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ElectricalMachine
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What is the formula for the magnetic field due to a solenoid?

A

╬╝nI\mu nI╬╝nI

B

╬╝n2\mu n^2╬╝n2

C

╬╝I2\mu I^2╬╝I2

D

╬╝n2I2\mu n^2 I^2╬╝n2I2

Correct Answer

тЪЩя╕П TE тАв Technical Concept & PrincipleElectricalMachine
Option A

╬╝nI\mu nI╬╝nI

Quick Summary:

The magnetic field inside a long, tightly wound, ideal solenoid carrying a current III is uniform, parallel to its axis, and given by B=╬╝nIB = \mu n IB=╬╝nI. Here, ╬╝\mu╬╝ is the magnetic permeability of the core material (╬╝=╬╝0╬╝r\mu = \mu_0 \mu_r╬╝=╬╝0тАЛ╬╝rтАЛ), nnn is the number of turns per unit length, and III is the electric current.

тЪЩя╕ПTETechnical SolutionConcept & Principle
ЁЯТб Explanation

The magnetic field inside a long, tightly wound, ideal solenoid carrying a current III is uniform, parallel to its axis, and given by B=╬╝nIB = \mu n IB=╬╝nI. Here, ╬╝\mu╬╝ is the magnetic permeability of the core material (╬╝=╬╝0╬╝r\mu = \mu_0 \mu_r╬╝=╬╝0тАЛ╬╝rтАЛ), nnn is the number of turns per unit length, and III is the electric current.

ЁЯФв Key Formulas

B=╬╝nIB = \mu n IB=╬╝nI тАФ Magnetic field inside a long solenoid

n=NLn = \frac{N}{L}n=LNтАЛ тАФ Turn density (turns per unit length)

Bend=12╬╝nIB_{end} = \frac{1}{2} \mu n IBendтАЛ=21тАЛ╬╝nI тАФ Magnetic field strength at either end of a solenoid

тЪЩя╕П Working Principle

When an electric current flows through the turns of a solenoid, each helical turn creates a magnetic field loop. Inside the solenoid, the magnetic field vectors produced by adjacent turns add constructively along the central axis, resulting in a strong, uniform magnetic field, while outside the solenoid, the field components cancel out, making the external field nearly zero.

ЁЯУМ Key Points
  • тЦ╕

    The magnetic field inside an ideal, infinitely long solenoid is uniform and directed along the axis.

  • тЦ╕

    The field strength depends directly on core permeability (╬╝\mu╬╝), turn density (nnn), and current (III).

  • тЦ╕

    The magnetic field strength at the extreme end of a long solenoid is exactly half of its value at the center.

тЬЕ Advantages
  • тЦ╕

    Produces a highly uniform and controllable magnetic field along its internal axis.

  • тЦ╕

    Field magnitude can be easily controlled by adjusting the excitation current or turn density.

тЭМ Disadvantages / Limitations
  • тЦ╕

    Magnetic flux leakage occurs at the ends, making the field non-uniform near edges.

  • тЦ╕

    High currents lead to I2RI^2RI2R resistive heating in the conductor windings.

ЁЯЫая╕П Applications / Uses
  • тЦ╕

    Electromagnets, relays, and electromechanical actuators.

  • тЦ╕

    Inductors and transformers in electrical power systems and machines.

ЁЯУД Additional Information
  • тЦ╕

    In free space, ╬╝=╬╝0=4╧А├Ч10┬░тИТ7┬аH/m\mu = \mu_0 = 4\pi \times 10┬░{-7} \text{ H/m}╬╝=╬╝0тАЛ=4╧А├Ч10┬░тИТ7┬аH/m, so B=╬╝0nIB = \mu_0 n IB=╬╝0тАЛnI.

  • тЦ╕

    Option B (╬╝n2\mu n^2╬╝n2), Option C (╬╝I2\mu I^2╬╝I2), and Option D (╬╝n2I2\mu n^2 I^2╬╝n2I2) are mathematically incorrect and do not represent any magnetic field formula.

ЁЯУК Diagram / Illustration
Magnetic Field of an Ideal SolenoidB = ┬╡ ┬╖ n ┬╖ I┬╡ = Permeability of Core Material (┬╡тВА ┬╖ ┬╡с╡г)n = Number of Turns per Unit Length (N / L)I = Electric Current through Solenoid
тЬЕ

A is correct тАФ The magnetic field inside an ideal long solenoid is given by B=╬╝nIB = \mu n IB=╬╝nI, where nnn is the number of turns per unit length.

Core Concepts Used
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Ampere's Circuital Law Solenoids and Electromagnets Magnetic Permeability
ЁЯТб EXAM TIP

Remember that at the precise physical end of a long solenoid, the field drops to Bend=12╬╝nIB_{end} = \frac{1}{2} \mu n IBendтАЛ=21тАЛ╬╝nI, a common trick question in GATE and AE/JE competitive exams.

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