Question:

In an $L - R$ circuit, the inductive reactance is equal to $\sqrt{3}$ times the resistance '$R$' of the circuit. An e.m.f. $\text{E} = \text{E}_0 \sin(\omega t)$ is applied to the circuit. The power consumed in the circuit is

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Power is only dissipated in the resistance $R$, never in the pure inductor $L$.
Updated On: May 12, 2026
  • $\frac{\text{E}_0^2}{4\text{R}}$
  • $\frac{E_0^2}{6R}$
  • $\frac{\text{E}_0^2}{8\text{R}}$
  • $\frac{E_0^2}{12R}$
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The Correct Option is C

Solution and Explanation


Step 1: Concept

Average power $P = V_{rms} I_{rms} \cos \phi = \frac{E_0}{\sqrt{2}} \cdot \frac{E_0}{\sqrt{2}Z} \cdot \frac{R}{Z} = \frac{E_0^2 R}{2Z^2}$.

Step 2: Meaning

Impedance $Z = \sqrt{R^2 + X_L^2}$. Given $X_L = \sqrt{3}R$.

Step 3: Analysis

$Z^2 = R^2 + (\sqrt{3}R)^2 = 4R^2$.
$P = \frac{E_0^2 R}{2(4R^2)} = \frac{E_0^2 R}{8R^2}$.

Step 4: Conclusion

The power consumed is $\frac{E_0^2}{8R}$. Final Answer: (C)
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