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AN439 Datasheet(PDF) 4 Page - STMicroelectronics

Part # AN439
Description  The use of TRIACs is limited by their switching behavior
PDF  16 Pages
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Manufacturer  STMICROELECTRONICS [STMicroelectronics]
Direct Link  http://www.st.com
Logo STMICROELECTRONICS - STMicroelectronics

AN439 Datasheet(HTML) 4 Page - STMicroelectronics

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TRIAC turn-off description
AN439
4/16
Figure 4.
Relative variation of (dI/dt)c versus (dV/dt)c for a 4 A standard TRIAC
(typical values)
In practice, the current waveform, and thus the dI/dtOFF, is imposed by the load. Generally
we cannot change it.
So, in TRIAC applications, it is always necessary to know the dI/dtOFF of the load to choose
a TRIAC with a suitable (dI/dt)c. This is the most important parameter.
Suppose a circuit in which the dI/dtOFF reaches 2 times the specified (dI/dt)c. The standard
4 A TRIACs, characterized by the curves in Figure 4, will be not suitable even if the dV/dtOFF
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
For the European mains, i.e. VRMS = 220 V at 50 Hz, the slope will be:
Equation 2
For 110 V, 60 Hz mains, the slope will be: dV/dtOFF ≈ 0.06 V/µs.
These relatively low dV/dtOFF correspond to the left points on the curves in Figure 4. The
dI/dtOFF only depends on the load rms current and the mains frequency. For resistive loads,
as for most other loads, we will have:
Equation 3
Area of spurious firing at
commutation
Safe area
Area of spurious firing at
commutation
Safe area
)
t
·
ω
sin(
V
V
Max
Mains
·
=
s
/
V
1
.
0
10
f
·
2
2
V
dt
/
dV
6
)
Hz
(
)
V
(
RMS
)
s
/
V
(
OFF
µ
π
µ
·
·
·
-
=
≈
)
A
(
RMS
3
)
Hz
(
)
A
(
RMS
)
ms
/
A
(
OFF
I
5
.
0
10
f
2
2
I
dt
/
dI
·
·
·
·
·
-
π
=
≈



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