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Circuits, electronics and noise

Source-follower voltage gain

Midband gate-to-source voltage gain of a MOSFET source follower, where R is the total AC resistance from source to ground, with the load in parallel.

Ref
ELN-25
Rev
v1
Field
Circuits, electronics and noise
Result
Av [V/V]

A source follower (common drain) has a gate-to-source gain of gm R/(1 + gm R), where R is the total AC resistance from source to ground including the load in parallel. The gain is always less than one, and approaches 1 as gm R becomes large. The output resistance is about 1/gm, so the stage buffers a high-impedance signal to drive a low impedance.

Midband gate-to-source voltage gain of a MOSFET source follower, where R is the total AC resistance from source to ground, with the load in parallel. It is always below 1.

Calculator

Solve for
V/V
S
1e-40.1
Ω
100100,000
  • Loop gain, gm R4
  • Output resistance, about 1/gm250 Ω
  • Gain loss, 1 − Av0.2

What drives the result

Each variable is moved across its typical range while the others stay at the values above. The longest bar is the key driver.

Voltage gain (V/V) current value 0.8 V/V
gmTransconductanceKey driver
0.09090.99
RSource resistance in parallel with the load
0.2860.998
  • With gm R = 4 the follower passes 80 % of the input voltage to the output, losing 20 %.
  • Its output resistance of about 250 Ω is why it can drive loads that would overwhelm a high-impedance source.
Chart data as tables

Ranked variables

VariableTypical rangeLowest resultHighest resultSwing (V/V)Local stepChange in result
gm Transconductance1e-4 to 0.1 S0.090910.99010.8992+10%+1.85 %
R Source resistance in parallel with the load100 to 100,000 Ω0.28570.99750.7118+10%+1.85 %

Sweep of Source resistance in parallel with the load

Source resistance in parallel with the load (Ω)Voltage gain (V/V)
1000.2857
237.10.4868
562.30.6922
1,3340.8421
3,1620.9267
7,4990.9677
17,7800.9861
42,1700.9941
100,0000.9975

Sweep one variable

Voltage gain (V/V)Hover, touch, or use the arrow keys on the chart
0.40.60.81 100500200010k50k Source resistance in parallel with the load (Ω), log scale now 0.8

Variables and how each one contributes

Av

Voltage gain

Result · V/V

What the equation gives you. Everything else feeds it.

gm

Transconductance

S · typical 1e-4 to 0.1

The transconductance, in S. A larger gm brings the gain closer to 1. Raising it by 10 % (to 0.0044) moves the result by +1.85 %, from 0.8 to 0.8148 V/V.

R

Source resistance in parallel with the load

Ω · typical 100 to 100,000

The total resistance from source to ground (the load in parallel with the source resistor), in Ω. A larger R brings the gain closer to 1. Raising it by 10 % (to 1,100) moves the result by +1.85 %, from 0.8 to 0.8148 V/V.

Worked example with the values above

  1. Loop gain: gm R = 0.004 × 1,000 = 4.
  2. Denominator: 1 + gm R = 5.
  3. Av = 4 / 5 = 0.8.

Assumptions and limits

  • A long-channel NMOS device in strong inversion and the square-law model.
  • Triode and saturation formulas used only in their stated regions, and body effect ignored.

Common mistakes

  • Using the triode formula when Vds is above Vgs − Vth, or the saturation formula when it is below.
  • Forgetting that k here has no factor of one half in the triode formula.
  • Applying the saturation gm formula to a device in weak inversion or velocity saturation.

Statistics and uncertainty

Real transistors depart from the square-law model, especially at short channel lengths, where velocity saturation changes the current dependence. The threshold voltage varies from part to part, so results with small overdrive are very sensitive to it.

Where it is used

  • Bias and gain estimates for MOSFET amplifiers, switches and current sources.
  • Quick checks of simulation results by hand.

Maths you need

  • MOSFET regions: cut-off, triode and saturation
  • Overdrive voltage: Vov = Vgs − Vth
  • Small-signal model: gm and ro at a bias point

Related formulas

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