Rk
Workbench / Gain Stages

Cathode Bias & Bypass

Size Rk, its wattage and the bypass capacitor shelf.

Bias Point

Valves sharing Rk

Bypass Capacitor

to RaRg1MRk1.5 kΩCk25 µF+1.50V
Self-bias network

Resistor Wattage

00.10.20.30.40.5DISSIPATION W1.5 mW
Exact Rk
1.5 kΩ
Nearest E24
1.5 kΩ
gives Vk = 1.50 V
Use resistor ≥
0.25 W
dissipates 1.5 mW
Full-bypass corner
8.2 Hz
shelf starts 4.24 Hz
Bypass gain boost
+5.7 dB
Ck for 20 Hz
10.3 µF
rated ≥ 6.3 V
GAIN CONTRIBUTION OF BYPASSED CATHODE1101001k10k-15-10-50FREQUENCY (Hz)dBRk·Ck(Rk∥rk)·Ck
Gain relative to fully bypassed
Engineering Notes

How it works

In a cathode-biased (self-biased) stage the grid sits at 0 V through the grid-leak Rg, while the plate current flowing through Rk lifts the cathode above ground. Relative to its cathode, the grid is therefore negative by exactly Vk; the valve biases itself.

Rk = Vk / (Ik × N) P = Vk × Ik × N

N is the number of valves sharing one resistor (a push-pull pair often shares one). Choose a resistor rated at least twice the dissipation; it runs cooler and drifts less.

The bypass capacitor

Without Ck the signal current also develops a voltage across Rk, opposing the input (local negative feedback). Gain drops, distortion and output impedance improve. Fitting Ck shorts Rk at audio frequencies, but only above a shelf. The cathode looks back into the valve with an impedance of roughly:

rk_int = (Ra + rp) / (µ + 1)

so the response is a shelving filter with two corners:

f₁ = 1/(2π·Rk·Ck) f₂ = 1/(2π·(Rk ∥ rk_int)·Ck)

Guitar amps deliberately use small bypass caps (0.68–2.2 µF) to cut bass and tighten distortion, while hi-fi designs choose Ck so that f₂ sits well below 20 Hz. The capacitor's voltage rating only needs to exceed Vk with margin.