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Physics
When a voltage V=V0 cos ω t is applied across a resistor of resistance R, the average power dissipated per cycle in the resistor is given by
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Q. When a voltage $V=V_{0} \cos \omega t$ is applied across a resistor of resistance $R$, the average power dissipated per cycle in the resistor is given by
Alternating Current
A
$\frac{V_{0}}{\sqrt{2} R}$
B
$\frac{V_{0}}{\sqrt{2} \omega R}$
C
$\frac{V_{0}^{2}}{2 R}$
D
$\frac{V_{0}^{2}}{2 \omega R}$
Solution:
$P=E_{ \text{rms }} I_{ \text{rms }} \cos \phi$
$\cos \phi=\frac{R}{Z}$
$\cos \phi=1$ for resistor
$V_{ \text{rms }}=\frac{V_{0}}{\sqrt{2}}$
$P=\frac{V_{0}}{\sqrt{2}}, \frac{V_{0}}{R \sqrt{2}}(1)$
$\left(\because I_{ \text{rms }}=\frac{V_{ \text{rms }}}{R}=\frac{V_{0}}{R \sqrt{2}}\right)$
$P=\frac{V_{0}^{2}}{2 R}$