Prove that two transformation laws of the Christoffel symbols are the same

In summary, the given transformation law can be simplified by relabeling the dummy indices and differentiating the left and right sides of \delta^{\lambda '}_{\mu '} with respect to x^{\alpha '}.
  • #1
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Homework Statement



Prove that the transformation law

[itex]\Gamma^{\sigma '}_{\lambda '\rho '}=\frac{\partial x^\nu}{\partial x^{\lambda '}}\frac{\partial x^\rho}{\partial x^{\rho '}}\frac{\partial x^{\sigma '}}{\partial x^{\mu}}\Gamma^{\mu}_{\nu\rho}+\frac{\partial x^{\sigma '}}{\partial x^{\mu}}\frac{\partial^2 x^\mu}{\partial x^{\lambda '}\partial x^{\rho '}}[/itex]

is equivalent to

[itex]\Gamma^{\sigma '}_{\lambda '\rho '}=\frac{\partial x^\lambda}{\partial x^{\lambda '}}\frac{\partial x^\rho}{\partial x^{\rho '}}\frac{\partial x^{\sigma '}}{\partial x^{\sigma}}\Gamma^{\sigma}_{\lambda\rho}-\frac{ \partial x^\mu}{\partial x^{\lambda '}}\frac{\partial x^{\lambda}}{\partial x^{\rho '}}\frac{\partial^2 x^{\sigma '}}{\partial x^{\mu}\partial x^{\lambda}}[/itex]

The Attempt at a Solution



The first term is easy, just relabel the dummy indices [itex] \nu \rightarrow \lambda [/itex] and [itex] \mu \rightarrow \sigma [/itex]. But for the rest of the problem, I have no clue what to do.
 
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  • #2
Maybe this is too late. It's a trick. Differentiate the far left and right of

[tex]\delta^{\lambda '}_{\mu '} = \frac{\partial x^{\lambda '}}{\partial x^{\mu '}} = \frac{\partial x^{\lambda '}}{\partial x^\rho} \frac{\partial x^\rho}{\partial x^{\mu '}}[/tex]

with respect to [itex]x^{\alpha '}[/itex].
 

Related to Prove that two transformation laws of the Christoffel symbols are the same

1. What are the two transformation laws of the Christoffel symbols?

The first transformation law of the Christoffel symbols states that the components of the symbols transform like the components of a tensor under a change of coordinates. The second transformation law states that the components of the symbols are invariant under a change of affine parameter.

2. Why is it important to prove that these two transformation laws are the same?

Proving that the two transformation laws of the Christoffel symbols are the same ensures the consistency and validity of the mathematical framework used in General Relativity. It also allows for easier and more accurate calculations of the symbols in different coordinate systems.

3. How can one prove that these two transformation laws are equivalent?

The two transformation laws can be proven to be equivalent by using the properties of tensors and the definition of the affine parameter. This involves manipulating and equating the components of the symbols in different coordinate systems.

4. Are there any real-world applications of these transformation laws?

Yes, the transformation laws of the Christoffel symbols are used extensively in the calculations and predictions of physical phenomena in General Relativity, such as gravitational lensing and the bending of light around massive objects.

5. Are there any exceptions to these transformation laws?

No, the transformation laws of the Christoffel symbols hold true in all cases and for all coordinate systems. They are fundamental principles in the mathematical description of General Relativity.

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