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Self Inductance of a Solenoid: JEE Physics Derivation

Derive the self-inductance of a solenoid step-by-step. Understand the concepts of magnetic flux, flux linkage, and the formula L = μ₀n²Al.

3 min readPublished 4 June 2026
Electromagnetic InductionL = μ₀n²Al

TITLE: Self Inductance of a Solenoid: JEE Physics Derivation DESCRIPTION: Derive the self-inductance of a solenoid step-by-step. Understand the concepts of magnetic flux, flux linkage, and the formula L = μ₀n²Al.

Concept Overview

This question tests the understanding of electromagnetic induction, specifically how to derive the self-inductance of a long solenoid. The derivation involves calculating the magnetic field inside the solenoid, determining the magnetic flux through each turn, and then calculating the total flux linkage. This process directly leads to the formula for self-inductance, L=μ0n2AlL = \mu_0 n^2 Al, which is a fundamental concept in AC circuits and electrical engineering.

Step 1: Magnetic Field Inside a Solenoid We begin by recalling the formula for the magnetic field (BB) inside a long solenoid. For a solenoid with nn turns per unit length and carrying a current II, the magnetic field is uniform and given by:

B=μ0nIB = \mu_0 n I

Here, μ0\mu_0 is the permeability of free space, and nn is the number of turns per unit length. This formula arises from Ampere's Law applied to a solenoid.

Step 2: Magnetic Flux Through One Turn Next, we calculate the magnetic flux (Φ\Phi) through a single turn of the solenoid. The solenoid has a cross-sectional area AA. Since the magnetic field is uniform and perpendicular to the area, the flux through one turn is:

Φ=B×A\Phi = B \times A

Substituting the expression for BB from Step 1, we get:

Φ=(μ0nI)×A\Phi = (\mu_0 n I) \times A

This represents the magnetic flux passing through the area enclosed by one loop of the solenoid.

Step 3: Total Flux Linkage The self-inductance is defined in terms of flux linkage, which is the total magnetic flux linking all the turns of the coil. If the solenoid has a total length ll, and nn is the turns per unit length, then the total number of turns (NN) is N=nlN = nl. The total flux linkage is the flux through one turn multiplied by the total number of turns:

Flux Linkage=N×Φ\text{Flux Linkage} = N \times \Phi

Substituting the expressions for NN and Φ\Phi:

Flux Linkage=(nl)×(μ0nIA)\text{Flux Linkage} = (nl) \times (\mu_0 n I A) Flux Linkage=μ0n2lAI\text{Flux Linkage} = \mu_0 n^2 l A I

This quantity represents the sum of the magnetic flux passing through each individual turn of the solenoid.

Step 4: Definition of Self-Inductance Self-inductance (LL) is defined as the ratio of the total flux linkage to the current producing it. Mathematically, this is expressed as:

L=Flux LinkageIL = \frac{\text{Flux Linkage}}{I}

This definition arises from Faraday's Law of induction, where the induced EMF is proportional to the rate of change of flux linkage, and the constant of proportionality is the inductance.

Step 5: Deriving the Formula for L Now, we substitute the expression for total flux linkage from Step 3 into the definition of self-inductance from Step 4:

L=μ0n2lAIIL = \frac{\mu_0 n^2 l A I}{I}

The current II cancels out, leaving us with the formula for the self-inductance of a solenoid:

L=μ0n2lAL = \mu_0 n^2 l A

This is the final derived formula for the self-inductance of a long solenoid, where ll is the length of the solenoid and AA is its cross-sectional area.

Key Takeaways:

  • The magnetic field inside a long solenoid is uniform and given by B=μ0nIB = \mu_0 n I.
  • Magnetic flux through a single turn is Φ=BA\Phi = BA.
  • Self-inductance (LL) is defined as the ratio of total flux linkage to the current, L=NΦIL = \frac{N\Phi}{I}.
  • The self-inductance of a solenoid depends on its geometry (length, area) and the permeability of the core material (μ0\mu_0 for vacuum/air).

Answer: L=μ0n2lAL = \mu_0 n^2 l A

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