Understanding Metric Connection and Geodesic Equations in General Relativity"

Mr-R
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Dear all,

In my journey through learning General relativity. I have stumbled upon this problem. I have to calculate the geodesic equation for R^{3} in cylindrical polars. I am not sure how to use the metric connection. The indices confuse me. I would appreciate it if someone could shade some light on it. Every time I try to calculate it I get zero, sometimes due to the first metric tensor and sometime the terms in the parentheses are zeros.

\Gamma_{bc}^{a}=\frac{1}{2}g^{ad}(\partial_{b}g_{dc}+\partial_{c}g_{db}-\partial_{d}g_{bc})

As I understand it, the index d is the dummy index and runs from 1 to 3 in this case, right? What about b and c? how do I use them?

Thanks in advance
 
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Mr-R said:
As I understand it, the index d is the dummy index and runs from 1 to 3 in this case, right? What about b and c?

Yes and a, b and c can be 1, 2 or 3 giving 27 gamma's.

Mr-R said:
I am not sure how to use the metric connection. The indices confuse me.

You have to calculate all the gamma's, but a lot of them are equals or vanish.

Mr-R said:
Every time I try to calculate it I get zero, sometimes due to the first metric tensor and sometime the terms in the parentheses are zeros.

\Gamma_{bc}^{a}=\frac{1}{2}g^{ad}(\partial_{b}g_{dc}+\partial_{c}g_{db}-\partial_{d}g_{bc})

What did you find for the metric in these coordinates?
 
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I actually got it now :smile:

Thanks bloby
 
Ok, you're welcome.
 
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