JEE Challenger
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Match Parameters of Series LCR Circuit Driven by Sinusoidal Voltage

A series LCR circuit is connected to a 45sin(ωt)45 \sin(\omega t) Volt source. The resonant angular frequency of the circuit is 105 rad s110^5\text{ rad s}^{-1} and current amplitude at resonance is I0I_0. When the angular frequency of the source is ω=8×104 rad s1\omega = 8 \times 10^4\text{ rad s}^{-1}, the current amplitude in the circuit is 0.05I00.05 I_0. If L=50 mHL = 50\text{ mH}, match each entry in List-I with an appropriate value from List-II and choose the correct option.

List-IList-II(P) I0 in mA(1) 44.4(Q) The quality factor of the circuit(2) 18(R) The bandwidth of the circuit in rad s1(3) 400(S) The peak power dissipated at resonance in Watt(4) 2250(5) 500\begin{array}{ll} \textbf{List-I} & \textbf{List-II} \\ (P)\ I_0\text{ in mA} & (1)\ 44.4 \\ (Q)\ \text{The quality factor of the circuit} & (2)\ 18 \\ (R)\ \text{The bandwidth of the circuit in rad s}^{-1} & (3)\ 400 \\ (S)\ \text{The peak power dissipated at resonance in Watt} & (4)\ 2250 \\ & (5)\ 500 \end{array}

Options

A

P2,Q3,R5,S1P \rightarrow 2, Q \rightarrow 3, R \rightarrow 5, S \rightarrow 1

B

P3,Q1,R4,S2P \rightarrow 3, Q \rightarrow 1, R \rightarrow 4, S \rightarrow 2

Correct
C

P4,Q5,R3,S1P \rightarrow 4, Q \rightarrow 5, R \rightarrow 3, S \rightarrow 1

D

P4,Q2,R1,S5P \rightarrow 4, Q \rightarrow 2, R \rightarrow 1, S \rightarrow 5

Step-by-Step Solution

To find the matching entries, we analyze the series LCRLCR circuit driven by the voltage V(t)=45sin(ωt) VV(t) = 45 \sin(\omega t)\text{ V}.

1. Calculation of Resistance (RR) and Capacitance (CC)

The given parameters are:

  • Voltage amplitude, V0=45 VV_0 = 45\text{ V}
  • Resonant angular frequency, ω0=105 rad s1\omega_0 = 10^5\text{ rad s}^{-1}
  • Inductance, L=50 mH=0.05 HL = 50\text{ mH} = 0.05\text{ H}

At resonance: ω0=1LC    C=1ω02L=1(105)2×0.05=2×109 F\omega_0 = \frac{1}{\sqrt{LC}} \implies C = \frac{1}{\omega_0^2 L} = \frac{1}{(10^5)^2 \times 0.05} = 2 \times 10^{-9}\text{ F}

At source frequency ω=8×104 rad s1\omega = 8 \times 10^4\text{ rad s}^{-1}:

  • Inductive reactance: XL=ωL=(8×104)×0.05=4000 ΩX_L = \omega L = (8 \times 10^4) \times 0.05 = 4000\ \Omega
  • Capacitive reactance: XC=1ωC=1(8×104)×(2×109)=6250 ΩX_C = \frac{1}{\omega C} = \frac{1}{(8 \times 10^4) \times (2 \times 10^{-9})} = 6250\ \Omega
  • Difference in reactance: XLXC=40006250=2250 Ω|X_L - X_C| = |4000 - 6250| = 2250\ \Omega

The current amplitude at frequency ω\omega is given as: I=V0R2+(XLXC)2=0.05I0=120(V0R)I = \frac{V_0}{\sqrt{R^2 + (X_L - X_C)^2}} = 0.05 I_0 = \frac{1}{20} \left(\frac{V_0}{R}\right)

Equating the impedances: R2+(2250)2=20R\sqrt{R^2 + (2250)^2} = 20R R2+22502=400R2    399R2=22502R^2 + 2250^2 = 400 R^2 \implies 399 R^2 = 2250^2 R=2250399225019.975112.64 Ω112.5 ΩR = \frac{2250}{\sqrt{399}} \approx \frac{2250}{19.975} \approx 112.64\ \Omega \approx 112.5\ \Omega


2. Evaluation of List-I Items

(P) Current amplitude at resonance (I0I_0) in mA: I0=V0R45112.5 A=0.4 A=400 mAI_0 = \frac{V_0}{R} \approx \frac{45}{112.5}\text{ A} = 0.4\text{ A} = 400\text{ mA}     (P)(3)\implies (P) \rightarrow (3)

(Q) Quality factor (QQ) of the circuit: Q=ω0LR=105×0.05112.5=5000112.544.44Q = \frac{\omega_0 L}{R} = \frac{10^5 \times 0.05}{112.5} = \frac{5000}{112.5} \approx 44.44     (Q)(1)\implies (Q) \rightarrow (1)

(R) Bandwidth of the circuit in rad s1\text{rad s}^{-1}: Bandwidth=ω0Q=RL112.50.05=2250 rad s1\text{Bandwidth} = \frac{\omega_0}{Q} = \frac{R}{L} \approx \frac{112.5}{0.05} = 2250\text{ rad s}^{-1}     (R)(4)\implies (R) \rightarrow (4)

(S) Peak power dissipated at resonance in Watt: At resonance, the phase angle ϕ=0\phi = 0, so: Ppeak=V0I0=45×0.4=18 WP_{\text{peak}} = V_0 I_0 = 45 \times 0.4 = 18\text{ W}     (S)(2)\implies (S) \rightarrow (2)


Conclusion

Matching the results:

  • P3P \rightarrow 3
  • Q1Q \rightarrow 1
  • R4R \rightarrow 4
  • S2S \rightarrow 2

This corresponds to Option B.