NVAEasyJEE 2025LCR Circuits & Resonance

JEE Physics 2025 Question with Solution

An inductor of reactance 100Ω100 \, \Omega, a capacitor of reactance 50Ω50 \, \Omega, and a resistor of resistance 50Ω50 \, \Omega are connected in series with an AC source of 10V10 \, V, 50Hz50 \, Hz. Average power dissipated by the circuit is _____ W.

Answer

Correct answer:1

Step-by-step solution

Standard Method

Given: XL=100ΩX_L = 100 \, \Omega, XC=50ΩX_C = 50 \, \Omega, R=50ΩR = 50 \, \Omega, Vrms=10VV_{\text{rms}} = 10 \, V, and frequency f=50Hzf = 50 \, Hz.

Find: Average power dissipated by the circuit.

In a series LCR circuit, the total impedance is

Z=R2+(XLXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}

Substituting the given values,

Z=502+(10050)2Z = \sqrt{50^2 + (100 - 50)^2} Z=502+502=2500+2500=5000Z = \sqrt{50^2 + 50^2} = \sqrt{2500 + 2500} = \sqrt{5000} Z=502ΩZ = 50\sqrt{2} \, \Omega

The RMS current is

Irms=VrmsZI_{\text{rms}} = \frac{V_{\text{rms}}}{Z} Irms=10502=152AI_{\text{rms}} = \frac{10}{50\sqrt{2}} = \frac{1}{5\sqrt{2}} \, \text{A}

Only the resistor dissipates average power, so

P=Irms2RP = I_{\text{rms}}^2 R

Substituting,

P=(152)2×50P = \left(\frac{1}{5\sqrt{2}}\right)^2 \times 50 P=150×50=1WP = \frac{1}{50} \times 50 = 1 \, \text{W}

Therefore, the average power dissipated by the circuit is 1W1 \, \text{W}.

Step-by-Step Calculation

Given: Inductive reactance XL=100ΩX_L = 100 \, \Omega, capacitive reactance XC=50ΩX_C = 50 \, \Omega, resistance R=50ΩR = 50 \, \Omega, RMS voltage Vrms=10VV_{\text{rms}} = 10 \, V, and frequency f=50Hzf = 50 \, Hz.

Find: Average power dissipated by the circuit.

  1. First calculate the net reactance:
XLXC=10050=50ΩX_L - X_C = 100 - 50 = 50 \, \Omega
  1. Now find the impedance of the series circuit:
Z=R2+(XLXC)2Z = \sqrt{R^2 + (X_L - X_C)^2} Z=(50)2+(50)2=2500+2500=5000Z = \sqrt{(50)^2 + (50)^2} = \sqrt{2500 + 2500} = \sqrt{5000} Z=502ΩZ = 50\sqrt{2} \, \Omega
  1. Calculate the RMS current:
Irms=VrmsZ=10502=152AI_{\text{rms}} = \frac{V_{\text{rms}}}{Z} = \frac{10}{50\sqrt{2}} = \frac{1}{5\sqrt{2}} \, \text{A}
  1. Average power is dissipated only in the resistor:
Pavg=Irms2RP_{\text{avg}} = I_{\text{rms}}^2 R Pavg=(152)2×50P_{\text{avg}} = \left(\frac{1}{5\sqrt{2}}\right)^2 \times 50 Pavg=125×2×50=150×50=1WP_{\text{avg}} = \frac{1}{25 \times 2} \times 50 = \frac{1}{50} \times 50 = 1 \, \text{W}

Therefore, the required average power dissipated is 1W1 \, \text{W}.

Common mistakes

  • Using P=VIP = VI directly with total voltage and current without accounting for phase difference is incorrect, because average power in an AC LCR circuit depends on the resistive part only. Use P=Irms2RP = I_{\text{rms}}^2 R instead.

  • Adding XLX_L and XCX_C directly as 100+50100 + 50 is wrong, because inductive and capacitive reactances oppose each other. First find the net reactance as XLXCX_L - X_C.

  • Treating the given 10V10 \, V as peak voltage instead of RMS voltage leads to an incorrect current. The solution uses the supplied AC source voltage directly as VrmsV_{\text{rms}} in the impedance relation.

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