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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 n2μ0πR2.

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’ 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=πR2

The magnetic field inside the solenoid is given by,

role="math" localid="1658135700537" B=μ0nI

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,

ϕ=B.A

Substitute μ0nIfor B andπR2 for A into above equation.

ϕ=μ0nI.πR2ϕ=μ0nI.πR2

The inductance of the solenoid is given by,

L=NϕI

Substitute μ0nIπR2for ϕinto above equation.

L=Nμ0nLπ2IL=Nμ0nLπ2I

Substitute nIfor N into above equation.

L=nIμ0nIπR2ILI=n2μ0πR2

Hence the self-inductance per unit length of the solenoid isn2μ0πR2

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Most popular questions from this chapter

Question: The preceding problem was an artificial model for the charging capacitor, designed to avoid complications associated with the current spreading out over the surface of the plates. For a more realistic model, imagine thin wires that connect to the centers of the plates (Fig. 7.46a). Again, the current I is constant, the radius of the capacitor is a, and the separation of the plates is w << a. Assume that the current flows out over the plates in such a way that the surface charge is uniform, at any given time, and is zero at t = 0.

(a) Find the electric field between the plates, as a function of t.

(b) Find the displacement current through a circle of radius in the plane mid-way between the plates. Using this circle as your "Amperian loop," and the flat surface that spans it, find the magnetic field at a distance s from the axis.

Figure 7.46

(c) Repeat part (b), but this time uses the cylindrical surface in Fig. 7.46(b), which is open at the right end and extends to the left through the plate and terminates outside the capacitor. Notice that the displacement current through this surface is zero, and there are two contributions to Ienc.

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Problem 7.61 The magnetic field of an infinite straight wire carrying a steady current I can be obtained from the displacement current term in the Ampere/Maxwell law, as follows: Picture the current as consisting of a uniform line charge λmoving along the z axis at speed v (so that I=λv), with a tiny gap of length E , which reaches the origin at time t=0. In the next instant (up to t=E/v) there is no real current passing through a circular Amperian loop in the xy plane, but there is a displacement current, due to the "missing" charge in the gap.

(a) Use Coulomb's law to calculate the z component of the electric field, for points in the xy plane a distances from the origin, due to a segment of wire with uniform density -λ . extending from toz1=vt-Etoz2=vt .

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