Common Source Amplifier.
We’ve studied MOSFET small-signal equivalent models and the biasing of MOSFET amplifiers in the previous three lectures. We’ll now apply those skills by looking closely at three basic MOSFET amplifier types:
1. Common source amplifiers, including configurations with a source resistor (called source degeneration).
2. Common gate amplifiers.
3. Common drain (or source follower) amplifiers.
All of these amplifier types are appropriate for discrete
component designs. In the case of IC amplifiers, we’ll also show corresponding designs implemented in CMOS, beginning in Common Source Small-Signal Amplifier
This type of amplifier is shown in Fig. 4.43a, as biased by a
combination of voltage and current sources:

Assuming sufficiently large values for the coupling capacitors (CC1 and CC2) and the bypass capacitor (CS) – so that their reactances are very small at the frequency of operation – the equivalent small-signal circuit for this amplifier is shown in

The text mentions performing the small-signal analysis directly on the amplifier circuit, as illustrated in Fig. 4.43(c). We do not recommend this approach. It is better to take the time and construct the small-signal equivalent circuit, as we’re doing here. Small-Signal Amplifier Characteristics
As we did when studying BJT amplifiers, we’ll calculate the following quantities for this MOSFET common source
amplifier: Rin, Av, Gv, Gi, and Rout.
• Input resistance, Rin. From the small-signal circuit above, and noting that i_{g} =0 , then
R_{in } = R _{G}
• Partial small-signal voltage gain, Av. From the output side of the small-signal circuit
V _{0} = - G_{m}V _{gs }(r_{0}||R_{D}||R_{L})
while at the input,
V _{i}=V_{gs}
Substituting (3) into (2), we find that the partial voltage gain as

• Overall small-signal voltage gain, Gv. As we did with BJT
amplifiers, we can derive an expression for Gv in terms of Av. By definition,

Applying voltage division at the input of the small-signal
equivalent circuit,

Substituting (6) into (5) and using (4) we find

• Overall small-signal current gain, Gi. Using current division at the output in the small-signal model above

while at the input,
V_{gs}= i_{i}R_{G}
Substituting (9) into (8) we find that the overall small-signal current gain is

Notice that as R_{G} ®¥ in this last expression, i G _{i}® ¥. Is thisa problem? (To help answer this question, notice that as R_{G} ®. ¥, i_{i}® 0.) Also, what does G_{i} as R_{G} ¥ mean for the overall small-signal output power of this amplifier?
• Output resistance, Rout. To calculate the output resistance, we first set v_{sig =0 , which also means that gm vgs =0 . The input impedance of the dependent current source is infinite.
Consequently,
Rout= r0|| RD
Summary
In summary, we find for the CS small-signal amplifier that it has a
o High input resistance [see (1)].
o Relatively high small-signal voltage gain [see (7)].
o Very high small-signal current gain [see (10)].
o Relatively high output resistance [see (11)].
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