powder coated.
Inside, the two speakers are coax
ially mounted – a small dome tweeter
and a carbon-fibre woofer, both with
Kaptan high-temperature voice coils
and Barium ferrite magnets. The
enclosure is ported and its stated
frequency response is from 110Hz
to 15kHz.
Branded Redback, these rugged
loudspeakers may be used in a wide
range of applications such as inside
or outside the home, in hotels, clubs,
80 Silicon Chip
schools and other public address uses.
Several models are available with
either 30 or 60 watt power handling.
For domestic use there is a model
with 8-ohm impedance, while for PA
use a unit with an in-built 100V line
transformer is available.
This has multiple taps to allow it
to be used at maximum power levels
of 10, 20 or 30 watts in the case of the
lower power model, or 20, 30 or 60
watts for the higher power model. All
models are also available finished in
white rather than black.
Further information on the Redback
range of weatherproof loudspeakers
can be obtained from any Altronics
stockist or from Altronics Distributors,
174 Roe Street, Perth, WA 6000. Phone
(09) 328 2199.
Digital sound
level meter
How often have you wanted to
measure the loudness of sounds you
are experiencing? Perhaps you have
wanted to measure the sound level
of passing traffic (especially those
noisy garbage trucks late at night) or
perhaps you have wanted to know just
how quiet your hifi listening room is.
And for your neighbours’ sake, you
might also want to know how loud it
is when you turn up the volume on
your amplifier.
For more serious applications, you
might want to measure sound levels
inside and outside factories, or you
may want to measure the exhaust
noise from trucks to make sure they
comply with noise regulations. For
all those tasks you need a sound level
meter and this model from TES is just
the ticket.
The Tes 1350 sound level meter has
a 3½-digit liquid crystal display which
indicates sound levels in dB. The
instrument has two ranges: 35-100dB
(LO) and 65-130dB (HI). Measurements can be taken with either A or C
weighting and the response can be set
to fast or slow. In the fast mode, the
meter averages sound over a period of
0.2 seconds, while in the slow mode
it averages sound over a 1.5-second
period.
More importantly, the meter has a
“max hold” facility so that you can
record the loudest sound over a short
period of time; the stored reading
reduces by less than 1dB every three
minutes. An internal calibration signal
at 1kHz is also provided, allowing you
to calibrate the meter for a level of
94dB. Quoted accuracy is within ±2dB
and resolution is ±0.1dB. Frequency
response from the electret microphone
is typically from 30Hz to 12kHz.
For acoustic analysis applications,
the meter has AC and DC outputs
available via a 3.5mm stereo jack
socket.
The meter is powered from a 9V
alkaline battery and the battery life is
quoted as approximately 100 hours. It
is supplied with a foam-lined carrying case and comes with a miniature
screwdriver for calibration.
The TES 1560 digital sound level meter is available from Jaycar
Electronics stores at $259.00 (Cat.
QM-1580).
CD-ROM database for
all semiconductors
IC/Discrete, the world’s largest semi
conductor database, is now available
on CD-ROM at a subscription price
of $4,500. This price includes the
IC/Discrete parameter database and
52 CD-ROM image discs containing
scanned manufacturers’ data sheets
(scanned at 300 dpi). Any page of information can be printed out on any
standard laser printer. Images may
also be downloaded to disc for use in
CAD systems.
The database contains around
1,500,000 devices and their parameters (940,000 currently available
and 530,000 discontinued devices),
1,900,000 suggested alternatives, 1200
manufacturers and 664,000 data sheet
pages. It also includes Australian and
overseas distributors, pinout information and the ability to add in-house
part numbers.
The database may be searched
using eleven different criter
ia, including part number, generic number,
characteristic parameters, function,
keyword, manufacturer’s part number
and so on. System requirements to run
IC/Discrete are an IBM or compatible
80286 AT or better, 640Kb RAM or
more, a hard disc drive with at least
3Mb free, a VGA monitor, DOS 3.1
or later and a CD-ROM drive with
controller card.
For further information, contact
Greg Jenkins, Hintons Information
Services, 10 East Parade, Eastwood
NSW 2122. Phone (02) 804 6022.
Hewlett-Packard’s
colour inkjet plotter
CAD users will be interested in
the new HP DesignJet 650C plotter, a
colour and monochrome inkjet plotter,
intended for people who typically plot
20 or more designs per day.
The HP DesignJet 650C plotter is
available in two models – the AO size
(36 inches wide) for $16,999 and the
A1 size (24-inches wide) for $13,998.
Prices have also been reduced on the
AO and A1-size HP DesignJet 600
monochrome inkjet plotters to $12,688
and $10,688, respectively.
The plotter’s four ink cartridges,
in cyan, yellow, magenta and black
(CYMK), let users create a full range
of colours. Users can design detailed
plots that use colour to differentiate
data and highlight specific areas. For
instance, colour can be used to show
various layers of electronic circuits
or changes to an existing design plan.
The plotter features three modes of
operation – draft, final and enhanced
– for monochrome and colour, so users
can choose from a variety of levels of
speed and print quality. The highest
print quality is 300 dots per inch
(dpi) colour and addressable 600 dpi
monochrome. In the enhanced colour
mode, the plotter takes a second pass
to produce smooth, even area fills.
For further information, contact an
authorised dealer or Hewlett-Packard
by phoning (03) 272 2651.
VIDEO
& TV
SERVICE PERSONNEL
TV & VIDEO FAULT LIBRARIES
AVAILABLE AS PRINTED MANUALS $90 EACH + $10 DELIVERY
BOTH MANUALS VIDEO & TV
$155 + $15 DELIVERY
OR AS A PROGRAM FOR IBM COMPATIBLES $155 + $10 DELIVERY
FOR MORE INFORMATION
CONTACT
TECHNICAL APPLICATIONS FAX / PHONE (07) 378 1064
PO BOX 137 KENMORE 4069
August 1993 81
THE SOUTHERN
A single board Z80-based compute
Here is a single board computer designed especially for
the 1990s generation of students. With a series of addon boards, smart sockets, fully commented Monitor & an
intelligent EPROM emulator, it can teach many aspects
of microprocessor & microcontroller techniques of
programming.
By PETER CROWCROFT & CRAIG JONES
82 Silicon Chip
board computer (SBC) in
the early 80s will remember
how quickly their limitations were
met. The worst was that when you
had written a program of about 6080 lines of code, the calculation of
forward and backward subroutine
jumps and the actual data entry
became a real chore. Second, there
was no easy way to store your work
when you turned off the power to the
board. Third, some SBC suppliers
did not publish their Monitor and so
disregarded a whole area of teaching
programming and worked against the
very aim that the SBC was supposed
to promote.
With the advances in electronics
over the last few years there was an
opportunity to launch a modern, updated SBC. It had to meet all the above
objections. But it had to be more; it had
to be able to introduce students to the
real world of current day µP and µC
programming techniques. We wanted
to be able to take a student who had
never programmed before and after a
few hours (after the kit was constructed) have them writing programs using
Monitor system calls and software and
KEYBOARD
DISPLAYS
Z80
POWER
SUPPLY
MEMORY
DECODER
ROM
RAM
Fig.1: the concept of the Southern Cross is simple with a
Z80, RAM, EPROM & decoding.
also look at how to use the routines in
the Monitor for your own programs
and how to do software and hardware
single stepping to debug your own
programs. Full documentation on
programming the Southern Cross SBC
is contained in the user manual which
comes with the kit.
Features
The Southern Cross comes on a
large, single-sided PC board measuring 248 x 130 mm. It is
designed around a Z80
microprocess or and
nine CMOS ICs. The
system runs at 4MHz
but a speed con
trol
has been built into the
board for those times
that speed control is
more efficiently carried out in hardware
than in software.
All the circuit features of the Southern
Cross are shown in the
block diagram of Fig.1.
The complete circuit
is shown in Fig.2. In
the bottom lefthand corner of the circuit is the 5 x 4 keypad and 74C923
keyboard encoder (IC9). The 74C923
continuously monitors the keypad
matrix, looking for a keypress. When
one is detected, it produces a 5-bit
number and its pin 13 output (Data
Available) is set high. Two capacitors
are connected to the 74C923. C9 sets
the speed at which the chip scans the
keypad matrix while C11 provides
keypad debouncing.
The 5-bit data from IC9 is buffered
by IC8, a 74HC244 octal Tristate buffer, which feeds the data bus. The Z80
N CROSS
er for the 1990s
hardware interrupts, almost before
they knew it.
In the first article of this series, we
will introduce the Southern Cross
SBC, its features, its circuit diagram
and describe the construction.
In future articles we will look at
how to connect it to a Personal Computer to aid in code development and
introduce two add-on boards which
give the Southern Cross SBC access
to the outside world. Further on, we
will introduce an EPROM emulator
and look at how it can be used with a
PC for program development. We will
I/O
DECODER
CLOCK
controls IC8 through the I/O address
decoder chip IC3. The keyboard buffer
chip (IC8) has two unused input lines.
These have been taken to connector
CN4 where they are available for
other uses.
Output interface
The output interface consists of
six 7-segment common cathode LED
displays and an 8-ohm loudspeaker
driven by transis
tor Q7. Latch IC1
drives the display segments and
decimal points via two resistor networks, SIL1 & SIL2. Latch IC4 drives
the common cathodes of each display
as well as the speaker via seven NPN
transistors.
Both latches IC1 & IC4 are controlled
by I/O decoder chip IC3. IC4 has one
unused output line (pin 16) which
is taken to connector CN4, as is the
speaker output line.
The core of the Southern Cross consists of the Z80 (IC6), the I/O address
decoder (IC3), memory decoder (IC2),
RAM (IC7) and EPROM (IC6).
The reset circuit consists of pushbutton switch S21 in conjunction
with resistor R19 and capacitor C15.
Pressing the reset button resets the Z80
CPU and the display latch IC4. R19
and C15 also provide the power-on
Fig.2 (following page): this is the
complete circuit of the Southern
Cross computer. It has a 5 x 4 keypad
for data entry & program execution &
a 6-digit display as the major output
interface.
August 1993 83
▼
A
NYONE WHO USED a single
84 Silicon Chip
August 1993 85
CN1
K
1uF
SIL1
LED1
0.1
1
SW1
100pF
Memory decoding
The Z80 has a full address space
of 64K and 16K of this is used for
memory, 8K for the EPROM and 8K
for RAM. Depending on which section of memory is being addressed,
the EPROM or RAM must be selected
and this is done by IC2, a 3-to-8 line
decoder. Three address lines, A13, A14
& A15, are used as input to IC2 and
two of its output lines become CHIP
SELECT signals for the memory chips;
the EPROM from 0000H to 1FFFH and
RAM from 2000H to 3FFFH.
Each input/output (I/O) device
needs one I/O port address for itself.
To get this unique address, we need to
decode one of the 256 I/O addresses
provided by the Z80 and this is done
by IC3, another 3-to-8 line decoder.
The connection of address line A7
to the enable (E3) pin 6 of IC3 effectively divides the memory map into
two halves. If A7 is low, the decoder
is disabled and no I/O ports on the
Southern Cross are selected.
The upper half of this memory
map is further divided in half by
86 Silicon Chip
1k
1k
Q6
1k
Q5
CN4
0.1
100
100k
100k
S17
S1
S2
S3
S4
S18
S5
S6
S7
S8
S19
S9
S10
S11
S12
S20
S13
S14
S15
S16
IC9 74C923
IC8 74HC244
0.1
3.3uF
P1
0.1
1uF
S21
Fig.3: this is the component overlay of the Southern Cross. It uses a single sided
board & 54 links to keep costs low. Take care with the orientation of the keypad
switches (S1-S20) – see text.
reset circuit. It holds the reset line at
ground immediately power is applied
to the board. C15 then charges up via
R19 and the line goes high (and the
reset is removed) after several milliseconds.
Q4
1
22k
10k
2.2k
RESET
PAD
74HCU04
560
10M
22k
22k
22k
22k
22k
33pF
Q3
B1
0.1
1
DISP6
1k
1
XTL1
DISP5
Q7
IC7 6264
IC5 Z80ACPU
IC6 27C64
1
33pF
Q2
IC4 74HC273
1
DISP4
1k
SIL2
1
CN3
DISP3
1k
10uF
Q1
0.1
1k
0.1
DISP2
IC1 74HC273
1
IC3 74HC138
1
IC2 74HC138
DB1
10uF
330
7805
CN2
AC/DC
DISP1
1
1000uF
address line A6, connected to enable
pin 4 (E1) of IC3. Thus, 64 locations
from 80H to BFH are available to the
Southern Cross. If A6 is high, then
a quarter of the address space, from
C0H to FFH, is available for use by
other devices.
To get eight I/O ports from this
64 block, address lines 0, 1 & 2 are
decoded by IC3. You can see seven
decoded ports, 80H to 86H, on the
diagram. Ports 80H to 83H are taken
to the expansion port. Ports 84 and 85
communicate with the displays; port
86 connects to the keyboard. Port 87H
is not used.
Clock circuit
As mentioned above, the clock
frequency for the Z80 is 4MHz and
this is provided by an oscillator built
around a 74HCU04 inverter and a
4MHz crystal. For those applications
where a slower clock is desirable, a
second variable oscillator is provided.
This is built around three inverters
(IC10d-f) and is varied with trimpot
P1. The change over from the fixed
to the variable clock circuit is via the
Fast/Slow switch SW1.
Expansion connectors
There are three expansion sockets.
On the right of the board is CN4. This
contains two input lines and two
output lines, as well as ground and
+5V lines. As we shall see later in this
series, serial downloading of programs
from a PC comes via this socket. Experiments which can use single bits
can also use this connector.
At the top centre of the board is the
I/O connector CN1 which has connections to ports 80h to 83h, the reset line
and supply connections.
Finally, on the left of the board all
the address, data and Z80 control lines
are taken to a 40-pin header connector,
CN3. Expansion projects too big to be
accommodated at the other sock
ets
can be performed using the signals
available here.
Monitor program
The Southern Cross SBC can do
nothing on its own. It requires a set of
instructions in the form of a program to
tell it what to do. This is stored in the
27C64 EPROM and is called a “monitor”. The basic function of a “monitor”
is to allow memory locations to be
viewed and changed and to allow program execution. It also contains many
useful programs which you can use
to develop your own programs. This
use of the monitor will be discussed
in detail later in this series.
The fully commented monitor for
the Southern Cross SBC is supplied
on a floppy disc with the kit. It can be
printed out for study. It is a deliberately simple monitor without program
tricks or cryptic code. Its purpose is
to teach, not to impress or confuse
the beginner.
Programming of the Southern Cross
begins with the simple examples listed
in the User Manual which comes with
the kit. First, one LED segment in one
of the six segment displays is turned
on. Gradually, the student is shown
how to assemble code and enter it into
the Southern Cross.
Several demonstration programs
are built into the monitor. Function
8 (pressing the ‘Fn’ function key then
the ‘8’ key) will play a tune. You
can then enter your own tune, press
Function A and the tune you entered
will play.
Function C brings up a random
4-digit hex number which you must
be find within 20 tries (9 tries is our
best).
Other Function key assignments
include:
• Function 0 – start program execution.
• Function 1 – ready to receive Intel
hex file in serial download.
• Function 4 – move a block of memory defined by Function 2 (begin block)
and Function 3 (end block) to the
address displayed.
• Function 5 – calculate a check sum
on the block of memory defined by
Function 2 (start) & Function 3 (end).
• Function 6 – relative branch calculator.
• Function B – toggle the speaker
off/on. If you get tired of the speaker
beeping when you press a key, you
can turn it off and have a variable off
period of the displays instead.
• Function D – test the Relay Board
if attached.
• Function E – test the 8 x 8 LED dot
matrix board if attached.
• Function F – brings up the time/
day/date in the Smartwatch socket if
attached.
Saving programs
One of the big problems with SBCs
in the 1980s was that when you turned
off the power, your programs in RAM
were lost. The solution in those days
was to build a battery-backed RAM
board but these days Dallas Semiconductor has neatly solved the problem
with their Smartsocket DS1213B.
This can be fitted in the RAM socket
underneath the 6264 RAM IC. It has a
battery life of 10 years. When power
is turned off, the Smartsocket senses
this and the built-in battery takes over
and all your programs are safely kept
in the RAM.
Time & date option
Dallas Semiconductor also has a
Smartsocket of the same physical size
which incorporates a time and date
function. This is the DS1216B. You
can set the time and the date and it is
permanently saved in the chip until
you alter it.
Two simple changes to the board allow the DS1216B to be used. Function
F then brings up the time and date on
the displays. The date comes up in the
standard DD/MM/YY format or you
can change a single bit in the Monitor
Where to buy the kit
The Southern Cross computer kit was designed in Australia for DIY Electronics, GPO Box 904, Hong Kong. The kit containing all the components,
documentation and floppy disc with the monitor program may be ordered
in Australia from Alpine Technology, PO Box 934, Mt. Waverley, Vic 3149.
Phone or fax (03) 751 1989. You may pay by Bankcard, Mastercard, cheque
or money order. Buyers outside Australia should contact DIY Electronics in
Hong Kong. Phone (852) 725 0610. The kit costs are as follows:
Southern Cross Computer..............................................................$172.00
Dallas DS1213B SmartSocket..........................................................$55.00
Dallas DS1216B SmartSocket..........................................................$74.00
Technical manual of IC data sheets................................................. $10.00
The kit will be sent to buyers from Hong Kong by registered airmail and this
is included in the purchase price. Note that there is no copyright on the PC
artwork, program code or documentation and buyers are encouraged to
copy and modify the software provided.
PARTS LIST
1 PC board, 247 x 130mm
21 keypad switches
1 miniature slide switch (SW1)
1 4MHz crystal
1 5V buzzer
Semiconductors
2 74HC273 8-bit latches
(IC1,IC4)
2 74HC138 3-to-8 line decoders
(IC2,IC3)
1 Z80A microprocessor (IC5)
1 27C64 8K EPROM (IC6)
1 6264 8K static RAM (IC7)
1 74HC244 octal Tristate buffer
(IC8)
1 74HC923 keypad encoder
(IC9)
1 74HCU04 hex inverter (IC10)
7 BC547 NPN transistors
(Q1-Q7)
1 5mm red LED (LED1)
1 7805 5V regulator (REG1)
1 bridge rectifier (DB1)
6 CM1-5615S red 7-segment
common cathode displays
(DISP1-6)
Sockets & connectors
1 40-pin socket
2 28-pin sockets
4 20-pin sockets
2 16-pin sockets
1 14-pin socket
1 16-way rightangle socket (CN1)
1 2.5mm DC socket (CN2)
1 40-way rightangle socket (CN3)
1 6-way header & socket (CN4)
Capacitors
1 1000µF 35VW electrolytic
2 10µF 16VW electrolytic
1 3.3µF 16VW electrolytic
2 1µF 16VW electrolytic
7 0.1µF monolithic
1 100pF ceramic
2 33pF ceramic
Resistors (0.25W, 5%)
1 10MΩ
7 1kΩ
1 100kΩ
1 560Ω
6 22kΩ
1 330Ω
1 10kΩ
1 100Ω
1 2.2kΩ
2 4 x 100Ω SIL resistor arrays
(SIL1, SIL2)
1 20kΩ trimpot (P1)
Miscellaneous
Heatsink for regulator, tinned
copper wire, rubber feet.
August 1993 87
The Southern Cross single board computer is intended as a learning tool for
those who want to know more about microprocessors. It uses the Z80 8-bit
microprocessor & all the other parts are readily available.
program to use the American MM/DD/
YY format if you wish. The day of the
week can also be indicated using the
decimal points.
Construction
The Southern Cross computer is
built on a single-sided PC board.
The top is screen printed with the
component overlay diagram while
the copper pattern on the underside
has a solder mask which covers all
the board except around the solder
pads. This makes soldering easier
and reduces the risk of solder shorts
on the copper pattern.
The first thing to do is to place all
the components into a container and
then check them off against the parts
list. The component overlay shows
where all the parts go. First, there are
54 links to be inserted. Next, insert
the resistors and we suggest you check
each one for correct value with your
multimeter. Your can also insert the
two resistor packages, SIL1 and SIL2,
at this stage.
Sockets are used for all the ICs and
they all oriented the same way, with
the end notch pointing to the top of
the board. Watch the polarity of the
electrolytic capacitors, C1, C2, C3, C5,
C11 & C15. The buzzer B1 must also
be correctly oriented.
There are seven BC547 transistors to
88 Silicon Chip
be inserted and their case orientation
should match the shapes shown on
the board overlay.
The six LED displays are oriented
with their decimal points adjacent
to the driver transistors. For LED1,
the cathode lead is the shorter of the
two and should be at the top of the
PC board. The bridge rectifier, DB1,
should be inserted so that the “+”
symbol on the package is adjacent to
the “+” on the PC overlay. The 7805
voltage regulator’s leads should be
bent with pliers before it is soldered
in place. It is assembled on the board
together with its heatsink, as shown
in the photograph.
Each keypad switch has a flat part
on one of its sides. This faces towards
the bottom of the PC board as shown
in Fig.2. All 21 key switches are
identical. Sixteen of the same colour
are supplied for the hex numbers 1-F.
Now insert all the miscellaneous
components such as the Speed and
Reset switches, the 20kΩ trimpot P1,
the various connectors and the 4MHz
crystal. Lastly, insert the integrated
circuits in their sockets, making sure
that they are oriented correctly.
When all the components have been
installed on the board, check your
work very carefully. In particular,
check the following points: electrolytic capacitors around the correct
way; ICs in their sockets the right way
around; and all the links on the board.
We also suggest that you fit four
rubber feet to the corners of the
Southern Cross PC board. This will
prevent the component leads on the
underside from damaging your bench
or desk surface and will prevent any
shorts if you place the board on a
metal surface.
Now set the Speed switch to the
F (fast) position and connect a 9V or
12V AC or DC plugpack. The Southern
Cross should then beep, the power LED
should light and the numbers ‘2000’
should appear in the group of four
Address displays.
If the board does not work when
you turn it on, remember that the
problem is almost certainly a mistake
you made during construction. The
most common cause of kit failure is
bad soldering or forgetting to solder a
pad. Also common is incorrect insertion of components or solder shorting
across two pads.
Use your multimeter to check that
+5V is present at the respective pins
of the ICs, as shown on the circuit
diagram of Fig.2.
If the Southern Cross is completely
dead when the power is connected
(and LED1 does not come on), then
clearly the place to look for faults is
around the bridge recti
fier and the
7805 regulator. Similarly, if some of
the board is active and some parts are
not, then this will indicate where to
SC
direct your attention.
LED BRAKE LIGHT INDICATOR
This “brilliant” brake light indicator employs 60
high intensity LEDs (550-1000mCd) to produce
a display that is highly visible, even in bright
sunlight. The intensity produced is equal to or
better than the LED brake indicators which are
now included in some late model “upmarket”
vehicles. The LED displays used in most of
these cars simply make all the LEDs turn on
every time the brakes are applied. The circuit
used in this unit can perform in this manner
and, for non-automotive applications, it can be
customised to produce a number of sweeps (110) starting at the centre of the display and with a
variable sweep rate. It not only looks spectacular
but also attracts more attention.
All the necessary “electronics” is assempled
on two identical PCBs and the resulting overall
length of the twin bargraph display is 460mm.
It’s simple to install into a car since only two
connections are required: Earth and the brake
LASER SCANNER ASSEMBLIES
These are complete laser scanners as used in
laser printers. Include IR laser diode optics and
a very useful polygon scanner ( motor-mirror).
Produces a “fan” of light (approx. 30 deg) in one
plane from any laser beam. We provide information on polygon scanner only. Clearance:
$60
400 x 128 LCD DISPLAY MODULE –
HITACHI
These are silver grey Hitachi LM215XB dot
matrix displays. They are installed in an attractive housing and a connector is provided.
Data for the display is provided. BRAND NEW
units at a low:
$40
LASER OPTICS
The collimating lens set is used to improve the
beam (focus) divergence. The 1/4-wave plate
and the beam splitter are used in holography
and experimentation. All are priced at a fraction
of their real value:
1/4 wave plate (633nM) ..............................$20
Collimating lens sets ..................................$45
Polarizing cube beam splitters ....................$65
GREEN LASER TUBES
We have a limited supply of some 0.5mW
GREEN ( 560nm) HeNe laser tubes. Because
of the relative response of the human eye,
these appear as bright as about a 2mW red
tube: Very bright. We will supply this tube and
a suitable 12V laser power supply kit for a low:
$299
CCD ELEMENT
BRAND NEW high sensitivity monolythic single
line 2048 element image sensors as used in
fax machines, optical charachter recognition
and other high resolution imaging applications:
Fairchild CCD122. Have usable response in
the visible and IR spectrum. Supplied with 21
pages of data and a typical application circuit.
$30
INFRARED TUBE AND SUPPLY
These are the key components needed for
making an INFRARED NIGHT VIEWER. The
tubes will convert infrared light into visible light
on the phosphor screen. These are prefocussed
tubes similar to type 6929. They do not require
a focus voltage. Very small: 34mm diameter,
68mm long. All that is needed to make the tube
light connecting wire. The case for the prototype
unit which would be suitable for mounting on
the rear parcel shelf, was mainly made from
two aluminium “L” brackets that were screwed
together to make a “U” section. A metal rod and
its matching holders (commonly available from
hardware shops) are used for the supporting leg.
$60
for both the PCBs, all the onboard components &
instructions: the 60 LEDs are included! We also
have available a similar kit that does not have
the sweeping feature. It produces similar results
to the commercial units installed in cars: all the
LEDs light up when power is applied.
$40
for both the PCBs and all the onboard components. This kit is also supplied with the 60 LEDs
and it uses different PCBs, that have identical
dimensions to the ones supplied in the above
mentioned kit.
operational is a low current EHT power supply,
which we provide ready made or in kit form:
powered by a 9V battery and typically draws
20mA. INCREDIBLE PRICING:
$90
For the image converter tube and an EHT
power supply kit!
All that is needed to make a complete IR night
viewer is a lens an eyeiece and a case: See
EA May and Sept. 1990.
ALUMINIUM TORCHES – INFRARED
LIGHTS
These are high quality heavy-duty black anodised aluminium torches that are powered by
four “D” cells. Their focussing is adjustable from
a spot to a flood. They are water resistant and
shock proof. Powered by a krypton bulb – spare
bulb included in cap.
$42
Note that we have available a very high quality
INFRARED FILTER and a RUBBER lens cover
that would convert this torch to a good source
of IR: $15 extra for the pair.
PASSIVE NIGHT VIEWER BARGAIN
This kit is based on an BRAND NEW passive
night vision scope, which is completely assembled and has an EHT coaxial cable connected.
This assembly employs a high gain passive
tube which is made in Russia. It has a very
high luminous gain and the resultant viewer
will produce useful pictures in sub-moonlight
illumination. The viewer can also be assisted
with infrared illumination in more difficult situations. It needs an EHT power supply to make
it functional and we supply a suitable supply
and its casing in kit form. This would probably
represent the best value passive night viewer
that we ever offered!
BECAUSE OF A SPECIAL PURCHASE OF
THE RUSSIAN-MADE SCOPES, WE HAVE
REDUCED THE PRICE OF THIS PREVIOUSLY ADVERTISED ITEM FROM $550 TO
A RIDICULOUS:
$399
This combination will be soon published as a
project in EA. NOTE THE REDUCED PRICE:
LIMITED SUPPLY. Previous purchasers of the
above kit please contact us.
24VDC TO MAINS VOLTAGE INVERTERS
In the form of UNINTERRUPTABLE POWER
SUPPLIES (UPS’s).These units contain a
300W, 24V DC to 240V 50Hz mains inverter.
Can be used in solar power systems etc. or
for their original intended purpose as UPS’s.
THESE ARE VERY COMPACT, HIGH QUALITY UPS’s. They feature a 300W - 450W (50Hz)
SINEWAVE INVERTER. The inverter is powered by two series 12V 6.5Ahr (24V). batteries
that are built into the unit. There is only one
catch: because these NEW units have been
in storage for a while, we can not guarantee
the two batteries for any period of time but we
will guarantee that the batteries will perform
in the UPS’s when these are supplied. We will
provide a 3-month warranty on the UPS’s but
not the batteries. A circuit will also be provided.
PRICED AT A FRACTION OF THEIR REAL
VALUE: BE QUICK! LIMITED STOCK!
$239
ATTENTION ALL MOTOROLA
MICROPROCESSOR PROGRAMMERS
We have advanced information about two
new STATE OF THE ART microprocessors
to be released by Motorola: 68C705K1 and
68HC705J1. The chips are fully functional
micros containing EPROM/OTPROM and RAM.
Some of the features of these new LOW COST
chips include:
*16 pin DIL for the 68HC705K1 chip * 20 pin
DIL for the 68HC705J1 chip * 10 fully programmable bi-directional I/O lines * EPROM
and RAM on chip * Fully static operation
with over 4MHz operating speed.
These two chips should become very popular.
We have put together a SPECIAL PACKAGE
that includes a number of components that
enable “playing” with the abovementioned
new chips, and also some of the older chips.
IN THIS PACKAGE YOU WILL GET:
* One very large (330 x 220mm) PCB for the
Computer/Trainer published in EA Sept. 93; one
16x2 LCD character display to suit; and one
adaptor PCB to suit the 68HC705C8.
* One small adaptor PCB that mates the
programmer in EA Mar. 93 to the “J” chip,
plus circuit.
* One standalone programmer PCB for programming the “K” chip plus the circuit and a
special transformer to suit.
THE ABOVE PACKAGE IS ON SPECIAL AT
A RIDICULOUS PRICE OF:
$99
Note that the four PCBs supplied are all silk
screened and solder masked, and have plated
through holes. Their value alone would be in
excess of $200! A demonstration disc for the
COMPUTER/TRAINER is available for $10.
No additional software is currently available.
Previous purchasers of the COMPUTER/
TRAINER PCB can get a special credit towards
the purchase of the rest of the above package.
PLASMA BALL KIT
This kit will produce a fascinating colourful
changing high voltage discharge in a standard
domestic light bulb. The EHT circuit is powered
from a 12V supply and draws a low 0.7A. We
provide a solder masked and screened PCB, all
the onboard components (flyback transformer
included), and the instructions at a SPECIAL
introductory price of:
$ 25
We do not supply the standard light bulb or
any casing. The prototype supply was housed
in a large coffee jar, with the lamp mounted
on the lid – a very attractive low-cost housing!
Diagrams included.
LASER DIODE KIT – 5mW/670nm
Our best visible laser diode kit ever! This one is
supplied with a 5mW 670nm diode and the lens,
already mounted in a small brass assembly,
which has the three connecting wires attached.
The lens used is the most efficient we have
seen and its focus can be adjusted. We also
provide a PCB and all on-board components
for a driver kit that features Automatic Power
Control (APC). Head has a diameter of 11mm
and is 22mm long, APC driver PCB is 20 X
23mm, 4.5-12V operation at approx 80mA.
$85
PRECISION STEPPER MOTORS
This precision 4-wire Japanese stepper motor
has 1.8 degree steps – that is 200 steps per
revolution! 56mm diameter, 40mm high, drive
shaft has a diameter of 6mm and is 20mm long,
7.2V 0.6A DC. We have a good but LIMITED
supply of these brand new motors:
$20
HIGH INTENSITY LEDs
Narrow angle 5mm red LED’s in a clear housing.
Have a luminous power output of 550-1000mCd
<at> 20mA. That’s about 1000 times brighter
than normal red LED’s. Similar in brightness
SPECIAL REDUCED PRICE: 50c Ea or 10
for $4, or 100 for $30.
IR VIEWER “TANK SET”
ON SPECIAL is a set of components that can
be used to make a complete first generation
infrared night viewer. These matching lenses, tubes and eyepieces were removed from
working tank viewers, and we also supply a
suitable EHT power supply for the particular
tube supplied. The power supply may be ready
made or in kit form: basic instructions provided.
The resultant viewer requires IR illumination.
$180
We can also supply the complete monocular
“Tank Viewer” for the same price, or a binocular
viewer for $280: Ring.
MINI EL-CHEAPO LASER
A very small kit inverter that employs a switchmode power supply: Very efficient! Will power a
1mW tube from a 12V battery whilst consuming
about 600 mA! Excellent for high-brightness
laser sights, laser pointers, etc. Comes with
a compact 1mW laser tube with a maximum
dimension of 25mm diameter and an overall
length of 150mm. The power supply will have
overall dimensions of 40 x 40 x 140mm, making
for a very compact combination.
$59
For a used 1mW tube plus the kit inverter.
OATLEY ELECTRONICS
PO Box 89, Oatley, NSW 2223
Phone (02) 579 4985. Fax (02) 570 7910
MAJOR CARDS ACCEPTED WITH
PHONE & FAX ORDERS
P & P FOR MOST MIXED ORDERS
AUSTRALIA: $6; NZ (Air Mail): $10
August 1993 89
Silicon Chip
Preamplifier For Amateur TV; 1Mb Printer Buffer;
2-Chip Portable AM Stereo Radio, Pt.2; Installing
A Hard Disc In The PC.
November 1989: Radfax Decoder For Your PC
(Displays Fax, RTTY & Morse); FM Radio Intercom
For Motorbikes, Pt.2; 2-Chip Portable AM Stereo
Radio, Pt.3; Floppy Disc Drive Formats & Options;
The Pilbara Iron Ore Railways.
BACK ISSUES
September 1988: Hands-Free Speakerphone;
Electronic Fish Bite Detector; High Performance
AC Millivoltmeter, Pt.2; Build The Vader Voice;
Motorola MC34018 Speakerphone IC Data; What
Is Negative Feedback, Pt.4.
November 1988: 120W PA Amplifier Module
(Uses Mosfets); Poor Man’s Plasma Display;
Automotive Night Safety Light; Adding A Headset
To The Speakerphone; How To Quieten The Fan
In Your Computer; Diesel Electric Locomotives.
December 1988: 120W PA Amplifier (With Balanced Inputs), Pt.1; Diesel Sound Generator;
Car Antenna/Demister Adaptor; SSB Adaptor For
Shortwave Receivers; Why Diesel Electrics Killed
Off Steam; Index to Volume 1.
January 1989: Line Filter For Computers; Ultrasonic Proximity Detector For Cars; 120W PA Amplifier (With Balanced Inputs) Pt.1; How To Service
Car Cassette Players; Massive Diesel Electrics In
The USA; Marantz LD50 Loudspeakers.
March 1989: LED Message Board, Pt.1; 32-Band
Graphic Equaliser, Pt.1; Stereo Compressor For
CD Players; Amateur VHF FM Monitor, Pt.2; Signetics NE572 Compandor IC Data; Map reader
For Trip Calculations; Electronics For Everyone
–Resistors.
April 1989: Auxiliary Brake Light Flasher; Elec-
tronics For Everyone: What You Need to Know
About Capacitors; Telephone Bell Monitor/ Transmitter; 32-Band Graphic Equaliser, Pt.2; LED
Message Board, Pt.2.
May 1989: Electronic Pools/Lotto Selector; 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; NSW 86 Class Electric
Locomotives.
September 1989: 2-Chip Portable AM Stereo
Radio (Uses MC13024 and TX7376P) Pt.1;
Alarm-Triggered Telephone Dialler; 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: Introducing Remote Control; FM
Radio Intercom For Motorbikes Pt.1; GaAsFet
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.
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;
PC Program Calculates Great Circle Bearings.
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;
VOX With Delayed Audio; Relative Field Strength
Meter; 16-Channel Mixing Desk, Pt.3; Active CW
Filter For Weak Signal Reception; How To Find
Vintage Radio Receivers From The 1920s.
May 1990: Build A 4-Digit Capacitance Meter;
High Energy Ignition For Cars With Reluctor Distributors; The Mozzie CW Transceiver; Waveform
Generation Using A PC, Pt.3; 16-Channel Mixing
Desk, Pt.4.
Please send me a back issue for:
❏ January 1989
❏ March 1989
❏ July 1989
❏ September 1989
❏ January 1990
❏ February 1990
❏ June 1990
❏ July 1990
❏ November 1990
❏ December 1990
❏ April 1991
❏ May 1991
❏ September 1991
❏ October 1991
❏ February 1992
❏ March 1992
❏ July 1992
❏ August 1992
❏ December 1992
❏ January 1993
❏ May 1993
❏ June 1993
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September 1988
April 1989
October 1989
March 1990
August 1990
January 1991
June 1991
November 1991
April 1992
September 1992
February 1993
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November 1988
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December 1988
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January 1992
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April 1993
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90 Silicon Chip
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Detach and mail to:
Silicon Chip Publications, PO Box 139,
Collaroy, NSW, Australia 2097.
Or call (02) 979 5644 & quote your credit card
details. Fax (02) 979 6503.
June 1990: Multi-Sector Home Burglar Alarm;
Low-Noise Universal Stereo Preamplifier; Load
Protection Switch For Power Supplies; A Speed
Alarm For Your Car; Design Factors For Model
Aircraft; Fitting A Fax Card To A Computer.
July 1990: Digital Sine/Square Generator, Pt.1
(Covers 0-500kHz); Burglar Alarm Keypad & Combination Lock; Simple Electronic Die; Low-Cost
Dual Power Supply; Inside A Coal Burning Power
Station; Weather Fax Frequencies.
August 1990: High Stability UHF Remote Transmitter; Universal Safety Timer For Mains Appliances (9 Minutes); Horace The Electronic Cricket;
Digital Sine/Square Wave Generator, Pt.2.
September 1990: Music On Hold For Your 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; The Fruit Machine; Two-Tone Alarm Module;
Laser Power Supply; LCD Readout For The Capacitance Meter; How Quartz Crystals Work; The
Dangers When Servicing Microwave Ovens.
February 1991: Synthesised Stereo AM Tuner,
Pt.1; Three Inverters For Fluorescent Lights; LowCost Sinewave Oscillator; Fast Charger For Nicad
Batteries, Pt.2; How To Design Amplifier Output
Stages; Tasmania's Hydroelectric Power System.
March 1991: Remote Controller For Garage
Doors, Pt.1; Transistor Beta Tester Mk.2; Synthesised AM Stereo Tuner, Pt.2; Multi-Purpose I/O
Board For PC-Compatibles; Universal Wideband
RF Preamplifier For Amateurs & TV.
April 1991: Steam Sound Simulator For Model
Railroads; Remote Controller For Garage Doors,
Pt.2; Simple 12/24V Light Chaser; Synthesised
AM Stereo Tuner, Pt.3; A Practical Approach To
Amplifier Design, Pt.2; Playing With The Ansi.Sys
File; FSK Indicator For HF Transmissions.
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; Setting Screen Colours
On Your PC.
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; Electric Vehicle Transmission
Options; Tuning In To Satellite TV, Pt.1.
July 1991: Battery Discharge Pacer For Electric
Vehicles; Loudspeaker Protector For Stereo Amplifiers; 4-Channel Lighting Desk, Pt.2; How To Install
Multiple TV Outlets, Pt.2; Tuning In To Satellite
TV, Pt.2; PEP Monitor For Amateur Transceivers.
August 1991: Build A Digital Tachometer; Masthead Amplifier For TV & FM; PC Voice Recorder;
Tuning In To Satellite TV, Pt.3; Installing Windows
On Your PC; Step-By-Step Vintage Radio Repairs.
September 1991: Studio 3-55L 3-Way Loudspeaker System; Digital Altimeter For Gliders
& Ultralights, Pt.1; Build A Fax/Modem For Your
Computer; The Basics Of A/D & D/A Conversion;
Windows 3 Swapfiles, Program Groups & Icons.
October 1991: Build A Talking Voltmeter For Your
PC, Pt.1; SteamSound Simulator Mk.II; Magnetic
Field Strength Meter; Digital Altimeter For Gliders
& Ultralights, Pt.2; Getting To Know The Windows
PIF Editor.
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; Error Analyser For CD Players Pt.3;
Modifying The Windows INI Files.
December 1991: TV Transmitter For VCRs With
UHF Modulators; Infrared Light Beam Relay;
Solid-State Laser Pointer; Colour TV Pattern
Generator, Pt.2; Windows 3 & The Dreaded Un
recoverable Application Error; Index To Volume 4.
January 1992: 4-Channel Guitar Mixer; Adjustable
0-45V 8A Power Supply, Pt.1; Baby Room Monitor/FM Transmitter; Automatic Controller For Car
Headlights; Experiments For Your Games Card;
Restoring An AWA Radiolette Receiver.
February 1992: Compact Digital Voice Recorder;
50-Watt/Channel Stereo Power Amplifier; 12VDC/240VAC 40-Watt Inverter; Adjustable 0-45V 8A
Power Supply, Pt.2; Designing A Speed Controller
For Electric Models.
March 1992: TV Transmitter For VHF VCRs; Studio Twin Fifty Stereo Amplifier, Pt.1; Thermostatic
Switch For Car Radiator Fans; Telephone Call
Timer; Coping With Damaged Computer Direct
ories; Valve Substitution In Vintage Radios.
April 1992: Infrared Remote Control For Model
Railroads; Differential Input Buffer For CROs; Studio Twin Fifty Stereo Amplifier, Pt.2; Understanding
Computer Memory; Switching Frequencies in
Model Speed Controllers; Aligning Vintage Radio
Receivers, Pt.1.
Alarm; The Interphone Digital Telephone Exchange, Pt.2; General-Purpose 3½-Digit LCD
Panel Meter; Track Tester For Model Railroads;
Build A Relative Field Strength Meter.
October 1992: 2kW 24VDC To 240VAC Sinewave
Inverter; Multi-Sector Home Burglar Alarm, Pt.2;
Mini Amplifier For Personal Stereos; Electronically
Regulated Battery Charger (Charges 6V, 12V &
24V Lead-Acid Batteries).
November 1992: MAL-4 Microcontroller Board,
Pt.1; Simple FM Radio Receiver; Infrared Night
Viewer; Speed Controller For Electric Models, Pt.1;
2kW 24VDC To 240VAC Sinewave Inverter, Pt.2;
Automatic Nicad Battery Discharger; Modifications
To The Drill Speed Controller.
December 1992: Diesel Sound Simulator For
Model Railroads; Easy-To-Build UHF Remote
Switch; MAL-4 Microcontroller Board, Pt.2; Speed
Controller For Electric Models, Pt.2; 2kW 24VDC
To 240VAC Sine
wave Inverter, Pt.3; Index To
Volume 5.
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; Restoring A
1920s Kit Radio
February 1993: Three Simple Projects For Model
Railroads; A Low Fuel Indicator For Your Car;
Audio Level/VU Meter With LED Readout; Build
An Electronic Cockroach; MAL-4 Microcontroller
Board, Pt.3; 2kW 24VDC To 240VAC Sinewave
Inverter, Pt.5; File Backups With LHA & PKZIP.
March 1993: Build A Solar Charger For 12V
Batteries; An Alarm-Triggered Security Camera;
Low-Cost Audio Mixer for Camcorders; Test Yourself On The Reaction Trainer; A 24-Hour Sidereal
Clock For Astronomers.
April 1993: Solar-Powered Electric Fence; Build
An Audio Power Meter; Three-Function Home
Weather Station; 12VDC To 70VDC Step-Up Voltage Converter; Digital Clock With Battery Back-Up;
A Look At The Digital Compact Cassette.
May 1993: Nicad Cell Discharger; Build The
Woofer Stopper; Remote Volume Control For Hifi
Systems, Pt.1; Alphanumeric LCD Demonstration
Board; Low-Cost Mini Gas Laser; The Microsoft
Windows Sound System.
May 1992: Build A Telephone Intercom; LowCost Electronic Doorbell; Battery Eliminator For
Personal Players; Infrared Remote Control For
Model Railroads, Pt.2; A Look At Large Screen
High Resolution Monitors; OS2 Is Really Here;
Aligning Vintage Radio Receivers, Pt.2.
June 1993: Windows-Based Digital Logic
Analyser, Pt.1; Build An AM Radio Trainer, Pt.1;
Remote Control For The Woofer Stopper; A Digital
Voltmeter For Your Car; Remote Volume Control
For Hifi Systems, Pt.2; Double Your Disc Space
With DOS 6.
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; What’s New In Oscilloscopes?;
A Look At Hard Disc Drives.
July 1993: Build a Single Chip Message Recorder; Light Beam Relay Extender; Build An AM
Radio Trainer, Pt.2; Windows Based Digital Logic
Analyser; Pt.2; Low-Cost Quiz Game Adjudicator;
Programming The Motorola 68HC705C8 Micro
controller – Lesson 1; Antenna Tuners – Why
They Are Useful.
July 1992: Build A Nicad Battery Discharger;
8-Station Automatic Sprinkler Timer; Portable
12V SLA Battery Charger; Off-Hook Timer For
Telephones; Multi-Station Headset Intercom, Pt.2;
Understanding The World Of CB Radio.
August 1992: Build An Automatic SLA Battery
Charger; Miniature 1.5V To 9V DC Converter;
Dummy Load Box For Large Audio Amplifiers;
Internal Combustion Engines For Model Aircraft;
Troubleshooting Vintage Radio Receivers.
September 1992: Multi-Sector Home Burglar
PLEASE NOTE: all issues from November 1987
to August 1988, plus the October 1988, February
1989 & August 1989 issues, are now sold out. All
other issues are presently in stock, although stocks
are low for older issues. For readers wanting articles from sold-out issues, we can supply photostat
copies (or tearsheets) at $6.00 per article (incl.
p&p). When supplying photostat articles or back
copies, we automatically supply any relevant notes
& errata at no extra charge.
August 1993 91
ASK SILICON CHIP
Got a technical problem? Can’t understand a piece of jargon or some technical principle? Drop us a line
and we’ll answer your question. Write to: Ask Silicon Chip, PO Box 139, Collaroy Beach, NSW 2097.
AND or OR gates
with diodes
V+
A
Z
1k
I was very interested
in the Quizmaster circuit
B
A
Z
featured in the July 1993
issue of SILICON CHIP but I
was confused over the use
C
B
of diode gating. According
to your text on page 71,
1k
diodes D1-D4 make up an
C
AND gate.
I am used to seeing diAND
OR
odes and a resistor used
A
B
C
Z
A
B
C
Z
to make an OR gate and it
0
0
0
0
0
0
0
0
seems to me that the func0
0
1
0
0
0
1
1
tion of your circuit really is
0
1
0
0
0
1
0
1
an OR function too. After
0
1
1
0
0
1
1
1
all, if any of the Q1-Q4 out1
0
0
0
1
0
0
1
puts go low, the output of
1
0
1
0
1
0
1
1
the diode gate will also go
1
1
0
0
1
1
0
1
low and operate the buzzer
1
1
1
1
1
1
1
1
and so on.
Z = A.B.C
Z = A+B+C
Surely, that describes an
to label a gate with the AND or OR
OR function since Q1 or
Q2 or Q3 or Q4 going low will cause function.
In the case of the diode logic gate in
something to happen. Am I right? (B.
the Quizmaster, all inputs being high
S., Rooty Hill, NSW).
• That’s a good question, B. S, and result in a high output at the junction
one that has perplexed many people of the four diode cathodes. This is the
trying to come to grips with the rules AND function without a doubt. Howof logic. The truth is that the AND ever, since we are more interested in
and OR functions are closely related, the condition when one of the inputs
as are the NAND and NOR functions. goes low, you could argue that it’s an
It depends on what logic convention OR function but the voltage output is
you apply as to whether you decide the wrong polarity for positive logic.
Skippy not easily
frightened
With your Woofer Stopper still
on my mind, I saw just the right few
minutes of a TV travel program. I
see that commercial “Electronic
Kangaroo Warners” cost over $200
to fit to cars and off-road vehicles.
Your Woofer Stopper circuit would
be ideal as a roo stopper too. I also
need an “electronic mouse trap”.
When can we build one? (P. T., New
Norfolk, Tas).
• The Woofer Stopper can be quite
92 Silicon Chip
effective at stopping dogs from
barking when used as a teaching
system, as described in the article.
However, we have serious doubts
as to whether it would be of any
use as a kangaroo scarer to prevent
collisions with cars. Because of the
limited range, we just cannot see it
being a viable project.
We have not described an electronic mouse trap and also cannot
see the point of one either since
the good old mechanical spring
type is quite effective. It’s much
cheaper too.
On the other hand, if the junction of
the diode cathodes had a “pull-down”
resistor instead of the 10kΩ “pull-up”
resistor used in our circuit, it would
be more clearly an OR gate. The two
gate diagrams and their truth tables
show just how close the functions
can be. It all depends on the logic
convention you adopt in thinking
about the circuit.
To build or
not to build
I am interested in building the Car
Digital Voltmeter described in the June
1993 issue of SILICON CHIP. However,
the price of the advertised kit is about
the same as for an economy digital
multimeter advertised in the same
issue. Also you can buy a digital panel
meter for around the same price.
Faced with this choice, I wonder if
I should bother building the voltmeter
and just buy a meter to do the job. I
want it to monitor the battery in my
boat by the way. (P. S., Leichhardt,
NSW).
• On the face of it, the obvious choice
is to just buy a meter and not bother
with building a kit. However, meters
with liquid crystal displays may not
be the best choice if they are to be
used in cars or boats, unless you can
guarantee that they will not be exposed
to sunlight for more than short periods
of time. Intense heat and sunlight kills
liquid crystal displays.
It is also true that the more money
you pay for an instrument with a liquid
crystal display, the more reliable it is
likely to be. So if you spend $30 or so
on a digital multimeter, it may not have
a very long life if used permanently in
a car or boat.
Bird scarer
wanted
You’ve done the Woofer Stopper in
the May 1993 issue of SILICON CHIP.
Now how about extending the idea to
produce a bird scarer. There must be
plenty of people with fruit trees who
would want such a system as well
as those who are plagued by damage
from sulphur crested cockatoos. (R. G.,
Punchbowl, NSW).
• We have tried the Woofer Stopper on
birds such as rainbow lorikeets and it
has no effect whatsoever. As far as we
can determine, birds will only respond
to a loud sound such as a gun going
off or a distress call from one of their
number. On this basis, an ultrasonic
device such as the Woofer Stopper
would be useless.
It might be better to record the distress call of the birds you want to scare
using the single chip Voice Recorder
described in the July 1993 issue. You
could then feed this recording to a
power amplifier and speaker to broadcast it to the birdies.
Woofer Stopper
doesn’t work
I built the Woofer Stopper as described in the May 1993 issue of
SILICON CHIP but I’ve found it to be
ineffective on the little dog next door.
It doesn’t seem to affect it in the least.
I’ve measured the signal at both sides
of the tweeter with my oscilloscope
and have found it to be 20kHz and 10V
peak to peak. So why doesn’t it work?
(B. M., Campsie, NSW).
• The fact that you have measured a
20kHz square wave at both sides of
the tweeter indicates that the circuit
is probably working as it should but
that the tweeter might be faulty. When
you switch the circuit on and off,
you should at least hear a fairly loud
click from the tweeter and while it is
running you should be able to hear
some hiss. If you have young children
in the household they should be able
to hear it too. Don’t subject them to
it at close range because it will hurt
their ears.
You can also test a piezoelectric
tweeter by connecting a resistor across
it (virtually any value will do) and
then briefly connecting a 9V or 12V
battery across it. Each time you do
so, the tweeter will click fairly loudly.
The reason for connecting a resistor
across the tweeter for this test is to
discharge its capacitance which can
be as much as 0.3µF. If the capacitor
is not discharged by a shunt resistor,
it will only click once when initially
connected. If your tweeter does not
click, it’s probably faulty.
By the way, the Woofer Stopper can
Problem with
TV reception
Because I am located behind
a hill and approximately 100km
from Brisbane, my TV reception
leaves a lot to be desired. I have
had to run a 300-ohm ribbon cable
from the house to the top of a hill
500 metres away to get any reception at all and, for this reason, I
am anxious to build the masthead
amplifier described in the August
1991 issue of SILICON CHIP. However, I note that it is designed for
75-ohm cable.
I would be grateful if you could
advise me of the modifica
tions
necessary to make the unit suitable
for use with 300-ohm cable. (B. B.,
Maleny, Qld).
• We do not think that our mast-
be made to work with virtually any
speaker but a tweeter will naturally
work better because of its extended
high frequency response, whether or
not it is a piezoelectric or dynamic
type. If you use an 8-ohm speak
er,
the circuit can be expected to draw a
lot more current, around 1.5A or so,
rather than the 100mA or less with a
piezo tweeter.
Finally, there’s no guarantee that
the Woofer Stopper will work with
all dogs. The dog next door might be
deaf or just too stupid to know that he
is being reprimanded.
Puzzling problem with
National VCR
I have a puzzling problem with
sound on my National NV300 VCR.
I find that when I buy a new good
quality tape and record on it from any
source, I get a very low sound level.
However, if I go to my collection of
older tapes and repeat the same route
and playback the finished recording,
both picture and sound are perfect.
By the way, the picture on the new
tape is perfect; only the sound drops
down. When I turn the TV volume up,
I can just hear it in the background. If
I put one of my older tapes back in,
everything returns to normal.
I have taken some of the new tapes
back to the store I purchased them
head amplifier would be suitable
for driving such a long cable length.
In fact, you could have problems
sending the signal over such a long
run with any masthead amplifier.
An alternative suggestion is to
use your existing antenna mounted on the hilltop to drive another
identical antenna close by which
faces down the hill. You would
then have a third antenna at your
homesite pointing up the hillside.
You may find it beneficial to
drive the downward pointing antenna with a masthead amplifier
and our August 1991 design would
be quite suitable for that, driving
75 ohm cable. This concept is not
new and was originally suggested
in “Wireless World” magazine
many years ago. It should work
well.
from. When these were tried on another VCR, all seemed to work OK.
Recently a workmate approached
me with an identical problem in his
VCR, which carries the General brand.
He uses good quality video cassettes
and some or most of his older recordings have a better sound than a newly
bought tape. Unfortunately, I could not
help him. I cannot seem to solve the
mystery with my own machine. I’ve
examined and thoroughly cleaned
around the audio head assembly and
checked to ensure that the new tapes
are not out of alignment.
Perhaps another reader may help
with a valuable clue in this matter.
Sure I could take my VCR to a service
centre but I would never get to know
the real reason for this annoying prob
lem. (R. P., Sheffield, Tas).
• This is a fairly common problem
with old National VCRs, R. P. Replace
the audio/control head and your problems should be fixed. It won’t be cheap
though – it’ll cost you about $140 to
have the part replaced.
Coil information for
metal locator
I have come across your simple
metal detector circuit in the March
1991 issue of SILICON CHIP and have
completed the circuit as detailed.
However, I am at a loss as to the gauge
August 1993 93
Problem with the
Baby Room Monitor
I have written to you previously
about a problem I have getting the
Baby Room Monitor described in
January 1992 to trans
mit. Your
suggestion on that occasion was to
disable the VOX circuit by removing Q2 and Q3 but unfortunately
this had no effect.
I am a relatively experienced kit
constructor and am confident that
there are no solder bridges, dry
joints, wrongly inserted polarised
components, etc. I have even replaced IC1, a rather expensive stabin-the-dark, but no transmission.
of the enamelled copper wire used for
the search coil and the dimensions of
the former. I would be grateful if you
could supply this information.
I find great value from the magazine
and wish more simple circuits could
be included. Perhaps a yearly compilation of all circuits could be included
in a magazine. Keep up the good work.
(M. G., Glendalough, WA).
• The gauge of the wire is not overly
critical – 24 or 26 SWG (approx. 0.5mm
diameter) would work equally as well.
The diameter of the coil itself is also
not critical but a good size would be
around 15cm.
Optical illusion
with car voltmeter
I just noticed on the cover of your
June edition that the LED display of
your depicted Car Voltmeter has the
least significant digit showing a “mirror image” of a 6! Since I am going to
build this project, I was wondering if
there is a possible wiring error in this
design or just a malfunction of the “f”
segment actually showing an 8! Or
perhaps you used too slow a shutter
speed when taking the picture while
the display was changing?
Either way, could you please clarify
this before I proceed with building the
project. My worries were triggered by a
different and simpler design published
by another magazine where the display constantly switched (flickered)
between two values when the input
voltage varied slightly or was halfway
94 Silicon Chip
I have now discovered that I can
tune the transmitter and transmit
expelled breath sounds if a probe
is touched to pin 12 or 14 of IC1.
Any attempt at transmitting speech
is muffled and distorted, regardless
of VR1’s setting. If I remove the
probe, the transmission ceases. (R.
O., Waverley, NSW)
• On re-reading your first letter,
we noticed that you are using an
IC socket. This socket will prevent
the transmitter from operating at
its correct frequency due to the
extra capacitance. If you solder
the IC directly onto the board, the
transmitter should then work as
published.
between the least significant digit
numbers. To my knowledge, this can
be caused by an inconsistent up-count
when the display is blanked. Is your
design also prone to this?
Why can’t the voltage to frequency
converter in your design be used outside your specified range of 8-17V? Is
it caused by non-linearity occurring
outside the range and how bad is it?
Could you please tell me how to modify the design to read down to at least
4V fairly accurately without major
surgery, or could the range be shifted
by changing just one component? (M.
S., Edgewater, WA).
• You should be awarded full marks
for observation but there is nothing
wrong with the kit. Your analysis
regarding shutter speed is correct.
We were unable to use a high shutter
speed because it was a time exposure,
in order to be able to display the digit.
Note that any digital display can be
subject to jitter of the least significant
digit, especially if the quantity being
measured is itself varying.
The circuit can not easily be modified to read down to 4V. That’s because
the circuit is powered by the battery
it is measuring and needs a regulated
rail of at least 5V.
Test procedure
for clocks
I repair clock radios as a hobby. I
don’t have much trouble with the radio
portion, if I can get parts. However, I
have problems with IC clock chips and
the display. In most cases, one or more
segments of the LCD fail to illuminate.
Can you suggest a test or procedure
for determining whether the fault lies
in the display or in the clock chip? I
have most of the test equipment of a
small service shop.
Also, can you suggest a book that
might be helpful in understanding the
function of clock ICs? I enjoy SILICON
CHIP very much and have been a subscriber for the past four years. (T. G.,
Lavender Bay, NSW).
• There is no simple test to diagnose
whether the fault lies in the display
or in the clock chip when you have
missing segments on an LCD. The only
thing you can do is to check for continuity between the relevant pins of the
LCD and the clock chip. Failing that,
it is a lottery as to whether the fault
lies in the clock chip and the display.
Our experience though suggests that
the liquid crystal displays are far less
reliable than the clock chips.
Unfortunately, we cannot refer you
to any books on the subject and data
on clock chips is now quite hard to
get since most of them are sourced
from Asia.
Drifting around the
Greek Islands
I am writing to ask for your help
with the VHF FM Monitor Receiver
that was published in SILICON CHIP
in March 1989. I recently built this
project and have had a lot of trouble
with it. I can only pick-up a couple
of Greek stations which transmit on
about 151.75MHz.
If I take my hand off the tuning pot
after I finish tuning, I lose the station
or I get a very distorted sound. I have
ob
served all precautions regarding
earthing of components on the double-sided board. I also tried to earth
the body of the tuning pot but with
no success. It seems that this project
is very temperamental. If I even move
the board in a different direction, I get
distortion and I lose the signal. (P. T.,
Canterbury, NSW).
• It seems likely that your receiver
is working as it should but it needs
earthing and shielding. We suggest
you assemble the receiver board onto
an earthed metal baseplate and fit the
tuning shaft with an insulating knob.
This should greatly reduce the effect
of hand capacitance when you are
SC
tuning.
MARKET CENTRE
Cash in your surplus gear. Advertise it here in Silicon Chip.
CLASSIFIED ADVERTISING RATES
ANTIQUE RADIO
Advertising rates for this page: Classified ads: $10.00 for up to 12 words plus 50
cents for each additional word. Display ads (casual rate): $20 per column centimetre (Max. 10cm). Closing date: five weeks prior to month of sale.
To run your classified ad, print it clearly in the space below or on a separate sheet
of paper, fill out the form & send both with your cheque or credit card details to:
Silicon Chip Classifieds, PO Box 139, Collaroy Beach, NSW 2097. Or fax the
details to (02) 979 6503.
ANTIQUE RADIO RESTORATIONS:
specialist restoration service provided
for vintage radios, test equipment &
sales. Service includes chassis rewiring, recondensering, valve testing &
mechanical refurbishment. Rejuvenation of wooden, bakelite & metal cabinets. Plenty of parts – require details
for mail order. About 1200 radios within
16,000 square feet. Two-year warranty
on full restoration. Open Saturday
10am-4.30pm; Sunday 12.30-4.30pm.
109 Cann St, Bass Hill, NSW 2197
Phone (02) 645 3173 BH or (02) 726
1613 AH.
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
_____________ _____________ _____________ _____________ _____________
FOR SALE
WEATHER FAX programs for IBM XT/
ATs *** “RADFAX2” $35 is a high resolution, shortwave fax, Morse & RTTY
receiving program. Suitable for CGA,
EGA, VGA and Hercules cards (state
which). Needs SSB HF radio & Radfax
decoder. *** “SATFAX” $45 is a NOAA,
Meteor & GMS weather satellite picture
receiving program. Needs EGA or VGA
plus “WEATHER FAX” PC card. ***
“MAXISAT” $75 is similar to SATFAX
but needs 2Mb expanded memory
(EMS 3.6 or 4.0) and 1024 x 768 SVGA
card. All programs are on 5.25-inch or
3.5-inch disks (state which) & include
documentation. Add $3 postage. Only
from M. Delahunty, 42 Villiers St, New
Farm, Qld 4005. Phone (07) 358 2785.
❏ Bankcard ❏ Visa Card ❏ Master Card
Card No.
✂
Enclosed is my cheque/money order for $__________ or please debit my
RCS RADIO PTY LTD
Signature__________________________ Card expiry date______/______
Name ______________________________________________________
Street ______________________________________________________
Suburb/town ___________________________ Postcode______________
RCS Radio Pty Ltd is the only company that manufactures and sells every
PC board and front panel published
in SILICON CHIP, ETI and EA.
RCS Radio Pty Ltd,
651 Forest Rd, Bexley 2207.
Phone (02) 587 3491
August 1993 95
TRANSFORMER REWINDS
ALL TYPES OF TRANSFORMER REWINDS
TRANSFORMER REWINDS
Reply Paid No.2, PO Box 438, Singleton, NSW
2330. Ph: (065) 76 1291. Fax: (065) 76 1003.
ICL 286 Board
Kits
All in one board with two serial,
printer, IBM keyboard, high
density floppy & IDE mono
video interface. Up to 4Mb
RAM, 80286-16cpu, MS-DOS
compatible, 130 page manual,
small size 170mm x 255mm.
Max I/O kit for PCs, 7 relays,
ADC, DAC, stepper driver, TTL
inputs, with software
$169
PC I/O card with 8255 chip 24
I/O lines programmable as inputs
or outputs
$69
1.5 watt AM broadcast transmitter XTAL locked
$49
2.5 watt FM broadcast transmitter 88-108MHz.
$49
Digi-125 audio power amp
(over 19,000 sold since 1987)
50 watt/8 $14 125 watt/4 $19
New 200 watt/2 version $29
Infrared relay kit
$9
Remote control tester
$4
$299
Ampo little PC
All in one NEC V40 CPU board,
MS-DOS compatible, high density floppy. SCSI hard disk, 2
serial, printer, solid state hard
disk, IBM keyboard interface,
(4W), CMOS single +5V rail,
up to 768Kb RAM, 384Kb
ROM, 145mm x 250mm, 98page manual.
$299
P.C. Computers
MEMORY & DRIVES
PRICES AT JULY 10th, 1993
SIMM
1Mb x 9
70ns
1Mb x 3
70ns
4Mb (72-pin)
4Mb x 9
70ns
4Mb x 8
80ns
$63
$60
$245
$235
$210
DRAM DIP
1 x 1Mb
70ns
$6.25
256 x 4
70ns
$6.25
1Mb x 4
Z or D $26.00
DRIVES
SEAG 42Mb
SEAG 89Mb
SEAG 107Mb
SEAG 130Mb
SEAG 214Mb
28ms
14ms
15ms
16ms
16ms
$205
$292
$310
$335
$470
IBM PS.2
50/55/70
70/35
90/95
2Mb
4Mb
4Mb
$145
$235
$235
TOSHIBA
T3200SX
T44/6400
T5200
T5200
4Mb
4Mb
2Mb
8Mb
$265
$245
$150
$575
MAC
2Mb SI & LC
4Mb P’Book
$110
$270
CO-PROCESSORS
387SX to 25
$110
387DX to 33
$110
Sales tax 20%. Overnight delivery. Credit cards welcome.
All Electronic Components..........80
Altronics .....................IFC,63,76-78
Antique Radio Restorations.........95
A-One Electronics.................. 26-27
Boston Technology......................39
Cebus Australia...........................11
David Reid Electronics ................3
Ring for Latest Prices
Dick Smith Electronics...14-17,OBC
1st Floor, 100 Yarrara Rd, PO Box 382, Pennant Hills, 2120.
Emona Pty Ltd.............................11
Tel: (02) 980 6988
Fax: (02) 980 6991
PELHAM
36 Regent St, Kensington,
SA. Phone (08) 332 6513.
THE HOMEBUILT DYNAMO: (plans)
brushless, 1000 watt at 740 revs. $A85
postpaid airmail from Al Forbes, PO
Box 3919 - SC, Auckland, NZ. Phone
Auckland (09) 818 8967 any time.
Advertising Index
Instant PCBs................................96
Jaycar ................................... 45-52
JV Tuners.....................................11
Oatley Electronics.....................5,89
PC Computers.............................96
UNUSUAL BOOKS: electronic devices,
fireworks, locksmithing, radar invisibility,
surveillance, self-protection, unusual
chemistry and more. For a complete
catalog send 95c in stamps to: Vector
Press, Dept S, PO Box 434, Brighton
SA 5048.
Extra BASIC STAMP modules $66 incl
p&p. Reprogram
mable for reuse. For
more info send SAE for data sheet &
circuits. Quantity prices available. Bank
card, Master, Visa or cheque with order.
Parallax of USA products distributor &
technical support in Australia. MicroZed
Computers, PO Box 634, Armidale
2350. Fax (067) 728987.
PAY TV & SATELLITE Scrambling News
Monthly, with the latest on descrambling
techniques & addresses, where to buy
the latest descramblers. Send stamp for
info. John Papp, Box 37885 Winnellie,
N.T. 0821.
GLOBAL ELECTRONIC SERVICES:
kits; consultancy; sales & design. Please
write/fax requirement to: Mr Lucas, PO
Box 755, Saint Helier, Jersey JE4 8ZZ,
Channel Islands (UK). Fax (0 534)
80570.
Silicon Chip Back Issues........90,91
PRINTED CIRCUIT boards for the
hobbyist. For service & enquiries contact: T. A. Mowles (08) 326 5590.
A 4Mb SIMM can now be used in my
Printer Buffer kit and my PC Printer
Port driven Z80 Micro Development
board has a Basic Interpreter. Short
form kit prices include postage. Buffer
$52, Z80 Dev. $76, or send $2 for my
3.5-inch promo disk to Don McKenzie,
29 Ellesmere Crescent, Tullamarine
3043. Phone (03) 338 6286.
Transformer Rewinds...................96
_________________________________
SOLVE YOUR SMALL circuit development problems quickly, try this one.
Parallax BASIC STAMP. A general purpose small circuit module, it is really a
25 x 50mm board with a computer chip
(4MHz PIC 16C56), EEPROM, 8 I/O sink
25mA or source 20mA board space includes 6 x 10 pad prototyping area. Has
216 type battery connections. Program it
on a PC with our development kit which
includes one BASIC STAMP $245 incl
p&p. Commands in
clude POT (crude
A/D), PWM (crude D/A), BUTTON ,
SERIN, SEROUT, SOUND & SLEEP.
96 Silicon Chip
WANTED
Do you have a good circuit idea? If so,
why not submit it for publication in Circuit Notebook and earn yourself some
money? Send your idea to Silicon Chip
Publications, PO Box 139, Collaroy
Beach, NSW 2097.
Pelham........................................96
Peter C. Lacey Services..............40
RCS Radio ..................................95
Resurrection Radio......................63
Rod Irving Electronics .......... 66-71
Silicon Chip Binders....................61
Silicon Chip Order Form..............75
Technical Applications.................81
PC Boards
Printed circuit boards for SILICON
CHIP projects are made by:
• RCS Radio Pty Ltd, 651 Forest
Rd, Bexley, NSW 2207. Phone (02)
587 3491.
• Marday Services, PO Box 19-189,
Avondale, Auckland, NZ. Phone (09)
828 5730.
• H. T. Electronics, 35 Valley View
Crescent, Hackham West, SA 5163.
Phone (08) 326 5590.
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