MHT CET · Physics · Alternating Current
A series LCR circuit with resistance \(R=500 \mathrm{ohm}\) is connected to an a.c. source of \(250 \mathrm{~V}\). When only the capacitance is removed, the current lags behind the voltage by \(60^{\circ}\). When only the inductance is removed, the current leads the voltage by \(60^{\circ}\). The impedance of the circuit is
- A \(\frac{500}{\sqrt{3}} \Omega\)
- B \(500 \sqrt{3} \Omega\)
- C \(250 \Omega\)
- D \(500 \Omega\)
Answer & Solution
Correct Answer
(D) \(500 \Omega\)
Step-by-step Solution
Detailed explanation
When capacitance is removed
\(
\begin{aligned}
& \tan \phi=\tan 60^{\circ}=\frac{X_L}{R} \\
& \therefore \frac{X_L}{R}=\sqrt{3} \text { or } X_L=R \sqrt{3}
\end{aligned}
\)
When inductance is removed,
\(
\begin{aligned}
& \frac{X_C}{R}=\tan 60^{\circ}=\sqrt{3} \\
& \therefore X_C=R \sqrt{3} \\
& \therefore X_C=X_L
\end{aligned}
\)
Impedance, \(\mathrm{Z}=\sqrt{\mathrm{R}^2+\left(\mathrm{X}_{\mathrm{L}}=\mathrm{X}_{\mathrm{C}}\right)^2}=\mathrm{R}=500 \Omega\)
\(
\begin{aligned}
& \tan \phi=\tan 60^{\circ}=\frac{X_L}{R} \\
& \therefore \frac{X_L}{R}=\sqrt{3} \text { or } X_L=R \sqrt{3}
\end{aligned}
\)
When inductance is removed,
\(
\begin{aligned}
& \frac{X_C}{R}=\tan 60^{\circ}=\sqrt{3} \\
& \therefore X_C=R \sqrt{3} \\
& \therefore X_C=X_L
\end{aligned}
\)
Impedance, \(\mathrm{Z}=\sqrt{\mathrm{R}^2+\left(\mathrm{X}_{\mathrm{L}}=\mathrm{X}_{\mathrm{C}}\right)^2}=\mathrm{R}=500 \Omega\)
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