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Total Impedance |Z|
6.8513
ohms (Ohm)
Impedance |Z| (kOhm) 0.006851 kOhm
Impedance |Z| (Ohm) 6.85125 Ohm
Impedance |Z| (mOhm) 6,851.25 mOhm
Phase angle (degrees) 18.1815 deg
Phase angle (radians) 0.317327 rad
Capacitive reactance Xc 0.3183 Ohm
Inductive reactance Xl 12.5664 Ohm
Angular frequency omega 6,283.1853 rad/s

What this calculator does

This tool computes the total complex impedance of an AC network where a series-RC branch (a resistor R_C in series with a capacitor C) is connected in parallel with a series-RL branch (a resistor R_L in series with an inductor L), all driven at a sinusoidal frequency f. It reports the impedance magnitude \(|Z|\) in kOhm, Ohm and mOhm, plus the phase angle in degrees and radians.

Series RC branch in parallel with series RL branch across an AC source
A series-RC branch in parallel with a series-RL branch forms the circuit this calculator analyzes.

How to use it

Enter each component value and pick its unit from the dropdown (the factor converts to SI). Provide the drive frequency and its unit, then read the magnitude and phase. A positive phase angle means the network is net inductive (current lags the voltage); a negative angle means it is net capacitive (current leads).

The formula explained

The capacitor contributes a reactance \(X_c = \frac{1}{\omega\cdot C}\) and the inductor \(X_l = \omega\cdot L\), where \(\omega = 2\pi f\). The branches are written as complex numbers \(Z_1 = R_C - jX_c\) and \(Z_2 = R_L + jX_l\). They combine using the parallel rule $$Z = \left|\frac{Z_1 \cdot Z_2}{Z_1 + Z_2}\right|$$ Multiplying numerator and denominator by the conjugate of the denominator gives the real and imaginary parts \(Z_r\) and \(Z_i\), from which \(|Z| = \sqrt{Z_r^2 + Z_i^2}\) and \(\text{phase} = \operatorname{atan2}(Z_i, Z_r)\).

Phasor diagram showing capacitive and inductive branch impedances and resultant total impedance with phase angle
Each branch impedance is a complex number; combining them gives total impedance magnitude and phase angle θ.

Worked example

With R_C = 10 Ohm, C = 500 uF, R_L = 10 Ohm, L = 2 mH and f = 1 kHz: \(\omega = 6283.19\ \text{rad/s}\), \(X_c = 0.3183\ \text{Ohm}\) and \(X_l = 12.566\ \text{Ohm}\). Working the complex algebra gives \(Z_r = 6.5092\) and \(Z_i = 2.1378\), so $$|Z| = 6.851\ \text{Ohm} \qquad \text{phase} = +18.15^\circ$$ i.e. slightly inductive.

FAQ

What does a positive phase mean? The overall network behaves inductively, so the current lags the applied voltage.

What happens at DC (f = 0)? The capacitor blocks DC, so the RC branch is open and only the RL branch conducts. This tool treats very low or zero frequency as the open-capacitor limit.

Why three impedance units? kOhm, Ohm and mOhm are the same value at different scales so you can read whichever matches your circuit conveniently.

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