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SemTest
Pt.1: By JIM ROWE
Check all those semiconductors in your collection
with this easy-to-build test set!
How many discrete semis have you got in your collection?
Hundreds? Thousands? Are they all good? Don’t know? With our
new Discrete Semiconductor Test Set you will be able to test a
wide range of active components: LEDs, Diodes, Bipolar Junction
Transistors, Mosfets, SCRs and Programmable Unijunction
Transistors (PUTs), for gain (where applicable), voltage breakdown
and leakage. You can even run tests on IGBTs and Triacs!
O
F COURSE, THERE are lots of
semiconductor testers out there.
These range from the handy pocketsized instruments produced by Peak
Electronic Design Ltd in the UK to
large laboratory bench instruments
made by Agilent and costing many
thousands of dollars. The former group
are not able to test the range of semiconductors that we would like, while
the latter instruments are beyond the
42 Silicon Chip
reach of all but a few research labs.
So Publisher Leo Simpson set me
the task of producing a new design. It
had to be easy to drive and would be
somewhat similar in concept to the
“Test Set For Transistors & Diodes”
featured in Electronics Australia magazine way back in the July and August
1968 issues (yes, back in the olden
days – and it was my design too!).
It was pretty simple – using a bunch
of rotary switches, a 50µA moving coil
meter and olde-worlde point-to-point
wiring – but it could perform most of
the basic tests that were needed on
the discrete semiconductor devices
of the day.
I took one look at that old 1968 design and shuddered: all that point-topoint wiring – all those switches – no
PCB – an analog meter. Gaaakkk! What
could Leo be thinking? Not only that,
siliconchip.com.au
it was designed long before Mosfets
were even thought of and we would
have to include them, of course.
In the fullness of time (a silly expression glossing over the trials and
tribulations – not to mention the blood,
sweat and tears – of producing a completely new design), we came up with
the SemTest. It’s otherwise known as
a Discrete Semiconductor Test Set –
which is too much of a mouthful.
It’s around half the physical size of
the 1968 design and it’s controlled by
a microprocessor, with a 16x2 LCD
panel used to display the device to
be tested, the test to be run and the
test results. There are a minimum
of front panel controls: one rotary
switch, one pot and five pushbuttons.
And the curly problem of catering to
all the different semiconductor sizes
and pin-outs has been solved by employing an 18-pin ZIF (zero insertion
force) socket.
These sockets are normally used
for programming microprocessors but
they are ideal for this application.
All the parts inside the case are accommodated on two medium-sized
PCBs which are connected together
by three IDC cables.
However, before we jump into describing the circuitry of the SemTest in
detail, we need to discuss the tests it
can perform on each type of the most
commonly used discrete semiconductors. After all, if you are contemplating
building the SemTest, you will want to
understand all the tests that it can run.
TESTS AVAILABLE ON THE DISCRETE SEMICONDUCTOR TEST SET
Device Type
Diodes, including
zener & schottky
(also Diacs)
LEDs
Bipolar Junction
Transistors
(NPN or PNP)
Mosfets
(N-channel or
P-channel)
SCRs & PUTs
(also Triacs)
Test Parameter
Extended description
IR (BV)
Reverse avalanche current with BV (600V) applied*
IR (OPV)
Reverse leakage current with OPV (10/25/50/100V) applied*
VF (OPV)
Forward voltage drop with OPV (10/25/50/100V) applied*
VR (BV)
Zener/avalanche voltage with BV (600V) applied*
IR (OPV)
Reverse leakage current with OPV (10V) applied*
VF (OPV)
Forward voltage drop with OPV (10/25/50/100V) applied*
V(BR)CBO (BV)
Breakdown voltage with e o/c, BV (600V) applied*
V(BR)CEO (BV)
Breakdown voltage with b o/c, BV (600V) applied*
ICBO (OPV)
Leakage current with e o/c, OPV (10/25/50/100V) applied*
ICEO (OPV)
Leakage current with b o/c, OPV (10/25/50/100V) applied*
hFE with IB = 50A (OPV)
Forward current gain with IB = 50A, OPV applied*
hFE with IB = 200A (OPV)
Forward current gain with IB = 200A, OPV applied*
hFE with IB = 1mA (OPV)
Forward current gain with IB = 1mA, OPV applied*
V(BR)DSS (BV)
Breakdown voltage with g-s short, BV (600V) applied*
IDSS (OPV)
Leakage current with g-s short, OPV (10/25/50/100V) applied*
IDS vs VGS (OPV) (gfs)
d-s current vs VGS (0-12V), OPV (10/25/50/100V) applied*
V(BR)AKS (BV)
Breakdown voltage with g-k or g-a short, BV (600V) applied*
IAKS (OPV)
a-k current with g-k or g-a short, OPV (1/25/50/100V) applied*
IAK with IG = 50A (OPV)
a-k current with IG = 50A, OPV (1/25/50/100V) applied*
IAK with IG = 200A (OPV)
a-k current with IG = 200A, OPV (1/25/50/100V) applied*
IAK with IG = 1mA (OPV)
a-k current with IG = 1mA, OPV (1/25/50/100V) applied*
VAK(ON) (OPV)
a-k voltage drop when on, OPV (10/25/50/100V) applied*
*Both BV and OPV are always applied via appropriate current limiting series resistors
RSERIES
A
A
DUT*
VOLTAGE
DIVIDER
RELAY9
K
siliconchip.com.au
ADC0
(DEVICE
VOLTAGE)
K
OFF = FWD
ON = REV
ADC1
(DEVICE
CURRENT)
Diodes & LEDs
These sound simple enough but
there are different sorts: standard
silicon and germanium signal & rectifier diodes, zener/avalanche diodes,
schottky barrier diodes, LEDs and
Diacs (bipolar breakover diodes,
which are actually a 2-terminal thyristor). The new tester can perform basic
tests on all of these devices.
A simplified version of the diode
test circuitry used in the SemTest is
shown in Fig.1. It’s very straightforward, yet can be used to measure any
of four basic diode parameters:
(1) VF – the voltage drop when conducting in the forward direction;
(2) IR – the leakage current which flows
when a reverse “operating” voltage
(OPV) of 10V/25V/50V/100V is applied via an appropriate series current
limiting resistance;
(3) IR – the current which flows when
+V (BV OR OPV)
* DIODE, ZENER OR LED
RSHUNT
Fig.1: the basic diode test circuitry. It uses Relay9 to switch the polarity of
the diode under test, a shunt resistor to allow current measurements and a
voltage divider to interface with the microcontroller.
a higher “breakdown” voltage (BV) of
600V is applied (again via a suitable
series current limiting resistor); and
(4) VR – the voltage drop when the diode is conducting in the reverse direction in “avalanche” breakdown mode.
All four of these tests can be applied
to test zener/avalanche diodes, signal
& rectifier diodes, schottky diodes
and even Diacs. The last two tests
are not available for testing LEDs as
these devices can be damaged if sufficient current flows during avalanche
breakdown.
In fact, before you do an IR test on
a LED, the SemTest warns you of possible damage if the lowest operating
voltage of 10V is not selected.
The diode test circuit of Fig.1 uses
RELAY9 to switch the polarity of the
diode under test. When RELAY9 is off
(not energised), the diode’s anode (A)
is connected to the test voltage source
(+V) via series current-limiting resistor RSERIES.
Note that test voltage +V is switched
between the operating voltage (OPV)
and the breakdown voltage (BV) level
by the microcontroller, which also
changes the value of series resistor
February 2012 43
RSERIES
DUT*
C
+V (BV OR OPV)
C
B
B
E
ADC0
(DEVICE
VOLTAGE)
VOLTAGE
DIVIDER
RELAY10
E
OFF = NPN
ON = PNP
RELAY11
ADC1
(DEVICE
CURRENT)
OFF = BVceo, Iceo or hFE
ON = BVcbo or Icbo
RELAY6
RSHUNT
RELAY5
+Ibias
–Ibias
OFF = BVcbo, BVceo,
Icbo or Iceo
ON = Hfe (PNP)
OFF = BVcbo, BVceo,
Icbo or Iceo
ON = Hfe (NPN)
NOTE: ±Ibias LEVELS ARE
SET VIA RELAYS 3 & 4
* NPN OR PNP BIPOLAR TRANSISTOR
Fig.2: the basic test configuration for bipolar junction transistors (BJTs). It
uses four relays to perform all of the basic tests normally required on NPN
or PNP devices.
RSERIES to suit the various tests. In
operation, the micro switches +V on
only during the actual test and then
off again at the end of the test.
For the “reverse bias” tests, the micro energises RELAY9 which simply
reverses the diode polarity so that the
cathode (K) is connected to +V instead
of the anode.
The rest of the diode test circuit
includes a voltage divider, used to allow the micro to measure the voltage
across the diode under test, by means
of the micro’s analog-to-digital (A/D)
converter input ADC0. The micro
also switches the voltage divider’s
ratio to suit the voltage source used
for each test.
Finally, there’s a shunt resistor
(R SHUNT ) connected between the
cathode (or anode) of the diode and
ground. The top of this resistor is connected to the ADC1 input of the micro
so it can measure the voltage across
RSHUNT and then calculate the device
current. Again, the value of RSHUNT is
switched by the micro, in this case to
suit the current range required for the
selected test.
By the way, since the voltage drop
across RSHUNT effectively adds to
the device voltage as measured via
the voltage divider and the microcontroller’s ADC0 input, this has
44 Silicon Chip
the potential to introduce a small error
in the device voltage measurement.
This voltage drop across RSHUNT is
quite small, with a maximum of 2.0V
for a “full scale” current reading of
20mA (or 200µA on the low range).
To eliminate this problem, the
firmware automatically corrects the
reading. It does that by subtracting
100mV for each 1mA of device current on the higher range, or for each
10µA of current on the low range (ie,
it automatically subtracts the voltage
across the RSHUNT).
Testing Diacs
Before we move on, let’s look at how
a Diac can be tested with the SemTest.
It should connected to the diode A and
K terminals (either way around) and
first given the diode VF test with the
lowest (10V) setting for OPV. This will
show you whether the Diac is shorted
(which will give a reading of no more
than about 0.25V and a current of about
2.5mA) or “OK” (which will give a
reading of close to 10V).
If you do get a reading of very close
to 10V, you can repeat the above test at
25V or 50V until the Diac breaks over
into conduction. Typical Diacs break
over at between 25V and 35V, with a
current of less than 200µA.
When the Diac does switch into
conduction, the VF reading suddenly
drops to a much lower level – probably around 5-10V – while the current
jumps up into the 3-10mA region. If
the Diac behaves as described, you
then do the test in the other direction:
ie, switch back to the 10V setting for
OPV and then test it with the IR (OPV)
test selected.
This will let you check the Diac’s
operation in the reverse direction. You
should again see it drawing a current
of less than 200µA with only 10V applied, with the current jumping up to
between 5mA and 15mA when you
select an operating voltage of 25V or
50V so that it “breaks over” again.
If your Diac gives these expected
results in both tests, it is working as
it should.
Testing transistors
Testing bipolar junction transistors
or “BJTs” is more complex than with
diodes, because there are NPN and
PNP types and they have three leads
rather than two. Fig.2 shows the test
configuration for BJTs. This uses four
relays to perform all of the basic measurements normally required for NPN
or PNP devices:
(1) ICBO – the leakage current passed
between collector and base, with a selected operating voltage (OPV) applied
and the emitter open-circuit;
(2) ICEO – the leakage current passed
between collector and emitter, again
with a selected operating voltage
(OPV) applied but this time with the
base open-circuit;
(3) V(BR)CBO – the breakdown voltage
measured between collector and base,
with the emitter open-circuit but with
a breakdown voltage (BV) source
applied via a series current-limiting
resistor;
(4) V(BR)CEO – the breakdown voltage
measured between collector and emitter, with the base open circuit but
with a breakdown voltage (BV) source
applied via a series current-limiting
resistor; and
(5) hFE – the common-emitter forward
current gain, measured at any of three
base current levels (IB = 50µA, 200µA
or 1mA). The choice of base current
levels is provided to cope with small
and medium-power devices.
As you can see from Fig.2, RELAY10
is used for setting up the BJT circuit
for testing either NPN or PNP devices.
RELAY11 is used to perform the base/
emitter switching for the various tests,
siliconchip.com.au
RSERIES
DUT*
D
S
+V (BV OR OPV)
D
22
G
G
ADC0
(DEVICE
VOLTAGE)
VOLTAGE
DIVIDER
RELAY12
S
1M
OFF = N–CH
ON = P–CH
ADC1
(DEVICE
CURRENT)
RELAY13
RSHUNT
OFF = G–S SHORT
ON = G CONNECTED
TO Vgs
10k
* N–CH OR P–CH
ENHANCEMENT
MODE MOSFET
RELAY14
ADC2
(MEASURE
Vgs)
Vgs
10k
ADJUST
–Vgs
+Vgs
K
ADJUST
+Vgs
OFF = +Vgs (N–CH)
ON = –Vgs (P–CH)
VR10a
10k
ZD3
12V
K
VR10b
10k
ZD4
12V
A 10k
10k
A
–Vgs
Fig.3: the Mosfet test circuit. Only three relays are used and these allow all the main tests normally required for
both N-channel and P-channel Mosfets. The positive VGS (gate-source) voltage is derived from zener diode ZD3 and
varied by VR10a, while the “negative” VGS voltage is derived from ZD4 and varied by VR10b.
while RELAY5 is used to switch on
positive base bias current (+IBIAS) for
hFE testing of NPN devices. RELAY6
is used to switch on negative base bias
current (-IBIAS) for hFE testing of PNP
devices.
Additional relays (RELAY3 and
RELAY4, not shown in Fig.2) are
used to switch both +IBIAS and -IBIAS
between the various current levels.
As with the diode testing circuit,
either operating voltage (OPV) or
breakdown voltage (BV) can be applied
to the transistor being tested, via series current-limiting resistor RSERIES.
Again the micro switches the OPV/
BV source on only for the actual test,
and then off when the test is ended.
It also changes the value of RSERIES to
suit each kind of test.
As before, there is a voltage divider
across the device being tested, feeding
the micro’s ADC0 input so that the
micro can measure the device voltage
VDEV. Again, the micro changes the
divider ratio to suit each kind of test.
The device current is also measured
in exactly the same way as for diodes,
with shunt resistor RSHUNT used to
effectively convert the device current
into a small voltage for measurement
via the micro’s ADC1 input. The micro
siliconchip.com.au
can also switch the value of RSHUNT
to provide two current ranges: 20mA
and 200µA.
We should point out here that, as
before, the small voltage drop across
RSHUNT will effectively add to the device voltage measurement, introducing a small measurement error for V(BR)
CBO and V(BR)CEO. Again the software
corrects for this error by subtracting
100mV for each 1mA of device current
on the higher range, or for each 10µA
of current on the low range.
Testing Mosfets
Testing metal-oxide-semiconductor
field effect transistors or “Mosfets” is
not significantly more complicated
than with BJTs, even though Mosfets
are a voltage-controlled transconductance device rather than a currentcontrolled transadmittance device.
As with BJTs there are again two
types, in this case N-channel and Pchannel devices, with different polarity requirements for both drain-source
voltage and gate bias voltage. There’s
also a difference in terms of breakdown
voltage and leakage current measurement, of course.
Note, however, that the SemTest is
only capable of testing junction FET
or “JFET” devices in a limited sense,
as these operate in depletion mode
rather than in enhancement mode as
used by modern Mosfets.
Whereas Mosfets pass virtually zero
drain-source current with zero gate
bias and need gate bias in order to pass
significant drain-source current, JFETs
work the other way around; they pass
a significant drain-source current with
zero gate bias and need gate bias to be
applied in order to “throttle back” the
drain-source current. This means they
require “negative” gate bias, in contrast with the “positive” bias needed
by Mosfets.
Despite this limitation, the SemTest
is capable of testing JFETs for one quite
important parameter: IDSS – the drainsource gate current with the gate tied
to the source (ie, the zero-bias channel
current). This is done via the same Idss
test used for Mosfets (see below), the
difference being that with Mosfets the
reading should be very low (usually
well below 200µA), while for JFETs
the reading will be relatively high
(probably 10-20mA).
The Mosfet test circuit is shown
in simplified form in Fig.3 and it’s
relatively straightforward. Only three
relays are used but these allow the
February 2012 45
RSERIES
A
+V (BV OR OPV)
DUT*
A
(AG)
G
K
ADC0
(DEVICE
VOLTAGE)
VOLTAGE
DIVIDER
(KG)
K
RELAY15
RELAY16
OFF = SCR
ON = PUT
ADC1
(DEVICE
CURRENT)
RSHUNT
OFF = G shorted to K (SCR) or A (PUT)
ON = G connected to ±Ibias
+Ibias (VIA RLY5)
OR
–Ibias (VIA RLY6)
* SCR OR PUT
Fig.4: the test circuit for SCRs and PUTs uses two relays for switching and
is similar to that used to test bipolar junction transistors (BJTs). It carries
out five basic tests.
SemTest to perform all three of the
main tests normally needed for either
N-channel or P-channel Mosfets:
(1) IDSS – the drain-source current with
zero gate bias (ie, gate tied to source).
This can be measured with any selected operating voltage (OPV) applied
between drain and source, via a series
current-limiting resistor;
(2) V(BR)DSS – the drain-source breakdown voltage, again measured with
gate tied to source but in this case with
the higher voltage source (BV) applied
between drain and source, via a highervalue current limiting resistor; and
(3) ID – the drain-source current which
flows at any gate bias voltage VGS (variable between 0V and approximately
12V), with any selected operating voltage (OPV) applied between drain and
source. This allows the transfer characteristic of a device to be measured,
and its transconductance worked out.
As you can see from Fig.3, the
Mosfet drain-source voltage and drain
current are measured in exactly the
same way as for BJTs and diodes, us-
ing a voltage divider feeding ADC0 for
the voltage measurement and shunt
resistor RSHUNT feeding ADC1 for the
current measurement. The OPV/BV
switching and RSERIES switching are
managed by the micro as before, as is
the voltage divider ratio and the value
of RSHUNT.
The main differences between Fig.3
and the earlier test circuits are in the
gate switching circuitry, involving
RELAY13 and RELAY14. The first of
these relays carries out the primary
gate switching, shorting the Mosfet’s
gate to the source for the IDSS and V(BR)
DSS tests when it is not energised or
connecting the gate to a bias voltage
source VGS when it is energised (for
the ID versus VGS test).
RELAY14 then performs the job
of selecting either a “positive” VGS
source for N-channel devices, or a
“negative” VGS source for P-channel
devices.
The positive VGS source is derived
from the test voltage (OPV) via zener
diode ZD3 and varied by potentiome-
ter VR10a, while the “negative” VGS
source is also derived from OPV but
via ZD4 and varied by VR10b. The
latter is only negative by comparison
to the Mosfet’s source terminal, which
in the case of a P-channel device is
connected to OPV.
This explains why VR10a is adjusted upwards from ground (0V) to
increase +VGS (for N-channel devices),
while conversely VR10b is adjusted
downwards from the device source
voltage (representing zero VGS) to
increase -VGS for P-channel devices.
Since VR10a and VR10b are the two
sections of a dual-ganged 10kΩ+10kΩ
pot, they are simply wired in converse
fashion so that the effective gatesource voltage advances from zero as
the pot is turned clockwise.
The micro is able to work out the
effective gate voltage for any setting
of VR10a or VR10b via the connection
from the VGS source, as selected by
RELAY14, to a third ADC input of the
micro (ADC2). But because this only
allows the micro to measure the “raw”
gate voltage VG, relative to ground,
this means that for P-channel devices
it also has to measure the source-drain
voltage of the device and subtract
the measured gate voltage from it,
to calculate the effective gate-source
bias (-VGS).
With N-channel devices this isn’t
necessary, although the small voltage
developed across current measuring
shunt resistor RSHUNT will reduce
the effective gate-source bias for these
devices, by the same factor of 100mV
for each 1mA of current on the higher
current range or 10µA of current on
the lower range.
As with the hFE measurements
for BJTs, the firmware automatically
makes this correction.
What about IGBTs?
Although they’re not widely used
in general electronics, insulated-gate
bipolar junction transistors or IGBTs
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46 Silicon Chip
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The lower board in the SemTest carries the PIC microcontroller,
the power supply components and the test voltage selector switch.
are encountered in automotive ignition systems, fuel-injection controllers, high power inverters and AC
induction motor drives.
They can be regarded as very much
like an N-channel Mosfet and an NPN
BJT/PNPN silicon-controlled switch
combined, with a collector as the main
positive electrode and an emitter as
the main negative electrode. However,
they have a gate electrode for voltage
control instead of a base electrode for
current control.
IGBTs are usually quite high-power
devices, so the modest test currents
available inside the SemTest mean
that it isn’t really possible to use it to
fully characterise the performance of
an IGBT.
However, you can perform basic
tests on an IGBT by connecting it
to the SemTest’s Mosfet testing terminals (C to the drain terminal, E to
the source terminal and G to the gate
terminal). You then test it as if it were
an N-channel Mosfet, making a mental
conversion of the test results into the
equivalent parameters for an IGBT.
For example, the voltage reading
you get for V(BR)DSS will correspond to
the IGBT’s V(BR)CES (collector-emitter
breakdown voltage with the gate
shorted to the emitter), while the readsiliconchip.com.au
ing you get for IDSS will correspond
to the IGBT’s ICES (collector-emitter
leakage current with gate shorted to
emitter).
You’ll even be able to get an idea
of the IGBT’s gate threshold voltage
VGE(TH), by using the Mosfet ID vs
VGS test and finding the gate voltage
where ID (corresponding to the IGBT’s
collector-emitter current ICE) begins
rising from its ICES “off” level.
Testing SCRs & PUTs
The fourth main type of discrete
semiconductor device that the SemTest
is capable of testing is thyristors or
silicon-controlled switches (SCSs) – in
particular, SCRs (silicon-controlled
rectifiers) and PUTs (programmable
unijunction transistors).
Note that another name for an SCR
is a cathode-gate SCS, while a PUT
is more accurately described as an
anode-gate SCS. They are both PNPN
devices, and similar apart from the
different gate connections. So in that
sense they are essentially just two different “flavours” of SCS devices, like
NPN and PNP bipolars or N-channel
and P-channel Mosfets.
As a result, the circuitry needed for
testing SCRs and PUTs is not all that
different from that needed for BJTs, as
can be seen from the simplified circuit
shown in Fig.4.
Despite its simplicity, this circuit
allows the following measurements
to be carried out on SCRs and PUTs:
(1) V(BR)AKS – the breakdown voltage
for an SCR, with its gate tied to the
cathode and a source of high voltage (BV) applied between anode and
cathode via the usual current-limiting
resistor RSERIES;
(2) V(BR)AKS – the breakdown voltage for
a PUT, in this case with its gate tied
to the anode and the high voltage (BV)
applied between anode and cathode,
again via RSERIES;
(3) IAKS – the anode-cathode current
for either an SCR or a PUT, with
its gate tied to either the cathode
(SCR) or anode (PUT), and with any
selected operating voltage (OPV) applied between anode and cathode via
a current-limiting resistor RSERIES.
In other words, the “OFF” current of
the device;
(4) IAK – the anode-cathode current for
either an SCR or a PUT, with any selected operating voltage (OPV) applied
between anode and cathode, and its
gate connected to any of three sources
of bias current: +50µA, +200µA or
+1mA in the case of an SCR, or -50µA,
-200µA or -1mA in the case of a PUT.
February 2012 47
This view shows the partially-completed top board. It carries the LCD, the ZIF socket (not yet mounted) and most of
the relays. It’s connected to the bottom PCB via three IDC cables.
These measurements allow you to gain
a good idea of the device’s triggering
sensitivity; and
(5) VAK – the anode-cathode voltage for
either an SCR or a PUT when it has
switched ON and is conducting. In
other words, Vak is the device voltage
drop in its conducting state.
These measurements are really all
that are needed to test and roughly
characterise most PUTs and low-tomedium-power SCRs in general use.
But please note that because of current limitations, the SemTest is not
really capable of testing high-power
SCRs – except in a basic “shorted or
open” sense.
Apart from anything else, the maximum gate bias current provided by the
SemTest is only 1mA, which may not
be enough to trigger a high-power SCR.
As shown in Fig.4, the device voltage and current measurement arrangements for SCRs and PUTs are exactly
the same as for BJTs. The only real
differences are with regard to gate
switching, where RELAY15 controls
the initial SCR/PUT switching and
RELAY16 controls whether the gate
is connected to the cathode (SCR)
or anode (PUT), or to a bias current
48 Silicon Chip
source (via RELAY5 or RELAY6, with
the actual bias current level selected
via RELAY3 and RELAY4).
Triac testing
Triacs are another common form of
discrete thyristor device, more widely
encountered than SCRs. They’re used
to control mains AC in many electrical
appliances.
Because Triacs are essentially gatecontrolled AC switches, the only way
to fully characterise their behaviour
is in a tester which allows them to be
tested under AC conditions. However,
because a Triac is very much like a pair
of SCRs connected in inverse parallel,
it’s possible to use the SemTest’s SCR/
PUT tests to perform a full range of
measurements on a Triac.
For example, if you connect a Triac
to the SemTest’s SCR terminals with its
A1 electrode connected to the cathode
terminal, its A2 electrode to the anode
terminal and its gate to the gate terminal (where else?), you can do all the
SCR tests described above, ie, V(BR)AKS,
IAKS and IAK for any of the three levels
of +IBIAS and even VAK(ON). So you can
give it a fairly thorough “DC workout”
in its main operating “quadrant”.
If you then leave it connected in
exactly the same way but this time
check it as if it were a PUT, you can
thoroughly test it in a second quadrant. Finally, if you swap the A1 and
A2 electrode connections so that A2
goes to the cathode terminal and A1
to the anode terminal, you will be able
to test it in the other two quadrants,
ie, by testing it again as an SCR and
then as a PUT.
So for a quick and dirty test, you
just run the SCR tests on the Triac for
just one quadrant. If you want to test
in the other three quadrants, you need
to run the tests three more times, as
just described.
The only limitation to this procedure is that the maximum gate bias
current which the SemTest can provide is ±1mA, which as with SCRs
may simply not be enough to trigger
high-power Triacs.
Summary
That should give you a good idea
of the discrete semiconductor devices
that our new SemTest is capable of
testing and measuring. Next month,
we will present the full circuit details
SC
and start the construction.
siliconchip.com.au
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