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AN1889 Datasheet(PDF) 16 Page - STMicroelectronics

Part # AN1889
Description  The need to choose a high value of the fly-back voltage
PDF  33 Pages
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Manufacturer  STMICROELECTRONICS [STMicroelectronics]
Direct Link  http://www.st.com
Logo STMICROELECTRONICS - STMicroelectronics

AN1889 Datasheet(HTML) 16 Page - STMicroelectronics

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ESBT driving circuit
AN1889
16/33
5
ESBT driving circuit
As already mentioned in the Chapter 1: ESBT: theory and evolution, a simple constant
voltage is enough to supply the base of the ESBT, nevertheless it could not be sufficient to
properly drive the device when very high voltage level and/or high switching frequencies are
handled. First problem is related to the dynamic saturation phenomenon always present in
all "bipolar devices" during turn-on operations. This phenomenon is related to the delay of
the voltage drop between Collector and Emitter to reach the static value (VCESAT in any
bipolar datasheet). It is evident that the higher is the working frequency, the worse this effect
will be. A common used method to moderate this effect consists in heavily injecting the base
with minority carriers in the fastest possible way, practically by providing a very high current
peak at turn-on. The consequent high base current acts in contrast with the need not to over
saturate the device since this will badly impact the turn-off loss: as a result, in fact, the
benefits got at the turn-on could become a weakness for the turn OFF performance. A
particular modulation of the base current that allow the optimization of both switching
phases can be achieved with the circuit in the figure below.
Figure 6.
ESBT driving circuit and relevant waveforms
With reference to Figure 6 VB is kept constant thanks to the electrolytic capacitor CB', while
VB can be chosen according to the device characteristic and the peculiarity of the topology
in use. By using a relatively low (non electrolytic) CB value, VB will be higher than VB' during
the first part of the turn-on, accomplishing the current spike need. From this value, both the
maximum current value and duration of the initial spike can be adjusted: the lower is the
capacitor value, the shorter will be the spike duration and the higher will be the voltage VB
limited only by the zener voltage.
A small RB is enough to control the base current both at Turn ON and Conduction.
The zener diode allows a tight base current control, by setting the exact difference between
VB and VB, finally linked with the base current spike. The relevant waveforms in fly-back
operation are those reported in Figure 6. The proposed circuit allow us to achieve an
optimization of base current behavior in the first zone described without jeopardizing the
turn-off behavior: the big pulse of base current during the first instants of turn-on (achieved
thanks to the proper choice of the capacitor CB) strongly acts in reducing the effect of
E
ES
SB
BT
T
R
RBB
R
RCC
V
VBB
V
VBB’’
D
DZZ
C
CBB’’
C
CBB
V
VCCCC
Fig. 6a
Fig. 6b
IB
IB
IB
IC
VCE



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