Fun Magnetic Scalar Potential Problem

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SUMMARY

The discussion centers on solving a magnetic scalar potential problem involving two cylindrical shells, where the outer shell has a radius of b and the inner shell has a radius of a, with a paramagnetic material filling the space between them. The magnetic field is determined using the equations H = B/(μ₀) + M and H = -grad W, alongside the cylindrical Laplace equation for the magnetic scalar potential W. The user struggles with boundary conditions and the need for a function for the magnetization density M to find the H-field, ultimately seeking general guidance rather than a complete solution.

PREREQUISITES
  • Understanding of magnetic scalar potential and its applications
  • Familiarity with cylindrical coordinates and Laplace's equation
  • Knowledge of magnetic fields and paramagnetic materials
  • Proficiency in vector calculus, particularly gradient and divergence operations
NEXT STEPS
  • Study the derivation and application of the cylindrical Laplace equation in electromagnetism
  • Explore the relationship between magnetization density M and magnetic field H in paramagnetic materials
  • Learn about boundary conditions in electromagnetic problems and their implications
  • Investigate numerical methods for solving complex boundary value problems in electromagnetism
USEFUL FOR

Students and professionals in physics and engineering, particularly those focusing on electromagnetism, magnetic materials, and boundary value problems in cylindrical geometries.

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"Fun" Magnetic Scalar Potential Problem

Homework Statement



An infinite cylindrical shell of radius b is placed inside a constant field B which points along the upwards z-axis. A second cylindrical shell of radius a<b is placed inside the first cylindrical shell, and the volume from b>r>a is filled with a paramagnetic material of permeability u. Find the magnetic field everywhere.

Homework Equations



H = B/(u_0) + M

H = -grad W

Laplacian W = -grad M

W is continuous over all boundaries.
The change in dW/dr over a boundary is equal to the negative change in Magnetization over the boundary.

Cylindrical laplace equation solution (From my undergraduate E+M notebook)

W(r, phi) = D_0 + A_0*(a+b*phi) +
$\EPSILON$ [r^n + (A_n*r^-n)]*[B_n*cos(n*phi)+C_n*sin(n*phi)]

Another version of this equation can be found here http://www.cord.edu/faculty/gealy/physics315/SepVarsCyl.pdf" on page two.

Summed from n = 1 to infinity


The Attempt at a Solution



Since there's no free current in this situation, I tried using magnetic scalar potential to solve this problem. Unfortunately, I end up with too many variable in the proposed Laplace equation solutions that I need to create to use the boundary conditions.

In my main attempt I had four boundary conditions and seven types of variables.

My main problem is that I need to find the H field to find the B-field, but in order to find the H-field, I also need a function for the paramagnetic material's Magnetization density M.

The forum wants me to post my attempts, but I've already filled three pages of notebook paper with failed algebra and I doubt that that would be constructive. I'm not really looking for an exact solution, I really just need general guidance.
 
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Usually you have B = μ0 (H + M) = μ0 μ H, which determines M to be (μ-1) H. In vacuum, of course, μ = 1.
 

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