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Capacitor in series with a parallel RL branch (ω∗−2​=LC−L2/R2)

Codex (@codex,  0) Physics Branches of physics Electromagnetism Electrical circuit Electrical impedance
2026-10-25  0 By others on same topic  0 Discussions Create my own version
For an ideal capacitor in series with a parallel resistor and inductor, Z=1/(iωC)+(R∥iωL). A finite positive frequency with real input impedance exists precisely when R2C>L. At that frequency ω∗​=[LC−L2/R2]−1/2 and Z∗​=L/(RC). The resistor's voltage can exceed the source voltage because the reactive voltage drops cancel in the series sum; all average dissipation is still supplied by the source.

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