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A short circular cylinder of radius and length L carries a "frozen-in" uniform magnetization M parallel to its axis. Find the bound current, and sketch the magnetic field of the cylinder. (Make three sketches: one forL>>a, one forL<<a, and one forL≈a.) Compare this bar magnet with the bar electret of Prob. 4.11.

Short Answer

Expert verified

The value of bound current is K→b=Mϕ^.

Draw the magnetic field of the cylinder for L>>a.

Draw the magnetic field of the cylinder for L<<a.

Draw the magnetic field of the cylinder for L≈a.

Step by step solution

01

Write the given data from the question.

Consider a short circular cylinder of radius and length carries a "frozen-in" uniform magnetization parallel to its axis.

02

Determine the formula of bound current.

Write the formula of bound current.

K→b=M→×s→..........(1)

Here, M→is frozen-in uniform magnetization ands→ is distance from axis.

03

Determine the value of bound current and draw the magnetic field of the cylinder for L>>a, for L<<a and for L≈a.

Draw the circuit diagram of magnetic field of the cylinder for L>>a.

Figure 1

Draw the circuit diagram of magnetic field of the cylinder for L<<a.

Figure 2

Draw the circuit diagram of magnetic field of the cylinder for L≈a.

Figure 3

Determine the bound current is given by:

Substitute ϕ^for s→into equation (1).

k→b=Mϕ^

Thus, the field is made up of a solenoid with the following dimensions: L, a, and for the surface current.

The lines of the magnetic field are drawn above. They resemble the bar electret case in appearance, but inside they are entirely different since the magnetic field does not have discontinuities at the top or bottom like the electric field does.

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Most popular questions from this chapter

Suppose the field inside a large piece of magnetic material is B0, so that H0=(1/μ0)B0-M, where M is a "frozen-in" magnetization.

(a) Now a small spherical cavity is hollowed out of the material (Fig. 6.21). Find the field at the center of the cavity, in terms of B0 and M. Also find H at the center of the cavity, in terms of H0 and M.

(b) Do the same for a long needle-shaped cavity running parallel to M.

(c) Do the same for a thin wafer-shaped cavity perpendicular to M.

Figure 6.21

Assume the cavities are small enough so M, B0, and H0 are essentially constant. Compare Prob. 4.16. [Hint: Carving out a cavity is the same as superimposing an object of the same shape but opposite magnetization.]

Calculate the torque exerted on the square loop shown in Fig. 6.6, due to the circular loop (assume is much larger than or ). If the square loop is free to rotate, what will its equilibrium orientation be?

How would you go about demagnetizing a permanent magnet (such as the wrench we have been discussing, at point in the hysteresis loop)? That is, how could you restore it to its original state, with M = 0 at / = 0 ?

Notice the following parallel:

{∇·D=0∇×E=0,ε0E=D-P(Nofreecharge)∇·B=0∇×H=0,μ0H=B-μ0M(Nofreecharge)

Thus, the transcription D→B,E→H,P→μ0M,ε0→μ0,, turns an electrostatic problem into an analogous magnetostatic one. Use this, together with your knowledge of the electrostatic results, to rederive.

(a) the magnetic field inside a uniformly magnetized sphere (Eq. 6.16);

(b) the magnetic field inside a sphere of linear magnetic material in an otherwise uniform magnetic field (Prob. 6.18);

(c) the average magnetic field over a sphere, due to steady currents within the sphere (Eq. 5.93).

A sphere of linear magnetic material is placed in an otherwise uniform magnetic field B0. Find the new field inside the sphere.

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