NVAMediumJEE 2026LCR Circuits & Resonance

JEE Physics 2026 Question with Solution

Using a variable frequency ac voltage source the maximum current measured in the given LCR circuit is 50mA50 \, \text{mA} for V=5sin(100t)V = 5 \sin(100t) The values of LL and RR are shown in the figure. The capacitance of the capacitor (CC) used is _____ μF\mu \text{F}.

Series LCR circuit with an inductor of 2 H, a resistor of 100 ohm, a capacitor C, and an AC source V equals 5 sin 100 t.

Answer

Correct answer:50

Step-by-step solution

Standard Method

Given: Maximum current is 50mA50 \, \text{mA}, source voltage is V=5sin(100t)V = 5 \sin(100t), so the peak voltage is 5V5 \, \text{V} and angular frequency is ω=100rad/s\omega = 100 \, \text{rad/s}. From the figure, L=2HL = 2 \, \text{H} and R=100ΩR = 100 \, \Omega.

Find: The capacitance CC.

The maximum current is

Imax=50mA=0.05AI_{\max} = 50 \, \text{mA} = 0.05 \, \text{A}

For a series LCR circuit,

Imax=VpeakZI_{\max} = \frac{V_{\text{peak}}}{Z}

So the impedance is

Z=VpeakImax=50.05=100ΩZ = \frac{V_{\text{peak}}}{I_{\max}} = \frac{5}{0.05} = 100 \, \Omega

Since Z=100ΩZ = 100 \, \Omega and R=100ΩR = 100 \, \Omega, the impedance equals the resistance. Therefore the circuit is in resonance, so the reactances cancel:

XL=XCX_L = X_C

That is,

ωL=1ωC\omega L = \frac{1}{\omega C}

Hence,

C=1ω2LC = \frac{1}{\omega^2 L}

Substituting ω=100rad/s\omega = 100 \, \text{rad/s} and L=2HL = 2 \, \text{H},

C=1(100)2×2=120000  FC = \frac{1}{(100)^2 \times 2} = \frac{1}{20000} \; \text{F} C=5×105  F=50×106  FC = 5 \times 10^{-5} \; \text{F} = 50 \times 10^{-6} \; \text{F}

Therefore, the capacitance is 50μF50 \, \mu \text{F}.

Using Resonance Condition Explicitly

Given: At maximum current, the measured current is 0.05A0.05 \, \text{A} and the applied voltage is V=5sin(100t)V = 5 \sin(100t). The figure gives R=100ΩR = 100 \, \Omega and L=2HL = 2 \, \text{H}.

Find: The value of CC.

First calculate the impedance from peak values:

Z=50.05=100ΩZ = \frac{5}{0.05} = 100 \, \Omega

Now compare with the resistance from the figure:

R=100ΩR = 100 \, \Omega

Thus,

Z=RZ = R

In a series LCR circuit, this happens only at resonance, where

XLXC=0X_L - X_C = 0

So,

XL=XCX_L = X_C

Using

XL=ωL,XC=1ωCX_L = \omega L, \qquad X_C = \frac{1}{\omega C}

we get

ωL=1ωC\omega L = \frac{1}{\omega C}

Rearranging,

C=1ω2LC = \frac{1}{\omega^2 L}

Now substitute the known values:

C=1(100)2×2=120000  FC = \frac{1}{(100)^2 \times 2} = \frac{1}{20000} \; \text{F}

Convert to microfarads:

120000  F=5×105  F=50μF\frac{1}{20000} \; \text{F} = 5 \times 10^{-5} \; \text{F} = 50 \, \mu \text{F}

Therefore, the correct numerical answer is 50.

Common mistakes

  • Using the given current as an rms current instead of the maximum current is incorrect because the question explicitly states maximum current. Use peak values consistently with V=5sin(100t)V = 5 \sin(100t) and Imax=50mAI_{\max} = 50 \, \text{mA}.

  • Ignoring the figure and assuming the wrong inductance is incorrect. The image shows L=2HL = 2 \, \text{H}, not 10H10 \, \text{H}. Using the wrong value changes the capacitance completely.

  • Not recognizing the resonance condition is a conceptual error. Since Z=Vpeak/Imax=100ΩZ = V_{\text{peak}}/I_{\max} = 100 \, \Omega and this equals RR, the reactive part must be zero, so use XL=XCX_L = X_C.

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