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ElectricalMachine
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The magnetic field at a point d distance away from long wire due to the electric current I in it is ____________

A

A) ╬╝0I2r\frac{\mu_0 I}{2r}2r╬╝0тАЛIтАЛ

B

B) ╬╝0Ir\frac{\mu_0 I}{r}r╬╝0тАЛIтАЛ

C

C) ╬╝0I2╧Аr\frac{\mu_0 I}{2\pi r}2╧Аr╬╝0тАЛIтАЛ

D

D) ╬╝0I╧Аr\frac{\mu_0 I}{\pi r}╧Аr╬╝0тАЛIтАЛ

Correct Answer

тЪЩя╕П TE тАв Technical Concept & PrincipleElectricalMachine
Option C

╬╝0I2╧Аr\frac{\mu_0 I}{2\pi r}2╧Аr╬╝0тАЛIтАЛ

Quick Summary:

The magnetic field intensity at a distance rrr from an infinitely long, straight conductor carrying a steady current III is inversely proportional to the distance and directly proportional to the current. According to Ampere's Circuital Law, this relationship is given by B=╬╝0I2╧АrB = \frac{\mu_0 I}{2\pi r}B=2╧Аr╬╝0тАЛIтАЛ. Thus, Option C represents the correct mathematical expression for the magnetic field.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

The magnetic field intensity at a distance rrr from an infinitely long, straight conductor carrying a steady current III is inversely proportional to the distance and directly proportional to the current. According to Ampere's Circuital Law, this relationship is given by B=╬╝0I2╧АrB = \frac{\mu_0 I}{2\pi r}B=2╧Аr╬╝0тАЛIтАЛ. Thus, Option C represents the correct mathematical expression for the magnetic field.

ЁЯФв Key Formulas

B=╬╝0I2╧АrB = \frac{\mu_0 I}{2\pi r}B=2╧Аr╬╝0тАЛIтАЛ тАФ Magnetic field at distance rrr from a long straight current-carrying wire

тИоBтЛЕdl=╬╝0Ienc\oint B \cdot dl = \mu_0 I_{\text{enc}}тИоBтЛЕdl=╬╝0тАЛIencтАЛ тАФ Ampere's Circuital Law

тЪЩя╕П Working Principle

When an electric current flows through a straight conductor, it produces magnetic flux lines in concentric circles around the wire. Applying Ampere's Circuital Law around a closed circular path of radius rrr gives тИоBтЛЕdl=B(2╧Аr)=╬╝0Ienc\oint B \cdot dl = B(2\pi r) = \mu_0 I_{\text{enc}}тИоBтЛЕdl=B(2╧Аr)=╬╝0тАЛIencтАЛ, which yields B=╬╝0I2╧АrB = \frac{\mu_0 I}{2\pi r}B=2╧Аr╬╝0тАЛIтАЛ.

ЁЯУМ Key Points
  • тЦ╕

    The magnetic field lines form concentric circles around the conductor.

  • тЦ╕

    The magnitude of the magnetic field BBB decreases linearly as the distance rrr increases (BтИЭ1/rB \propto 1/rBтИЭ1/r).

  • тЦ╕

    The direction of the magnetic field is determined by the Right-Hand Thumb Rule.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Calculating magnetic forces between parallel current-carrying conductors in transmission lines.

  • тЦ╕

    Designing inductor coils and understanding electromagnetic interference (EMI) around heavy current conductors.

ЁЯУД Additional Information
  • тЦ╕

    Option A (╬╝0I2r\frac{\mu_0 I}{2r}2r╬╝0тАЛIтАЛ) represents the magnetic field at the center of a circular current-carrying loop of radius rrr.

  • тЦ╕

    Option C (╬╝0I2╧Аr\frac{\mu_0 I}{2\pi r}2╧Аr╬╝0тАЛIтАЛ) is correct for a long straight conductor at distance rrr (or ddd).

ЁЯУК Diagram / Illustration
Magnetic Field of Long Straight WireB =┬╡тВА I2╧А rWhere ┬╡тВА = Permeability of free space, r = Distance from wire
тЬЕ

C is correct тАФ The magnetic field due to a long current-carrying conductor at a distance rrr is given by B=╬╝0I2╧АrB = \frac{\mu_0 I}{2\pi r}B=2╧Аr╬╝0тАЛIтАЛ.

Core Concepts Used
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Ampere's Circuital Law Biot-Savart Law Magnetic Field due to Straight Conductor
ЁЯТб EXAM TIP

Always distinguish between a straight conductor (B=╬╝0I2╧АrB = \frac{\mu_0 I}{2\pi r}B=2╧Аr╬╝0тАЛIтАЛ) and a circular loop center (B=╬╝0I2rB = \frac{\mu_0 I}{2r}B=2r╬╝0тАЛIтАЛ); the factor of ╧А\pi╧А appears in the denominator for straight wires due to the circular perimeter 2╧Аr2\pi r2╧Аr integration path.

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