Gate to cathode capacitor, impact on Triac immunity and reliability
Introduction
Triacs and SCRs are power semiconductors which are usually directly connected to the grid
line. As is well known, the AC grid voltage can be highly perturbed by important voltage
variation during very short times, for example, mechanical relay contact bounce, universal
motor disturbances. Several electromagnetic standards describe how appliances have to be
tested to check their immunity to such events. For example, the IEC 61000-4-4 standard
gives the test procedures and immunity requirements respectively for fast transient voltages.
To increase power-semiconductor device immunity, most designers add a capacitor across
the power device control terminal (the gate for SCRs or Triacs) and its reference terminal (K
or A1 respectively for SCRs and Triacs). This capacitor helps stabilize the control terminal
potential and so is believed to help increase resistance to fast voltage rises (dV/dt). As this
capacitor is also placed between the power device and the control circuit, which could be a
logic gate or a microcontroller unit (MCU), it acts as a filter on the path from the line to the
sensitive control circuit, and helps filter the noise coming from line disturbances.
This paper demonstrates why a gate to cathode capacitor is not efficient to improve Triac
immunity to fast voltage transients, especially for non-sensitive devices. This Application
note demonstrates that such capacitors can increase the risk of failure for repetitive or
accidentally high dI/dt.
The results presented in this Application note have been produced over a considerable
period of time. Some products, which are used as examples to present these results, may
no longer be available. However, the results presented apply to classes and types of
product, and thus are equally applicable to similar products available in the market.
AN4030Gate to cathode capacitor, impact on dV/dt immunity
1 Gate to cathode capacitor, impact on dV/dt immunity
1.1 dV/dt test method
To characterize device immunity, semiconductor companies give the maximum dV/dt rate
which can be applied across a device without a risk of triggering it.
The test schematic features a dV/dt generator which applies a voltage-versus-time linear
slope (see Figure 1). The test equipment detects if the voltage across the DUT (device
under test) decreases below a given threshold. For a given dV/dt level, if the device voltage
drops below this threshold, this means that the device has switched on. The DUT capability
is then lower than this dV/dt rate. The dV/dt parameter specified in the device datasheet is
then the minimum rate that all devices were able to withstand during the tests.
Figure 1.dV/dt test simplified schematic
20 Ω
dV/dt generator
(LEMSYS 50)
V
+
V
(Fixed value: usually 67% x V
dV/dt
peak
t
<V
DRM
V
DRM
T
Device
under test
I
T
Triac
or
SCR
Gate to
cathode
capacitor
The dV/dt parameter is usually measured under the following conditions:
●Peak applied voltage = 67% of V
●
Maximum junction temperature (125 °C most of the time)
●Gate open
DRM
These test conditions are the worst case, as the dV/dt immunity decreases if both the
junction temperature and the impedance between G and K increase.
The following figures give an example of a 600 V SCR dV/dt measurement. A 402 V peak
voltage is applied, as it represents 67% of the specified V
. In Figure 2, the device
DRM
remains off. There is no current increase. In Figure 3, the same device switches on
approximately 2 µs after the voltage reaches its peak and stable level. According to these
two results, it could be said that the tested SCR is able to withstand a 150 V/µs rate.
Doc ID 022635 Rev 13/15
Gate to cathode capacitor, impact on dV/dt immunityAN4030
Figure 2.c test with a 150 V/µs slope
V
T
402 V
I
T
Figure 3.600 V SCR test with a 160 V/µs slope
V
402 V
1.2 dV/dt improvement for SCR
To understand why a semiconductor can be triggered by a dV/dt slope applied across its
terminals, it should be kept in mind that semiconductor devices are composed of several
silicon layers. An SCR features four layers, alternatively doped by holes (P area) or by
electrons (N area). Each PN junction presents a spurious capacitance (see Figure 4). When
a voltage slope is applied, a spurious capacitive current (I
capacitances. This current can then flow to the cathode through the P1-N1 junction and
cause device switch-on. To solve this issue, an impedance, for example a resistor (refer to
gate to cathode resistor in Figure 4), could be added between the gate and cathode
terminals. The spurious capacitive current is then shunted and avoids the device being
triggered.
T
I
T
) is induced by these
CAP
4/15Doc ID 022635 Rev 1
AN4030Gate to cathode capacitor, impact on dV/dt immunity
Figure 4.SCR simplified silicon structure and spurious capacitive current
I
CAP
Cathode (K)
N1
P1
N2
P2
C
N1/P1
C
P1/N2
C
N2/P2
Anode (A)
R
GK
Gate (G)
A better solution could be found if a capacitor is used instead of a resistor. A high-voltage
gate to cathode capacitor is not necessary because only a low voltage (V
is around 1 V
GK
typically) is applied across this capacitor.
Figure 5 shows the typical relative dV/dt increase versus gate-cathode capacitance for an
8 A sensitive SCR series (I
max = 0.2 mA). The SCR dV/dt could be improved more than
GT
ten times with a 100 nF gate to cathode capacitor.
It should be noted that a gate to cathode resistor is still used in parallel with the gate to
cathode capacitor to discharge it after gate current removal.
For non–sensitive SCRs (I
above around 5 mA), a gate to cathode capacitor does not
GT
improve dV/dt immunity a lot. Indeed, these devices already feature a very low internal gate
to cathode resistor. So adding any external component is not very efficient to shunt the
spurious capacitive current.
Doc ID 022635 Rev 15/15
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