To find the matching entries, we analyze the series L C R LCR L C R circuit driven by the voltage V ( t ) = 45 sin ( ω t ) V V(t) = 45 \sin(\omega t)\text{ V} V ( t ) = 45 sin ( ω t ) V .
1. Calculation of Resistance (R R R ) and Capacitance (C C C )
The given parameters are:
Voltage amplitude, V 0 = 45 V V_0 = 45\text{ V} V 0 = 45 V
Resonant angular frequency, ω 0 = 10 5 rad s − 1 \omega_0 = 10^5\text{ rad s}^{-1} ω 0 = 1 0 5 rad s − 1
Inductance, L = 50 mH = 0.05 H L = 50\text{ mH} = 0.05\text{ H} L = 50 mH = 0.05 H
At resonance:
ω 0 = 1 L C ⟹ C = 1 ω 0 2 L = 1 ( 10 5 ) 2 × 0.05 = 2 × 10 − 9 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} ω 0 = L C 1 ⟹ C = ω 0 2 L 1 = ( 1 0 5 ) 2 × 0.05 1 = 2 × 1 0 − 9 F
At source frequency ω = 8 × 10 4 rad s − 1 \omega = 8 \times 10^4\text{ rad s}^{-1} ω = 8 × 1 0 4 rad s − 1 :
Inductive reactance:
X L = ω L = ( 8 × 10 4 ) × 0.05 = 4000 Ω X_L = \omega L = (8 \times 10^4) \times 0.05 = 4000\ \Omega X L = ω L = ( 8 × 1 0 4 ) × 0.05 = 4000 Ω
Capacitive reactance:
X C = 1 ω C = 1 ( 8 × 10 4 ) × ( 2 × 10 − 9 ) = 6250 Ω X_C = \frac{1}{\omega C} = \frac{1}{(8 \times 10^4) \times (2 \times 10^{-9})} = 6250\ \Omega X C = ω C 1 = ( 8 × 1 0 4 ) × ( 2 × 1 0 − 9 ) 1 = 6250 Ω
Difference in reactance:
∣ X L − X C ∣ = ∣ 4000 − 6250 ∣ = 2250 Ω |X_L - X_C| = |4000 - 6250| = 2250\ \Omega ∣ X L − X C ∣ = ∣4000 − 6250∣ = 2250 Ω
The current amplitude at frequency ω \omega ω is given as:
I = V 0 R 2 + ( X L − X C ) 2 = 0.05 I 0 = 1 20 ( V 0 R ) 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) I = R 2 + ( X L − X C ) 2 V 0 = 0.05 I 0 = 20 1 ( R V 0 )
Equating the impedances:
R 2 + ( 2250 ) 2 = 20 R \sqrt{R^2 + (2250)^2} = 20R R 2 + ( 2250 ) 2 = 20 R
R 2 + 2250 2 = 400 R 2 ⟹ 399 R 2 = 2250 2 R^2 + 2250^2 = 400 R^2 \implies 399 R^2 = 2250^2 R 2 + 225 0 2 = 400 R 2 ⟹ 399 R 2 = 225 0 2
R = 2250 399 ≈ 2250 19.975 ≈ 112.64 Ω ≈ 112.5 Ω R = \frac{2250}{\sqrt{399}} \approx \frac{2250}{19.975} \approx 112.64\ \Omega \approx 112.5\ \Omega R = 399 2250 ≈ 19.975 2250 ≈ 112.64 Ω ≈ 112.5 Ω
2. Evaluation of List-I Items
(P) Current amplitude at resonance (I 0 I_0 I 0 ) in mA:
I 0 = V 0 R ≈ 45 112.5 A = 0.4 A = 400 mA I_0 = \frac{V_0}{R} \approx \frac{45}{112.5}\text{ A} = 0.4\text{ A} = 400\text{ mA} I 0 = R V 0 ≈ 112.5 45 A = 0.4 A = 400 mA
⟹ ( P ) → ( 3 ) \implies (P) \rightarrow (3) ⟹ ( P ) → ( 3 )
(Q) Quality factor (Q Q Q ) of the circuit:
Q = ω 0 L R = 10 5 × 0.05 112.5 = 5000 112.5 ≈ 44.44 Q = \frac{\omega_0 L}{R} = \frac{10^5 \times 0.05}{112.5} = \frac{5000}{112.5} \approx 44.44 Q = R ω 0 L = 112.5 1 0 5 × 0.05 = 112.5 5000 ≈ 44.44
⟹ ( Q ) → ( 1 ) \implies (Q) \rightarrow (1) ⟹ ( Q ) → ( 1 )
(R) Bandwidth of the circuit in rad s − 1 \text{rad s}^{-1} rad s − 1 :
Bandwidth = ω 0 Q = R L ≈ 112.5 0.05 = 2250 rad s − 1 \text{Bandwidth} = \frac{\omega_0}{Q} = \frac{R}{L} \approx \frac{112.5}{0.05} = 2250\text{ rad s}^{-1} Bandwidth = Q ω 0 = L R ≈ 0.05 112.5 = 2250 rad s − 1
⟹ ( R ) → ( 4 ) \implies (R) \rightarrow (4) ⟹ ( R ) → ( 4 )
(S) Peak power dissipated at resonance in Watt:
At resonance, the phase angle ϕ = 0 \phi = 0 ϕ = 0 , so:
P peak = V 0 I 0 = 45 × 0.4 = 18 W P_{\text{peak}} = V_0 I_0 = 45 \times 0.4 = 18\text{ W} P peak = V 0 I 0 = 45 × 0.4 = 18 W
⟹ ( S ) → ( 2 ) \implies (S) \rightarrow (2) ⟹ ( S ) → ( 2 )
Conclusion
Matching the results:
P → 3 P \rightarrow 3 P → 3
Q → 1 Q \rightarrow 1 Q → 1
R → 4 R \rightarrow 4 R → 4
S → 2 S \rightarrow 2 S → 2
This corresponds to Option B .