Reactance Calculator
Calculate capacitive reactance, inductive reactance, total RLC impedance, resonance frequency and phase angle for AC circuits.
⚡ Key Insight: Capacitors oppose low frequency and pass high frequency. Inductors oppose high frequency and pass low frequency. At resonance, XL = XC, so the reactive part cancels and a series RLC circuit becomes mostly resistive.
〰️ Reactance — Frequency Dependence
Frequency increases → Reactance Ω Resonance Inductor XL = 2πfL Capacitor XC = 1/(2πfC) XC high at low f XL low at low f
Capacitance
Frequency
AC Voltage (optional)
Presets: 100µF @ 50Hz10µF @ 60Hz100nF @ 1kHz1nF @ 100kHz22pF @ 10MHz

Capacitive Reactance
Capacitor
🧠 Behavior: Lower capacitance or lower frequency gives higher Xc. Higher frequency makes a capacitor easier for AC to pass.
Frequency
converted to Hz
Capacitance
converted to farads
Current @ V
I = V / Xc
Admittance
1 / Xc
Phase
-90°
current leads voltage
Formula
1/(2πfC)
capacitive
Inductance
Frequency
AC Voltage (optional)
Presets: 10mH @ 1kHz1H @ 50Hz100µH @ 100kHz47µH @ 1MHz5mH @ 60Hz

Inductive Reactance
Inductor
🧠 Behavior: Higher inductance or higher frequency gives higher Xl. Inductors increasingly block AC as frequency rises.
Frequency
converted to Hz
Inductance
converted to henries
Current @ V
I = V / Xl
Admittance
1 / Xl
Phase
+90°
current lags voltage
Formula
2πfL
inductive
Resistance
Inductance
Capacitance
Frequency
AC Voltage (optional)
Presets:Audio filterSMPS tankRF exampleSpeaker crossover

Series RLC Impedance
XL
2πfL
XC
1/(2πfC)
Net Reactance
X = XL − XC
Phase Angle
atan(X/R)
Current @ V
I = V / |Z|
Resonance f₀
1/(2π√LC)
Inductance
Capacitance
Resistance / ESR (optional)
Presets:10mH + 100nF100µH + 100nFCrossoverRF LC tank

Resonant Frequency
XL = XC
🎯 At resonance: Inductive reactance equals capacitive reactance. In a series RLC circuit, impedance is minimum and mostly equal to resistance.
XL at f₀
same as XC
XC at f₀
same as XL
Q Factor
if R entered
Bandwidth
f₀ / Q
Angular Frequency
ω₀ = 2πf₀
Formula
1/(2π√LC)
LC resonance

📐 Reactance Formulas

Capacitor
XC = 1 / (2πfC)
I = V / XC
Phase = -90°
Current leads voltage
Inductor
XL = 2πfL
I = V / XL
Phase = +90°
Current lags voltage
Series RLC
X = XL − XC
|Z| = √(R² + X²)
θ = atan(X/R)
I = V / |Z|
Resonance
f₀ = 1/(2π√LC)
XL = XC at f₀
Q = XL / R
BW = f₀ / Q

📋 Quick Reference

🟠 Common Capacitors
100 nF @ 1 kHz1.59 kΩ
1 µF @ 1 kHz159 Ω
10 µF @ 50 Hz318 Ω
100 µF @ 50 Hz31.8 Ω
🔵 Common Inductors
10 µH @ 100 kHz6.28 Ω
100 µH @ 100 kHz62.8 Ω
10 mH @ 1 kHz62.8 Ω
1 H @ 50 Hz314 Ω
🎯 Useful Frequencies
Mains50 / 60 Hz
Audio midband1 kHz
SMPS range50–500 kHz
RF / crystalMHz

📚 Engineering Notes

Capacitors block DC but pass ACAt 0 Hz, XC becomes infinite. As frequency rises, XC falls, which is why capacitors are used for coupling, bypassing and filtering high-frequency noise.
Inductors pass DC but oppose ACAt 0 Hz, XL is nearly zero except winding resistance. As frequency rises, XL increases, so inductors are used for chokes, filters and energy storage in switching circuits.
Reactance is not resistanceReactance stores and releases energy instead of dissipating it as heat. It still limits AC current, but the voltage/current phase relationship changes.
Series vs parallel RLC mattersThis calculator uses the common series RLC impedance formula. Parallel RLC has a different impedance behavior and is often used for tuned RF circuits.

What is Reactance?

Reactance is the opposition to AC current caused by capacitors and inductors. It is measured in ohms, like resistance, but it depends strongly on frequency and causes a phase shift between voltage and current.

Capacitive Reactance vs Inductive Reactance

Capacitive reactance uses XC = 1/(2πfC), so it decreases when frequency or capacitance increases. Inductive reactance uses XL = 2πfL, so it increases when frequency or inductance increases.

❓ Frequently Asked Questions

Reactance is measured in ohms (Ω), just like resistance. The difference is that reactance depends on frequency and shifts phase, while ideal resistance does not.
A capacitor charges and discharges each AC cycle. At higher frequency, it cycles faster, so more AC current can pass for the same voltage. That makes the effective opposition, XC, lower.
An inductor resists change in current. At higher frequency, current changes faster, so the inductor produces a larger opposing voltage. That makes XL higher.
That condition is resonance. In a series RLC circuit, the inductive and capacitive reactances cancel, leaving mainly resistance. Current is highest if resistance is low.
💡 Rule of Thumb: For a quick mental check, a 1 µF capacitor has about 159 Ω reactance at 1 kHz. A 10 mH inductor has about 63 Ω reactance at 1 kHz.