LC Circuits.

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Oscillations in an LC Circuit
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LC Circuits

When the capacitor is fully charged: energy in the E field is Q2max/2C When the capacitor is discharging, the current through the solenoid generates a B field with energy: LI2/2 When the capacitor is fully discharged all the energy is in the B field, and the current is maximum. At this time the induced emf of the solenoid keeps the current going so that the capacitor is charged in the opposite direction. And this keeps going and going and …. f. Total energy of the system at any time: U = Q2/2c+LI2/2 g. Just like a spring-mass system U = kx2/2 + mv2/2

LCR Circuits

Maxwell’s Equations

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