You are asked to referee a grant application, which proposes to determine whether the magnetization of iron is due to "Ampere" dipoles (current loops) or "Gilbert" dipoles (separated magnetic monopoles). The experiment will involve a cylinder of iron (radius Rand length L=10R), uniformly magnetized along the direction of its axis. If the dipoles are Ampere-type, the magnetization is equivalent to a surface bound current Kb=Mϕ^if they are Gilbert-type, the magnetization is equivalent to surface monopole densities σb=±Mat the two ends. Unfortunately, these two configurations produce identical magnetic fields, at exterior points. However, the interior fields are radically different-in the first case Bis in the same general direction as M, whereas in the second it is roughly opposite to M. The applicant proposes to measure this internal field by carving out a small cavity and finding the torque on a tiny compass needle placed inside.

Assuming that the obvious technical difficulties can be overcome, and that the question itself is worthy of study, would you advise funding this experiment? If so, what shape cavity would you recommend? If not, what is wrong with the proposal?

Short Answer

Expert verified

The fields are equal in both the proposed model for spherical, needle and water shaped cavity. Therefore, I advise to found it.

Step by step solution

01

Write the given data from the question.

The radius of the cylinder is R.

The length of the cylinder,L=10R

The magnetic field is B.

The surface bound current is Kb=Mϕ^

The magnetization is M.

02

Determine the formulas to calculate the field expression.

For Ampere’s dipoles

The expression for the field inside the material is given as follows.

B0=μ0M

For Gilbert’s dipoles

The field inside the material is equivalent to the magnetic field at the midpoint between the two-point charges.

B0=0

The expression of field of magnetized sphere is given as follows.

B=23μ0M

03

Calculate the expression for the field.

Calculate the expression for the filed, if the cavity is spherical in the shape.

B=B023μ0M

Substituteμ0M forB0into above equation.

B=μ0M23μ0MB=13μ0M

Therefore, the field inside the spherical cavity is 13μ0M.

Calculate the expression for the filed, if the cavity is needle type in the shape.

B=B0μ0M

Substituteμ0MforB0into above equation.

B=μ0Mμ0MB=0

Therefore, the field inside the needle type cavity is 0.

Calculate the expression for the filed, if the cavity is water shaped.

B=μ0M

Therefore, the field inside the water shaped cavity is μ0M.

Consider the dipole to be Gilberts dipoles.

The field inside the material is equivalent to the magnetic field at the midpoint between the two-point charges.

B0=0

The field at the centre of the cavity, if cavity is spherical in shape.

B=B0+13μ0M

Substitute0forB0into above equation.

B=0+13μ0MB=13μ0M

Therefore, the field inside the spherical cavity is 13μ0M.

The field at the centre of the cavity, if cavity is needle type shape.

B=B0

Substitute0forB0into above equation.

B=0

Therefore, the field inside the needle type cavity is0.

The field at the centre of the cavity, if cavity is water shaped.

B=B0+μ0M

Substitute0forB0into above equation.

B=0+μ0MB=μ0M

Therefore, the field inside the water shaped cavity is μ0M.

Since the fields are equal in both the proposed model for spherical, needle and water shaped cavity. Therefore, I advise to found it.

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Most popular questions from this chapter

Notice the following parallel:

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

Thus, the transcription DB,EH,Pμ0M,ε0μ0,, 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).

Starting from the Lorentz force law, in the form of Eq. 5.16, show that the torque on any steady current distribution (not just a square loop) in a uniform field B is m×B.

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<rR is

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

What is the field outside the sphere?

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?


In Prob. 6.4, you calculated the force on a dipole by "brute force." Here's a more elegant approach. First writeB(r)as a Taylor expansion about the center of the loop:

,B(r)B(r0)+[(rr0)0]B(r0)

Wherer0the position of the dipole and 0is denotes differentiation with respect tor0. Put this into the Lorentz force law (Eq. 5.16) to obtain

.F=IdI×[(r0)B(r0)]

Or, numbering the Cartesian coordinates from 1 to 3:

Fi=Ij,k,l=13εijk{rldlj}[0lBk(r0)],

Where εijk is the Levi-Civita symbol (+1ifijk=123,231, or312; 1ifijk=132, 213, or 321;0otherwise), in terms of which the cross-product can be written (A×B)i=j,k=13εijkAjBk. Use Eq. 1.108 to evaluate the integral. Note that

j=13εijkεljm=δilδkmδimδkl

Whereoil is the Kronecker delta (Prob. 3.52).




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