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AN1889 Datasheet(PDF) 16 Page - STMicroelectronics |
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AN1889 Datasheet(HTML) 16 Page - STMicroelectronics |
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16 / 33 page ![]() 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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