An inductor of inductance L and resistor of resistance R are joined in series and connected by a source of frequency ω. Power dissipated in the circuit is:
A
(R2+ω2L2)V
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B
V2R(R2+ω2L2)
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C
V(R2+ω2L2)
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D
√R2+ω2L2V2
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