RLC Impedance Calculator
Calculate series RLC impedance, reactance, phase angle, and current from resistance, inductance, capacitance, frequency, and voltage.
About RLC impedance
RLC impedance examples
| Inputs | Result | Interpretation |
|---|---|---|
| 100 Ω, 100 mH, 10 µF, 50 Hz, 230 V | Z = 303.8226 Ω; I = 0.757 A | The circuit is predominantly capacitive. |
| 50 Ω, 10 mH, 100 µF, 159.1549 Hz, 100 V | Z ≈ 50 Ω; I ≈ 2 A | The circuit is at its ideal series resonance. |
| 20 Ω, 50 mH, 5 µF, 1 kHz, 12 V | Z ≈ 283.04 Ω; I ≈ 0.0424 A | Inductive reactance dominates at high frequency. |
How to calculate RLC impedance
- Enter the series resistance in ohms.
- Enter inductance in millihenries and capacitance in microfarads.
- Provide the source frequency and RMS voltage.
- Select Calculate impedance to view reactances, impedance, phase, and current.
RLC impedance FAQ
What is the difference between resistance and impedance?
Resistance dissipates energy and is the real part of impedance. Impedance also includes frequency-dependent inductive and capacitive opposition.
Why does impedance change with frequency?
Inductive reactance rises with frequency while capacitive reactance falls. Their changing difference alters both impedance magnitude and phase.
What happens at series resonance?
Inductive and capacitive reactance cancel at ideal series resonance. The remaining impedance equals resistance, so current is at its maximum for a fixed voltage.
Is the calculated current peak or RMS?
The displayed current is RMS because the input field requests RMS voltage. For a sine wave, peak current is RMS current multiplied by the square root of two.
Can this calculate a parallel RLC network?
No, this page applies the series impedance equation. Use the RLC circuit calculator and select parallel mode for ideal parallel branches.