Question:

A voltage \( v = v_0 \sin(\omega t) \) applied to a circuit drives a current \( i = i_0 \sin(\omega t + \phi) \) in the circuit. The average power consumed in the circuit over a cycle is:

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The average power in an AC circuit with sinusoidal voltage and current is given by \( P_{\text{avg}} = \frac{i_0 v_0}{2} \cos \phi \), where \( \phi \) is the phase difference.
  • Zero
  • \( i_0 v_0 \cos \phi \)
  • \( \frac{i_0 v_0}{2} \)
  • \( \frac{i_0 v_0}{2} \cos \phi \)
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The Correct Option is D

Solution and Explanation

To find the average power consumed in the circuit, we begin with the instantaneous power, which is the product of the voltage \( v(t) \) and the current \( i(t) \):
\[ p(t) = v(t) \cdot i(t) = (v_0 \sin(\omega t)) \cdot (i_0 \sin(\omega t + \phi)) \]
Using the trigonometric identity for the product of sines:
\[ \sin A \sin B = \frac{1}{2} [\cos(A-B) - \cos(A+B)] \]
Substitute \( A = \omega t \) and \( B = \omega t + \phi \):
\[ \sin(\omega t) \sin(\omega t + \phi) = \frac{1}{2} [\cos(-\phi) - \cos(2\omega t + \phi)] \]
\(\cos(-\phi) = \cos(\phi)\), thus:
\[ p(t) = v_0 i_0 \frac{1}{2} [\cos(\phi) - \cos(2\omega t + \phi)] \]
To find the average power over a cycle, integrate this expression over one period \( T = \frac{2\pi}{\omega} \), then divide by \( T \):
\[ P_{\text{avg}} = \frac{1}{T} \int_0^T v_0 i_0 \frac{1}{2} [\cos(\phi) - \cos(2\omega t + \phi)] \, dt \]
This separates into two integrals:
\[ P_{\text{avg}} = \frac{v_0 i_0}{2T} \left[\int_0^T \cos(\phi) \, dt - \int_0^T \cos(2\omega t + \phi) \, dt \right] \]
The first term simplifies to:
\[ \int_0^T \cos(\phi) \, dt = \cos(\phi) \cdot T \]
And for the second term, the integral of cosine over a period is zero:
\[ \int_0^T \cos(2\omega t + \phi) \, dt = 0 \]
Therefore:
\[ P_{\text{avg}} = \frac{v_0 i_0}{2T} [\cos(\phi) \cdot T] = \frac{v_0 i_0}{2} \cos(\phi) \]
Hence, the average power consumed in the circuit over a cycle is:
\[ \frac{i_0 v_0}{2} \cos \phi \]
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