Metric Elements and Einstein Equations in a Variable-Dependent Formulation

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eljose
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I have two questions...let's suppose we have a metric in the form:

[tex]ds^2 =f(t)dt^2 +g(x)dx^2 +H(y)dy^2[/tex]

So every element of the metric only depend on a variable..my question is..does this mean that the Einstein Equations (vaccuum) are of the form:

[tex]R_ii =0[/tex] i=t,x,y ?..

-And the second question is i know that [tex]det(g_ab )=f(t)g(x)H(y)[/tex] but ..what's the form of the Lagrangian?..i guess:

[tex]L= \int_ V dVf(t)g(x)H(y)(f(t)R_00 +g(x)R_11+ H(y)R_22 )[/tex]:rolleyes: :cool: :frown:
 
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eljose said:
I have two questions...let's suppose we have a metric in the form:

[tex]ds^2 =f(t)dt^2 +g(x)dx^2 +H(y)dy^2[/tex]

So every element of the metric only depend on a variable..my question is..does this mean that the Einstein Equations (vaccuum) are of the form:

[tex]R_ii =0[/tex] i=t,x,y ?..

Yep. I threw this line element (with a k(z) dz^2 term added) into GrTensor II, the Riemann was zero, as well as the Ricci and the Einstein.
 
And a "Mixed" one?.. [tex]ds^2 = f(t)dt^2 + g_ij dx^i dx^j[/tex] Where Einstein summation is assumed...
 
This line element is just a simple diffeomorphism of normal Minkowski space. Consider changing the coordinates to T, X, and Y, such that:

[tex]dT = \sqrt{-f(t)} dt[/tex]
[tex]dX = \sqrt{g(x)} dx[/tex]
[tex]dY = \sqrt{H(y)} dy[/tex]

In these coordinates, the line element becomes:
[tex]ds^2 = - dT^2 + dX^2 + dY^2[/tex]