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Impedance and Reactance

Impedance Z = R + jX extends Ohm's law to AC; inductors and capacitors have frequency-dependent reactance.

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Z=R+jXV=IZZ = R + jX \qquad V = IZ

ElementImpedancePhase
ResistorRRV and I in phase
InductorjXL=jωLjX_L = j\omega Lcurrent lags by 90°
Capacitor−jXC=1jωC-jX_C = \dfrac{1}{j\omega C}current leads by 90°

Memory aid: ELI the ICE man — in an inductor (L), voltage E leads current I; in a capacitor (C), current I leads voltage E.

∣Z∣=R2+X2|Z| = \sqrt{R^2 + X^2} and θ=tan⁡−1(X/R)\theta = \tan^{-1}(X/R). Admittance is Y=1/Z=G+jBY = 1/Z = G + jB.

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