Colpitts Oscillator Calculator

Design a Colpitts LC oscillator with capacitive-divider feedback. Solves for oscillation frequency from L and the series-cap pair C1, C2.

Calculator Electronics Updated Apr 23, 2026
How to Use
  1. Enter inductor L and the two tap capacitors C1 and C2.
  2. Tool computes oscillation frequency f = 1/(2π·√(L·C_series)) and feedback ratio C1/C2.
Input
H (nH, uH, mH OK)
F (pF, nF OK)
F (pF, nF OK)
Presets
Colpitts Tank
Frequency
C_series
Feedback k
XL @ f

Show Work

Enter values.

Formulas

Oscillation f
f = 1 / (2π·√(L·C_s))
LC tank frequency.
C_s (series)
C_s = (C1·C2)/(C1+C2)
Equivalent cap.
Feedback ratio
k = C1 / (C1+C2)
0 = no feedback, 1 = full.
Loop gain
A·k > 1
Startup criterion.
XL at f
X_L = 2π·f·L
Inductor reactance.
Phase noise
∝ 1/Q
Higher tank Q = lower noise.

History

Edwin H. Colpitts, AT&T engineer, invented the capacitive-divider LC oscillator in 1918 while working on long-distance telephony and vacuum-tube amplifiers. His US patent 1,624,537 (filed 1919, granted 1927) documented the circuit that bears his name — a tuned-collector/tuned-base oscillator with capacitive feedback to the emitter.

The Colpitts topology dominated radio-receiver local oscillators from the 1920s through the 1970s because capacitor tolerances were easier to match than coil taps (Hartley) and the circuit had reliable startup across temperature. Ham-radio VFOs and early FM transmitters all used Colpitts with variable caps for tuning.

Modern integrated VCOs (PLLatino, MAX2622) inherit Colpitts topology in silicon — the LC tank is on-chip (spiral inductor + varactor diode + tap caps), with BJT or CMOS transistor for the active element. Phase noise targets of -120 dBc/Hz at 10 kHz offset are routine for modern RF synthesizers using this topology.

About This Calculator

Enter inductor L and the two divider capacitors C1 (tap to emitter/source) and C2 (tap to ground). The tool computes series-combined capacitance C_s = C1·C2/(C1+C2), oscillation frequency f = 1/(2π·√(L·C_s)), feedback ratio k = C1/(C1+C2), and inductor reactance X_L at f.

For reliable startup with BJT amplifier: target k ≈ 0.1-0.3 (i.e., C2 > C1 by factor of 3-10). Loop gain A_trans · k > 1 required; for JFET or MOSFET buffer, higher k needed. Inductor Q directly sets phase-noise floor — use silver-plated air-core coils for lowest noise. Everything runs client-side.

Frequently Asked Questions

Colpitts vs Hartley?

Colpitts: capacitive divider sets feedback ratio (C1 to emitter, C2 to ground). Hartley: inductive divider. Colpitts is easier to build with matched caps than matched coil taps, so it dominates in RF oscillator design.

Feedback ratio?

Voltage divider C1/C2 sets the feedback. For reliable startup: k = C2/(C1+C2) > 1/A (A = amp gain). Typically pick C1 < C2 by factor 5-10.

Why LC?

RC oscillators are limited by phase-noise and Q of the RC network. LC tanks with Q = 50-200 provide low phase-noise for RF synthesis; quartz extends this to Q > 10,000 in crystal oscillators.

Common Use Cases

VFO for Receiver

Ham radio VFO: variable C1 with L fixed sweeps across band.

RF Carrier

100 MHz FM transmitter local oscillator in 1970s car radios.

PLL VCO

Discrete LC VCO tuned by varactor across C1 or C2.

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