Part of JMAG-03 — Alternating Current: LCR, Resonance & Transformers

Reactance and the Impedance Triangle

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Inductive reactance XLX_L = omega*L increases linearly with frequency — an inductor passes DC freely but increasingly opposes higher frequencies. Capacitive reactance XCX_C = 1omegaC\frac{1}{omega*C} decreases with frequency — a capacitor blocks DC but freely passes high frequencies. Both have units of ohms but dissipate no power. In a series LCR circuit, impedance Z = sqrt(R2R^2 + (XLX_L - XCX_C)^2). The impedance triangle has R as the base, (XLX_L - XCX_C) as the perpendicular, and Z as the hypotenuse. The phase angle phi = arctan(XLXCR\frac{(X_L - X_C}{R}) determines whether voltage leads (inductive) or current leads (capacitive). Power factor cos(phi) = RZ\frac{R}{Z}. The phasor diagram is the visual representation: VRV_R along the current direction, VLV_L perpendicular leading, VCV_C perpendicular lagging. The resultant V is the vector sum. This triangle is the single most powerful tool for solving AC circuit problems.

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Reactance and the Impedance Triangle — Summary | NoteTube