Common drain

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Common drain amplifier
Common drain amplifier

A common-drain (commonly called a source follower) amplifier is one of the common configurations of FET electronic amplifier and is similar in operation to a BJT emitter follower (common collector circuit) in that the source voltage closely follows the voltage at the gate terminal.

Contents

(The parallel lines indicate components in parallel.)

Inherent voltage gain:

{V_\mathrm{out} \over V_\mathrm{in}} = {g_m (R_\mathrm{S} \| R_\mathrm{load}) \over 1 + g_m (R_\mathrm{S} \| R_\mathrm{load})}

The voltage gain is smaller than 1 (typical values are 0.7 to 0.9).

If g_m (R_\mathrm{S} \| R_\mathrm{load}) \gg 1, this approximates to:

Vout = Vin

This is called a source follower.

Input resistance:

r_\mathrm{in} = R_1 \| R_2,

As the gate current is ideally zero, the values of the resistors R1 and R2 can be made very high. Therefore the input resistance can be in the range of several hundreds of kiloohms.

Current gain:

A_\mathrm{vm} {r_\mathrm{in} \over R_\mathrm{load}}

Output resistance:

r_\mathrm{out} = R_\mathrm{S} \| {1 \over g_m}.

The output resistance will be quite low; several tens or hundreds of ohms are typical.

The variables not listed in the schematic are:

This circuit can also be DC coupled in which case wires replace the capacitors and R1 and R2 can be removed. The bias point is set by the previous circuit and this circuit provides the bias for the next. In this case the input resistance is infinite and the input impedance comes from the parasitic capacitances from gate to drain and gate to source. The source will follow the drain, but the voltage offset between the two is more current density dependent than for a common collector.

Rs can be replaced by a current source.

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