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FAST CHARGER
NICAD BATTER!
This Nicad Fast Charger is designed to
operate from a 12V car battery. It can
charge nicad battery packs from 6-12V
at currents up to 6A, or you can wire
the circuit to charge battery packs up
to 30V at reduced current.
and that ultimately leads to cell damage and loss of performance.
According to the battery manufacturers, the correct way to recharge a
nicad battery pack is to first discharge
each cell in the pack to its end point
(about 1. 1V) and then recharge it at
the 10-hour rate for 14 hours. Clear as
mud? OK, let's say that we have a
battery pack rated at 1300mAh. This
should ideally be recharged at a
130mA rate for 14 hours.
So why fast charge nicad batteries?
Well, there are many situations where
you may want to recharge a nicad
pack quickly, particularly if you are
involved with radio controlled models. For these applications, the bat-
Nicad battery packs are expensive
but many people risk damaging them
by using primitive fast charging techniques. At its crudest, a fast charger
consists simply of a pair ofresistive
leads connected to a car battery. The
idea behind the resistive leads is to
limit the charging current into the
battery but that doesn't stop overcharging if you don't constantly monitor the battery and disconnect the
leads at the correct time.
The same goes for many commercial fast chargers on the market. Often, there is no automatic shut-off
feature or the shut-off feature is unreliable. Instead, the charger just carries on pumping current into the cells
FUSE
+12V
PUSH-PULL
OUTPUT
VOLTAGE
CONVERTER
STOP
FIXED
VOLTAGE
DROP
NICAO
BATTERY
FEEDBACK
CURRENT
SENSING
RESISTOR
8-BITUPONLY
ANALOG TO
DIGITAL
CONVERTER
Fig.1: basic configuration of the Nicad Fast Charger. Power for the circuit comes
from a 12V battery & this drives a DC-DC converter which charges the battery
pack. The analog-to-digital converter, together with comparator IC8b, functions
as a peak detector & shuts down the converter at the end of the charging period.
32
SILICON CHIP
tery packs can handle considerably
higher charge (and discharge) currents
than ordinary nicad cells.
Of course, the risks of overcharging
and irreversible cell damage are much
greater if fast charging is employed.
And that's where this project comes
in. It detects when the battery is fully
charged and automatically switches
the unit off to prevent overcharging.
Unlike previous designs (eg, our
Megafast Nicad Charger in June 1988),
this charger uses digital circuitry to
detect when the battery is fully
charged. This ensures more reliable
operation than analog detection techniques - in fact, it's virtually foolproof. In operation, the circuit will
recharge a typical nicad racing pack
in about 20 minutes.
Large battery packs
There are several other features
which make this charger an attractive
unit. First, it can be switched in five
1.2V steps so that it can fast-charge
any nicad battery pack from 6-12V at
6A (ie, 6V, 7.2V, 8.4V, 9.6V & 12V).
The 6th switch position is labelled
"Custom" and that's the position you
select if you want to recharge a battery pack to greater than 12V (up to
about 30V).
It's this ability to recharge large
numbers of series-connected cells to
voltages greater than 12V that really
gives this unit the edge over previous
designs. For example, you may be
involved with electric flight models
and need to recharge a string of 24
cells to 28.8V. To do this however,
you have to change the number of
turns on the secondary of a transformer during construction from the
value normally recommended. In this
case, the lower ranges will still work
The Nicad Fast Charger is built into a standard plastic
instrument case. It can charge nicad battery packs from
6-12V at 6A or you can wire the circuit to charge a
custom battery pack (eg, 24 cells in series) at reduced
current.
but the current capability will be
greatly reduced. We'll say more about
this in Pt.2 next month.
The Nicad Fast Charger is also more
efficient than other fast charger designs we have seen. That translates
into more charges from the car battery. It also features reverse polarity
protection and there is provision for
trickle charging as well as fast charging. In addition, the circuit features a
low-voltage cutout feature to prev:ent
you from flattening your car's battery
- the usual source for most radio control modellers.
Note, however, that the circuit does
not feature automatic shut-off in the
trickle charge mode. That feature is
reserved for the fast-charge mode only
where it is much easier to detect the
fully-charged condition.
Charge status
Three LEDs on the front panel indicate the operating status of the
charger. When the Start button is
pressed, the Charging LED comes on
and remains on until the batteries are
fully charged. At this point, the Charging LED goes out and the End Of
Charge LED turns on.
·' The third LED is the Error indicator. It lights if the wrong charging
voltage is selected for the battery
connected.
In practice, the unit is very easy to
use. You simply connect the battery,
select the appropriate voltage and
press the Start switch. After that, it's
just a matter of waiting until the End
Of Charge indicator comes on.
Block diagram
Now take a look at the block diagram of Fig.1. This shows the basic
configuration of the Nicad Fast
Charger.
Power for the circuit comes from
the 12V car battery. This drives a DCDC converter circuit, the output voltage of which is controlled by the current through a current sensing resis-
tor in series with the nicad battery
pack. In operation, the output voltage
of the converter automatically adjusts
to maintain a constant voltage across
the resistor and thus a constant current through the nicad battery.
For example, if the nicad battery is
almost completely flat, then the output voltage of the converter automatically adjusts to maintain the correct
current. The advantage of this scheme
is that the power dissipation of the
circuit is low, with losses occuring
only in the push-pull converter driver
stages and across the current sensing
resistor. The ability of the converter
to produce an output greater than 12V
also makes it possible to charge nicad
battery packs to voltages greater than
the 12V produced by the battery.
The remaining circuitry is used to
monitor the charge on the nicad battery and shut the charger down when
the battery is fully charged. The full
charge condition is detected by the
small drop in battery voltage that
JANUARY 1991
33
;-
1.8
1.7
~
1.6
~=....
g
1.5
1.4
1.3
0
~
/
IC4
---G
CLK
MSB
OUT
BINARY COUNTER
IC 5
R
LSB
RESET
INPUT
07 06 05 04 03 02 01 00
/
I 8-BIT
I DIGITAL
I OUTPUT
I
81 82 83 84 85 86 87 88
REFERENCE
DAC
IC6
10
15
20
CHARGE TIME (MINUTES)
Fig.2: typical charging curve for a
single cell in a 7.2V 1300mAh racing
pack. Note how the voltage falls at the
.end of the charging cycle. This voltage
drop is detected by the AID converter,
which then shuts the circuit down to
prevent overcharging.
occurs as the battery heats up under
overcharge conditions - see Fig.2. ·It
works like this.
First, the battery voltage is dropped
by a fixed value and then applied to
the inverting input of a comparator
(IC8b) and also to an up-only 8-bit
analog-to-digital (AID) converter. The
output of the AID converter then
drives the non-inverting input of the
comparator.
Thus, IC8b compares the analog
input and output voltages of the AID
converter. Normally, the output of
IC8b is low but if the battery voltage
falls, the voltage on the inverting input ofIC8b will fall below the voltage
on the non-inverting input (since the
AID converter can only count up to a
peak). The output of IC8b will thus
switch high to shut down the pushpull converter circuit and end battery
charging.
Fig. 3 shows the basic arrangement
of the up-only AID converter. It consists of comparator IC8a, a gated clock
(IC4), and a binary counter (IC5) with
its 8-bit output connected to the 8-bit
input of a digital-to-analog converter
DAC (IC6). This produces an analog
output which corresponds to the
count provided by the binary counter.
Thus, when the binary counter has
a count of 00000000, the analog output will be at 0V. Conversely, when
the counter has a count of 11111111,
the analog output will be at its maximum - say 5V. For the remaining 254
counts in between these two extremes,
the analog output is incremented by
34
BATTERY
SAMPLE
I
~
GATED
CLOCK
COMPARATOR
SILICON CHIP
Fig.3: block diagram of the up-only AID converter. When the output ofIC8a is
high, IC4 clocks binary counter IC5. This counter then drives digital-to-analog
converter IC6 and this produces an analog output which corresponds to the
count in the binary counter. As soon as the sampled battery voltage drops below
the DAC output, IC8a's output goes low & stops the clock, thus freezing the DAC
output at its peak.
about 20mV for each count.
Because of the very small increment between each count, it is necessary to include a reference voltage for
the DAC so that the analog output is
repeatable and accurate.
The analog output from the DAC is
fed to the inverting input of comparator IC8a where it is compared with a
sample of the battery voltage on the
non-inverting input. This comparator
controls a clock circuit. When the
DAC output is lower than the battery
voltage, the comparator output is high
and so the clock signal is applied to
the binary counter. This in turn increments the binary counter and so
the analog output voltage from the
DAC rises.
When this voltage just exceeds the
sampled battery voltage, IC8a's output switches low and stops the clock.
Thus, the DAC analog output voltage
is held (or frozen) at its peak.
Fig.4 shows the waveforms involved in this operation. Note that
the steps shown for the DAC output
are not to scale, since in reality, they
only increment in 20mV steps. When
first powered up, the DAC output is
at 0V because the binary counter (IC5)
is initially reset. Thus, the comparator output is initially high, the clock
is enabled and the DAC output steadily increases until it just exceeds the
sampled battery voltage. The comparator output then goes low, the
clGJck stops and the DAG output remains steady.
If the battery voltage later rises
again due to charging, the comparator again switches high and restarts
the clock to increment the DAC output voltage. However, when the battery voltage subsequently falls (ie,
when it is being overcharged), the
DAC output remains as it is since the
comparator output stays low. Thus,
the DAC is a peak hold circuit which
registers the peak battery voltage and
holds it until the counter is reset.
Circuit details
Fig.5 shows the final circuit of the
Nicad Fast Charger. Despite the apparent complexity, it's really quite
straightforward. In fact, you should
be able to identify most of the circuit
COMPARATOR
OUTPUT
CLOCK
OUTPUT
ANALOG
VOLTAGE
(DOTTED)
_____
~---_,,.,.
✓--,
' .....
__ _
Fi'g.4: these waveforms
show how the DAC output
increases until it just
exceeds the sampled battery
voltage during charging.
Notice how the comparator
output again switches high
& enables the clock when
the battery voltage later
rises due to charging. The
DAC output then rises until
it again exceeds this new
level.
functions by comparing it with Fig.1
and Fig.3.
The push-pull converter circuit is
right at the top of Fig.5 and includes
ICl (TL494), Mosfet transistors Q1Q4, transformer Tl, and rectifier diodes D4 and D5.
ICl is really at the heart of the converter circuit. This is a dedicated
switchmode IC from Texas Instruments and it includes all the necessary circuitry for generating complementary square wave pulses at its pin
9 & 10 outputs. These outputs are
pulse width modulated by internal
error amplifiers to regulate the output voltage of the converter.
The inputs to the internal error
amplifiers are at pins 1 & 2 (+Cl &
-Cl) for one amplifier, and at pins 16
& 15 (+CZ & -C2) for the other. In addition, the IC contains an internal
sawtooth oscillator, a 5V reference
(pin 14) and a "dead time" control
comparator. The latter is included to
prevent the push-pull outputs at pins
9 & 10 from rising and falling at exactly the same time.
The dead time input is at pin 4 and
is tied to the 5V reference at pin 14
via a 4. 7µF capacitor. When the dead
time input is at the reference voltage
(5V), the output transistors are off and
as this voltage drops to ground, the
dead time decreases to a minimum.
In this circuit, the dead time control is used to provide a soft start.
When power is first applied, the 4.7µF
capacitor pulls the dead time input
(pin 4) to +5V and thus prevents the
output transistors inside ICl from
switching on. The 4. 7µF capacitor
then charges via the 4 7kQ resistor on
pin 4 and as it does so, the duty cycle
of the output transistors gradually
increases until full control is gained
by the error amplifiers.
Error amplifiers
Now let's look at the role of the two
error amplifiers.
The first error amplifier, with inputs at pins 1 & 2, is primarily used to
shut down the converter when the
nicad battery is fully charged. Its noninverting input (pin 1) is connected
to the +5V reference while the inverting input (pin 2) is connected to a
control line which, in turn, is controlled by comparator IC8lr.
When this control line is above +5V,
the converter functions normally.
However, when the line drops below
PARTS LIST
1 Plastic instrument case, 259 x
190 x 82mm
1 PC board, code SC14101911,
167 x 222mm
1 Dynamark front panel label, 249 x
75mm
1 metal rear panel, 249 x 76 x
1.5mm
1 finned heatsink, 110 x 74 x 33mm
1 Neosid 17/742/10 iron powder
ring core
1 Siemens EC-41 N27 ferrite
transformer kit
1 panel mount 3AG fuse holder
1 10A 3AG fuse
2 cordgrip grommets
1 SPOT miniature momentary
pushbutton switch (S1)
1 2-pole 6-way rotary switch (S2)
1 DPDT miniature toggle switch
(S3)
4 5mm red LEDs (LED1-LED4)
3 5mm LED bezels
5 T0-220 insulating mounting kits
6 10mm-long screws and nuts to
suit insulating bushes
26 PC stakes
2 battery clamps to suit 12V battery
1 polarised socket (to suit nicad
battery pack)
1 1-metre length twin of automotive
wire (1 0A or greater)
1 3.5-metre length of 1.25mm
enamelled copper wire
1 450mm-length of 0.8mm tinned
copper wire
1 1.5-metre length of light-duty
hookup wire
4 self-tapping screws
4 rubber feet
2 10kQ miniature horizontal
trimpots
Semiconductors
1 TL494 switchmode IC (IC1)
1 4050 hex buffer (IC2)
1 LM833 dual op amp (IC3)
1 555 timer (IC4)
1 4020 binary counter (IC5)
1 DAC0800 DIA converter (IC6)
+5V, the output of the error amplifier
switches high and reduces the pulse
width to zero, thus effectively shutting the converter down to end battery charging.
A secondary function of this control line is to shut down the converter
1 TL072 dual op amp (IC?)
1 LM393 dual comparator (IC8)
4 BUZ71, MTP3055 Mosfets
(Q1-Q4)
2 BC337 NPN transistors (Q5,Q6)
1 BYX98 10A stud mount diode
(D1)
21N40021A diodes (D2,D3)
2 BYW29, MBR1645 16A Schottky
diodes (D4,D5)
1 15V 5W zener diode (ZD1)
2 30V 1W zener diodes (ZD2,ZD3)
1 3.3V 400mW zener diode (ZD4)
2 5.6V 400mW zener diodes
(ZD5,ZD8)
1 9V 400mW zener diode (ZD6)
1 zener diode (ZD7 - see text)
1 LM336-2.5V reference diode
(REF1)
1 MCR100-6 SCR (SCR1)
Capacitors
1 2200µF 50VW PC electrolytic
1 2200µF 16VW PC electrolytic
1 47µF 16VW PC electrolytic
5 10µF 16VW PC electrolytic
5 4. 7µF 16VW PC electroly1ic
1 2.2µF 16VW PC electroly1ic
2 1µF 16VW PC electroly1ic
1 0.47µF 16VW PC electrolytic
2 0.1 µF monolithic
1 0.1 µF metallised polyester
3 .022µF metallised polyester
1 .01 µF metallised polyester
1 .001 µF metallised polyester
Resistors (0.25W, 5%)
1 2.2MQ
2 4.7kQ
1 470kQ
2 4.7kQ 1%
2 220kQ
5 3.3kQ
5 100kQ
1 1.5kQ
2 47kQ
31kQ
1 33kQ
1 820Q
1 22kQ 1%
1 680Q 0.5W
1 20kQ 1%
2 47Q
1 15kQ
410Q
12 10kQ
1 1Q 1W
1 6.8kQ
2 0.22Q 5W WW
Miscellaneous
Solder, heatsink compound.
if the voltage on the 12V car battery
drops below a preset level. This is
achieved by connecting the control
line to the +12V supply via a voltage
divider consisting of a lkQ resistor
and an 820Q resistor. Thus, if the battery voltage drops below 11 V, the
JANUARY 1991
35
junction of the voltage divider drops
below 5V and the error amplifier turns
off ICl.
The second error amplifier, with
inputs at pins 15 & 16, is used to
regulate the output voltage of the
converter. In operation, the voltage
across the current sensing resistor (2
x 0.22Q 5W resistors in parallel) is
fed to the non-inverting input at pin
16 and compared with a sample of
the +5V reference on the inverting
input at pin 15.
Thus, if the current through the
0.22Q resistors (and thus through the
nicad battery) rises above a preset
value, the output of the error amplifier also rises and this reduces the
width of the pulses from ICl to bring
the current back down again. Conversely, if the current falls below the
desired value, the error amplifier output also falls and the pulse width
increases.
The gain of this error amplifier is
set by the 4 70kQ feedback resistor
between pins 3 and 15. Trimpots VRl
& VR2 are used to set the voltage on
the inverting input (pin 15) , with S3a
used to select either trimpot wiper to
provide fast or trickle charging.
The complementary PWM outputs
from ICl appear at pins 9 & 10 (El &
E2) and are switched at a rate of about
20kHz. This frequency is determined
by the 33kQ resistor and .00lµF ea~
pacitor on pins 5 & 6, which set the
frequency of the internal oscillator to
about 40kHz.
Actually, El & E2 are the uncommitted emitter outputs of complementary switching transistors inside ICl.
These emitters drive paralleled buffer
stages IC2a, IC2b & IC2c on one phase
of the output waveform and IC2d,
IC2e & IC2f on the other. Their outputs then drive Mosfet transistors Ql ,
Q2 , Q3 & Q4 which in turn switch the
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which is a dedicated sw itchmode
device to drive Mosfet transistors Q1Q4 in push-pull mode. These then
drive step-up transformer Tl, the
output of which is rectified to produce
a DC voltage to charge the battery.
IC8a, IC4, IC5, IC6 & IC7 form the AID
converter shown in Fig.3. As soon as
the sampled battery voltage falls by
80m V from its peak, the output of
IC8b switches high & turns on SCR1 to
shut down the converter circuit (ICl,
Q1-Q4 & Tl).
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I 11,:11,,,;:;, \
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IC8b, even if the nicad battery pack is
completely short circuit.
The output of the fixed voltage drop
selected by S2 represents the battery
voltage and is applied to pin 3 of
comparator stage IC8a. Its pin 1 output controls the reset input (pin 4) of
555 timer IC4 which is wired as an
astable oscillator with a frequency of
about 100Hz. This frequency is set by
the two associated lO0kQ resistors
and the .022µF capacitor on pins 6 &
2.
The finned heatsink is fastened to the rear panel via the mounting screws used
to secure the four Mosfet transistors. Its job is to substantially increase heat
dissipation & thus keep the Mosfet transistors cool.
primary of transformer Tl.
Thus, when pin 10 of IC1 goes high,
Ql & Q2 turn on and switch the Sl
terminal of the transformer primary
to ground. When pin 10 goes low
again, these transistors switch off and
Q3 & Q4 switch on and drive the
other half of the primary. The lOQ
resistors in the gates of the Mosfets
are there to ensure that the paralleled Mosfet pairs share the current
equally, while DZ, ZD2, D3 & ZD3
protect the Mosfets by suppressing
spikes generated by the transformer.
In summary then, the power
Mosfets in each phase of the circuit
alternately switch the Sl & F2 terminals of a centre-tapped transformer
primary to ground, so that the transformer is driven in push-pull mode.
The resultant AC waveform is then
stepped up by the secondary of the
transformer and rectified using
Schottky diodes D4 & D5 .
Inductors 11 & 12 and the associated 2200µF capacitor filter the diode
outputs and the resultant DC output
is then applied to the nicad battery.
This battery (which may consist of
many individual cells) is connected
across the converter output in series
with the parallel 0.22Q current sensing resistors.
Thus, the voltage developed across
the 0.22Q resistors depends on the
current through the nicad battery. This
voltage is filtered using a 10kQ resis40
SILICON CHIP
tor and 0. lµF capacitor and fed back
to one of the error amplifiers to regulate the converter output, as described
previously.
In addition to the nicad battery
pack, the converter output also drives
the Charge LED (LED 1) via S2, a
fixed voltage drop , a 680Q resistor
and transistor Q5. During charging,
SCR1 is off and Q5 is turned on via
the lkQ resistor connected between
Sl and the anode of SCRl. Thus,
when Q5 is on, LED 1 lights to indicate that charging is in progress.
Fixed voltage drop
Switch S2 selects the fixed voltage
drop and this in turn sets the charging voltage to suit the nicad battery
pack. In position 1, the voltage drop
is provided solely by the lO0kQ resistor on the anode of D6. This is the 6V
range for charging a 6V battery pack
or five 1.2V cells in series.
The remaining switch positions
select LED4-ZD7 for the 7.2V, 8.4V,
9.6V, 12V and custom ranges respectively. These selected voltage drops
are there simply to reduce the voltage
applied to the inverting input of
comparator IC8b, since the DAC tracking circuitry can only operate from a
range of 5 to 9.5V.
Because of this limited operating
range, D6 and its associated components are included to ensure that there
is always at least 5.6V on pin 6 of
Normally, the output of IC8a is high
and so IC4 is enabled and it clocks
binary counter IC5 via diode DlO. DlO
and the associated lOkQ pullup resistor ensure that this clock signal swings
only between +5V and+ 12V to match
the supply rails to IC5.
In order to operate correctly, the
DAC requires a reference voltage to
provide a fixed current via the 1 %
4.7kQ resistor to its VREF+ (pin 14)
input. The 9.55V reference used is
derived from the +5V reference of IC1
via op amp IC3b which has a gain of
1.91. In addition, the +5V reference
from IC1 is buffered using unity gain
non-inverting stage IC3a to provide a
+5V supply rail for IC5 & IC6.
IC7a (TL072) converts the output
current from pin 4 of IC6 to a voltage
output and applies this to the inverting (pin 2) input of IC8a. The 1 %
4.7kQ feedback resistor across IC7a
ensures that its output voltage is
within the 5V to 9.55V range.
As soon as the DAC output exceeds
the sampled battery voltage, IC8a
switches its pin 1 output low and
stops the clock (IC4). This freezes the
binary counter and thus also freezes
the DAC at its peak count as described
previously. However, if the battery
voltage subsequently rises again (ie,
as charging proceeds), IC8a will again
switch its output high and the DAC
output (pin 1, IC7a) will again increase to slightly greater than the battery voltage before freezing at this new
level.
End-of-charge detection
In addition to driving ICBa, the
output of IC7a is also reduced by
80mV and applied to the pin 5 input
of IC8b. This 80mV reduction in level
is derived by using IC7a to drive a
voltage divider network (3.3kQ &
100kQ) which is connected in parallel with a 2.5V reference diode (REF1).
The resulting 80mV-reduced signal is
A single large PC board makes it easy to build this project, despite the circuit
complexity. There are just two trimpot adjustments to make when the assembly
is completed: the fast & trickle charge rates.
then derived from the tap of the voltage divider and applied directly to
IC8b where it is compared with the
sampled battery voltage.
As stated earlier, when the nicad
battery is fully charged, further charging results in a slight reduction in
output voltage (see Figs.2 & 4). So, as
soon as the nicad battery voltage falls
by 80mV from its peak value, pin 7 of
IC8b goes high and turns on SCRl via
D9 and a 3.3kQ resistor. This then
pulls the control line to pin 2 of ICl
to about 3.4V (1V across the SCR +
1.8V across LED 2 + 0.6V across D7)
and so the converter shuts down and
battery charging ceases.
Because it is now forward biased,
LED 2 lights to indicate the end of
charge condition. At the same time,
the SCR pulls the base of Q5 low and
this turns off to extinguish charge
indicator LED 1.
Once triggered, the SCR can only
be switched off by reducing the curr!;lnt through it to zero. This task is
performed by Reset (Start) switch Sl
which also resets binary counter IC5,
by pulling its reset pin to +lZV. S3b
disables the AID converter circuitry
by holding the reset line to IC5 high,
when the trickle charge mode is selected.
This means that the batteries are
left on charge when trickle charge is
selected. There is no automatic shutdown for this mode. This is not a
problem though because trickle charging is not likely to cause cell damage.
Error detector
Comparator IC7b provides an error
warning if SZ is set to a range that is
too low to suit the battery on charge.
When this happens, IC7a's output will
eventually rise above 9.3V and this
triggers IC7b which switches its output high. This triggers SCRl via ZDB
& DB to shut down the charger and at
the same time lights the error LED
(LED 3).
Note that ZD8 is necessary because
IC7b's output does not go fully .to
ground since it is an bp amp rather
than a comparator. Without the zener
diode, the SCR would be triggered by
IC7b as soon as power was applied to
the circuit.
The output ofIC7b also drives transistor Q6 via ZD8 and a 15kQ resistor.
When IC7b's output switches high,
Q6 turns on and pulls pin 4 of IC4
low to prevent further clocking of IC5.
What about the reverse situation,
where the range selected is too high
for the battery being charged? In this
situation, the battery will never fully
charge and LED 1 (Charge) will usually remain off or be very dim.
That's all we have room for this
month. Next month, we will give the
full construction details.
SC
JANUARY 1991
41
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