When an alternating potential V = V0 sin ω t is applied, a current \(\rm I=I_0 \sin \left(\omega t-\frac{\pi}{2}\right)\) flows in a given circuit. The electric power consumed in the given circuit per cycle, is
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2I0V0
2
√2I0V0
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\(\rm \frac{I_0V_0}{2}\)
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zero
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