In a series LR circuit, the inductive reactance is equal to the resistance R of the circuit. An emf $E = E_0\cos wt$ is applied to the circuit. The average power dissipated in one cycle in the circuit is: |
$\frac{{E_0}^2}{R}$ $\frac{{E_0}^2}{4R}$ $\frac{{E_0}^2}{2R}$ $\frac{{E_0}^2}{8R}$ |
$\frac{{E_0}^2}{4R}$ |
The correct answer is Option (2) → $\frac{{E_0}^2}{4R}$ Given: In a series $LR$ circuit, $X_L = R$. Applied emf: $E = E_0 \cos \omega t$ Impedance: $Z = \sqrt{R^2 + X_L^2} = \sqrt{R^2 + R^2} = \sqrt{2}R$ RMS voltage: $V_{rms} = \frac{E_0}{\sqrt{2}}$ RMS current: $I_{rms} = \frac{V_{rms}}{Z} = \frac{E_0/\sqrt{2}}{\sqrt{2}R} = \frac{E_0}{2R}$ Average power dissipated: $P = I_{rms}^2 R = \left(\frac{E_0}{2R}\right)^2 R = \frac{E_0^2}{4R}$ Final Answer: $\;\; P = \frac{E_0^2}{4R}$ |