Magnetization of a material with linear susceptibility

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Discussion Overview

The discussion revolves around the magnetization of a paramagnetic material with linear susceptibility when placed in a uniform magnetic field. Participants explore the relationship between the applied magnetic field and the resulting magnetization density, considering the effects of the material's properties and geometry.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions whether the magnetization density of a highly permeable paramagnetic material will always align with the applied magnetic field, suggesting that the fields created by the material's magnetization may need to be considered.
  • Another participant asserts that for linear materials, the magnetization will align with the applied field, explaining that M, B, and H are related, and boundary conditions should be applied when solving for fields inside and outside the material.
  • A different participant raises a concern about the anisotropic nature of some linear materials, suggesting that the magnetization may only align with the applied field if it is parallel to one of the principal axes of the material.
  • One participant acknowledges the relationship between the internal and external fields, noting that a uniform field inside the material would necessitate changes in the field outside, particularly in the context of designing magnetic shielding.
  • A participant clarifies that "linear" often implies isotropic and homogeneous conditions unless stated otherwise.
  • Another participant describes a specific scenario involving a hollowed cylinder filled with paramagnetic material, noting that while the magnetization aligns with the calculated B-field, it does not align with the applied uniform magnetic field, leading to complications in solving the problem.
  • One participant suggests that solving for magnetostatic fields numerically is feasible and mentions using an iterative method with magnetic scalar potential as a possible approach.

Areas of Agreement / Disagreement

Participants express differing views on the alignment of magnetization with the applied field, particularly in relation to material anisotropy and specific geometries. The discussion remains unresolved regarding the implications of these factors on magnetization behavior.

Contextual Notes

Participants reference specific conditions such as linearity, isotropy, and homogeneity, which may affect the outcomes of their discussions. There are also mentions of the need to solve complex geometries numerically, indicating potential limitations in analytical approaches.

hylander4
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Fairly simple question:

If a highly permeable material (of any shape) is placed in a uniform magnetic field, will the material's magnetization density always line up with the uniform magnetic field, or do I have to take into account the fields that are created as the material becomes magnetized?

The material is paramagnetic.

I've wasted so much time re-reading my E+M textbook to figure this out, but it never seems to tell us how to compute the magnetization created by magnetic fields. We're generally just given objects that are already magnetized.
 
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If the magnetic material is linear, then yes the magnetization will line up with the applied field. That is the definition of linear. For linear materials, M, B, and H are trivially related. So if you find one, then you find all of them. You would solve for the fields separately inside and outside the material as if the material were not even there, but being careful to use the susceptibility of the material inside and the susceptibility of free space outside, then match up the two regions using boundary conditions.

Conceptually, you can think of the applied field as inducing bound net electric currents in the materials that give rise to the magnetization field.

Here is a http://faculty2.uml.edu/cbaird/all_homework_solutions/5magnetic_cylinder.pdf" of an originally unmagnetized cylinder being placed in an originally uniform external magnetic field.
 
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That makes sense. The field inside the paramagnetic material will follow the applied field and thus change the direction/magnitude of the field outside the paramagnetic material.

For some reason I was thinking that a uniform field on the inside of the material would require the field outside the material to stay pointing in the same direction (which I knew was impossible, since I'm actually designing magnetic shielding...and magnetic shielding wouldn't shield if it didn't change field line directions).

Thanks a lot for your help!
 
Yes, I meant the simplest textbook case of a linear, isotropic, homogenous material. But that is a mouthful, so unless otherwise stated, "linear" often implies all of this.
 
I've hit a snag. Using magnetic scalar potential, I calculated the B-field inside a hollowed cylinder filled with linear/isotropic/homogenous paramagnetic metal (there is a shell of known thickness filled with paramagnetic material, and then an empty inner cylinder). The magnetization lines up with the calculated B-field within the material (it has to), but the B-field within the material doesn't line up with the applied uniform magnetic field.

The cylinder inside the paramagnetic shield, which is a vacuum, is the only area where the resulting magnetic field lines up with the applied magnetic field.

This is annoying, because it means that I have to solve the Laplace equation for the exotic shape of the shield I'm actually using, and I'm pretty sure than I can only solve it numerically.
 
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Solving for magnetostatic fields numerically is actually not that bad. If using the magnetic scalar potential, you can use a http://en.wikipedia.org/wiki/Relaxation_%28iterative_method%29" type approach which is fairly easy to implement.
 
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