I have question about Maxwell's 2nd equation

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Discussion Overview

The discussion revolves around Maxwell's second equation, specifically the implications of ∇⋅B = 0 and whether ∇⋅H can be non-zero in anisotropic media. Participants explore the relationship between magnetic fields, magnetic monopoles, and the properties of magnetic polarization and current.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant questions if ∇⋅H can be non-zero, suggesting that if it can, it might indicate the existence of magnetic monopoles due to a perceived similarity between magnetic polarization and current.
  • Another participant asserts that ∇⋅H can indeed be non-zero in anisotropic or non-homogeneous materials, but challenges the idea that this implies the existence of magnetic monopoles, stating that a monopole would be a source for B.
  • Confusion arises regarding the distinction between B and H fields, with one participant expressing difficulty in understanding why ∇⋅H can be non-zero while ∇⋅B cannot.
  • Some participants clarify that the absence of a source term in ∇⋅B = 0 indicates there are no magnetic monopoles, while the non-zero divergence of H relates to magnetization sources.
  • One participant prefers an intuitive understanding of Gauss's law, emphasizing that magnetic field lines are loops and that B cannot exist without H, referencing the behavior of magnetized materials.
  • Another participant attempts to correct a misunderstanding about the notation used in Maxwell's equations, suggesting a need for clarity between the nabla operator and the Laplace operator.
  • Multiple participants correct the notion that the Laplace operator is relevant in this context, emphasizing that the original notation is appropriate.

Areas of Agreement / Disagreement

Participants express differing views on the implications of ∇⋅H being non-zero, with some asserting it indicates magnetic monopoles while others refute this idea. There is no consensus on the interpretation of the relationship between B and H fields or the implications of the divergence of H.

Contextual Notes

Some participants exhibit confusion regarding the mathematical notation and its implications, particularly the distinction between the nabla operator and the Laplace operator. The discussion also highlights the complexity of the relationship between magnetic fields and the conditions under which they operate.

yang hg
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2nd maxwell's equation is ∇⋅B = 0. Then Can ∇⋅H be non-zero? I know that there is anisotropic media regarding permeability. If ∇⋅H can be non-zero in anisotropic media, I think it show that there is magnetic monopole because I think magnetic polarization and current is same essentially. Is this idea correct? If not, teach me what is wrong. thanks in advance.^^
 
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yang hg said:
Can ∇⋅H be non-zero?
Yes. If the material is not isotropic or homogeneous.

yang hg said:
If ∇⋅H can be non-zero in anisotropic media, I think it show that there is magnetic monopole because I think magnetic polarization and current is same essentially. Is this idea correct?
No. A magnetic monopole would be a source for ##\vec B##.
 
Orodruin said:
No. A magnetic monopole would be a source for →BB→\vec B.
maxwell's second equation imply there is no magnetic monopole. But you tell me monopole is source for B. It is contradiction.​
And I cannot understand that ∇⋅H can be non-zero. I'm confused B with H. What makes B and H have this different property? Plz help me.
 
yang hg said:
maxwell's second equation imply there is no magnetic monopole. But you tell me monopole is source for B. It is contradiction.
No, it is not. It is precisely the fact that there is no source on the right-hand side of ##\nabla \cdot \vec B = 0## that tells you there is no monopole. A monopole by definition would mean that the right-hand side would be non-zero.
 
Orodruin said:
No, it is not. It is precisely the fact that there is no source on the right-hand side of ##\nabla \cdot \vec B = 0## that tells you there is no monopole. A monopole by definition would mean that the right-hand side would be non-zero.
I get it. Then what is meaning of ∇⋅H ≠ 0? ie. if ∇⋅H = 1, what is physics meaning of 1?
 
That would be dimensionally inconsistent.

Since ##\vec H = \vec B/\mu_0 - \vec M##, ##\nabla \cdot \vec H = - \nabla \cdot \vec M##. The right-hand side would therefore be a source of magnetisation.
 
From an intuitive understanding perspective I prefer the integral form.

The way I understand gauss's law is this: (quite possible that it is wrong lol)

Integral of B over a closed surface S = 0. Ie Magnetic field lines are loops, if field leaves the surface it must come back in somewhere, then, B cannot exist without H. If considering something that is pre magnetized (as in above), then the little unpaired electrons in that magnetized material are producing the H to create B given the reluctance path of the magnetic loop (that's where load lines come in for designing with permanent magnets). Ie the M in the equation above is actually Br/u (where Br = remnant flux density).

So far as I know we have not ever identified a magnetic mono pole, so therefore integral of B or H over a closed surface = 0.
 
yang hg said:
2nd maxwell's equation is ∇⋅B = 0. Then Can ∇⋅H be non-zero? I know that there is anisotropic media regarding permeability. If ∇⋅H can be non-zero in anisotropic media, I think it show that there is magnetic monopole because I think magnetic polarization and current is same essentially. Is this idea correct? If not, teach me what is wrong. thanks in advance.^^

You have everything correct but need to have delta right side up ∆. I am sorry that Maxwell made an error as is should be it Laplace operator right side up. So by cubing the H you can make correct calculations. I am not trying to make this up you can try it if you like. I can only tell you what I know.
 
Last edited:
snowflakesarepowder said:
You have everything correct but need to have delta right side up ∆
No, this is incorrect. There is a difference between ##\nabla## and the Laplace operator ##\Delta##.
 

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