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Question

An inductor of inductance L and resistor R are joined together in series and connected by a source of frequency ω. The power dissipated in the circuit is

\(\frac{V^{2}R}{R^{2}+\omega^{2}L^{2}}\)

\(\frac{V^{2}R}{\sqrt{R^{2}+\omega^{2}L^{2}}} \)

\(\frac{R^{2}+\omega^{2}L^{2}}{V} \)

\(\frac{V}{R^{2}+\omega^{2}L^{2}} \)

Solution

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