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Q.Using phasor diagram, derive an expression for the impedance of a series LCR-circuit. What do you mean by the resonance condition of a series LCR-circuit? Calculate its resonant frequency. OR A series LCR circuit connected to a variable frequency 230 V source. L = 5.0 H, C = 80 μF, R = 40 Ω.

(a) Determine the source frequency which drives the circuit in resonance.
(b) Obtain the impedance of the circuit and the amplitude of current at the resonating frequency.
(c) Determine the rms potential drops across the three elements of the circuit. Show that the potential drop across the LC combination is zero at the resonating frequency.
Himachal HpboseHPBOSE Plus Two Board 2026Subjective· 5mImportance★★★★★
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Figure — Stem 'Using phasor diagram, derive an expression for the impedance of a series LCR-circuit' requires the phaso
Figure — Stem 'Using phasor diagram, derive an expression for the impedance of a series LCR-circuit' requires the phaso

Adding the phasors for VRV_R, VLV_L, VCV_C gives Z=R2+(XL−XC)2Z=\sqrt{R^2+(X_L-X_C)^2}; at resonance the reactances cancel, current is maximum, and ω0=1/LC\omega_0=1/\sqrt{LC}.

Setting up the phasor diagram: In a series LCR circuit driven by v=v0sin⁡ωtv = v_0\sin\omega t, the same current i=i0sin⁡(ωt+ϕ)i = i_0\sin(\omega t+\phi) flows through all three elements. Represent the current phasor I0I_0 along a reference axis. Then:

  • Voltage across R, VR=I0RV_R = I_0R, is IN PHASE with the current (along the same axis).
  • Voltage across L, VL=I0XLV_L = I_0X_L (where XL=ωLX_L=\omega L), LEADS the current by 90°90° (drawn perpendicular, rotated +90°+90°).
  • Voltage across C, VC=I0XCV_C = I_0X_C (where XC=1/ωCX_C=1/\omega C), LAGS the current by 90°90° (drawn perpendicular, rotated −90°-90°, i.e. opposite to VLV_L).

Since VLV_L and VCV_C are exactly opposite (180° apart) on the phasor diagram, they combine to a single net phasor of magnitude (VL−VC)(V_L - V_C), perpendicular to VRV_R.

Resultant voltage (vector sum of VRV_R and (VL−VC)(V_L-V_C), which are mutually perpendicular):

V0=VR2+(VL−VC)2=I0R2+(XL−XC)2V_0 = \sqrt{V_R^2 + (V_L-V_C)^2} = I_0\sqrt{R^2+(X_L-X_C)^2}

Defining impedance Z=V0/I0Z = V_0/I_0:

Z=R2+(XL−XC)2\boxed{Z = \sqrt{R^2+(X_L-X_C)^2}}

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