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Workbench / Gain Stages

Gain Stage Response

Full frequency response of a common-cathode stage.

Valve

Circuit

B+Ra100 kΩCc22 nFRL1 MΩout12AX7inRs68 kΩRk1.5 kΩCk22 µF
Common-cathode triode stage
STAGE FREQUENCY RESPONSE1101001k10k100k-1001020304050FREQUENCY (Hz)dB−3dB 11.1 Hz−3dB 22.9 kHz
Gain (dB)
Midband gain
59.2×
35.5 dB
Low −3 dB
11.1 Hz
High −3 dB
22.9 kHz
Miller input C
104 pF
Output impedance
38.5 kΩ
Coupling corner
6.97 Hz
Ck corner 4.82 Hz
Engineering Notes

How it works

This calculator builds the complete small-signal model of a common-cathode stage and evaluates it as a complex transfer function at 260 frequencies. Three mechanisms shape the curve:

1 · Cathode bypass shelf

Below the bypass corner, Ck stops shorting Rk and local degeneration returns. The valve is modelled as a Thévenin source µ·Vg in series with rp, so the cathode impedance Zk appears multiplied by (µ+1):

Vp/Vg = −µ·Zload / (Zload + rp + (µ+1)·Zk), Zk = Rk ∥ 1/(jωCk)

2 · Coupling capacitor high-pass

Cc and the next stage's grid leak RL form a first-order high-pass filter, driven from the stage's output impedance (Ra ∥ rp):

f₋₃ ≈ 1 / (2π·Cc·(RL + Ra∥rp))

3 · Miller effect roll-off

The tiny grid–plate capacitance is multiplied by the gain of the stage. Together with the source impedance (previous stage output + grid stopper) it forms a low-pass filter. High-µ valves like the 12AX7 suffer most, which is why guitar amps use 68 kΩ grid stoppers as gentle treble taming.

Cin = Cgk + Cga·(1 + A) ; f_high ≈ 1 / (2π·Rs·Cin)

The −3 dB points are read directly from the computed curve, so interactions between the filters are fully accounted for.