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ElectricalBasic Electrical
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Frequency for series resonance is given by

A

f0=2&╧А\pi╧А;LC

B

f0=12&╧А\pi╧А;LC

C

f0=1/2&╧А\pi╧А;тИЪLC

D

f0=1/2&╧А\pi╧А;

Correct Answer

Concept & PrincipleElectricalBasic Electrical
Option C

f0=1/2&╧А\pi╧А;тИЪLC

Quick Summary: In an RLC series circuit, resonance occurs when the inductive reactance equals the capacitive reactance, i.e., $X_L = X_C$. At this frequency, the imaginary part of the impedance becomes zero, resulting in a purely resistive circuit where the current is in phase with the applied voltage.

ЁЯТб Explanation

In an RLC series circuit, resonance occurs when the inductive reactance equals the capacitive reactance, i.e., XL=XCX_L = X_CXLтАЛ=XCтАЛ. At this frequency, the imaginary part of the impedance becomes zero, resulting in a purely resistive circuit where the current is in phase with the applied voltage.

ЁЯФв Key Formulas

XL=2╧АfLX_L = 2\pi f LXLтАЛ=2╧АfL тАФ Inductive Reactance

XC=12╧АfCX_C = \frac{1}{2\pi f C}XCтАЛ=2╧АfC1тАЛ тАФ Capacitive Reactance

f0=12╧АLCf_0 = \frac{1}{2\pi\sqrt{LC}}f0тАЛ=2╧АLCтАЛ1тАЛ тАФ Resonant Frequency

тЪЩя╕П Working Principle

The condition for series resonance is ╧ЙL=1╧ЙC\omega L = \frac{1}{\omega C}╧ЙL=╧ЙC1тАЛ, where ╧Й=2╧Аf0\omega = 2\pi f_0╧Й=2╧Аf0тАЛ. Solving for f0f_0f0тАЛ gives f0┬░2=14╧А2LCf_0┬░2 = \frac{1}{4\pi^2 LC}f0тАЛ┬░2=4╧А2LC1тАЛ, which simplifies to f0=12╧АLCf_0 = \frac{1}{2\pi\sqrt{LC}}f0тАЛ=2╧АLCтАЛ1тАЛ. At this point, the total impedance Z=R2+(XLтИТXC)2Z = \sqrt{R^2 + (X_L - X_C)^2}Z=R2+(XLтАЛтИТXCтАЛ)2тАЛ reaches its minimum value Z=RZ = RZ=R.

ЁЯУМ Key Points
  • тЦ╕

    At resonance, impedance is minimum and equal to resistance RRR.

  • тЦ╕

    Circuit current is maximum at the resonant frequency.

  • тЦ╕

    The phase angle between voltage and current is zero degrees.

  • тЦ╕

    The power factor of the circuit is unity (1.0).

тЬЕ Advantages
  • тЦ╕

    Used for voltage magnification in series circuits.

  • тЦ╕

    Essential for tuning in radio and communication receivers.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Can lead to dangerously high voltages across L and C components.

  • тЦ╕

    Highly dependent on the stability of component values over temperature.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Radio frequency tuning circuits.

  • тЦ╕

    Band-pass filter designs in signal processing.

ЁЯУД Additional Information
  • тЦ╕

    The quality factor QQQ of the series resonant circuit is defined as Q=1RLCQ = \frac{1}{R}\sqrt{\frac{L}{C}}Q=R1тАЛCLтАЛтАЛ.

  • тЦ╕

    Option A is incorrect because it is missing the frequency inverse relationship; Option B and D are algebraically incorrect.

ЁЯУК Diagram / Illustration
Series Resonance Frequency12╧АтИЪLC
тЬЕ

C is correct тАФ The resonant frequency for a series RLC circuit is derived as f0=12╧АLCf_0 = \frac{1}{2\pi\sqrt{LC}}f0тАЛ=2╧АLCтАЛ1тАЛ.

Core Concepts Used
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Inductive Reactance Capacitive Reactance Resonance Condition
ЁЯТб EXAM TIP

Always remember that at resonance, the energy stored in the magnetic field of the inductor is equal to the energy stored in the electric field of the capacitor, causing them to exchange energy back and forth.

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