A series LCR circuit has L=0.1 H, C=100 µF, R=10 Ω, connected to an AC source of peak voltage V0=200 V at angular frequency ω=100 rad/s. Find the impedance and the rms current.
Solution — Step by Step
XL=ωL=100×0.1=10Ω
XC=ωC1=100×100×10−61=0.011=100Ω
Z=R2+(XL−XC)2=102+(10−100)2
Z=100+8100=8200≈90.55Ω
Vrms=2V0=2200≈141.4 V
Irms=ZVrms=90.55141.4≈1.56 A
Final answers: Z≈90.55 Ω, Irms≈1.56 A.
Why This Works
In a series LCR circuit, the inductor’s voltage leads the current by 90°, the capacitor’s voltage lags by 90°, and the resistor’s voltage is in phase. Adding these as phasors gives the impedance triangle: Z=R2+(XL−XC)2.
When XL>XC, the circuit is inductive; when XL<XC, capacitive. Here XC≫XL, so the circuit is strongly capacitive.
Alternative Method
Use phasor diagrams: draw VR along the current direction, VL perpendicular up, VC perpendicular down. The resultant gives the source voltage, and its magnitude divided by I gives Z.
The killer mistake: forgetting to convert capacitance from µF to F. Plugging C=100 directly gives XC=10−4 Ω — completely wrong. Always write C=100×10−6 F before computing XC.
Common Mistake
Students sometimes use peak voltage V0 to compute current: I=V0/Z. That gives the peak current I0, not Irms. Remember: Irms=Vrms/Z, where both rms quantities equal peak divided by 2.
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