This problem concerns the calculation of average power dissipated in an AC circuit over a full cycle. In an AC circuit, voltage and current are defined as follows:
Voltage: \( v = v_0 \sin \omega t \)
Current: \( i = i_0 \sin (\omega t + \phi) \)
The average power \( P \) is determined by the integral:
\( P = \frac{1}{T} \int_0^T v \cdot i \, dt \)
Where \( T \) represents the waveform's period. Substituting the voltage and current expressions yields:
\( P = \frac{1}{T} \int_0^T v_0 \sin \omega t \cdot i_0 \sin (\omega t + \phi) \, dt \)
\( = \frac{v_0 i_0}{T} \int_0^T \sin \omega t \cdot \sin (\omega t + \phi) \, dt \)
Applying the trigonometric identity \( \sin A \sin B = \frac{1}{2} [\cos(A-B) - \cos(A+B)] \), we get:
\( \sin \omega t \sin (\omega t + \phi) = \frac{1}{2}[\cos(\phi) - \cos(2\omega t + \phi)] \)
Substituting this back into the power equation:
\( P = \frac{v_0 i_0}{2T} \left( \int_0^T \cos \phi \, dt - \int_0^T \cos(2\omega t + \phi) \, dt \right) \)
Given that \( \cos(\phi) \) is a constant with respect to \( t \) and the integral of a cosine function over a complete period is zero:
\( \int_0^T \cos(2\omega t + \phi) \, dt = 0 \)
\( \int_0^T \cos \phi \, dt = T \cos \phi \)
Therefore, the average power is:
\( P = \frac{v_0 i_0}{2} \cos \phi \)
Consequently, the average power consumed in the circuit over a cycle is \( \frac{i_0 v_0}{2} \cos \phi \).