Covariant Derivative: What Is $\nabla^0 A_{\alpha}$?

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Homework Help Overview

The discussion revolves around the covariant derivative, specifically the expression for $\nabla^0 A_{\alpha}$ in the context of differential geometry and tensor calculus.

Discussion Character

  • Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to understand the relationship between $\nabla_0 A_{\alpha}$ and $\nabla^0 A_{\alpha}$. Some participants provide a transformation involving the metric tensor and the connection coefficients.

Discussion Status

Participants are exploring the definitions and relationships between different forms of the covariant derivative. Some guidance has been offered regarding the transformation of the covariant derivative using the metric tensor, but no consensus has been reached.

Contextual Notes

There may be assumptions regarding the properties of the metric tensor and the connection coefficients that are not fully articulated in the discussion.

S.P.P
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just a quick query, I know that,

[itex]\nabla_0 A_{\alpha}= \partial_0 A_{\alpha} - \Gamma^{\beta}_{0 \alpha} A_{\beta}[/itex]

But what does
[itex]\nabla^0 A_{\alpha}[/itex] equal?
 
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Since [itex]\nabla^0A_\alpha = g^{0\beta}\nabla_\beta A_\alpha[/itex] you have

[tex]\nabla^0A_\alpha = g^{0\beta}\partial_\beta A_\alpha - g^{0\beta}\Gamma^{\gamma}_{\phantom{\gamma}\alpha\beta}A_\gamma[/tex]
 
You're welcome.
 
shoehorn said:
You're welcome.

Don't take it personally, it's rare to get thanked for help here.
 

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