Z = √(R² + (2π·f·L)²)
With no capacitor, impedance follows from the geometric sum of resistance and inductive reactance.
With no capacitor, impedance follows from the geometric sum of resistance and inductive reactance.
Select a target and calculate.
With no capacitor, impedance follows from the geometric sum of resistance and inductive reactance.
R=10 Ω, L=50 mH and f=50 Hz give XL≈15.71 Ω and Z≈18.62 Ω.
Linear ideal components in sinusoidal steady state with no capacitance in the branch; skin effect, core loss and saturation are excluded.
This calculator determines the impedance of a series resistor-inductor circuit with no capacitor, the most common practical case of a choke or motor winding on an AC supply.
For a series R-L circuit, resistance and reactance add geometrically: Z=√(R²+XL²) with XL=2π·f·L.
Z = √(R² + (2π·f·L)²)
Z = √(R² + (2π·f·L)²)XL = 2π·f·L| Symbol / input | Meaning |
|---|---|
| Impedance Z | Magnitude of the complex AC impedance of the series circuit. |
| Resistance R | Resistive part, e.g. choke or motor-winding resistance. |
| Inductance L | Effective inductance at the considered frequency without saturation. |
| Frequency f | Frequency of the sinusoidal AC supply. |
R is the resistive winding resistance, L the effective inductance and f the mains or operating frequency.
Take R from a DC measurement, L from a datasheet or bridge measurement, and use the actual operating frequency.
R=10 Ω, L=50 mH and f=50 Hz give XL≈15.71 Ω and Z≈18.62 Ω.
At low frequencies R dominates; at high frequencies XL dominates impedance.
R and Z are resistances, L an inductance and f a frequency.
Estimating inrush current of chokes and motor windings on AC supply, and a preliminary step before a full RLC calculation when no capacitor is present.
Linear ideal components in sinusoidal steady state with no capacitance in the branch; skin effect, core loss, saturation and harmonics are excluded.
Common mistake: Do not misuse the existing RLC calculator with C=0; this calculator is more direct and clear for the pure RL case.
Estimating inrush current of chokes and motor windings on AC supply, and a preliminary step before a full RLC calculation when no capacitor is present.
R is the resistive winding resistance, L the effective inductance and f the mains or operating frequency.
Linear ideal components in sinusoidal steady state with no capacitance in the branch; skin effect, core loss, saturation and harmonics are excluded.