Capacitive Reactance Calculator

Calculate Xc = 1/(2πfC) for AC circuits. Solve for reactance, frequency, or capacitance. Log-scale plot of reactance vs. frequency shows how caps block DC and pass AC.

Calculator Electronics Updated Apr 18, 2026
How to Use
  1. Pick what to solve for: Xc, frequency, or capacitance.
  2. Enter the other two values using suffixes (k, M for ohms; pF, nF, uF for capacitance; Hz, kHz, MHz for frequency).
  3. The log-log chart shows reactance across the audio + RF frequency range with your operating point highlighted.
  4. Remember: Xc ≠ resistance. It stores and releases energy — doesn't dissipate it.
Input
Hz (kHz, MHz OK)
F (pF, nF, uF OK)
Ω (k, M OK)
Presets
Reactance vs. Frequency
Reactance Xc
Ω
Frequency
Hz
Capacitance
Angular ω
rad/s

Show Work

Enter values to see the calculation.

Formulas

Reactance
Xc = 1 / (2π f C)
Opposition to current flow in an AC circuit.
Frequency
f = 1 / (2π Xc C)
Solve for f given Xc and C.
Capacitance
C = 1 / (2π f Xc)
Solve for C given f and Xc.
Angular Frequency
ω = 2π f
Radians per second; ω = 2πf.
Impedance
Zc = −j Xc
Complex impedance: magnitude Xc, phase −90°.
Ohm's Law (AC)
V = I × Xc
Voltage across the cap at reactance Xc.

History of Reactance

When alternating current became practical in the 1880s, engineers ran into a puzzle: a capacitor in an AC circuit drew current without dissipating heat, apparently in violation of Ohm's law. Heinrich Hertz and Oliver Heaviside, working independently in the late 1880s, showed that the current through a capacitor is 90° out of phase with the voltage — so the "resistance" felt by the source isn't ordinary resistance. Heaviside coined the term reactance around 1893 and developed the operational calculus that let engineers treat capacitors and inductors with the same algebra as resistors.

The formalism was completed by Charles Proteus Steinmetz at General Electric in 1893, when he published the use of complex numbers to represent AC impedance: Z = R + jX, where j = √−1 rotates the vector by 90°. Reactance became the imaginary component of impedance — and suddenly every AC circuit problem reduced to familiar DC-style algebra with complex arithmetic. That representation is still what every filter and power-factor-correction calculation uses today, 130 years later.

Physically, reactance is frequency-dependent opposition to AC. A capacitor dissipates zero average power because it returns stored energy to the source each cycle; only the resistive part of impedance turns electrical energy into heat. The frequency dependence — high Xc at low frequency, low Xc at high frequency — is the basis of every frequency-selective filter, every AC-coupling capacitor, and every power-supply bypass cap on your bench.

About This Calculator

Pick what to solve for (Xc, frequency, or capacitance), enter the other two with standard suffixes (nF, µF, Hz, kHz, MHz), and this calculator returns the third using Xc = 1 / (2πfC). Preset buttons jump to common working points: 60 Hz line, 1 kHz audio, 1 MHz switching.

Everything runs client-side; no values leave your browser. For real capacitors at very high frequencies, ESR (equivalent series resistance) and parasitic inductance dominate beyond the self-resonant frequency — see the datasheet for your specific part. This calculator handles the ideal case.

Frequently Asked Questions

What is capacitive reactance?

Reactance is the AC equivalent of resistance — it opposes current flow — but unlike resistance, it's frequency-dependent and doesn't dissipate energy (no heat). At DC (f=0), Xc is infinite (cap blocks DC). At infinite frequency, Xc is zero (cap looks like a short).

Why is there a 2π in the formula?

Reactance depends on angular frequency ω (radians/second), not frequency f (cycles/second). Since ω = 2πf, the formula Xc = 1/(ωC) becomes Xc = 1/(2πfC).

Is reactance the same as impedance?

No — impedance Z is the combination of resistance R and reactance X. For a pure capacitor, Z = −jXc (purely imaginary, 90° out of phase). In an RC circuit, Z = √(R² + Xc²). Impedance is what you use for total AC analysis; reactance is just the capacitive part.

What's the phase shift across a capacitor?

Current leads voltage by 90° (i.e., current peaks a quarter-cycle before voltage does). Mnemonic: ICE — In a Capacitor, I (current) comes before (leads) E (voltage).

When is this calculation important?

AC analysis: filter design (low-pass, high-pass), impedance matching, bypass cap sizing, AC coupling decisions, audio crossovers, antenna tuning. Any time you care about how a cap behaves at a specific frequency.

How does this differ from capacitor reactance in series vs. parallel circuits?

Xc depends only on f and C, not on how the cap is connected. What changes is the overall impedance calculation. Series: Z = R + jX terms add. Parallel: admittances (1/Z) add. Use a complex-number impedance calculator for anything more than a single-component analysis.

Common Use Cases

Bypass Cap Sizing

Decoupling cap near an IC needs Xc < 1Ω at the circuit's switching frequency. For 100MHz: C ≥ 1/(2π × 100MHz × 1Ω) ≈ 1.6nF.

Passive Low-Pass / High-Pass Filter

Cutoff frequency is where Xc = R. Set R and solve for C (or vice versa). Classic audio tone control.

AC Coupling

Pick a coupling cap so Xc << input impedance at the lowest frequency you want to pass. Audio amps: cap chosen so Xc < 1/10 of input Z at 20Hz.

Antenna Matching Networks

Tuned circuits use Xc cancellation against Xl to match antenna impedance. Compute Xc for the target band to size matching caps.

Power Factor Correction

Capacitor banks correct inductive loads in industrial power. Sized from kVAR reactive power and line frequency.

Power Supply Ripple Rejection

Reservoir and bypass caps have low Xc at the ripple frequency (100–120Hz for line-powered supplies, 10–100kHz for switchers).

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