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Find the self-inductance per unit length of a long solenoid, of radius R , carrying n turns per unit length.

Short Answer

Expert verified

The self-inductance per unit length of the solenoid is n20蟺搁2.

Step by step solution

01

Write the given data from the question.

The radius of the solenoid is R .

02

Determine the self-inductance per unit length of a solenoid.

Let鈥 assume the solenoid having the length l , number of the turns N and cross-sectional area is A . The current carried by the solenoid is I.

The area of the solenoid is given by,

A=R2

The magnetic field inside the solenoid is given by,

role="math" localid="1658135700537" B=0nI

Here nis the number of the turns per unit length.

The number of the turns per unit length.

n=NIN=nI

The magnetic flux is given by,

=B.A

Substitute 0nIfor B andR2 for A into above equation.

=0nI.R2=0nI.R2

The inductance of the solenoid is given by,

L=NI

Substitute 0nIR2for into above equation.

L=N0nL2IL=N0nL2I

Substitute nIfor N into above equation.

L=nI0nIR2ILI=n20R2

Hence the self-inductance per unit length of the solenoid isn20R2

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Most popular questions from this chapter

In a perfect conductor, the conductivity is infinite, so E=0(Eq. 7.3), and any net charge resides on the surface (just as it does for an imperfect conductor, in electrostatics).

(a) Show that the magnetic field is constant (Bt=0), inside a perfect conductor.

(b) Show that the magnetic flux through a perfectly conducting loop is constant.

A superconductor is a perfect conductor with the additional property that the (constant) B inside is in fact zero. (This "flux exclusion" is known as the Meissner effect.)

(c) Show that the current in a superconductor is confined to the surface.

(d) Superconductivity is lost above a certain critical temperature (Tc), which varies from one material to another. Suppose you had a sphere (radius ) above its critical temperature, and you held it in a uniform magnetic field B0z^while cooling it below Tc. Find the induced surface current density K, as a function of the polar angle.

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I(t)={(1-t)I0for0t1/afort>/a

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Prove Alfven's theorem: In a perfectly conducting fluid (say, a gas of free electrons), the magnetic flux through any closed loop moving with the fluid is constant in time. (The magnetic field lines are, as it were, "frozen" into the fluid.)

(a) Use Ohm's law, in the form of Eq. 7.2, together with Faraday's law, to prove that if =and is J finite, then

Bt=(vB)

(b) Let S be the surface bounded by the loop (P)at time t , and S'a surface bounded by the loop in its new position (P')at time t+dt (see Fig. 7.58). The change in flux is

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Use B=0to show that

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(Where R is the "ribbon" joining P and P' ), and hence that

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(For infinitesimal dt ). Use the method of Sect. 7.1.3 to rewrite the second integral as

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And invoke Stokes' theorem to conclude that

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Together with the result in (a), this proves the theorem.

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R=0C

(b) Suppose you connected a battery between 1 and 2, and charged them up to a potential differenceV0. If you then disconnect the battery, the charge will gradually leak off. Show thatV(t)=V0e-t/r, and find the time constant,, in terms of 0and .

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