Jackson's 6.4 - Uniformly magnetized conducting sphere

In summary, the conversation discusses a problem involving a uniformly magnetized and conducting sphere rotating about its magnetization axis. The first part of the problem involves using Ohm's law and Maxwell's equations to show that the motion of the sphere induces an electric field and a uniform volume charge density in the conductor. The second part of the problem focuses on using symmetry arguments to show that the lowest possible electric multipolarity is quadrupole, and that only a quadrupole field exists outside of the sphere. The solution for this problem involves using special relativity transformations to compute the electric field in the laboratory frame, and a detailed multipole analysis to determine the surface charge distribution.
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leo.
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Homework Statement


A uniformly magnetized and conducting sphere of radius [itex]R[/itex] and total magnetic moment [itex]m = 4\pi MR^3/3[/itex] rotates about its magnetization axis with angular speed [itex]\omega[/itex]. In the steady state no current flows in the conductor. The motion is nonrelativistic; the sphere has no excess charge on it.

(a) By considering Ohm's law in the moving conductor, show that the motion induces an electric field and a uniform volume charge density in the conductor, [itex]\rho = -m\omega /\pi c^2 R^3[/itex].

(b) Because the sphere is electrically neutral, there is no monopole electric field outside. Use symmetry arguments to show that the lowest possible electric multipolarity is quadrupole. Show that only a quadrupole field exists outside and that the quadrupole moment tensor has nonvanishing components, [itex]Q_{33} = -4m\omega R^2/3c^2[/itex], [itex]Q_{11}=Q_{22}=-Q_{33}/2[/itex].

Homework Equations



Ohms Law [itex]\mathbf{J}=\sigma \mathbf{E}[/itex] and Maxwell's equations. If I understood, we are considering a steady current, so that [itex]\nabla \cdot \mathbf{J} = 0[/itex], which reduces to magnetostatics.

The Attempt at a Solution



The first thing I believe is to find the magnetic field due to the magnetization. This is known to be [itex]\mathbf{B}=2\mu_0 \mathbf{M}/3[/itex] on the inside of the sphere. The only thing I don't feel fine with this is that this result was derived for the case of [itex]\mathbf{J} = 0[/itex], using the magnetic scalar potential method. The issue is that this is not the case here. The sphere is rotating, so we have a motion of charges, which would make a nonzero current.

Now, when trying to solve the problem, I must use that [itex]\mathbf{J}=\sigma \mathbf{E}[/itex] to find [itex]\mathbf{E}[/itex] as the problem asks. In that case I must find [itex]\mathbf{J}[/itex]. My thought was that since [itex]\nabla\times \mathbf{B}=\mu_0\mathbf{J}[/itex] we could compute just the curl. But the magnetic field I've found is constant, which gives zero current. Actually, this is not inconsistent, since the result above was derived assuming zero current.

Searching online I've seem people changing frames to the rotating frame of the sphere. In that frame there really is no current, since the points on the sphere are at rest. But the formula for transforming the fields to the rotating frame appear to be non trivial to derive, some of then recurring to special relativity, while at this point in the book, the reader isn't expected yet to use relativity theory.

Other approaches for changing frame seems handwavying to me. One merely says that in the rotating frame there is no magnetic field and that the Lorentz force must match in the two frames, but without much explanation of the details.

In summary, I didn't even find how to get started. What should I do?
 
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  • #2
I found a solution on-line, perhaps the same one that you found, and I've asked for permission from the PF staff to provide you the "link". (Normally under PF rules, homework helpers are not supposed to furnish complete solutions). ## \\ ## That on-line solution uses a relativistic transformation of the fields in a rotating frame. The solution appears to be a good one, and uses Gauss' law to compute the (uniform) charge distribution from the electric field in the laboratory frame, and also computes the surface charge distribution, but the problem and its solution really exceeds the limits of my understanding of E&M. ## \\ ##Perhaps you have already found the "link" that I mentioned above. In any case, I don't see a solution to this without using special relativity transformations. The non-zero electric field is the result of a transformation to get the electric field in the laboratory frame. The electric field is zero in the frame that is rotating with the sphere. ## \\ ## Once he gets the bulk charge density, he computes the surface charge distribution with a detailed multipole analysis that is beyond anything I worked through when we used J.D. Jackson's textbook for a two course E&M sequence in graduate school in 1979. ## \\ ## One thing that is also a puzzle in his solution is, if I understand it correctly, in the laboratory frame, this charge density is stationary even though the object is rotating. The static charge is a result of the static/constant electric field, and is needed to get the resulting electric field (that is non-zero in the laboratory frame) inside the sphere.
 
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Related to Jackson's 6.4 - Uniformly magnetized conducting sphere

What is Jackson's 6.4 - Uniformly magnetized conducting sphere?

Jackson's 6.4 refers to a section in the textbook "Classical Electrodynamics" written by John David Jackson. It discusses the properties and behavior of a conducting sphere that is uniformly magnetized.

What is a conducting sphere?

A conducting sphere is a spherical object made of a material that allows the flow of electric charges, such as metals. This means that the sphere can conduct electricity and can be polarized by an applied electric field.

What does it mean for a conducting sphere to be uniformly magnetized?

A conducting sphere is uniformly magnetized when the magnetic dipole moment is the same at all points on the surface of the sphere. This means that the magnetic field inside and outside the sphere is uniform in all directions.

What are the properties of a uniformly magnetized conducting sphere?

The properties of a uniformly magnetized conducting sphere include a non-zero magnetic dipole moment, a magnetic field that is uniform in all directions both inside and outside the sphere, and the absence of any magnetic charges.

What are the applications of Jackson's 6.4 - Uniformly magnetized conducting sphere?

Jackson's 6.4 has various applications in the fields of materials science, electromagnetism, and geophysics. It can be used to understand the behavior of magnetic materials, design magnetic sensors, and study the Earth's magnetic field and its variations.

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