13
LED Drive Circuit Considerations for Ultra High CMR
Performance
Without a detector shield, the dominant cause of optocou-
pler CMR failure is capacitive coupling from the input side
of the optocoupler, through the package, to the detector
IC as shown in Figure 19. The HCPL-3020 and HCPL-0302
improve CMR performance by using a detector IC with
an optically transparent Faraday shield, which diverts the
capacitively coupled current away from the sensitive IC
circuitry. However, this shield does not eliminate the ca-
pacitive coupling between the LED and optocoupler pins
5-8 as shown in Figure 20. This capacitive coupling causes
Figure 19. Optocoupler input to output capacitance model for
unshielded optocouplers.
Figure 20. Optocoupler Input to output capacitance model for
shielded optocouplers.
Figure 21. Equivalent circuit for gure 15 during common mode
transient.
Figure 22. Not recommended open collector drive circuit.
Figure 23. Recommended LED drive circuit for ultra-high CMR IPM
dead time and propagation delay specications.
1
3
2
4
8
6
7
5
C
LEDP
C
LEDN
1
3
2
4
8
6
7
5
C
LEDP
C
LEDN
SHIELD
C
LEDO1
C
LEDO2
Rg
1
3
V
SAT
2
4
8
6
7
5
+
V
CM
I
LEDP
C
LEDP
C
LEDN
SHIELD
* THE ARROWS INDICATE THE DIRECTION
OF CURRENT FLOW DURING –dV
CM
/dt.
+5 V
+
V
CC
= 18 V
• • •
• • •
0.1
µF
+
1
3
2
4
8
6
7
5
C
LEDP
C
LEDN
SHIELD
+5 V
Q1
I
LEDN
1
3
2
4
8
6
7
5
C
LEDP
C
LEDN
SHIELD
+5 V
perturbations in the LED current during common mode
transients and becomes the major source of CMR failures
for a shielded optocoupler. The main design objective of
a high CMR LED drive circuit becomes keeping the LED in
the proper state (on or o ) during common mode tran-
sients. For example, the recommended application circuit
(Figure 17), can achieve 10 kV/µs CMR while minimizing
component complexity.
Techniques to keep the LED in the proper state are dis-
cussed in the next two sections.
14
Dead Time and Propagation Delay Specications
The HCPL-3020 and HCPL-0302 include a Propagation
Delay Dierence (PDD) specication intended to help
designers minimize dead time” in their power inverter
designs. Dead time is the time high and low side power
transistors are o. Any overlap in Ql and Q2 conduction
will result in large currents owing through the power
devices from the high voltage to the low-voltage motor
rails. To minimize dead time in a given design, the turn
on of LED2 should be delayed (relative to the turn o of
LED1) so that under worst-case conditions, transistor Q1
has just turned o when transistor Q2 turns on, as shown
in Figure 24. The amount of delay necessary to achieve
this condition is equal to the maximum value of the propa-
gation delay dierence specication, PDD max, which is
specied to be 500 ns over the operating temperature
range of –40° to 100°C.
Delaying the LED signal by the maximum propagation
delay dierence ensures that the minimum dead time is
zero, but it does not tell a designer what the maximum
dead time will be. The maximum dead time is equivalent
to the dierence between the maximum and minimum
propagation delay dierence specication as shown in
Figure 25. The maximum dead time for the HCPL-3020 and
HCPL-0302 is 1 ms (= 0.5 µs – (–0.5 µs)) over the operating
temperature range of –40°C to 100°C.
CMR with the LED On (CMR
H
)
A high CMR LED drive circuit must keep the LED on during
common mode transients. This is achieved by overdriving
the LED current beyond the input threshold so that it is not
pulled below the threshold during a transient. A minimum
LED current of 7 mA provides adequate margin over the
maximum I
FLH
of 6 mA to achieve 10 kV/µs CMR.
CMR with the LED O (CMR
L
)
A high CMR LED drive circuit must keep the LED o (V
F
V
F(OFF)
) during common mode transients. For example,
during a -dV
CM
/dt transient in Figure 21, the current ow-
ing through C
LEDP
also ows through the R
SAT
and V
SAT
of
the logic gate. As long as the low state voltage developed
across the logic gate is less than V
F(OFF)
the LED will remain
o and no common mode failure will occur.
The open collector drive circuit, shown in Figure 22, cannot
keep the LED o during a +dV
CM
/dt transient, since all the
current owing through C
LEDN
must be supplied by the
LED, and it is not recommended for applications requiring
ultra high CMR
1
performance. The alternative drive circuit,
which likes the recommended application circuit (Figure
17), does achieve ultra high CMR performance by shunting
the LED in the o state.
Note that the propagation delays used to calculate PDD and dead time are
taken at equal temperatures and test conditions since the optocouplers
under consideration are typically mounted in close proximity to each
other and are switching identical IGBTs.
15
Figure 24. Minimum LED skew for zero dead time.
Figure 25. Waveforms for dead time.
t
PHL MAX
t
PLH MIN
PDD* MAX = (t
PHL
-
t
PLH
)
MAX
= t
PHL MAX
-
t
PLH MIN
*PDD = PROPAGATION DELAY DIFFERENCE
NOTE: FOR PDD CALCULATIONS THE PROPAGATION DELAYS
ARE TAKEN AT THE SAME TEMPERATURE AND TEST CONDITIONS.
V
OUT1
I
LED2
V
OUT2
I
LED1
Q1 ON
Q2 OFF
Q1 OFF
Q2 ON
t
PLH
MIN
MAXIMUM DEAD TIME
(DUE TO OPTOCOUPLER)
= (t
PHL MAX
-
t
PHL MIN
) + (t
PLH MAX
-
t
PLH MIN
)
= (t
PHL MAX
-
t
PLH MIN
) – (t
PHL MIN
-
t
PLH MAX
)
= PDD* MAX – PDD* MIN
*PDD = PROPAGATION DELAY DIFFERENCE
NOTE: FOR DEAD TIME AND PDD CALCULATIONS ALL PROPAGATION
DELAYS ARE TAKEN AT THE SAME TEMPERATURE AND TEST CONDITIONS.
V
OUT1
I
LED2
V
OUT2
I
LED1
Q1 ON
Q2 OFF
Q1 OFF
Q2 ON
t
PHL MIN
t
PHL MAX
t
PLH MAX
PDD* MAX
(t
PHL-
t
PLH
)
MAX
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Data subject to change. Copyright © 2006 Avago Technologies Pte. All rights reserved. Obsoletes 5989-2947EN
AV01-0367EN - August 2, 2006

HCPL-3020-000E

Mfr. #:
Manufacturer:
Broadcom / Avago
Description:
Logic Output Optocouplers 0.2A IGBT Gate Drive
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
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