Understanding Metric Tensors in Riemannian Spaces

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In a 2D Riemannian space defined by ds^2 = dx^2 + x^2dy^2, the components of the metric tensor are confirmed as g_{11} = 1, g_{12} = 0, g_{21} = 0, and g_{22} = x^2. For the second question regarding the relationship between the Christoffel symbols of two metrics, it is clarified that e^z is the exponential function, and the correct formulation for the Christoffel symbols should include e^{-z}. The discussion emphasizes the importance of correctly applying derivatives with respect to all coordinates, as z is a function of multiple coordinates. The participants are encouraged to refine their calculations based on the provided corrections and clarifications. Understanding these concepts is crucial for correctly analyzing Riemannian spaces and their metrics.
yukcream
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Q1 If given a 2D Riemannian space, ds^2 = dx^2 + x^2dy^2, do the componets of the metric tensor are these:
g_11 = 1, g_12 = 0
g_21 = o, g_22 = x^2 ?

In addition, I got a question from my lecturer:
Q2. 2 metrics, defined in a Riemannian space, are given by ds^2 = g_ijdx^idy^j
and ds'^2 = g'_ij dx^idy^j = e^z g_ijdx^idy^j , respectively, where z is a function of the coordinates x^i.
Find the relation between the Chritoffel symbols corresponding to the 2 two metrics~~~
I have no ideal how to solve it and what is e here? treat it as a function or is it represents the persudo tensor?

Can anyone help me~~

yukyuk
 
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yukcream said:
Q1 If given a 2D Riemannian space, ds^2 = dx^2 + x^2dy^2, do the componets of the metric tensor are these:
<br /> g_{11} = 1, g_{12} = 0<br />
<br /> g_{21} = 0, g_{22} = x^2<br />
Yes, this is correct.

yukcream said:
In addition, I got a question from my lecturer:
Q2. 2 metrics, defined in a Riemannian space, are given by ds^2 = g_{ij}dx^idy^j
and ds&#039;^2 = g&#039;_{ij} dx^idy^j = e^z g_{ij}dx^idy^j, respectively, where z is a function of the coordinates x^i.
Find the relation between the Chritoffel symbols corresponding to the 2 two metrics~~~
I have no ideal how to solve it and what is e here? treat it as a function or is it represents the persudo tensor?
Can anyone help me~~
I assume you mean: ds^2 = g_{ij}dx^idx^j and ds&#039;^2 = g&#039;_{ij}dx^idx^j = e^z g_{ij}dx^idx^j. (Note that I have replaced references to y^j with references to x^j.)

The e^z here is the exponential function. Note that its partial derivatives are (,i is shorthand for \partial / \partial x^i):

e^z{}_{,i} = z_{,i}e^z

The formula for the Christoffel symbol in terms of the metric tensor is:

\Gamma^m{}_{ij} = \frac{1}{2}g^{km}(g_{ik,j} + g_{jk,i} - g_{ij,k})

This should be enough to get you started. If you still have trouble, post again.
 
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To jimmysnyder:

Hope I can understand what you mean~~
I work out the steps, am I correct?

\Gamma^m{}_{ij} = \frac{1}{2}g^{km} (-g_{ij,k}+g_{jk,i}+g_{ki,j})
\Gamma&#039;^m{}_{ij} = \frac{1}{2}g&#039;^{km} (-g&#039;_{ij,k}+g&#039;_{jk,i}+g&#039;_{ki,j})
\Gamma&#039;^m{}_{ij} = \frac{1}{2}e^{z(i)}g^{km} (-e^{z(i)}g_{ij,k}+e^{z(i)}g_{jk,i}+e^{z(i)}g_{ki,j}
\Gamma&#039;^m{}_{ij} = \frac{1}{2}e^{z(i)}g^km{}[-e^{z(i)}g_{ij,k}+z(i)_{,i}e^{z(i)}g_{jk,i}+e^{z(i)}g_{jk,i}+e^{z(i)}g_{ki,j}]
\Gamma&#039;^m{}_{ij} = e^{2z(i)}[\Gamma^m{}_{ij} + \frac{1}{2}g^{km}z(i)_{,i}g_{jk,i}]

Thx so much and you are so smart that you can correct my mistake as what i want to write is dx^j not dy^j~

yukyuk
 
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yukcream said:
\Gamma^m{}_{ij} = \frac{1}{2}g^{km} (-g_{ij,k}+g_{jk,i}+g_{ki,j})
\Gamma&#039;^m{}_{ij} = \frac{1}{2}g&#039;^{km} (-g&#039;_{ij,k}+g&#039;_{jk,i}+g&#039;_{ki,j})
So far, so good.

yukcream said:
\Gamma&#039;^m{}_{ij} = \frac{1}{2}e^{z(i)}g^{km} (-e^{z(i)}g_{ij,k}+e^{z(i)}g_{jk,i}+e^{z(i)}g_{ki,j}
The exponential factor that goes with g^{km} should be e^{-z}, because you want g&#039;^{np}g&#039;_{pm} = \delta^n{}_m. Also in order to make things more clear, I would remove the parameter from z and add parentheses as follows:
\Gamma&#039;^m{}_{ij} = \frac{1}{2}e^{-z}g^{km} (-(e^{z}g_{ij})_{,k} + (e^{z}g_{jk})_{,i} + (e^{z}g_{ki})_{,j})

The next steps are not correct, but if you start from the equation I have given you, I think you can get the rest.
 
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Once more question is :

Given a fame S' which is falling along -z-axis with constant acceleration in an inertial frame S. Find a form of metric in the S' frame, assume in Newtonian approximation of the absolute time (t=t').

I just know a definition that
a = sqrt(g_ij dx^idx^j) but how to get the g_ij??

yukyuk
 
jimmysnyder said:
So far, so good.
The exponential factor that goes with g^{km} should be e^{-z}. Also in order to make things more clear, I would remove the parameter from z and add parentheses as follows:
\Gamma&#039;^m{}_{ij} = \frac{1}{2}e^{-z}g^{km} (-(e^{z}g_{ij})_{,k} + (e^{z}g_{jk})_{,i} + (e^{z}g_{ki})_{,j})
The next steps are not correct, but if you start from the equation I have given you, I think you can get the rest.

I think my answer is correct~~
as z is only a function of coordinate x^i , derative of z wrt x^j & x^k will be zero ~ right? Do I make the mistake there?
 
yukcream said:
I think my answer is correct~~
as z is only a function of coordinate x^i , derative of z wrt x^j & x^k will be zero ~ right? Do I make the mistake there?
Yes, you have made a mistake. In this case, i is an index that takes all 4 values, 0, 1, 2, and 3. In your original post you have written "z is a function of the coordinates x^i". Note coordinates, not coordinate. That means it is a function of all 4 coordinates and partials must be taken with respect to each of them. The letters k and j are just different index letters that also take on the 4 values 0, 1, 2, and 3.
 
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