A resistance of $100\ \Omega$, inductor of self-inductance $\left(\dfrac{4}{\pi^2}\right)\ \text{H}$ and a capacitor of unknown capacitance are connected in series to an a.c. source of $200\ \text{V}$ and $50\ \text{Hz}$. When the current and voltage are in phase, the capacitance and power dissipated respectively are
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At resonance in LCR circuit, impedance is minimum and equals resistance.
Step 1: Condition for current and voltage in phase.
For series LCR circuit, current and voltage are in phase at resonance:
\[
X_L = X_C
\]
Step 2: Write expressions for reactances.
\[
X_L = \omega L,\quad X_C = \dfrac{1}{\omega C}
\]
Step 3: Equate reactances.
\[
\omega L = \dfrac{1}{\omega C}
\]
\[
C = \dfrac{1}{\omega^2 L}
\]
Step 4: Substitute given values.
\[
\omega = 2\pi f = 100\pi
\]
\[
L = \dfrac{4}{\pi^2}
\]
\[
C = \dfrac{1}{(100\pi)^2 \cdot \dfrac{4}{\pi^2}} = 2.5 \times 10^{-5}\ \text{F}
\]
Step 5: Calculate power dissipated.
At resonance, impedance $Z = R = 100\ \Omega$
\[
P = \dfrac{V^2}{R} = \dfrac{200^2}{100} = 400\ \text{W}
\]