The circuit's voltage is \( v = v_0 \sin(\omega t) \) and its current is \( i = i_0 \sin(\omega t + \varphi) \). The objective is to determine the average power consumed over one cycle. The instantaneous power \( p(t) \) is computed as:
\[ p(t) = v(t) \times i(t) = v_0 \sin(\omega t) \times i_0 \sin(\omega t + \varphi) \]
Applying the product-to-sum trigonometric identity, \(\sin A \sin B = \frac{1}{2}[\cos(A-B) - \cos(A+B)]\), yields:
\[ p(t) = \frac{1}{2}i_0 v_0 [\cos(\varphi) - \cos(2\omega t + \varphi)] \]
To ascertain the average power over a single cycle (with period \( T = \frac{2\pi}{\omega} \)), we average \( p(t) \):
\[ \text{Average Power} = \frac{1}{T} \int_0^T \frac{1}{2} i_0 v_0 [\cos(\varphi) - \cos(2\omega t + \varphi)] \, dt \]
The average value of the \(\cos(2\omega t + \varphi)\) term across a cycle is zero, as it completes an integer number of cycles within the period. Consequently,
\[ \text{Average Power} = \frac{1}{T} \int_0^T \frac{1}{2} i_0 v_0 \cos(\varphi) \, dt = \frac{1}{2} i_0 v_0 \cos(\varphi) \]
Therefore, the average power consumed in the circuit over a cycle is:
\( \frac{1}{2} i_0 v_0 \cos \varphi \)