Snubberless™ and logic level TRIAC behavior at turn-off
Introduction
The use of TRIACs is limited by their switching behavior. Indeed, there is a risk of spurious
triggering after conduction if the slope of the decreasing current is too high, and/or if the
slope of the reapplied voltage is too high. The designer must then take some precautions:
device over-rating, switching aid network (snubber), and junction temperature margin, and
so on. This generally involves additional costs.
After a brief discussion of commutation when a TRIAC is turned off, this article will describe
the behavior of the logic level and Snubberless TRIACs, which present high commutation
capabilities.
The TRIAC can be compared to two thyristors mounted in back-to-back and coupled with a
control area which allows the triggering of this Alternating Current Switch with only one gate
(see Figure 1).
Looking at the TRIAC silicon structure (see Figure 2), it can be noted that the conduction
areas, corresponding to these two thyristors, narrowly overlap each other on the control
area.
Figure 1.Simplified equivalent
schematic of TRIAC circuit
Figure 2.Example of TRIAC silicon
structure
A2
G
I
+
V
T
Gates
Ctrl
.
I
-
A1
A1G
N1
P1
N2
P2
I
+
Gates
Ctrl
N4
A2
I
-
P1
N2
P2
N3
During the conduction time, a certain quantity of charge is injected into the structure. The
biggest part of this charge disappears by recombination during the current decrease, while
another part is extracted after the turn-off by the reverse recovery current. Nonetheless, an
excess charge remains, particularly in the neighboring regions of the gate, which can induce
the triggering of the other conduction area when the mains voltage is reapplied across the
TRIAC. This is the problem of commutation.
For a given structure at a determined junction temperature, the turn-off behavior depends
on:
1.The quantity of charge which remains when the current drops to zero. The
quantity of the charge is linked to the value of the current which was circulating in the
TRIAC approximately 100 µs, about two or three times the minority carriers’ life time,
before the turn-off. Thus, the parameter to consider is the slope of the decreasing
current, called the turn-off dI/dt or dI/dt
. (see Figure 3)
OFF
2. The slope of the reapplied voltage during turn-off. This parameter is the
commutation dV/dt, called the turn-off dV/dt or dV/dt
current, proportional to the dV/dt
, flows into the structure, and therefore charges are
OFF
(see Figure 3). A capacitive
OFF
injected and added to those coming from the previous conduction.
2/16
AN439TRIAC turn-off description
Figure 3.dI/dt and dV/dt at turn-off
I
T
V
T
V
Mains
OUT
I
dI/dt
OFF
t
V
T
T
I
G
G
dV/dt
OFF
I
G
t
t
1.2 (dI/dt)c versus (dV/dt)c characterization
To characterize the turn-off TRIAC behavior, we consider a circuit in which the slope of the
decreasing current can be adjusted. In addition, the slope of the reapplied voltage can be
controlled by using, a circuit of resistors and capacitors connected across the TRIAC. For a
determined dV/dt
which induces the spontaneous triggering of the TRIAC. This is the critical dI/dt
the (dI/dt)c in TRIAC datasheets. This is also the way to trace the curve of the TRIAC
commutation behavior (see TRIAC datasheet curve “Relative variation of critical rate of
decrease of main current (dI/dt)c versus reapplied (dV/dt)c”).
In TRIAC datasheets, the commutation behavior is specified in different way according to
the TRIAC technologies. For standard TRIAC, a minimum (dV/dt)c is specified for a given
(dI/dt)c. For logic level TRIACs, a minimum (dI/dt)c is specified for two given (dV/dt)c (0.1
V/µs and 10 V/µs). For Snubberless TRIACs, a minimum (dI/dt)c is specified without
(dV/dt)c limitation.
Figure 4 represents the curve of the commutation behavior obtained with a standard 4 A
TRIAC. This TRIAC is available with different sensitivities:
●Z0402: I
●Z0405: I
●Z0409: I
●Z0410: I
GT
GT
GT
GT
For lower sensitive gate TRIACs (Z0409 and Z0410), the (dI/dt)c is slightly modified
according to the (dV/dt)c. For sensitive gate TRIACs (Z0402 and Z0405), this parameter
noticeably decreases when the slope of the reapplied voltage increases.
((dV/dt)c), we progressively increase the dI/dt
OFF
= 3 mA;
= 5 mA;
= 10 mA;
= 25 mA.
COM
until a certain level
OFF
OFF
, called
3/16
TRIAC turn-off descriptionAN439
Figure 4.Relative variation of (dI/dt)c versus (dV/dt)c for a 4 A standard TRIAC
(typical values)
Area of spurious firing at
Area of spurious firing at
commutation
commutation
Safe area
Safe area
In practice, the current waveform, and thus the dI/dt
we cannot change it.
So, in TRIAC applications, it is always necessary to know the dI/dt
a TRIAC with a suitable (dI/dt)c. This is the most important parameter.
Suppose a circuit in which the dI/dt
OFF
4 A TRIACs, characterized by the curves in Figure 4, will be not suitable even if the dV/dt
is equal to 0.1 V/µs.
1.3 Application requirements
1.3.1 TRIAC with resistive load
In this case, the TRIAC current and the mains voltage are in phase (see Figure 5). When the
TRIAC switches off (i.e. when the current drops to zero), the mains voltage is equal to zero
at this instant and will increase across the TRIAC according to the sinusoidal law:
Equation 1
)t·
ω
sin(VV
·=
MaxMains
For the European mains, i.e. V
Equation 2
=
= 220 V at 50 Hz, the slope will be:
RMS
, is imposed by the load. Generally
OFF
of the load to choose
OFF
reaches 2 times the specified (dI/dt)c. The standard
OFF
6
-
≈
)Hz()V(RMS)s/V(OFF
s/V1.010f·22Vdt/dV
µπµ···
For 110 V, 60 Hz mains, the slope will be: dV/dt
These relatively low dV/dt
dI/dt
only depends on the load rms current and the mains frequency. For resistive loads,
OFF
correspond to the left points on the curves in Figure 4. The
OFF
as for most other loads, we will have:
Equation 3
π=
4/16
≈ 0.06 V/µs.
OFF
-
3
≈
I5.010f22Idt/dI·····
)Hz()A(RMS)ms/A(OFF
)A(RMS
AN439TRIAC turn-off description
Figure 5.Current and voltage waveforms for resistive loads (phase control)
I
I
G
G
t
t
I
I
T
T
dI/dt
dI/dt
OFF
OFF
V
V
Mains
V
V
T
T
Mains
dV/dt
dV/dt
OFF
OFF
t
t
t
t
1.3.2 TRIAC with inductive load
An inductive load induces a phase lag between the TRIAC current and the mains voltage
(see Figure 6).
When the current drops to zero, the TRIAC turns off and the voltage is abruptly applied
across its terminals. To limit the speed of the reapplied voltage, a resistive / capacitive
network mounted in parallel with the TRIAC is generally used (see Figure 13). This
“snubber” is calculated to limit the dV/dt
the (dI/dt)c specified in the datasheet. The dI/dt
at a value for which the dI/dt
OFF
is also determined in this case by the
OFF
is lower than
OFF
load impedance (Z) and the mains rms voltage. (see. AN437 for RC snubber circuit design)
Figure 6.Current and voltage waveforms for inductive loads (phase control)
I
I
G
G
t
t
I
I
T
T
dI/dt
dI/dt
OFF
OFF
V
V
Mains
Mains
V
V
T
T
dV/dt
dV/dt
OFF
OFF
t
t
t
t
5/16
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