Compute reactance, impedance magnitude, phase angle, resonant frequency, and quality factor for RLC circuits. Essential for RF design, filters, and matching networks.
Impedance Z extends the concept of resistance to AC circuits. It is a complex number consisting of:
Z = R + jX, where \(j = \sqrt{-1}\) (electrical engineering notation).
The magnitude \(|Z| = \sqrt{R^2 + X^2}\) and phase angle \(\phi = \arctan(X/R)\). For pure inductors, \(X_L = 2\pi f L\) (positive), for capacitors \(X_C = -1/(2\pi f C)\) (negative in series, but often treated as positive magnitude with sign in formula). In series RLC, net reactance \(X = X_L - X_C\).
Reactance varies strongly with frequency:
This leads to three regimes in a series RLC circuit:
Series resonance: Impedance is minimum (\(Z_{\min} = R\)) and current is maximum. Phase crosses zero.
Parallel resonance: Impedance is maximum (\(Z_{\max} \approx Q \cdot X_L\) if \(R\) is small) and current is minimum. Phase also crosses zero but from positive to negative.
The resonant frequency is the same for both: \(f_r = \frac{1}{2\pi\sqrt{LC}}\).
Q indicates the sharpness of resonance:
Bandwidth (BW) is the range of frequencies where the power drops by half (-3 dB): \(BW = \frac{f_r}{Q}\).
A high-Q circuit is very selective (narrow bandwidth), used in oscillators and filters.
Actual inductors have winding resistance (DCR) and self-capacitance; capacitors have Equivalent Series Resistance (ESR) and Equivalent Series Inductance (ESL). These parasitics become significant at high frequencies, causing self-resonance and limiting impedance behaviour. For example, a capacitor’s impedance first decreases (capacitive), reaches a minimum at its self-resonant frequency, then increases (inductive).
Always check component datasheets for SRF (Self-Resonant Frequency) and ESR when designing precision circuits.
The maximum power theorem states that maximum power is delivered when the load impedance is the complex conjugate of the source impedance. In RF systems, matching networks (L‑networks, pi‑networks, transformers) transform impedances to 50 Ω. The goal is to cancel reactance and equal resistance.
Common matching elements: series/parallel capacitors and inductors, or transmission line stubs.
Impedance can be measured using:
Given: Series RLC with \(R = 100\,\Omega\), \(L = 0.1\,\text{H}\), \(C = 1\,\mu\text{F}\), \(f = 1000\,\text{Hz}\).
This matches the calculator's default output.
References & further reading: