RLC Parallel Resonance Calculator

Parallel tank resonance, Q, bandwidth and dynamic impedance including inductor ESR.

What it does

A parallel “tank” circuit has its highest impedance at resonance. Including the inductor’s series resistance (ESR) shifts the resonance slightly and sets the real-world Q.

Where it's used

Oscillator tanks, IF filters and antenna matching networks.

How to use it

  1. Enter the parallel resistance (the load or loss across the tank).
  2. Enter L and C.
  3. Optional: enter the inductor’s series resistance from its datasheet.

The formula explained

f₀
resonant frequency (shifted slightly by the inductor’s r)
Q
R·√(C/L) for the parallel tank
BW
f₀ / Q
r
inductor series resistance (ESR)

Worked example

A small RF tank: 10 µH and 100 pF.

Inputs:

The calculator gives:

Tips and common mistakes

Questions people ask

Why is the Q lower than the parallel resistor alone suggests?

Two losses act together: the parallel resistance and the coil’s own series resistance. In the example each one alone would give a Q of about 158, and together they give about 79.

What is the impedance of the tank at resonance?

The coil’s loss acts like a parallel “dynamic resistance” L / (C × r) — 50 kΩ in the example. In parallel with the 50 kΩ resistor that gives 25 kΩ at resonance.

Where are parallel tank circuits used?

In LC oscillators, in intermediate-frequency filters in radios, and in antenna matching. The tank passes signals near f₀ with little loss and shorts others to ground.

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