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

LC Oscillations

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A charged capacitor connected to an inductor creates LC oscillations at omega = 1/sqrt(LC). The energy shuttles between electric (Q^22C\frac{2}{2C}) and magnetic (LI2LI^2/2) forms, with total energy constant: Q^22C\frac{2}{2C} + LI2LI^2/2 = Q0Q_0^22C\frac{2}{2C}. This is mathematically identical to a spring-mass system: L corresponds to mass m, 1/C to spring constant k, Q to displacement x, and I to velocity v. When Q = Q0Q_0 (maximum charge), I = 0. When Q = 0, I = I0I_0 = Q0sqrt(LC\frac{Q_0}{sqrt(LC}) (maximum current). The oscillation period T = 2pisqrt(LC). In practice, resistance causes damped oscillations — energy is gradually lost to heat. A driven LC circuit with small R shows resonance when the driving frequency matches the natural frequency 1/sqrt(LC). This is the principle behind radio tuning circuits.

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