7.3. Body Effect and Source-Follower Voltage Transfer Relation

Suppose now, as in Fig. 7.3, that the body terminal is connected to VSS, which is signal ground. Following the definition of the body-effect transconductance, gmb, the component of Id due to source-body voltage Vsb is [from (4.1)]

Equation 7.9

Since the body is at zero potential (signal), this is

Equation 7.10

This component of current can be included in the circuit, as shown in Fig. 7.3, with an additional resistance in parallel with RS of value 1/gmb. That is, the body-effect ...

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