A series LCR circuit has L=0.1 H, C=100μF, R=10Ω, connected to an AC source V=220sin(100πt) V. Find (a) the impedance, (b) rms current, (c) phase angle, (d) average power dissipated.
Solution — Step by Step
From V=220sin(100πt): V0=220 V, ω=100π≈314 rad/s.
XL=ωL=314×0.1=31.4Ω.
XC=1/(ωC)=1/(314×100×10−6)=1/0.0314≈31.85Ω.
Z=R2+(XL−XC)2=100+(31.4−31.85)2
(XL−XC)2=(−0.45)2≈0.2. So Z≈100.2≈10.01Ω.
The circuit is essentially at resonance.
Vrms=V0/2=220/2≈155.6 V.
Irms=Vrms/Z=155.6/10.01≈15.55 A.
tanϕ=(XL−XC)/R=−0.45/10=−0.045, so ϕ≈−2.6° (current slightly leads voltage — capacitive dominance).
Average power: P=VrmsIrmscosϕ=155.6×15.55×cos(2.6°)≈2419×0.999≈2417 W.
Final answers:Z≈10.01Ω, Irms≈15.55 A, ϕ≈−2.6°, P≈2.42 kW.
Why This Works
This circuit is almost at resonance: ω2=1/(LC) gives ω0=1/0.1×10−4=1/0.00316≈316.2 rad/s, very close to ω=314. So XL≈XC, Z≈R, and the circuit looks purely resistive.
At resonance, power dissipation is maximum: Pmax=Vrms2/R. For Vrms=155.6 and R=10: Pmax=24,212/10=2421 W — matches our answer.
Alternative Method
Since the circuit is at resonance, skip Z entirely. Irms=Vrms/R=155.6/10=15.56 A. P=VrmsIrms=2421 W. Three lines instead of ten.
Common Mistake
Students confuse V0=220 V with Vrms=220 V. The expression V=220sin(ωt) has V0=220, not Vrms=220. Always check whether you’re given peak or rms when you see "220 V" — wall outlets give 220 V rms (peak 311 V), but in problem sin-form the coefficient is the peak.
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