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ElectricalBasic Electrical
PrevNext

Impedance at series resonance is equal to

A

0

B

1

C

RRR

D

тИЮ\inftyтИЮ

Correct Answer

Concept & PrincipleElectricalBasic Electrical
Option C

RRR

Quick Summary: At series resonance in an RLC circuit, the inductive reactance ($X_L = 2\pi fL$) and capacitive reactance ($X_C = \frac{1}{2\pi fC}$) are equal in magnitude but opposite in phase. Consequently, they cancel each other out, leaving only the ohmic resistance ($R$) as the net impedance of the circuit.

ЁЯТб Explanation

At series resonance in an RLC circuit, the inductive reactance (XL=2╧АfLX_L = 2\pi fLXLтАЛ=2╧АfL) and capacitive reactance (XC=12╧АfCX_C = \frac{1}{2\pi fC}XCтАЛ=2╧АfC1тАЛ) are equal in magnitude but opposite in phase. Consequently, they cancel each other out, leaving only the ohmic resistance (RRR) as the net impedance of the circuit.

ЁЯФв Key Formulas

Z=R2+(XLтИТXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}Z=R2+(XLтАЛтИТXCтАЛ)2тАЛ тАФ General formula for impedance

Zmin=RZ_{min} = RZminтАЛ=R тАФ Impedance at series resonance

тЪЩя╕П Working Principle

The total impedance of a series RLC circuit is given by Z=R2+(XLтИТXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}Z=R2+(XLтАЛтИТXCтАЛ)2тАЛ. At resonance, the resonant frequency fr=12╧АLCf_r = \frac{1}{2\pi\sqrt{LC}}frтАЛ=2╧АLCтАЛ1тАЛ is reached such that XL=XCX_L = X_CXLтАЛ=XCтАЛ. Substituting this into the impedance formula yields Z=R2+(0)2=RZ = \sqrt{R^2 + (0)^2} = RZ=R2+(0)2тАЛ=R. This state results in minimum impedance and maximum current flow.

ЁЯУМ Key Points
  • тЦ╕

    At resonance, the phase angle of the circuit is 0┬░.

  • тЦ╕

    The circuit behaves as a purely resistive load.

  • тЦ╕

    Current is maximum at resonance: Imax=VRI_{max} = \frac{V}{R}ImaxтАЛ=RVтАЛ.

  • тЦ╕

    Voltage across inductor and capacitor are equal in magnitude but 180┬░ out of phase.

тЬЕ Advantages
  • тЦ╕

    Maximum power transfer efficiency at resonant frequency.

  • тЦ╕

    Useful for frequency selection in tuning circuits.

тЭМ Disadvantages / Limitations
  • тЦ╕

    High currents at resonance can potentially damage components.

  • тЦ╕

    Voltage magnification can occur across L and C elements.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Radio frequency tuning circuits.

  • тЦ╕

    Oscillators and filters.

  • тЦ╕

    Band-pass filter design.

ЁЯУД Additional Information
  • тЦ╕

    Option A (0) is incorrect because resistance R is never zero in a practical RLC circuit.

  • тЦ╕

    Option D (тИЮ)\infty)тИЮ)is the condition for parallel resonance impedance in an ideal LC circuit, not series resonance.

ЁЯУК Diagram / Illustration
Impedance at ResonanceZ = R + j(XтВЧ - XъЬА)At Resonance: XтВЧ = XъЬАTherefore, Z = R
тЬЕ

C is correct тАФ At series resonance, the inductive and capacitive reactances cancel out, reducing total impedance to the circuit's resistive component, R.

Core Concepts Used
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Series RLC Resonance Complex Impedance Phasor Cancellation
ЁЯТб EXAM TIP

Remember that in a series circuit, resonance minimizes impedance, while in a parallel (tank) circuit, resonance maximizes impedance.

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