Undergrad Manipulating Christoffel Symbols: Questions & Answers

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SUMMARY

This discussion focuses on the manipulation of Christoffel symbols in the context of partial derivatives within general relativity. Participants clarify that the expression ##(\partial_\rho \Gamma^{\mu}_{\sigma\nu}) U^{\nu}## allows for the contravariant vector ##U^{\nu}## to be moved freely due to the nature of the partial derivative acting solely on the Christoffel symbol. The discussion references a specific example from the website Einstein Relatively Easy, which illustrates the relationship between Christoffel symbols and the derivatives of basis vectors.

PREREQUISITES
  • Understanding of Christoffel symbols in differential geometry
  • Familiarity with partial derivatives in tensor calculus
  • Knowledge of contravariant and covariant vectors
  • Basic principles of general relativity
NEXT STEPS
  • Study the properties of Christoffel symbols in Riemannian geometry
  • Learn about the Levi-Civita connection and its applications
  • Explore the derivation and implications of the Riemann curvature tensor
  • Investigate the role of basis vectors in tensor analysis
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Mathematicians, physicists, and students of general relativity who seek to deepen their understanding of tensor calculus and the manipulation of Christoffel symbols in theoretical frameworks.

whatisreality
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I have a couple of questions about how Christoffel symbols work. Why can they just be moved inside the partial derivative, as shown just beneath the first blue box here: https://einsteinrelativelyeasy.com/index.php/general-relativity/61-the-riemann-curvature-tensor

And if you had the partial derivative:
##(\partial _{\rho} \Gamma^{\mu}_{\sigma\nu}) U^{\nu}##
Where ##U^{\nu}## is any contravariant vector, does this commute? Could I just move the ##U^{\nu}## from the right of the bracket to the left of the bracket?
 
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whatisreality said:
I have a couple of questions about how Christoffel symbols work. Why can they just be moved inside the partial derivative, as shown just beneath the first blue box here: https://einsteinrelativelyeasy.com/index.php/general-relativity/61-the-riemann-curvature-tensor
The first blue box reads
$$
\Gamma_{\alpha\beta}^\gamma \vec e_\gamma = \frac{\partial \vec e_\beta}{\partial x^\alpha}.
$$
What do you mean by "just be moved inside the partial derivative"? There is no partial derivative on the left-hand side where the Christoffel symbol appears.

whatisreality said:
And if you had the partial derivative:
##(\partial _{\rho} \Gamma^{\mu}_{\sigma\nu}) U^{\nu}##
Where ##U^{\nu}## is any contravariant vector, does this commute? Could I just move the ##U^{\nu}## from the right of the bracket to the left of the bracket?

The partial derivative in this case acts only on the Christoffel symbol and ##(\partial_\rho \Gamma^\mu_{\sigma \nu})## should be treated as a number. You can freely move the ##U^\nu## around it.
 
Orodruin said:
The first blue box reads
$$
\Gamma_{\alpha\beta}^\gamma \vec e_\gamma = \frac{\partial \vec e_\beta}{\partial x^\alpha}.
$$
What do you mean by "just be moved inside the partial derivative"? There is no partial derivative on the left-hand side where the Christoffel symbol appears.
The partial derivative in this case acts only on the Christoffel symbol and ##(\partial_\rho \Gamma^\mu_{\sigma \nu})## should be treated as a number. You can freely move the ##U^\nu## around it.
But in the line directly beneath that box, it looks to me like the christoffel symbol got moved inside the partial derivative. That might not actually be what's happening, I'm not sure of that step.
 

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