How Does Kaluza-Klein Theory Link Electromagnetism and General Relativity in 5D?

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Discussion Overview

The discussion centers on Kaluza-Klein theory, specifically how it connects electromagnetism (EM) and general relativity (GR) within a five-dimensional framework. Participants explore the theoretical underpinnings, mathematical formulations, and implications of this theory, including its covariant treatment of EM and GR, the nature of the fifth dimension, and the role of differential geometry.

Discussion Character

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

Main Points Raised

  • Some participants express confusion about how EM can be integrated into a five-dimensional framework, questioning how electric and magnetic fields can coexist with spacetime dimensions.
  • One participant mentions that Kaluza proposed a 5-metric where the 4-spacetime metric is combined with electromagnetic potentials, but emphasizes the need for the 5-metric to be independent of the 4-coordinate.
  • Another participant discusses the elegance of expressing physical laws in the language of differential geometry and mentions the importance of fiber bundles in understanding Kaluza-Klein theory.
  • Some participants share resources and references, including Wikipedia and academic papers, to aid in understanding the theory and its mathematical framework.
  • There is a mention of the concept of degenerate dimensions and metrics, with participants seeking clarity on how these relate to the spacetime interval and the implications for Kaluza-Klein theory.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the specifics of how Kaluza-Klein theory integrates EM and GR, with various interpretations and levels of understanding expressed. Multiple competing views and uncertainties remain regarding the mathematical and conceptual aspects of the theory.

Contextual Notes

Some participants highlight limitations in their understanding of fiber bundles and differential geometry, indicating that further reading and study may be necessary to fully grasp the concepts discussed. There are also references to specific mathematical formulations that may not be universally understood among participants.

Who May Find This Useful

This discussion may be useful for individuals interested in theoretical physics, particularly those exploring the intersections of electromagnetism and general relativity, as well as students and researchers looking to deepen their understanding of Kaluza-Klein theory and its mathematical foundations.

kleinwolf
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I read only the overview that Kaluza Klein is a 5D theory, in which EM and GR are linked...but can somebody tells me how this is done, since from EM laws, you can, i thought make them covariant by replacing derivatives by covariant ones...(the ones including elements of the metric tensor)...so i think it should be something like : EM energy should be taken into account as itself modifiyng the metric through the GR field equ, but it's not clear (at least for me), how E and B (or the covariant EM tensor), can be put into only one more dimesion...do you know if the corresponding metric in 5D is singular, since I don't understand how you can displace your self in the EM field, which is of another nature than the space-time dimensions...
 
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Kaluza proposed a 5-metric in which the 4-spacetime metric was in the 0-3 part and the electromagnetic vector and scalar potentials were the in the i4 and 4j parts but also in the 0-3 part. The formalism is then the same as for general relativity, but with one dimension more. The action is analogue the Einstein-Hilbert action. However, to get the correct equations for gravity and electromagnetism there must be no dependence of the 5-metric on the 4 coordinate. To explain this Klein proposed the that the 5th dimension was compactified. This is all I can tell you about this. Try pages 13, 14 and 15 of http://arxiv.org/gr-qc/9805018 .
 
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kleinwolf said:
I read only the overview that Kaluza Klein is a 5D theory, in which EM and GR are linked...but can somebody tells me how this is done, since from EM laws, you can, i thought make them covariant by replacing derivatives by covariant ones...(the ones including elements of the metric tensor)...so i think it should be something like : EM energy should be taken into account as itself modifiyng the metric through the GR field equ, but it's not clear (at least for me), how E and B (or the covariant EM tensor), can be put into only one more dimesion...do you know if the corresponding metric in 5D is singular, since I don't understand how you can displace your self in the EM field, which is of another nature than the space-time dimensions...

Read my post (#2) in thread called "Fifth Dimensional physics", in General physics forum, dated 09-29-2005.

Well done hellfire I give you 7 out 10 for your reply.

regards

sam
 
pervect said:
Wikipedia has an exposition - if you understand fibre bundles, that is. (Unfortunately, I don't, at least not yet :-().

http://en.wikipedia.org/wiki/Kaluza-Klein_theory

It took me a while (a matter of years :rolleyes: ) to realize that ALL in physics must be put in the elegant language of differential geometry, that is bundle theory...:rolleyes: But I'm happy i did.:smile:

As for Maxwell's equations in vacuum, the most elegant form form them is

dF=0

and

\delta F=\mu_{0} j

,where d is the space-time Cartan exterior differential and \delta is its adjoint which one can prove it to be a codifferential...

Daniel.
 
dextercioby said:
It took me a while (a matter of years :rolleyes: ) to realize that ALL in physics must be put in the elegant language of differential geometry, that is bundle theory...:rolleyes: But I'm happy i did.:smile:
As for Maxwell's equations in vacuum, the most elegant form form them is
dF=0
and
\delta F=\mu_{0} j
,where d is the space-time Cartan exterior differential and \delta is its adjoint which one can prove it to be a codifferential...
Daniel.

Well, I can understand that much even without fibre bundles, as long as \delta F means d * F, where * is the Hodges dual.

Though frankly I'm more comfortable with covariant derivatives than exterior derivatives.

Unfortunately, I'm not even sure what books/articles I should read if I wanted to understand the Wikipedia article on KK theory (I don't think it would take an extrodinary amount of reading to understand fibre bundles from where I'm at, but I really don't know where to start).

I think there was some stuff on KK theory in MTW at a level I could follow, but I'm not quite sure where it was. Much like the OP, KK theory is on my list of interesting things I want to find out more about sometime.
 
So the extra dimension in KK is a space-like one...but what are degenerate dimension, in a degenerate metric ?...i still have not caught that...because those dimensions do not change the space-time interval on which relativity is based...but it can maybe have influence, because there is one more parameter in the metric elements for example...
 
Although I haven't read through it yet, this looks useful:
http://arxiv.org/abs/hep-ph/9810524
Early History of Gauge Theories and Kaluza-Klein Theories, with a Glance at Recent Developments
Authors: Lochlain O'Raifeartaigh (Dublin Institute for Advanced Studies), Norbert Straumann (University of Zuerich)
Comments: Revised and slightly extended version. Accepted for publication in Reviews of Modern Physics

http://www.iop.org/EJ/abstract/0034-4885/50/9/001
Kaluza-Klein theories
D Bailin et al 1987 Rep. Prog. Phys. 50 1087-1170



I also stumbled upon http://www.vttoth.com/kaluza.htm while googling. I haven't read through it.
 
There is a good chapter in these notes that describes the Kaluza-Klein theory http://www.unine.ch/phys/string/lecturesGR.ps.gz
 
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  • #10
On a flat spacetime manifold where one can choose a metric \eta_{\mu\nu}= \mbox{diag} \left(+1, -1, -1, -1\right)

\delta= \star d \star

Daniel.

P.S. A good survey on differential geometry & the em field on a flat spacetime is found in Bjo/rn Felsager's book: "Geometry, particles and fields".
 

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