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Switching a Resistive Load

Before we take up inductors, it is instructive to first understand what happens when we switch a resistive load. [Pg.206]

The analysis proceeds as follows ( Vds is the drain-to-source voltage at any given moment, Vgs is the gate-to-source voltage, and Id is the drain-to-source current)  [Pg.207]

So the drop across the 1 Q resistor is 2 V (using Ohm s law). Therefore Vds equals [Pg.207]

We proceed ramping up the gate voltage progressively in this manner. When 10 s have elapsed, Vgs is 10 V, Id is 10 A, and Vds is 0 V. After 10 s, no further change in Vds or Id can occur, even if Vgs is increased further. [Pg.207]

Note In general, if the gate voltage is increased beyond what it takes to dehver a specified maximum load current, we say that in effect, we are applying overdrive. This is usually considered wasteful in that sense, but in practice, overdrive helps reduce the on-resistance of the mosfet, and thereby decrease its conduction losses. [Pg.207]


Figure 5-2 The Voltage and Current Waveforms when Switching a Resistive Load... Figure 5-2 The Voltage and Current Waveforms when Switching a Resistive Load...

See other pages where Switching a Resistive Load is mentioned: [Pg.206]    [Pg.206]   


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