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By PETER SMITH
This simple project is ideal for testing DC
power supplies, shunt regulators & constant
current sources. It’s also a great way to check
battery capacity and can even be used as a
current limiter for an existing DC supply.
I
F YOU’RE INVOLVED with servicing or building power supplies,
you’ll wonder how you ever
managed without this ultra-useful
testbench tool! This electronic load enables you to observe DC power circuits
under a variety of load conditions, all
of which can be quickly “dialled-in”
using a single potentiometer.
58 Silicon Chip
An electronic load is good for testing
batteries too. But why use an electronic
load instead of a resistive load? Let’s
find out.
Resistance is futile
Electronic loads are often called
“dummy” loads. This name refers to
the fact that they replace or simulate a
real load. For example, a dummy load
might be used at the output terminals
of a DC power supply to allow measurement of ripple voltage at different
current levels. The dummy load enables us to conveniently program any
load resistance (and thus current flow)
that we desire.
Of course, a dummy load need not
be electronic – it could consist of a
rheostat or even a bunch of high-power resistors in series and/or parallel.
However, these methods tend to be
rather inflexible and lack adjustment
range and resolution.
Rather than providing a variable
load resistance, the electronic version
presented here provides variable curwww.siliconchip.com.au
CON4
+
CURRENT MUST NOT EXCEED 50W
CURRENT
*10A
*PRODUCT OF THE VOLTAGE AND
50W
*50V
VOLTAGE
MAXIMUM INPUT RATINGS
1k
R12
R14
.01
3W
1k
10k
C5
1.5nF
R10
6
IC1b
1k
7
2
3
S
D
SC
2002
G
E B C
_
CON2
+
SIMPLE 50W DC ELECTRONIC LOAD
CURRENT
SET
S2
RANGE
SELECT
10A
STW34NB20
BC327
_
+
CON1
1A
2
CON3
VR1
2k
10A
ADJ.
_
R3
10k
1
R2
47k
+V
R1
180
1W
REF1
ICL8069
+1.2V
+
ZD1
10V
1W
S1
POWER
Y
VR3
50k
10T
X
VR2
100k
1A
ADJ.
C1
47F
16V
R4
510k
C2
100nF
3
Z
R5
1k
4
C3
1nF
Q2
BC327
C
R9
IC1:
LMC6062
4
IC1a
8
1
C4
1nF
10k
R13
5
D3
R8
22
G
R11
S
bSTW34NB20
C7
100nF
100V
C6
47F
100V
NP
bQ1
D
www.siliconchip.com.au
9 - 12V DC
INPUTS
Fig.2 (right): the final circuit for the
Electronic Load. IC1b amplifies the
voltage across feedback resistor R14
by a factor of 10 and this allows R14
to be substantially reduced in value
(which, in turn, reduces its power
dissipation). Q2 and diodes D1-D3
clamp the output of IC1a when the
load voltage is very low, to protect Q1.
+V
B
E
+V
How it works
The Simple 50W Electronic Load is
based around an adjustable precision
current sink. Fig.1 shows the elements
of a basic current sink. It consists of
op amp IC1, power MOSFET Q1 and
resistor R1 and operates as follows:
Initially, both the inverting and
non-inverting inputs of IC1 are at 0V,
so the output is also at 0V. When a
voltage (VIN) is applied to the non-in-
R7
1k
R6
100k
Current limiting
Earlier on, we stated that the Electronic Load could be used to provide
current limiting for an existing power
supply. How do we do that? Simple
– just connect the load terminals in
series with the negative supply lead.
It’s then just a matter of winding
up the pot to set the required current
limit.
2x 1N4148
D2
D4
1N4148
D1
1N4148
rent sinking. This means that regardless of the applied voltage, the current
that it “swallows” remains exactly as
set. The required load current is simply “dialled in” via a multi-turn potentiometer, up to a maximum of 10A.
Note that, to handle both low and
high-power circuits, we’ve included
1A and 10A switch-selectable current
ranges.
POWER
_
FAST
BLOW
F1
12A
LOAD TERMINALS
Fig.1: the basic scheme for a
current sink. The current through
R1 depends on the voltage applied
to IC1’s non-inverting input and is
independent of the supply voltage.
September 2002 59
Table 2: Capacitor Codes
Value Alt. Value IEC Code EIA Code
100nF 0.1uF
100n
104
1.5nF .0015uF 1n5
152
1nF
.001uF 1n
102
reduce its power dissipation to sensible levels.
The basic current sink described
above has one major drawback when
used in high-current applications,
however. Consider the case where a
certain current is “dialled-in” but little
or no voltage is present across the load
terminals. In this case, insufficient
current flows in the circuit to generate
enough voltage across R14 to satisfy
the feedback loop.
This means that IC1a’s output will
be at the supply rail voltage, turning
Q2 fully on. If a low-impedance source
is now connected to the load terminals, a massive instantaneous current
will flow, limited only by the drain to
source “on” resistance of Q4 and the
.01Ω feedback resistor. Result – exit
one MOSFET!
To prevent this, we’ve included a
clamping arrangement for the op amp,
formed by diodes D1-D4, transistor
Q1 and resistor R6. This circuit works
as follows: when the load voltage is
below a certain threshold, Q2 turns
on (via D4) and so pin 1 of IC1a is
effectively clamped to four diode
drops above pin 2 – ie, approximately
2.9V.
As a result, IC1a’s output is effectively below the MOSFET’s gate
threshold voltage and so the current
flow through this device is kept to a
very low level. Conversely, when the
load voltage rises above the threshold,
Q2 turns off and plays no further role
in the circuit – ie, feedback control is
now via IC1b.
Fig.3: install the parts on the PC board as shown in this wiring diagram.
The .01Ω resistor looks like a thin metal U-shaped band and is mounted
by pushing it down until its shoulders contact the board (see photo).
Fig.4: if you can’t get a multi-turn pot (or just want to save money), here’s
how to wire up two low-cost pots as coarse and fine controls instead.
verting input, the op amp’s output
begins to rise rapidly towards the
positive supply rail. When this voltage
exceeds the MOSFETs gate threshold
voltage, it begins to conduct, causing
current (IO) to flow.
Obviously, the current flow through
resistor R1 causes a voltage drop
across it:
V = IO x R1
This, in turn, is fed back to the
inverting input of IC1. The op amp’s
output voltage will continue to rise
until this feedback voltage equals the
voltage on the non-inverting input
(VIN). Therefore, we can say that:
IO = VIN/R1
As you can see, the current flow
(IO) in the circuit is independent of
the applied voltage (V+). Instead, it
depends on the voltage applied to the
op amp’s non-inverting input (VIN).
Our final design (see Fig.2) expands
on the above by adding an additional
op amp stage (IC1b) in the feedback
loop. This stage amplifies the voltage
across the feedback resistor (R14) by
a factor of 10, as set by resistors R10
and R12. And that, in turn, allows us
to reduce the value of R14 and thus
Table 1: Resistor Colour Codes
No.
1
1
1
1
3
3
1
60 Silicon Chip
Value
510kΩ
180Ω 5%
100kΩ
47kΩ
10kΩ
1kΩ
22Ω
4-Band Code (1%)
green brown yellow brown
brown grey brown gold
brown black yellow brown
yellow violet orange brown
brown black orange brown
brown black red brown
red red black brown
5-Band Code (1%)
green brown black orange brown
not applicable
brown black black orange brown
yellow violet black red brown
brown black black red brown
brown black black brown brown
red red black gold brown
www.siliconchip.com.au
ELAN Audio
The Leading Australian
Manufacturer of Professional
Broadcast Audio Equipment
Featured Product of the Month
PC-BAL
PCI Format
Balancing
Board
Interface
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Cards to
Professional
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Not only do we make the best range of
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This is the completed PC board
assembly, ready for attachment to the
heatsink. Note that the standoffs fitted
to the rear of the board should be
removed once the heatsink is attached.
This arrangement provides a much
smoother current ramp, with less overshoot when cycling the input.
The load current is controlled by
external potentiometer VR3, which
varies the voltage applied to the
non-inverting input of IC1a. With
range switch S2 in the 1A position, the
maximum output from VR3 is 100mV.
Alternatively, when S2 selects the
10A position, the maximum output
is about 1V.
To ensure that the set current remains stable with tempera
ture and
input voltage variations, a precision
voltage reference IC (REF1) is used to
provide a steady 1.2V to the divider
networks. Trimpots VR1 and VR2 allow for full-scale adjustment of each
range, if required.
Unlike many electronic load circuits, this unit sources its supply
voltage independently of the load
terminals. This ensures that the circuit
continues to operate, even when the
voltage at the load terminals drops to
just a few volts. As the circuit draws
only about 390µA, it can be powered
from a 9V PP3 battery.
Alternatively, a 2.5mm DC socket
is provided for 9-12V DC plugpack
operation.
Construction
All parts except the potentiometer
(VR3) and range switch (S2) mount
on a 58 x 93.5mm single-sided PC
www.siliconchip.com.au
And we sell AKG and Denon Professional
Audio Products
For Technical Details and Professional Pricing Contact
board. Fig.3 shows how the parts are
installed.
Begin by installing the two wire
links and follow with all the 0.25W
resistors. Diodes D1-D4 and zener
diode ZD1 can go in next but watch
their orientation – the cathode (banded) ends must be aligned as shown.
Once the diodes are in, install all
remaining components in order of
their height. Transistor Q2 and power
resistor R14 should be left until last.
Before soldering R14, make sure that
its shoulders are seated firmly against
the PC board surface.
The mounting position for Q2 will
depend on the chosen heatsink. On
our prototype, we inserted it into the
PC board just far enough for proper
soldering. With 10mm spacers fitted
to the board, this placed Q2 near the
centre line of the heatsink for best heat
dissipation.
Elan Audio 2 Steel Crt
South Guildford WA 6055
Phone 08 9277 3500
08 9478 2266
Fax
email sales<at>elan.com.au
WWW elan.com.au
Subscribe &
Subscribe &
Get this FREE!*
Get this FREE!*
*Australia only. Offer valid only while
last.
*Australia only. Offer validstocks
only while
stocks last.
External hardware
The current set potentiometer
(VR3) and range switch (S2) are connected to the PC board via terminal
block CON3. You can use light-duty
hook-up wire for this job. The circuit
diagram (Fig.2) shows the pinouts
for CON3.
If you don’t need the fine resolution
of the 1A range, then you can save
wiring (and money) and connect VR3
directly to the 10A circuit, eliminating
the need for the range switch. Note
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September 2002 61
Parts List
1 PC board, code 04109021, 58 x
93.5mm
1 SPDT PC-mount sub-miniature
slide switch (S1) (Altronics
S-2060, Jaycar SS-0823)
1 SPDT miniature panel-mount
toggle switch (S2)
1 heatsink to suit (0.6°C/W
thermal resistance or lower)
4 2 way 5mm pitch terminal blocks
(CON2 - CON4)
3 M3 x 6mm cheese head screws
2 M3 x 10mm tapped spacers
1 M3 flat washer
2 PC-mount 3AG fuse clips
1 12A 3AG fast-blow fuse
1 BC327 PNP transistor (Q2)
1 ICL8069 1.23V voltage reference
(REF1) (Farnell 410-895)
4 1N4148 diodes (D1-D4)
1 1N4740A 10V, 1W zener diode
(ZD1)
Semiconductors
1 LMC6062IN dual CMOS op amp
(IC1) (Farnell 270-854)
1 STW34NB20 N-channel
MOSFET (Q1) (Farnell 498-180)
Resistors (0.25W, 1%)
1 510kΩ
3 10kΩ
1 180Ω 1W 5% 3 1kΩ
1 100kΩ
1 22Ω
1 47kΩ
that the wire length should be kept as
short as possible to reduce potential
noise pick-up.
It may help to tightly twist the wires
to VR3 or, even better, use a length
of shielded cable. The cable shield
should be connected to ground (CON3,
pin 3) at one end and to terminal “Y”
and the metal shell of the potentio
meter at the other end.
For most applications, a 10-turn
wire-wound potentiometer is preferred for VR3. However, these can
be expensive and difficult to obtain.
An alternative arrangement using
standard carbon track potentiometers
is shown in Fig.4. Here we’ve shown
Capacitors
1 47µF or 56µF 100V
non-polarised axial-lead
electrolytic (Altronics R-6415,
Jaycar RY-6916)
1 47µF 16V PC electrolytic
2 100nF 100V MKT polyester
1 1.5nF 63V MKT polyester
2 1nF 63V MKT polyester
how a 50kΩ dual-gang pot (VR3a &
VR3b) and a 500Ω pot (VR4) can be
wired together to give both coarse and
fine adjustments.
Keeping your cool
Apart from aesthetic reasons, there
is no real need to house your completed work. For long service life, it
can simply be mounted on a thick
aluminium baseplate.
However, if you prefer to build it
into a case, then allow for plenty of
ventilation. If the heatsink fins are
vertically arranged, then you should
install small spacers under the heat
sink to allow airflow up through the
Fig.5: this is the full-size etching pattern for the PC board.
62 Silicon Chip
1 0.01Ω 3W 1% power resistor
(Welwyn ‘OAR’ series)
(Farnell 327-4718)
Potentiometers
1 2kΩ miniature horizontal trimpot
(VR1)
1 100kΩ miniature horizontal
trimpot (VR2)
1 50kΩ multi-turn linear
potentiometer (VR3)
(Farnell 351-817) -or1 50kΩ dual-gang linear
potentiometer (VR3) (coarse
adjustment) -and1 500Ω linear potentiometer
(VR4) (fine adjustment)
Miscellaneous
Heatsink compound, 50mm-length
(approx.) tinned copper wire for links,
light duty hook-up wire
fins. Ventilation holes positioned
directly above and below the fins
will make the most of the “chimney”
effect.
Alternatively, if the fins are horizontally arranged, then you’ll almost
certainly require forced air cooling of
some kind.
A single 3mm hole is required for
attaching the power MOSFET. Try to
position this as close to the centre of
the heatsink as possible and be sure
to remove any sharp edges that result
from drilling. You can deburr the hole
using an oversize drill.
Mounting the MOSFET
50W continuous power dissipation
is quite a bit to ask from a single plastic power MOSFET, even in the larger
TO-247 package. Therefore, we have
to make sure that as much of the heat
as possible flows out of the package
and into the heatsink. In other words,
proper mounting of the power MOSFET (Q1) is vitally important!
Unlike many other projects described in SILICON CHIP, the MOSFET
should not be electrically isolated from
the heatsink. To mount it, first apply a
thin, even smear of heatsink compound
to the entire rear face of Q1 as well
as the area that it will contact on the
heatsink. That done, attach Q1 to the
heatsink using an M3 screw with a flat
washer and tighten it up firmly.
www.siliconchip.com.au
Note: direct connection between the
transistor and heatsink means lower
thermal resistance but it does have a
downside. Along with the centre pin,
the metal contact area of the transistor is connected to the drain, so the
heatsink is always at positive load
terminal potential.
That means that you have to make
sure that the heatsink doesn’t short
against anything when using the Electronic Load.
Prototype performance
We checked the full-power performance of our prototype with an
infrared thermometer and an ambient
temperature of 22°C. The heatsink
temperature rose to 70°C, with Q1
running about 10°C hotter.
Although the transistor temperature
was within specification, we hadn’t expected the thermal resistance between
it and the heatsink to be so high. A
little investigation revealed that the
heatsink surface was not completely
flat, resulting in only partial contact
with the transistor!
Watch this point when buying a
heatsink – make sure that the contact
area is completely flat.
Circuit protection
The 12A fast-blow fuse included
in the circuit provides only basic
over-current protection. No over-voltage or overload protection has been
included, which is why we’ve dubbed
it the “Simple” Electronic Load.
Having said that, the MOSFET
we’ve selected for this circuit is a
very robust device, so you’d have to
exceed the ratings listed in Fig.2 by a
fair margin in order to destroy it.
If you’re interested in increasing
the robustness even further, then one
option might be to use a special “pro-
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Video Processors, Colour Correctors, Stabilisers, TBC’s, Converters, etc.
QUESTRONIX
tected” MOSFET in place of the standard part specified for Q1. Manufac
turer STMicrolelectronics produce
a range of such devices, called OMNIFETs. Additional circuits built into
these devices add thermal, short-circuit and over-voltage protection to
normal MOSFET function.
A suitable device from the range is
the VNW100N04 (rated at 42V). This
is available locally from Farnell Electronic Components.
Note that the OMNIFET’s over-voltage protection is intended for transient
protection only. This means that you
should not apply a higher than specified maximum drain to source voltage
across the load terminals.
Check out the STMicrolelectronics
web site at http://us.st.com for more
details on these devices.
Calibration
Trimpots VR1 and VR2 provide
full-scale trim for their respective
ranges. To adjust them, insert a 10A
or higher rated ammeter in series with
the positive load terminal and connect
a suitable power source. Set S2 to the
1A range and apply power. Wind VR3
All mail: PO Box 348, Woy Woy NSW 2256
Ph (02) 4343 1970 Fax (02) 4341 2795
Visitors by appointment only
fully clockwise and adjust VR2 for a
reading of 1.00A on your meter.
Now toggle S2 to the 10A position
and repeat the procedure, this time
adjusting VR1. Be sure not to exceed
the maximum power rating, which
means that the input voltage must
not be above 5V when the load is
swallowing 10A.
The position of VR4 should now
correlate roughly with the desired
percentage of full-scale current. For
example, on the 10A range with VR4
at centre position, current draw should
be about 5A. Of course, for real accuracy you’ll need to leave your ammeter
connected.
Load modulation
As presented, this project is intended as a DC current sink. However,
the frequency response of the circuit
is such that it should be possible to
modulate the control voltage to IC1a
by various external means should you
have such a requirement.
No promises though – we haven’t
tried it! If you want to give it a go,
we suggest a maximum modulation
SC
frequency of about 1kHz.
K&W HEATSINK EXTRUSION. SEE OUR WEBSITE FOR
THE COMPLETE OFF THE SHELF RANGE.
www.siliconchip.com.au
September 2002 63
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