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ElectricalElectromagnetics Field Theory
PrevNext

In case of an inductance, current is proportional to

A

Voltage across the inductance

B

Magnetic field

C

Both (a) and (b)

D

Neither (a) nor (b)

Correct Answer

тЪЩя╕П TE тАв Technical Concept & PrincipleElectricalElectromagnetics Field Theory
Option B

Magnetic field

Quick Summary:

In an inductor, the current i(t)i(t)i(t) is fundamentally related to the magnetic flux linkage ╬ж\Phi╬ж through the relationship N╬ж=LiN\Phi = LiN╬ж=Li. Since the magnetic field BBB is directly proportional to the magnetic flux ╬ж\Phi╬ж (where ╬ж=тИлBтЛЕdA\Phi = \int B \cdot dA╬ж=тИлBтЛЕdA), the current is directly proportional to the strength of the magnetic field.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

In an inductor, the current i(t)i(t)i(t) is fundamentally related to the magnetic flux linkage ╬ж\Phi╬ж through the relationship N╬ж=LiN\Phi = LiN╬ж=Li. Since the magnetic field BBB is directly proportional to the magnetic flux ╬ж\Phi╬ж (where ╬ж=тИлBтЛЕdA\Phi = \int B \cdot dA╬ж=тИлBтЛЕdA), the current is directly proportional to the strength of the magnetic field.

ЁЯФв Key Formulas

╬ж=LiN\Phi = \frac{Li}{N}╬ж=NLiтАЛ тАФ Flux linkage relation to current

v=Ldidtv = L \frac{di}{dt}v=LdtdiтАЛ тАФ Voltage relation to rate of change of current

тЪЩя╕П Working Principle

According to Ampere's Law and the definition of self-inductance, the magnetic flux ╬ж\Phi╬ж produced by a coil is linearly proportional to the current iii flowing through it, assuming a linear magnetic material. The relationship is expressed as ╬ж=LiN\Phi = \frac{Li}{N}╬ж=NLiтАЛ. Because BBB is proportional to ╬ж\Phi╬ж, it follows that iтИЭBi \propto BiтИЭB. In contrast, the voltage across an inductor is proportional to the rate of change of current (v=Ldidtv = L \frac{di}{dt}v=LdtdiтАЛ), not the current itself.

ЁЯУМ Key Points
  • тЦ╕

    Current is proportional to flux (and thus magnetic field) in a linear inductor.

  • тЦ╕

    Voltage is proportional to the time derivative of the current, not the current magnitude.

  • тЦ╕

    The constant of proportionality is related to the geometry and core material properties (permeability ╬╝\mu╬╝).

  • тЦ╕

    This linear relationship holds only when the magnetic core is not saturated.

тЬЕ Advantages
  • тЦ╕

    Energy storage in magnetic field

  • тЦ╕

    Smooths current ripples in power electronics

тЭМ Disadvantages / Limitations
  • тЦ╕

    Cannot change current instantaneously (infinite voltage requirement)

  • тЦ╕

    Susceptible to magnetic saturation

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Transformers

  • тЦ╕

    Electromagnetic relays

  • тЦ╕

    Induction motors

ЁЯУД Additional Information
  • тЦ╕

    In highly non-linear magnetic materials (like iron cores), LLL becomes a function of iii, making the proportionality non-linear.

  • тЦ╕

    Option A is incorrect because voltage depends on the time derivative of current (di/dtdi/dtdi/dt), not the current value itself.

ЁЯУК Diagram / Illustration
Inductance Relationship
i(t)i(t)i(t)
B(t)тЛЕALB(t) \cdot (A / L)B(t)тЛЕLAтАЛ
тЬЕ

B is correct тАФ In a linear inductor, the magnetic field strength is directly proportional to the current flowing through the coil windings.

Core Concepts Used
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Ampere's Law Self-Inductance Magnetic Flux Linkage
ЁЯТб EXAM TIP

Always distinguish between integral relationships (current and flux) and differential relationships (voltage and current) when analyzing inductors.

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