Conditions on Christoffel Symbols?

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Homework Help Overview

The discussion revolves around the geodesic equation in the context of general relativity, specifically focusing on the conditions imposed on the Christoffel symbols, ##\Gamma^\mu~_{\alpha \beta}##, when the metric is expressed in a certain form. Participants are exploring how these conditions relate to the metric given by ##ds^2 = -c^2dt^2 +g_{ij}dx^idx^j##.

Discussion Character

  • Conceptual clarification, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants are attempting to understand how to demonstrate that the specified metric satisfies the conditions on the Christoffel symbols. Questions arise regarding the implications of setting ##x^i = constant## and the resulting differential changes.

Discussion Status

The discussion is active, with participants questioning the nature of the problem and the steps needed to show the relationship between the metric and the Christoffel symbols. There is a focus on clarifying terminology and concepts related to the metric and its components.

Contextual Notes

Participants are navigating potential ambiguities in the problem statement and the implications of the conditions on the Christoffel symbols. There is a noted emphasis on understanding the definitions and roles of the metric components in the context of the geodesic equation.

unscientific
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Homework Statement



Write down the geodesic equation. For ##x^0 = c\tau## and ##x^i = constant##, find the condition on the christoffel symbols ##\Gamma^\mu~_{\alpha \beta}##. Show these conditions always work when the metric is of the form ##ds^2 = -c^2dt^2 +g_{ij}dx^idx^j##.

Homework Equations

The Attempt at a Solution



The geodesic equation is:
\frac{d^2x^\mu}{d\tau^2} + \Gamma^\mu~_{\alpha \beta} \frac{dx^\alpha}{d\tau} \frac{dx^\beta}{d\tau}

Using the condition given
\Gamma^0~_{\alpha \beta} \frac{dx^\alpha}{d\tau} \frac{dx^\beta}{d\tau} = 0
\Gamma^0~_{00} = \Gamma^i~_{00} = 0

How do I show the metric is of the form ##ds^2 = -c^2dt^2 +g_{ij}dx^idx^j##?
 
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unscientific said:
How do I show the metric is of the form ##ds^2 = -c^2dt^2 +g_{ij}dx^idx^j##?
But is that the question? Aren't you simply being asked to show that such a metric does satisfy those conditions on ##\Gamma## ?
 
strangerep said:
But is that the question? Aren't you simply being asked to show that such a metric does satisfy those conditions on ##\Gamma## ?

If ##x^i = constant##, then wouldn't ##dx^i = 0##?
 
unscientific said:
If ##x^i = constant##, then wouldn't ##dx^i = 0##?
Yes, but I'm puzzled why you replied to my question this way. Just write the formula for the Chrisoffel symbols, and substitute the metric components that appear in the given line element ##ds^2##.
 
strangerep said:
Yes, but I'm puzzled why you replied to my question this way. Just write the formula for the Chrisoffel symbols, and substitute the metric components that appear in the given line element ##ds^2##.

What do you mean by "substitute the metric components that appear in the given line element ##ds^2##"?
 
unscientific said:
What do you mean by "substitute the metric components that appear in the given line element ##ds^2##"?
Which part of my sentence are you having trouble with? The word "substitute"? The word "metric"? The concept of metric components appearing a line element?

If the last one, then read this Wiki page.
 

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