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AN1232 数据表(PDF) 2 Page - STMicroelectronics |
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AN1232 数据表(HTML) 2 Page - STMicroelectronics |
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2 / 6 page ![]() Proposed model AN1232 2/6 1 Proposed model Figure 1. Npn Bipolar parasitic transistor Under impedance mismatch conditions the RF power transistor is subjected to a reflected wave with an amplitude that cannot be controlled and, in the worse case, with a voltage value that can exceed the BVdss of the device itself. Hence, the DMOS works as a voltage clamp for this wave. Under such conditions the device is subjected to an electric current whose amplitude is proportional to the power of the incident wave. Simultaneously, the DMOS experiences a temperature rise proportional to the duration, voltage swing (BVdss) and amplitude of the above current. In the DMOS cross section, shown in Figure 1, the presence of an npn bipolar parasitic transistor, in which the base and emitter are shorted by means of the DMOS source metallization, are clearly noticeable. Under static conditions the parasitic transistor is inhibited by the short circuit, but under dynamic conditions, when the reverse breakdown current flows through the device, the short circuit condition itself is modified. In fact, this current crosses the base-emitter junction through the base resistance which is increased by the depletion layer due to the reverse voltage. This results in a variation in Vbe. We can assume that: Equation 1 If Idis (base distributed current) and Rbe (base distributed resistance) are large enough, the potential on the emitter side opposed to the short circuit is sufficient to turn on the bipolar transistor, thus concentrating the current and destroying the device. A simplified model was developed (see Figure 2) to simulate the mismatch condition on the drain of the DMOS by means of the inductance L. V be R be I dis • = |
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