What Would a Magnetic Field Look Like in 4+1D Space?

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Discussion Overview

The discussion centers around the nature of magnetic fields in a hypothetical 4+1 dimensional space, exploring how the concepts of magnetism and electromagnetic fields might be represented in higher dimensions. Participants examine the implications of dimensionality on the representation of magnetic fields, particularly in relation to established theories in 3+1 dimensions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions how a magnetic field would be represented in 4+1 dimensions, suggesting that traditional field lines may not apply and proposing the idea of "planes" of force instead.
  • Another participant introduces the covariant formulation of electrodynamics, explaining that the electromagnetic field can be represented as a two-index antisymmetric tensor and can be generalized to arbitrary dimensions.
  • It is noted that in 3+1 dimensions, the magnetic field can be represented as a vector due to the special properties of that dimensionality, but this representation does not hold in higher dimensions.
  • A participant asks whether the 3+1D pseudovector for magnetism points along the magnetic field lines or the axis around which they curl, expressing confusion about the relationship between pseudovectors and bivectors.
  • Clarifications are made regarding the definitions of field lines and their relationship to the magnetic vector, with one participant stating that field lines are defined as the trajectories of the vector.
  • Another participant reflects on their understanding of tensors, suggesting that they now see tensors as higher-dimensional analogs of vectors and expressing a desire to revisit concepts like Clifford algebra.

Areas of Agreement / Disagreement

Participants express varying levels of understanding and confusion regarding the representation of magnetic fields in higher dimensions, with some agreeing on the nature of pseudovectors while others remain uncertain about specific relationships and definitions. The discussion does not reach a consensus on how to fully conceptualize magnetic fields in 4+1 dimensions.

Contextual Notes

Participants express uncertainty about the definitions and relationships between vectors, pseudovectors, and tensors, particularly in the context of higher dimensions. There are unresolved questions about the implications of these concepts for understanding magnetic fields in 4+1 dimensions.

granpa
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what would a magnetic field look like in 4+1D?

In 3+1D the field lines simply rotate around the axis which points along the direction of motion of the electron. But in 4+1D this is not defined. But if magnetism is simply a result of relativity then there should be a way to make the equations work in 4+1D.

Surely someone somewhere must have worked this out by now.

maybe instead of 'lines' of force one would instead use 'planes' of force??
 
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The answer can be best seen from the covariant formulation of electrodynamics. The electromagnetic field is represented as a two index antisymmetric tensor, called the field-strength tensor. Electrodynamics can be readily generalized to arbitrary dimensions in this formulation.
The point is that 3+1 D is so special that the magnetic field can be represented as a vector. The point is that if we look at how the magnetic field is situated in the field strength tensor (in 3+1 for now) we see that it is an antisymmetric tensor itself.
Now there is a theorem in linear algebra relating antisymmetric tensors, called the Hodge-dualism (of course there is more to this). And it so happens that there in 3D there is a one to one correspondence between a two index antisymmetric tensor and a axial vector (this has to do with why there is such a thing as a vector product in 3D, a vector product can also be defined in 7D, the reasons of these are even deeper and related to Clifford algebras.). Hence the magnetic field which is actually not a vector can be *represented* as a vector in 3+1. So in extra dimensions we cannot imagine it as a vector.
 
so its a psuedovector? (in 3+1D)
 
Yep, It's a pseudo vector.
 
Pardon my stupidity, but the 3+1D psuedovector for magnetism,
does it point in the direction of the magnetic field lines or
does it point along the axis that the magnetic field lines curl around
(i.e. the direction of motion of the electron)

edit:This is seeming more and more like a really dumb quesion. I am sure it must be pointing along the magnetic field lines. But my thinking is that a bivector is also a pseudovector and the magnetic field lines 'curl' or rotate around the axis. In 4D rotation is also a bivector. I'm probably just confusing myself here.

no wait, a bivector is a tensor but rotation in 4D reduces to a psuedovector in 3D.
I hate tensors.
 
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So by "field lines" you mean you mean the lines of the electric field?
 
I was thinking magnetic field lines.

see my edited post below
 
The field lines are by definition the trajectories of the vector. i.e. the magnetic vector is tangent to the magnetic field line by definition, similarly for the electric part.
 
Ok. Thank you. You've answered by question.
In higher dimensions its a tensor.
 
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This whole line of reasoning has made me think about tensors in a new light.
Tensors have always been mysterious to me but I think I understand them better now.
If a vector is a one dimensional line in a higher dimensional space then a tensor (like a bivector) would be a plane or manifold in a higher dimensional space.
Maybe I should look into clifford algebra again.
 

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