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ElectricalBasic Electrical
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In pure inductor circuit, angle between voltage and current is

A

0┬░0┬░0┬░

B

30┬░30┬░30┬░

C

60┬░60┬░60┬░

D

90┬░90┬░90┬░

Correct Answer

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

90┬░90┬░90┬░

Quick Summary:

In a pure inductive circuit, the current lags behind the voltage by an angle of 90┬░90┬░90┬░ (or ╧А2\frac{\pi}{2}2╧АтАЛ radians). This occurs because the induced back-EMF opposes the change in current, forcing the current waveform to reach its peak later than the voltage.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

In a pure inductive circuit, the current lags behind the voltage by an angle of 90┬░90┬░90┬░ (or ╧А2\frac{\pi}{2}2╧АтАЛ radians). This occurs because the induced back-EMF opposes the change in current, forcing the current waveform to reach its peak later than the voltage.

ЁЯФв Key Formulas

vL=Ldidtv_L = L \frac{di}{dt}vLтАЛ=LdtdiтАЛ тАФ Instantaneous voltage across an inductor

XL=2╧АfLX_L = 2\pi f LXLтАЛ=2╧АfL тАФ Inductive reactance in Ohms

╧Х=90┬░\phi = 90┬░╧Х=90┬░ тАФ Phase shift in a pure inductor

тЪЩя╕П Working Principle

According to Faraday's Law, the induced voltage across an inductor is given by v(t)=Ldidtv(t) = L \frac{di}{dt}v(t)=LdtdiтАЛ. For a sinusoidal current i(t)=ImsinтБб(╧Йt)i(t) = I_m \sin(\omega t)i(t)=ImтАЛsin(╧Йt), the resulting voltage is v(t)=╧ЙLImsinтБб(╧Йt+90┬░)v(t) = \omega L I_m \sin(\omega t + 90┬░)v(t)=╧ЙLImтАЛsin(╧Йt+90┬░). Thus, the phase difference ╧Х\phi╧Х between voltage and current is exactly 90┬░90┬░90┬░, confirming that the inductor is a purely reactive element that does not dissipate real power.

ЁЯУМ Key Points
  • тЦ╕

    A pure inductor has zero resistance and zero conductance.

  • тЦ╕

    The power factor of a purely inductive circuit is zero lagging.

  • тЦ╕

    Inductors store energy in the form of a magnetic field.

  • тЦ╕

    Real inductors always contain a small amount of internal series resistance (RRR).

тЬЕ Advantages
  • тЦ╕

    Inductors can be used as filters to block high-frequency noise.

  • тЦ╕

    Useful for energy storage in magnetic fields for power electronics converters.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Purely inductive circuits are theoretical; real inductors have parasitic resistance.

  • тЦ╕

    High inductive loads can cause voltage spikes during switching.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Tuned circuits and oscillators in radio frequency communication.

  • тЦ╕

    Chokes for smoothing current in DC power supplies.

ЁЯУД Additional Information
  • тЦ╕

    At 90┬░90┬░90┬░ phase shift, the average power consumption P=VIcosтБб(90┬░)=0P = VI \cos(90┬░) = 0P=VIcos(90┬░)=0 Watts.

  • тЦ╕

    Option A is 0, which corresponds to a purely resistive circuit.

  • тЦ╕

    Options B and C represent RL circuits where R>0R > 0R>0.

ЁЯУК Diagram / Illustration
Phase Relation in InductorVoltageCurrentTime (t) -> Phase Angle
тЬЕ

D is correct тАФ In a purely inductive circuit, the back-EMF created by the changing magnetic flux causes the current to lag the voltage by exactly 90┬░90┬░90┬░.

Core Concepts Used
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Inductive Reactance Phase Difference Lenz's Law
ЁЯТб EXAM TIP

Remember 'ELI' for inductors: In an Inductor (L), Current (I) comes after Voltage (E).

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