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An infinitely long circular cylinder carries a uniform magnetization Mparallel to its axis. Find the magnetic field (due toM) inside and outside the cylinder.

Short Answer

Expert verified

The value of magnetic field inside and outside the cylinder isB→ins=μ0Mz^ andB→out=0 .

Step by step solution

01

Write the given data from the question.

Consideran infinitely long circular cylinder carries a uniform magnetizationM parallel to its axis.

02

Determine the formula of magnetic field inside the cylinder.

Write the formula of magnetic field inside the cylinder.

B→=μ0K …… (1)

Here,μ0 is permeability andK is surface current.

03

Determine the value of magnetic field inside and outside the cylinder.

Thereisnovolumeboundcurrentsincethecylinder'smagnetizationishomogeneous;instead,thereissurfaceboundcurrent.

Determine the surface bound current.

K→b=M→×n→=Mz^×s^=Mϕ

This is the field of an infinite solenoid with surface current,nI=K=M therefore the outside field is and the inner field is:B→out=0

Determine the magnetic field inside the cylinder.

SubstituteMz^ forK into equation (1).

B→ins=μ0Mz^=μ0M→

Therefore, the value of magnetic field inside and outside the cylinder is B→ins=μ0Mz^ and B→out=0.

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Most popular questions from this chapter

On the basis of the naïve model presented in Sect. 6.1.3, estimate the magnetic susceptibility of a diamagnetic metal such as copper. Compare your answer with the empirical value in Table 6.1, and comment on any discrepancy.

For the bar magnet of Problem. 6.9, make careful sketches of M, B, and H, assuming L is about 2a. Compare Problem. 4.17.

A magnetic dipole m is imbedded at the center of a sphere (radius R) of linear magnetic material (permeability μ). Show that the magnetic field inside the sphere 0<r≤R is

μ4π{1r3[3(m.r^r^-m)]+2(μ0-μ)m(2μ0+μ)R3}

What is the field outside the sphere?

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.

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).

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