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A current Iflows down a wire of radius a.

(a) If it is uniformly distributed over the surface, what is the surface current density K?

(b) If it is distributed in such a way that the volume current density is inversely

proportional to the distance from the axis, what is J(s)?

Short Answer

Expert verified

(a) The surface current density corresponding to a current Iflowing down a wire of radius aisI2πa.

(b) The volume current density corresponding to a current Iflowing down a wire of radius ais I2πas.

Step by step solution

01

Given data

There is a wire of radius a carrying a current I.

02

Surface and volume current density

The surface current density if the current is uniformly distributed over a surface is

K=IL.....(1)

Here, L is the cross sectional length of the surface.

The total current in terms of volume current density is

I=Jda.....(2)

Here, the integration is over the cross sectional area.

03

Surface current density in wire of radius   

From equation (1), the surface current density on the surface of the wire of radius a is

K=I2πa

Thus, the uniform surface current density is I2πa.

04

Volume current density in wire of radius  

Let the volume current density be

J=ks.....3

Here, k is a constant and is the radial component of polar coordinate.

From equation (2),

I=k0a1s2πsds=k2πak=I2πa

Substitute this in equation (3) to get

J=I2πas

Thus, the volume current density is I2πas.

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Most popular questions from this chapter

Use the Biot-Savart law (most conveniently in the form of Eq. 5.42 appropriate to surface currents) to find the field inside and outside an infinitely long solenoid of radiusR, with n turns per unit length, carrying a steady current I.

A magnetic dipole m=m0z^ is situated at the origin, in an otherwiseuniform magnetic field B=B0z^ . Show that there exists a spherical surface, centered at the origin, through which no magnetic field lines pass. Find the radius of this sphere, and sketch the field lines, inside and out.

Another way to fill in the "missing link" in Fig. 5.48 is to look for a magnetostatic analog to Eq. 2.21. The obvious candidate would be

A(r)=0r(B×dl)

(a) Test this formula for the simplest possible case-uniform B (use the origin as your reference point). Is the result consistent with Prob. 5.25? You could cure this problem by throwing in a factor of localid="1657688349235" 12, but the flaw in this equation runs deeper.

(b) Show that (B×dl)is not independent of path, by calculating (B×dl)around the rectangular loop shown in Fig. 5.63.

Figure 5.63

As far as lknow,28the best one can do along these lines is the pair of equations

(i) localid="1657688931461" v(r)=-r×01E(λr)

(ii) A(r)=-r×01λB(λr)

[Equation (i) amounts to selecting a radial path for the integral in Eq. 2.21; equation (ii) constitutes a more "symmetrical" solution to Prob. 5.31.]

(c) Use (ii) to find the vector potential for uniform B.

(d) Use (ii) to find the vector potential of an infinite straight wire carrying a steady current. Does (ii) automatically satisfy A=0[Answer:(μol/2πs)(zs^-sz^) ].

Question: (a) Find the density ρof mobile charges in a piece of copper, assuming each atom contributes one free electron. [Look up the necessary physical constants.]

(b) Calculate the average electron velocity in a copper wire 1 mm in diameter, carrying a current of 1 A. [Note:This is literally a snail'space. How, then, can you carry on a long distance telephone conversation?]

(c) What is the force of attraction between two such wires, 1 em apart?

(d) If you could somehow remove the stationary positive charges, what would the electrical repulsion force be? How many times greater than the magnetic force is it?

A thin glass rod of radius Rand length Lcarries a uniform surfacecharge δ .It is set spinning about its axis, at an angular velocity ω.Find the magnetic field at a distances sR from the axis, in the xyplane (Fig. 5.66). [Hint:treat it as a stack of magnetic dipoles.]

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