Gamma How to Calculate Gamma: Step by Step

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SUMMARY

The discussion focuses on the calculation of the Christoffel symbols, specifically how to manipulate the equation \(\Gamma^k_{ij} = -\textbf{e}_j \cdot D_i\textbf{e}^k\) to derive \(D_i \textbf{e}^k = \Gamma^k_{ij} \textbf{e}^j\). Participants clarify the relationships between the vectors and tensors involved, emphasizing the properties of the identity tensor and the commutativity of the dot product. The conclusion drawn is that the original statement regarding the relationship between the Christoffel symbols and the covariant derivative is incorrect.

PREREQUISITES
  • Understanding of Christoffel symbols in differential geometry
  • Familiarity with covariant derivatives and tensor calculus
  • Knowledge of vector and tensor operations, specifically dot products
  • Concept of the identity tensor in linear algebra
NEXT STEPS
  • Study the properties of Christoffel symbols in Riemannian geometry
  • Learn about covariant differentiation and its applications in general relativity
  • Explore tensor algebra, focusing on operations involving the identity tensor
  • Investigate the implications of tensor commutativity in various contexts
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Mathematicians, physicists, and students studying differential geometry or general relativity, particularly those working with tensor calculus and Christoffel symbols.

John Creighto
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Can someone explain to me how to go from

\Gamma ^k_{ij}=-\bold{e}_j \cdot D_i \bold{e}^k

To

D_i \bold{e}^k = \Gamma ^k_{ij} \bold{e}^j \ \cdot \ \
 
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Try this:
\Gamma^k_{ij} = -\textbf{e}_j \cdot D_i\textbf{e}^k
\Gamma^k_{ij} = -D_i\textbf{e}^k \cdot \textbf{e}_j because \textbf{v} \cdot \textbf{u} = \textbf{u} \cdot \textbf{v}
\Gamma^k_{ij} \textbf{e}^j = -D_i\textbf{e}^k \cdot \textbf{e}_j \textbf{e}^j
\Gamma^k_{ij} \textbf{e}^j = -D_i\textbf{e}^k \cdot \textbf{1} because \textbf{e}_j \textbf{e}^j = \textbf{1}
\Gamma^k_{ij} \textbf{e}^j = -D_i\textbf{e}^k because \textbf{e} \cdot \textbf{1} = \textbf{e}
Well, I got close, but I don't know how to drop the minus sign. For the identity tensor, I believe \textbf{1} \cdot \textbf{v} = \textbf{v} \cdot \textbf{1} is true (though not true for other second rank tensors)
 
Last edited:
I think you are right, Davidcantwell!
<br /> \Gamma^k_{ij} \textbf{e}^j = -D_i\textbf{e}^k <br />
implies
<br /> \Gamma^k_{ij} = -\textbf{e}_j \cdot D_i\textbf{e}^k<br />
The original statement seems not correct.
 

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