Fiber bundles and the fiber for Electromagnetism.

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Discussion Overview

The discussion revolves around the concept of using a circle as the fiber over Minkowski spacetime to understand electromagnetism, particularly in relation to the classical vector potential. Participants explore the mathematical representation of this idea and its implications for electric and magnetic fields.

Discussion Character

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

Main Points Raised

  • One participant proposes that the circle can represent the fiber over Minkowski spacetime for electromagnetism, suggesting that a 3-dimensional surface in C_1XMinkowski space could encode the physics of the classical vector potential, A_μ.
  • There is a discussion about defining kinetic energy at a point in space and time as proportional to θ(X,t), with potential energy involving the divergence and curl of θ(X,t).
  • Some participants question the mathematical operations involved, such as whether ∇θ(X,t),t is a vector and the validity of taking the curl of a scalar.
  • Another participant suggests that if θ(X,t) represents the position along the circle, a vector F(X,t) may be needed to describe the movement of the surface in space, potentially leading to a representation of A_μ.
  • There are repeated inquiries about whether θ(X,t) can be considered fundamental and if various differential operations on it can yield the four components A(X,t)_μ.
  • One participant introduces the idea that distorting the surface could store energy, which might transform as a four-vector, linking it to the physics of electromagnetism.

Areas of Agreement / Disagreement

Participants express uncertainty and engage in debate regarding the mathematical framework and physical implications of their proposals. No consensus is reached on the validity of the ideas presented.

Contextual Notes

Participants acknowledge limitations in their mathematical precision and express confusion over the operations involving θ(X,t) and the implications for electric and magnetic fields.

Spinnor
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The circle is the fiber over Minkowski spacetime for electromagnetism?

I want to make connection to the classical vector potential via some " picture" involving this circle. Does the following come close?

Can I consider a 3 dimensional surface in C_1XMinkowski space that at a given slice of time has position in the circle dimension of θ(X,t)? Obviously a different observer would see a Lorentz transformed θ(X,t) --> θ'(X',t')

Given the right properties could this surface encode the physics of the classical vector potential, A_μ?

I am thinking we could define kinetic energy at X and time t as being proportional to θ(X,t),t? The potential energy would have parts from the divergence of θ(X,t), ∇°θ(X,t) and the curl of θ(X,t), ∇Xθ(X,t)?

So The electric field goes as something like ∇°θ(X,t) + θ(X,t),tEdit, we need a vector above and θ(X,t),t is not a vector. Damn!

2nd edit, ∇θ(X,t),t is a vector, does that work?

3rd edit, we can't take the curl of a scaler, ∇Xθ(X,t)?

And the magnetic field goes like ∇Xθ(X,t)?

How do you simply get electromagnetism from the circle?

Mathematics is a very precise language and I apologize for not being more precise.

Thanks for any help!
 
Last edited:
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So to recap, can we take θ(X,t) as fundamental and by various differential operations to θ(X,t) get the four components A(X,t)_μ?

Thanks for any help!
 
Please kill this thread 8^(
 
Spinnor said:
So to recap, can we take θ(X,t) as fundamental and by various differential operations to θ(X,t) get the four components A(X,t)_μ?

Thanks for any help!

This thread should be killed, and the above is false?
 
Spinnor said:
So to recap, can we take θ(X,t) as fundamental and by various differential operations to θ(X,t) get the four components A(X,t)_μ?

Thanks for any help!

If θ(X,t) were the position of an element of the surface along the circle we might also need a vector to map the possible movement of the surface in space? If the surface were "pushed" at two points in opposite directions, in the circle direction then, with the surface having the right physics, we would get a flow of the surface which could be represented by a vector, F(X,t)?

Then F(X,t) and θ(X,t) might after proper manipulation give us something like A_μ?

Kill this thread.
 
Spinnor said:
If θ(X,t) were the position of an element of the surface along the circle we might also need a vector to map the possible movement of the surface in space? If the surface were "pushed" at two points in opposite directions, in the circle direction then, with the surface having the right physics, we would get a flow of the surface which could be represented by a vector, F(X,t)?

Then F(X,t) and θ(X,t) might after proper manipulation give us something like A_μ?

Kill this thread.

Do we get the electric field goes like ∇°θ(X,t) + F(X,t),t
Magnetic field goes like ∇XF(X,t) ?
 
Spinnor said:
Do we get the electric field goes like ∇°θ(X,t) + F(X,t),t
Magnetic field goes like ∇XF(X,t) ?

I see flow going to zero in the plane whose points are equidistant from the opposite forces, even as the forces in the circle direction change with time. We need some other F, %^(
 
If we use forces to distort the surface in the top post we store energy in the surface. If we now move past this distorted surface, the stored energy in the distorted surface now transforms as a four-vector and we see both energy and momentum? So it now seems to me that there should be a function θ(X,t) that describes the "shape" of the surface as a function of space and time that encodes all the physics of something like A_μ? If we apply a force at one point of the surface that is like charge? If the force moves that is like current? The surface above with the right physics will act like the electromagnetic field?

Thanks for any help!
 

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