Wikipedia:

common source

Basic N-channel JFET common source circuit (neglecting biasing details).
Basic N-channel JFET common source circuit (neglecting biasing details).
Basic N-channel JFET common source circuit with source degeneration.
Basic N-channel JFET common source circuit with source degeneration.

A common-source (often abbreviated to CS) amplifier is one of the three possible amplifier circuit configurations that use a single field effect transistor (FET) as the active device. The name derives from the fact that the FET's source terminal is connected to neither the input nor the output path and hence is 'common'.

The CS amplifier is conceptually a voltage amplifier. The input voltage modulates the amount of current flowing through the FET, changing the voltage across the output resistance according to Ohm's law. Alternatively, the CS amplifier can be treated as a transconductance amplifier, with the input voltage modulating the current going to the load. However, the FET device's output resistance is not typically high enough for a decent voltage amplifier, or low enough for a reasonable transconductance amplifier. Another major drawback is the amplifier's limited high-frequency response. Therefore, in practice the output is routed through a common drain (CD) or common gate (CG) stage, which have more favorable output and frequency characteristics. Hybrid circuit arrangements are possible; an example is the cascode, which (in its FET incarnation) is a consolidated CS-CG amplifier.

Characteristics

At low frequencies, the common source (see Figure 1) has the following small signal characteristics. (The parallel lines indicate components in parallel.)

Voltage gain:

{A_\mathrm{v}} = {v_\mathrm{out} \over v_\mathrm{in}} = -g_m R_\mathrm{D}\,

Current gain:

{A_\mathrm{i}} = \infty\,

Input resistance:

r_\mathrm{in} = \infty\,

Output resistance:

r_\mathrm{out} = R_\mathrm{D}\,

The variables not listed in the schematic are:

Bandwidth

The bandwidth of the common source amplifier tends to be low, due to high capacitance resulting from the Miller Effect. The gate-drain capacitance is effectively multiplied by the factor 1 - Av, thus increasing the total input capacitance and lowering the overall bandwidth.

The bandwidth is approximately given by the following expression:

BW=f_{H_{3dB}}=\frac {1}{2\pi R_{source} [ C_{GS} + C_{GD}(1+g_m R_D)]}

See also

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