8 Parallel Connections

............................. 8-2

2. Parallel connections ......................................................................................... 8-3





This chapter explains the factors that inhibit current sharing and the notes when IGBT is connected in
parallel.


When connecting IGBT modules in parallel, it is necessary to properly manage the elements
characteristics.
Otherwise, a current sharing imbalance may occur depend on the characteristics distribution between
the parallel connected modules.

Chapter 8 Parallel Connections

8-2
1

Factors that inhibit current sharing
1.1 On-state current imbalance
An on-state current imbalance may be caused by the following two factors:
(1) V
CE(sat)
distribution
(2) Main circuit wiring resistance distribution

1) Current imbalance caused by V
CE(sat)
distribution
As shown in Fig. 8-1, a difference in the
output characteristics of two IGBT
modules connected in parallel can cause
a current imbalance.
The output characteristics of Q
1
and Q
2
shown in Fig. 8-1, can be approximated
as follows:

1
1
01
1
C
CEQ
I
r
V
V
×
+
=

(
)
2
1
1
1
/
C
C
I
I
V
r =

2
2
02
2
C
CEQ
I
r
V
V
×
+
=

(
)
2
1
2
2
/
C
C
I
I
V
r =


Based on the above, if the I
Ctotal
(=I
C1
+I
C2
)
collector current is made to flow through
the circuit of Q
1
and Q
2

connected in
parallel, then the IGBTs collector current
becomes the following:

(
) (
)
2
1
2
01
02
1
/
r
r
I
r
V
V
I
Ctotal
C
+
×
+ =

(
) (
)
2
1
1
02
01
2
/
r
r
I
r
V
V
I
Ctotal
C
+
×
+ =


V
CE(sat)
becomes a major factor in
causing current imbalances. Therefore,
in order to ensure the desired current
sharing it is necessary to pair modules
that have a similar V
CE(sat)
.


2) Main circuit wiring resistance distribution
The effect exerted on current sharing by the main circuits wiring resistance can be seen in Fig. 8-2.
The effect is larger with emitter resistance than with collector resistance, so collector resistance has
been omitted here. If there is resistance in the main circuit, then the parity of the slope of the IGBT
modules output characteristics will lessen, and the collector current will drop. So, depending on how
well the collector current can flow through this resistance, an electrical potential difference may appear,
I
C1
I
C2
Q
1
Q
2
I
C
(A
)
V
CE(sat) (V)
V
02
V
01
V
1
V
2
I
C
2
I
C
1
I
C1
I
C2
Q
1
Q
2
I
C1
I
C2
Q
1
Q
2
I
C
(A
)
V
CE(sat) (V)
V
02
V
01
V
1
V
2
I
C
2
I
C
1
Fig. 8-1 Example of a V
CE(sat)
pair

I
C1
I
C2
Q
1
Q
2
R
E1
R
E2
V
E1
V
E2
I
C1
I
C2
Q
1
Q
2
R
E1
R
E2
V
E1
V
E2

Fig. 8-2 The effect of main circuit wiring resistance
Chapter 8 Parallel Connections

8-3
the actual gate-emitter voltage drop (V
GE
=V VE), the IGBTs output characteristics change and the
collector current decline. Therefore, if R
E1
>R
E2
, then the slope of the Q
1
output characteristics will
lessen and if I
C1
<I
C2
then a current sharing imbalance will appear.
In order to reduce this imbalance, it is necessary to make the wiring on the emitter side as short and
as uniform as possible.

1.2 Factors of current imbalances at turn-on and turn-off
The factors of current imbalances at turn-on and turn-off can be divided into module characteristics
distribution and main circuit wiring inductance distribution.

1) Module Characteristics distribution
An IGBTs switching current imbalance is mostly determined by an on-state current imbalance,
therefore if the on-state current imbalance is controlled simultaneously, so will the switching voltage
imbalance.

2) Main circuit wiring inductance distribution
Since the previously explained effect of resistance on current sharing is much the same as that of
inductance on current sharing, inductance can be substituted for resistance in Fig. 8-2. As the
collector current changes very suddenly during IGBT switching, a voltage is generated at both ends of
inductance. The polarity of this voltage tends to hamper switching, so the switching time will increase.
Therefore, if inductance is not controlled, then switching time will be delayed and the current will be
concentrated into one of the modules. In order to reduce this imbalance, it is necessary to make the
wiring on the emitter side as short and as uniform as possible.


2

Parallel connections
2.1 Wiring
The ideal parallel connection wiring is both uniform and short, but when seen from the point of view
of equipment mass production, it is often to implement this fully. Therefore, it is necessary to design
a layout as close to the ideal as possible. For this purpose, several basic points of caution are
illustrated below.

1) Drive circuit wiring
When connecting IGBT modules in parallel, due to the gate circuits wiring inductance and the IGBTs
input capacitance, as the gate voltage rises a parasitic oscillation may occur. Therefore, in order to
prevent this oscillation, a gate resistor should be series wired to each of the modules gates. (As
illustrated in Fig. 8-3)
As stated previously, if the drive circuits emitter wiring is connected in a different position from the
main circuit, then the modules transient current sharing (especially at turn-on) will become
imbalanced. However, IGBT modules have an auxiliary emitter terminal for use by drive circuits. By
using this terminal, the drive wiring of each module becomes uniform, and transient current
imbalances attribute to drive circuit wiring can be controlled.
Furthermore, be sure to lead the wiring out from the center of the modules parallel connection, tightly
wind it together, and lay it out so that it is as far away from the main circuit as possible in order to avoid
mutual induction.
Chapter 8 Parallel Connections

8-4
2) Main circuit wiring
As stated previously, if the resistance or the inductance of the main circuit is not uniform, then the
current sharing of the modules connected in parallel will be unbalanced.
Furthermore, if the inductance of the main circuit is large, then the surge voltage at IGBT turn-off will
also be high (for details, refer to Chapter 5, Protection Circuit Design, of this manual). Therefore,
for the purpose of reducing wiring induction and maintaining the temperature balance of each module,
consider setting the modules that are to be connected in parallel as close together as possible and
making the wiring as uniform as possible.
Also, take out the collector and emitter lead wires from the center of the parallel connection, and, in
order to avoid mutual induction, do not wire them in parallel.

Rg
Rg
Rg
Wind tightly together
IGBT module
Take out from the center
and do not wire parallel to
main terminal parallel wiring
C
E
G
E
G
E
E
G
Rg
Rg
Rg
Wind tightly together
IGBT module
Take out from the center
and do not wire parallel to
main terminal parallel wiring
C
E
G
E
G
E
E
G

Fig. 8-3 Example of parallel connection layout

2.2 Relationship of module characteristics to current sharing
As stated previously, from among a modules individual characteristics, the V
CE(sat)
distribution has a
strong effect on current sharing.
When n-number of modules are connected in parallel, the following shows the maximum current that
can be applied under the worst case conditions where the entire current is concentrated into one
module:










+



+
=
100
1
100
1
1
1
)
(
(max)
n
I
I
C

100
1
1
×



=
)
(
ave
C
C
I
I
Chapter 8 Parallel Connections

8-5
Here I
C(max)
represents the maximum current
for a single element that the modules rated
RBSOA and power dissipation loss will allow.
It is especially important to pay attention to
power dissipation loss, because this changes
depending on the operating conditions
(switching frequency, drive conditions, heat
dissipation, snubber conditions, etc.). For
details on power dissipation loss, refer to
Chapter 6, Cooling Design, of this manual.
For example, if =16%, I
C(max)
=200A and n=4,
then I=634.4A, and the parallel connected
total current should be set so as not to
exceed this value. It is important not to
make the error of simply
calculatingI=200×4=800A.
Fig. 8-4 shows the difference of VCE(sat) and
the current imbalance proportion in parallel
connections. Because the temperature
coefficient of the output characteristic is a
positive characteristic as shown in Fig. 8-5,
the current imbalance proportion becomes
small U-series IGBT compared with N-series
IGBT.


VCE(sat) [V] (at 25) [= Von2
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0
10
20
30
40
1200V IGBT
U-series
N-series -Von1]
[ ]
(
at
1
25
)
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0
10
20
30
40
1200V IGBT
U-series
N-series -Von1]
[ VCE(sat) [V] (at 25) [= Von2
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0
10
20
30
40
1200V IGBT
U-series
N-series -Von1]
[ ]
(
at
1
25
)
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0
10
20
30
40
1200V IGBT
U-series
N-series -Von1]
[
Fig. 8-4 Current imbalance proportion in parallel
connections


0
50
100
150
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
V
CE
(
sat
) (V)
U-IGBT
N-IGBT
Tj=R.T.
Tj=125
Jc
A/cm
2
)
0
50
100
150
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5
V
CE
(
sat
) (V)
U-IGBT
N-IGBT
Tj=R.T.
Tj=125
Jc
A/cm
2
)

Fig. 8-5 Comparison of V
CE(sat)
-Jc characteristics
1. This Catalog contains the product specifications, characteristics, data, materials, and structures as of February 2004.
The contents are s