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Question: Derive the expression for the self-inductance of a long solenoid of cross sectional area A and lengt...

Derive the expression for the self-inductance of a long solenoid of cross sectional area A and length l, having n turns per length.

Explanation

Solution

Biot- Savart law helps to find the magnetic field inside the solenoid. Each turn nn is the solenoid has the lengthll. Then applying the Biot- Savart law we get the magnetic field inside the solenoid as
B=μ0nIlB = \dfrac{{{\mu _0}nI}}{l}
Where, μ0{\mu _0} is the permeability of free space, nnis the number of turns and IIis the current in the solenoid and ll is the length.
And the magnetic flux is proportional to the current through the solenoid. Thus the proportionality constant is the coefficient of self- inductance of the solenoid.

Complete Step by step solution
We are considering a solenoid with nn turns with length ll . The area of cross section is AA. The solenoid carriers current II and BB is the magnetic field inside the solenoid.
The magnetic field BB is given as,
B=μ0nIlB = \dfrac{{{\mu _0}nI}}{l}
Where, μ0{\mu _0} is the permeability of free space, nn is the number of turns and II is the current in the solenoid and ll is the length.
The magnetic flux is the product of the magnetic field and area of the cross section.
Here the magnetic flux per turn is given as,
ϕ=B×A\phi = B \times A
Substituting the values in the above expression,
ϕ=μ0nIl×A\phi = \dfrac{{{\mu _0}nI}}{l} \times A
Hence there is nn number of turns, the total magnetic flux is given as,

ϕ=μ0nIl×A×n ϕ=μ0n2IAl..............(1)  \phi = \dfrac{{{\mu _0}nI}}{l} \times A \times n \\\ \phi = \dfrac{{{\mu _0}{n^2}IA}}{l}..............\left( 1 \right) \\\

If LL is the coefficient of self-inductance of the solenoid, then
ϕ=LI...........(2)\phi = LI...........\left( 2 \right)
Comparing the two equations we get,

LI=μ0n2IAl L=μ0n2Al  LI = \dfrac{{{\mu _0}{n^2}IA}}{l} \\\ L = \dfrac{{{\mu _0}{n^2}A}}{l} \\\

So the expression for the coefficient of self-inductance is μ0n2Al\dfrac{{{\mu _0}{n^2}A}}{l}.

Note The flux through one solenoid coil is ϕ=B×A\phi = B \times A where the area of the cross section of each turn is AA.
For the nn number of turns then the total magnetic flux is ϕ=n×B×A\phi = n \times B \times A. The magnetic field is uniform inside the solution.