Two circuits are shown in the figure (a) \& (b). At a frequency of $\mathrm{rad} / \mathrm{s}$ the average power dissipated in one cycle will be same in both the circuits.


For figure (a)

$P_{\text {avg }}=\frac{v_{\mathrm{rms}}^{2}}{R}$

$\frac{\mathrm{v}_{\mathrm{rms}}^{2}}{\mathrm{Z}^{2}} \times \mathrm{R}=\frac{\mathrm{v}_{\mathrm{rms}}^{2}}{\mathrm{R}} \times 1$




$\mathrm{x}_{\mathrm{c}}=\mathrm{x}_{\mathrm{L}} \Rightarrow \frac{1}{\omega \mathrm{C}}=\omega \mathrm{L}$

$\omega^{2}=\frac{1}{\mathrm{LC}}=\frac{10^{6}}{0.1 \times 40}$


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