Christoffel symbols in differential geometry

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SUMMARY

This discussion focuses on the application and understanding of Christoffel symbols in differential geometry, specifically in the context of covariant derivatives. The participant clarifies the use of the product rule when dealing with multiple terms and highlights the significance of index notation, including the distinction between raised and lowered indices. Key equations provided include the covariant derivative expressions for tensors with raised and lowered indices, emphasizing the role of Christoffel symbols in these calculations.

PREREQUISITES
  • Understanding of covariant derivatives in differential geometry
  • Familiarity with tensor notation and operations
  • Knowledge of the product rule in calculus
  • Proficiency in manipulating indices in mathematical expressions
NEXT STEPS
  • Study the properties of Christoffel symbols in Riemannian geometry
  • Learn about the implications of index raising and lowering in tensor calculus
  • Explore the derivation of the covariant derivative formulas for various tensor types
  • Investigate the significance of dummy indices in tensor operations
USEFUL FOR

Students and researchers in mathematics and physics, particularly those specializing in differential geometry and general relativity, will benefit from this discussion on Christoffel symbols and their applications in covariant derivatives.

effy21
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Homework Statement


I'm having trouble figuring out how to use Christoffel symbols. Apart from the first three terms here, I can't understand what's going on between line 3 and 4. What formulas/definitions are being used? How do you find the product of two chirstoffel symbols? Where are all the minuses coming from?
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Homework Equations


VLSVKobSFLG6CNltthQb03nUqT8fKtKsJzs5Twvot-3WhcWjseaKRZ3DlMLGKQehHFAqfkOi_BemWY2MFoq3zTIXJoQy0cAA.png

The Attempt at a Solution


It looks like the product rule is needed when three terms are multiplied together. The indices p and l seem to be interchangeable.
 
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The reason for the minus sign is because there are two different rules for covariant derivatives, depending on whether the index is raised or lowered. I'm less comfortable with the comma and semi-colon notation, so let me use the notation I'm familiar with:

\nabla_i A^j = \partial_i A^j + \Gamma^j_{i k} A^k

where I'm using \nabla_i X to mean what you would write X_{; i} and \partial_i to mean what you would write X_{, i}

For tensors with lowered indices, you get a minus sign:

\nabla_i A_j = \partial_i A_j - \Gamma^k_{i j} A_k

For tensors with both kinds of indices, you get some minus signs and some plus signs:

\nabla_i A^{j}_{k} = \partial_i A^j_k + \Gamma^j_{i m} A^m_k - \Gamma^l_{i k} A^j_l

One other thing you have to remember is that in an expression such as \Gamma^j_{ik} A^k, the repeated index, k is a "dummy index", which means that you can just as well write it as \Gamma^j_{ip} A^p, or using any other symbol. What's important, though, is that you have to choose the "dummy" index so that it doesn't clash with any other index. So you can't choose i or j.
 
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