Embarassingly simple question - Christoffel symbols

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Discussion Overview

The discussion revolves around the definition and sign conventions of Christoffel symbols, particularly focusing on the symmetry properties and the placement of minus signs in their mathematical expressions. Participants explore differences between textbook definitions and a computer program's output, examining implications for calculations in general relativity.

Discussion Character

  • Debate/contested
  • Technical explanation

Main Points Raised

  • One participant states that their computer program (GRTensor II) calculates the Christoffel symbols as symmetric in the first two indices, leading to a specific equation involving partial derivatives.
  • Another participant questions the sign conventions and suggests checking the definitions used in the textbooks.
  • A different participant asserts that most textbooks define the Christoffel symbols as symmetric in the last two indices and indicate that the minus sign should be with the derivative when the first index is involved.
  • One participant expresses concern that their computer program may not align with textbook conventions, implying a potential discrepancy in results.
  • A later reply provides a reference to a document that shows a different ordering of indices for the Christoffel symbols, noting that this differs from the conventions used in some well-known textbooks.
  • Another participant acknowledges that the clarification helps resolve some confusion, but still has concerns about the physics involved.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the correct placement of the minus sign in the definition of the Christoffel symbols. Multiple competing views regarding the definitions and conventions remain present throughout the discussion.

Contextual Notes

There are limitations regarding the assumptions made about the conventions used in different textbooks and the computer program. The discussion highlights the dependency on definitions and the potential for different interpretations of the same mathematical concepts.

pervect
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OK, my computer program (GRTensor II) says that

[tex]\Gamma_{abc}[/tex] is symmetric in the first two indices. Which leads to the equation

[tex]\Gamma_{abc} = \frac{1}{2} ( \frac{\partial g_{bc}}{\partial a}+ \frac{\partial g_{ac}}{\partial b} - \frac{\partial g_{ab}}{\partial c} )[/tex]

And that's exactly what it calculates.

Unfortunately, my textbook seems to insist that the minus sign belongs on the first term above, not the last - but there would be no way for the symbol to be symmetric in the first two indices if that were true. Another text seems to agree with the first.

Right now I'm tempted towards beliving my computer program over the textooks. This gives the result that

[tex]\Gamma_{xtt} = \frac{1}{2} \frac{\partial g_{tt}}{\partial x}[/tex]

which is necessary to get the very simple result that the "forces" on a stationary body are just the gradient of gtt in nearly flat space-time (the Newtonian limit) which Pete mentions.


Does anyone know for sure where the minus sign belongs?
 
Last edited:
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Which textbook?
Did you check the sign-conventions? signature-conventions? and index-placement conventions?
[btw... I think you need, for example, "xa" not "a" in your first expression above.]
 
All textbooks I know define the Christoffel-Symbols in a way that they are symmetric in the last two indices and in that definition the minus-sign should be at the derivative by [tex]x^a[/tex] (when a is the first index as above). Also I´ve never seen any other convention anywhere else.
If your computer program uses another convention for indices I´d bet that it´s because of performace-issues (program might run faster with this method of storing data).

The physical content of both conventions is equivalent as long as other equations are altered accordingly where nessecary.
 
I was afraid of that. I had been assuming that my computer has been spitting out the same style results as the textbook :-(.
 
Sounds to me like your computer is using a different definition of the symbols.
 
ftp://grtensor.phy.queensu.ca/pub/grtensor/doc/grCalc.ps (page c18)
says
Christoffel symbol of the first kind17
[tex]\Gamma_{bca} := \frac{1}{2} \left(g_{ab,c}+g_{ac,b}-g_{cb,a}\right)<br /> \hrule[/tex]
17 Note that this index ordering differs from that of Misner-Thorne-Wheeler. We retain this ordering for consistency with earlier versions of GRTensor.

MTW (p 210), HE (p 40), ExactSolutions (p 45) say
[tex]\Gamma_{abc} := \frac{1}{2} \left(g_{ab,c}+g_{ac,b}-g_{bc,a}\right)<br /> \hrule[/tex]
 
Thanks a lot! This clears up a lot of issues. Now I've only got the physics to wory about.
 

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