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Christoffel Symbol |
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| Jun20-12, 07:22 AM | #1 |
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Christoffel Symbol
1. The problem statement, all variables and given/known data
2. Relevant equations 3. The attempt at a solution Does the Christoffel symbol [tex]\Gamma[/tex] have a dimension in physics? And if it does, what is its dimension? Thank you! |
| Jun20-12, 03:26 PM | #2 |
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The Christoffel symbols are arrays of real numbers. They are dimensionless.
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| Jun20-12, 03:38 PM | #3 |
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| Jun20-12, 03:41 PM | #4 |
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Christoffel Symbol
To OP: Can you think of any equation which contains the Christoffel symbols? That should help you answer the question.
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| Jun23-12, 04:58 AM | #5 |
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[tex]\frac{\partial e_i}{\partial U^j} = \Gamma_{ij}^k e_k[/tex] But not really sure is that makes it easier for me. I can certainly think of the derivatives case for the christoffel symbols. I had decided before anyone posted here, that the symbol would have 1/length because of the metric derivatives. But the responses here seem to be... a bit mixed. |
| Jun23-12, 05:17 AM | #6 |
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I am reading that the Rindler Christoffel Symbols are dimensionless.
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| Jun23-12, 05:19 AM | #7 |
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The curvature tensor is made up completely of christoffel symbols, you'd expect that to have a dimension of length.
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| Jun23-12, 08:12 AM | #8 |
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| Jun23-12, 08:27 AM | #9 |
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| Jun23-12, 11:14 AM | #10 |
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[tex]
(\partial_{\nu} \Gamma_\mu - \Gamma_\mu \partial_\nu) - (\partial_{\mu} \Gamma_\nu - \Gamma_\nu \partial_\mu) + \Gamma_\nu \Gamma_\mu - \Gamma_\mu \Gamma_\nu [/tex] Bracketed expressions are the derivatives of connection [tex] \frac{\partial \Gamma_\mu}{\partial x^{\nu}} - \frac{\partial \Gamma_\nu}{\partial x^{\mu}} + \Gamma_\nu \Gamma_\mu - \Gamma_\mu \Gamma_\nu [/tex] I know the first lot of terms from the curvature tensor are zero] [tex]\partial_{\mu}\partial_{\nu} - \partial_{\nu}\partial_{\mu}[/tex] |
| Jun23-12, 11:15 AM | #11 |
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But,you seem to be telling me that the dimensions of the Christoffel symbols are indeed 1/length?
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| Jun23-12, 11:16 AM | #12 |
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| Jun23-12, 12:02 PM | #13 |
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. However, generally the coordinates do not need to have dimension of length (for example, in spherical coordinates where some of the coordinates are angles.) For a given coordinate system it is possible for different Christoffel symbols to have different dimesions. |
| Jun23-12, 03:24 PM | #14 |
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Also, since the Christoffel symbols have dimension 1/length, the curvature tensor has dimensions 1/(length^2). This is exactly what you'd expect. Consider the Gaussian curvature of a 2D surface - it is the product of the two principle curvatures. Since each principle curvature is equal to 1/(radius of curvature), the Gaussian curvature has dimensions 1/(length^2).
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| Jun23-12, 08:25 PM | #15 |
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| Jun24-12, 12:33 AM | #16 |
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Look here to see some explicit examples of Christoffel symbols and curvature tensor components:
http://onlinelibrary.wiley.com/doi/1...2061.app12/pdf For example, if you use spherical coordinates in flat spacetime you can see that some of the Christoffel symbols have dimension 1/length while others are dimensionless (see equations L.14). All the curvature tensor components are zero in this case because the spacetime is flat. For the Schwarzchild metric, again you find some of the Christoffel symbols have dimesion 1/length while others are dimensionless (see equations L.21). Some components of the curvature tensor have dimension 1/length^2, while others are dimensionless (see equations L.22). [The symbol m in these expressions has the dimension of length.] |
| Jun24-12, 06:41 AM | #17 |
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ty very much
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