How do I determine the direction of M and H in a homogeneous cylinder?

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    Ampere's law Law
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Homework Help Overview

The discussion revolves around understanding the H-field and magnetization (M) in the context of a homogeneous cylinder with a current running along its axis. Participants are exploring the relationships between H, M, and the magnetic field B, particularly in scenarios where the current is zero or when considering the implications of Ampère's law.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants are questioning how to determine the direction of H and M, particularly in relation to the geometry of the cylinder and the nature of the magnetic fields involved. They are considering the implications of having a constant H-field and the conditions under which this holds true.

Discussion Status

The discussion is ongoing, with participants providing insights into the conditions affecting the direction of H and M. Some have suggested that the context and medium play significant roles in determining these directions, while others are exploring specific examples to clarify their understanding.

Contextual Notes

There is a focus on the assumption of a homogeneous magnetization and the implications of having no bound volume currents. Participants are also considering the relationship between the directions of K and M, and how this affects the overall understanding of the magnetic fields in the cylinder.

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Homework Statement


Hi all.

I'm trying to understand the H-field. From Ampére's law we have:

[tex]\oint {{\bf{H}} \cdot {\rm{d}}{\bf{l}}} = I_{free,enclosed}[/tex]

If I look at an object with zero free, enclosed current, the integral equals zero. The integral can be equal to zero even if H is not zero. But if the integral equals zero and if H is constant and parallel to dl, I can take it outside the integral, and hence H=0.

My question is: How do I know if H is in the same direction as dl and constant in magnitude?
 
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It will depend on the context. What kind of situations can you think of that would have a constant field of H? Generally, they will be infinite (or limits/approximations), right? Whether or not it is in the direction of your infinitesimal line element will depend on how you choose your amperian loop. Also, what kind of medium you are in could come into play if you are talking about H.
 
What about the magnitization M?

If we look at a cylinder, where a current I runs in the axis of the cylinder (z-axis), we can find B by the right-hand rule. Is there any way to find M?
 
Well yes, depending on what information you know about the current you could find the magnetization.

You know that in general that
[tex]\mathbf{J_b}=\nabla \times \mathbf{M}[/tex]

where you could use stoke's theorem to get the magnetization. There are a bunch of other relations you could potentially use. Again, it will depend on context.
 
I hope it's OK if we take an example. Let's say, for instance, that the magnetization of a cylinder is homogeneous so there are no bound volume currents. I am told that

[tex]\textbf K_b=K\hat{\phi}[/tex]

In this example, the direction of B is along the axis of the cylinder (right-hand rule). How would I be able to find the direction of M, and thereby H?

I know that K and M are perpendicular to each other (cross-product), but this means that M can either be in the phi-direction or z-direction?
 

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