In a sinusoidal alternating current (AC) circuit, the current and voltage vary as sine waves.
One key fact that you’ll need for the exam is that the mean (average) power delivered to a purely resistive load is exactly half the maximum power that can be delivered at the peak of the waveform.
\$P{\text{mean}} = \frac{1}{2}\,P{\text{max}}\$
Where
Since \$I{\text{rms}} = \dfrac{I{\text{max}}}{\sqrt{2}}\$ for a sine wave, the two expressions are equivalent.
\$P(t) = \tfrac{I_{\text{max}}^2 R}{2}\bigl(1-\cos(2\omega t)\bigr).\$
\$P{\text{mean}} = \tfrac{I{\text{max}}^2 R}{2} = \tfrac{1}{2}P_{\text{max}}.\$
Imagine a water pipe that fills and empties rhythmically.
The maximum flow rate is the peak of the wave, but because the pipe is only full half the time, the *average* flow is half the maximum.
Similarly, AC power oscillates, so the average (mean) power is half the peak power.
A 5 Ω resistor is connected to a 10 A peak sinusoidal current.
The same result can be found using RMS: \$I{\text{rms}} = 10/\sqrt{2} \approx 7.07\$ A, so \$P{\text{mean}} = I_{\text{rms}}^2 R \approx 7.07^2 \times 5 \approx 250\ \text{W}\$.
| Quantity | Formula | Example Value |
|---|---|---|
| Peak current \$I_{\text{max}}\$ | Given | 10 A |
| RMS current \$I_{\text{rms}}\$ | \$I_{\text{max}}/\sqrt{2}\$ | 7.07 A |
| Maximum power \$P_{\text{max}}\$ | \$I_{\text{max}}^2 R\$ | 500 W |
| Mean power \$P_{\text{mean}}\$ | \$I{\text{rms}}^2 R = \tfrac{1}{2}P{\text{max}}\$ | 250 W |