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ElectricalBasic Electrical
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In pure inductor circuit, average power is

A

0

B

1

C

тИЮ\inftyтИЮ

D

414

Correct Answer

тЪЩя╕П TE тАв Technical Concept & PrincipleElectricalBasic Electrical
Option A

0

Quick Summary:

In a pure inductive circuit, the average power dissipated over one complete cycle is zero. This occurs because the inductor stores energy in its magnetic field during one quarter of a cycle and returns that exact same energy to the source in the next quarter cycle.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

In a pure inductive circuit, the average power dissipated over one complete cycle is zero. This occurs because the inductor stores energy in its magnetic field during one quarter of a cycle and returns that exact same energy to the source in the next quarter cycle.

ЁЯФв Key Formulas

Pavg=VrmsIrmscosтБб(╧Х)P_{avg} = V_{rms} I_{rms} \cos(\phi)PavgтАЛ=VrmsтАЛIrmsтАЛcos(╧Х) тАФ General average power formula

╧Х=90┬░\phi = 90┬░╧Х=90┬░ тАФ Phase angle for a pure inductor

тЪЩя╕П Working Principle

In an AC circuit with a pure inductor, the voltage VVV leads the current III by a phase angle of 90┬░90┬░90┬░ (╧А/2{\pi/2}╧А/2 radians). The average power is calculated using the formula Pavg=VrmsIrmscosтБб(╧Х)P_{avg} = V_{rms} I_{rms} \cos(\phi)PavgтАЛ=VrmsтАЛIrmsтАЛcos(╧Х), where ╧Х\phi╧Х is the phase difference. Since ╧Х=90┬░\phi = 90┬░╧Х=90┬░, cosтБб(90┬░)=0\cos(90┬░) = 0cos(90┬░)=0, leading to zero net power consumption.

ЁЯУМ Key Points
  • тЦ╕

    A pure inductor is a lossless component.

  • тЦ╕

    Power factor (cos╧Хcos \phicos╧Х) for a pure inductor is 0 (lagging).

  • тЦ╕

    Energy is only stored in the magnetic field, not dissipated as heat.

  • тЦ╕

    The net work done over a full cycle is zero.

тЬЕ Advantages
  • тЦ╕

    Does not consume real power (no energy wastage).

  • тЦ╕

    Used effectively in reactive power compensation.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Cannot be used for heating or lighting purposes.

  • тЦ╕

    Causes voltage drops in transmission lines due to inductive reactance.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Induction motors (for magnetic field creation).

  • тЦ╕

    Tuned circuits and filters.

  • тЦ╕

    Smoothing reactors in power supplies.

ЁЯУД Additional Information
  • тЦ╕

    Option B (1) represents a purely resistive circuit where phase angle is 0.

  • тЦ╕

    Option C (infinity) is physically impossible for passive components.

  • тЦ╕

    Option D (1.414) represents the peak factor for a sinusoidal waveform (sqrt2\\sqrt{2}sqrt2).

ЁЯУК Diagram / Illustration
Average Power Formula
Pavg=VrmsIrmscosтБб(╧Х)P_{avg} = V_{rms} I_{rms} \cos(\phi)PavgтАЛ=VrmsтАЛIrmsтАЛcos(╧Х)
For Pure Inductor: ╧Х=90тИШ\phi = 90^\circ╧Х=90тИШ
cosтБб(90тИШ)=0тАЕтАКтЯ╣тАЕтАКPavg=0\cos(90^\circ) = 0 \implies P_{avg} = 0cos(90тИШ)=0тЯ╣PavgтАЛ=0
тЬЕ

A is correct тАФ The average power in a pure inductor is zero because it does not dissipate energy as heat, acting only as an energy storage element.

Core Concepts Used
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Inductive Reactance ($X_L$) Phase Angle ($phi$) Power Factor ($cos \phi$) Reactive Power
ЁЯТб EXAM TIP

Remember: Resistors dissipate real power (P=I2RP = I^2RP=I2R), whereas Inductors and Capacitors only exchange reactive power with the source.

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