Variation with respect to the metric

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gravity90
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Hi everyone!

There is something that I would like to ask you. Suppose you have

\frac{1}{\sqrt{-g}} \frac{\delta (\sqrt{-g} (g^{ab} u_a u_b + 1))}{\delta g^{cd}}

The outcome of this would be ##u_{c}u_{d}## or ##-u_{c} u_{d}## ?

I am really confused.
 
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δ(√-g)/δgμν = ½(√-g) gμν

δgαβ/δgμν = - ½ gαμgβν - ½ gανgβμ

From these you can derive the δ/δgμν's. (Do you really want to do that??)
 
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Thank you very much for your response. But why don't we use:

\frac{δg^{ab}}{δg^{cd}} = {δ^a}_c {δ^b}_d

or

\frac{δg_{ab}}{δg_{cd}} = {δ^c}_a{δ^d}_b ?
 
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gravity90 said:
Thank you very much for your response. But why don't we use:
\frac{δg^{ab}}{δg^{cd}} = {δ^a}_c {δ^b}_d
or
\frac{δg_{ab}}{δg_{cd}} = {δ^a}_c {δ^b}_d ?
Sure. (Except they need to be symmetrized.)

What will you use for δ(√-g)/δgcd ?
 
I will use:\frac{1}{√-g} \frac{δ(√-g)}{δg^{μν}} =- 1/2 g_{μν}

This is what I found in the Carroll's textbook and it seems right.

But the thing is that the indices a,b are mute (g^{ab} u_a u_b) so upon variation with respect to δg^{cd} or δg_{cd} we should get the same result.
 
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gravity90 said:
But the thing is that the indices a,b are mute (g^{ab} u_a u_b) so upon variation with respect to δg^{cd} or δg_{cd} we should get the same result.
Well, you have to decide which thing you want to hold fixed - ua or ua. This will be determined by the physics of the problem you're trying to solve.

If you're going to hold ua fixed, write the expression as gab ua ub and use δgab/δgcd.

Otherwise, if you're going to hold ua fixed, write it as gab ua ub and use δgab/δgcd. The two results will differ by a sign.
 
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I respect your math skills... but what the hell are are you guys talking about? Little g? What is little g?
 
Thank you again for your response. But what is the difference between keeping u^a or u_a from a physical point of view?
 

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