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.

Short Answer

Expert verified

There exists a spherical surface of radius μ0m02πB03, centered at the origin, through which no magnetic field lines pass.

Step by step solution

01

Given data

There is an magnetic dipole m=-m0z^ is situated at the origin, in an uniform magnetic field B=B0z^.

02

Magnetic field due to a dipole

The magnetic field due to a magnetic dipole m is

localid="1658559878707" Bdip=μ0m4π3r[2cosθr^+sinθθ^]

Here, μ0 is the permeability of free space.

03

Net magnetic field near origin

From equation (1), the net magnetic field near the origin is,

B=B0z^+Bdip=B0z^-μ0m04πr32c0sθr^+sinθθ^

The radial component of this field is,

B.r^=B0cosθ-μ0m04πr32cosθ=B0-μ0m02πr3cosθ

Thus, the net field is zero for any value of θ at radius R where

localid="1657777042303" B0-μ0m02πR3=0R=μ0m02πB33

The field lines are shown in the following figure


Thus, the magnetic field lines are absent in the sphere of radiusμ0m02πB33 .

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Most popular questions from this chapter

Suppose you have two infinite straight line chargesλ, a distance d apart, moving along at a constant speed υ(Fig. 5.26). How great would have tobe in order for the magnetic attraction to balance the electrical repulsion? Work out the actual number. Is this a reasonable sort of speed?

Consider the motion of a particle with mass m and electric charge qein the field of a (hypothetical) stationary magnetic monopole qmat the origin:

B=μ04qmr2r^

(a) Find the acceleration of qe, expressing your answer in terms of localid="1657533955352" q, qm, m, r (the position of the particle), and v(its velocity).

(b) Show that the speed v=|v|is a constant of the motion.

(c) Show that the vector quantity

Q=m(r×v)-μ0qeqm4πr^

is a constant of the motion. [Hint: differentiate it with respect to time, and prove-using the equation of motion from (a)-that the derivative is zero.]

(d) Choosing spherical coordinates localid="1657534066650" (r,θ,ϕ), with the polar (z) axis along Q,

(i) calculate , localid="1657533121591" Qϕ^and show that θis a constant of the motion (so qemoves on the surface of a cone-something Poincare first discovered in 1896)24;

(ii) calculate Qr^, and show that the magnitude of Qis

Q=μ04π|qeqmcosθ|;

(iii) calculate Qθ^, show that

dt=kr2,

and determine the constant k .

(e) By expressing v2in spherical coordinates, obtain the equation for the trajectory, in the form

drdϕ=f(r)

(that is: determine the function )f(r)).

(t) Solve this equation for .r(ϕ)

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)?

In calculating the current enclosed by an Amperian loop, one must,in general, evaluate an integral of the form

Ienc=sJda

The trouble is, there are infinitely many surfaces that share the same boundary line. Which one are we supposed to use?

I worked out the multipole expansion for the vector potential of a line current because that's the most common type, and in some respects the easiest to handle. For a volume current J:

(a) Write down the multipole expansion, analogous to Eq. 5.80.

(b) Write down the monopole potential, and prove that it vanishes.

(c) Using Eqs. 1.107 and 5.86, show that the dipole moment can be written

m=12(r×J)dτ

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