Alternating Current: Tricky Questions Solved (4)

easy 3 min read

Question

A series LCR circuit has L=0.1 HL = 0.1 \text{ H}, C=100μFC = 100 \mu\text{F}, R=10ΩR = 10 \Omega, connected to an AC source V=220sin(100πt) VV = 220 \sin(100 \pi t) \text{ V}. Find (a) the impedance, (b) rms current, (c) phase angle, (d) average power dissipated.

Solution — Step by Step

From V=220sin(100πt)V = 220\sin(100\pi t): V0=220 VV_0 = 220 \text{ V}, ω=100π314 rad/s\omega = 100\pi \approx 314 \text{ rad/s}.

XL=ωL=314×0.1=31.4ΩX_L = \omega L = 314 \times 0.1 = 31.4 \Omega.

XC=1/(ωC)=1/(314×100×106)=1/0.031431.85ΩX_C = 1/(\omega C) = 1/(314 \times 100 \times 10^{-6}) = 1/0.0314 \approx 31.85 \Omega.

Z=R2+(XLXC)2=100+(31.431.85)2Z = \sqrt{R^2 + (X_L - X_C)^2} = \sqrt{100 + (31.4 - 31.85)^2}

(XLXC)2=(0.45)20.2(X_L - X_C)^2 = (-0.45)^2 \approx 0.2. So Z100.210.01ΩZ \approx \sqrt{100.2} \approx 10.01 \Omega.

The circuit is essentially at resonance.

Vrms=V0/2=220/2155.6 VV_{rms} = V_0/\sqrt{2} = 220/\sqrt{2} \approx 155.6 \text{ V}.

Irms=Vrms/Z=155.6/10.0115.55 AI_{rms} = V_{rms}/Z = 155.6/10.01 \approx 15.55 \text{ A}.

tanϕ=(XLXC)/R=0.45/10=0.045\tan\phi = (X_L - X_C)/R = -0.45/10 = -0.045, so ϕ2.6°\phi \approx -2.6° (current slightly leads voltage — capacitive dominance).

Average power: P=VrmsIrmscosϕ=155.6×15.55×cos(2.6°)2419×0.9992417 WP = V_{rms} I_{rms} \cos\phi = 155.6 \times 15.55 \times \cos(2.6°) \approx 2419 \times 0.999 \approx 2417 \text{ W}.

Final answers: Z10.01ΩZ \approx \mathbf{10.01 \Omega}, Irms15.55 AI_{rms} \approx \mathbf{15.55 \text{ A}}, ϕ2.6°\phi \approx \mathbf{-2.6°}, P2.42 kWP \approx \mathbf{2.42 \text{ kW}}.

Why This Works

This circuit is almost at resonance: ω2=1/(LC)\omega^2 = 1/(LC) gives ω0=1/0.1×104=1/0.00316316.2 rad/s\omega_0 = 1/\sqrt{0.1 \times 10^{-4}} = 1/0.00316 \approx 316.2 \text{ rad/s}, very close to ω=314\omega = 314. So XLXCX_L \approx X_C, ZRZ \approx R, and the circuit looks purely resistive.

At resonance, power dissipation is maximum: Pmax=Vrms2/RP_{max} = V_{rms}^2/R. For Vrms=155.6V_{rms} = 155.6 and R=10R = 10: Pmax=24,212/10=2421 WP_{max} = 24,212/10 = 2421 \text{ W} — matches our answer.

Alternative Method

Since the circuit is at resonance, skip ZZ entirely. Irms=Vrms/R=155.6/10=15.56 AI_{rms} = V_{rms}/R = 155.6/10 = 15.56 \text{ A}. P=VrmsIrms=2421 WP = V_{rms} I_{rms} = 2421 \text{ W}. Three lines instead of ten.

Common Mistake

Students confuse V0=220 VV_0 = 220 \text{ V} with Vrms=220 VV_{rms} = 220 \text{ V}. The expression V=220sin(ωt)V = 220\sin(\omega t) has V0=220V_0 = 220, not Vrms=220V_{rms} = 220. Always check whether you’re given peak or rms when you see "220 V220 \text{ V}" — wall outlets give 220 V220 \text{ V} rms (peak 311 V311 \text{ V}), but in problem sin-form the coefficient is the peak.

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