Calculating the components of the Ricci tensor

In summary, there appears to be a mistake in the question as the given values for the connection coefficients do not result in the expected value of ##R_{22}=e^{2x}##.
  • #1
jore1
6
0
Homework Statement
Given the line element ## ds^2=a^2dt^2 -a^2dx^2 - \frac{a^2e^{2x}}{2}dy^2 +2a^2e^xdydt -a^2dz^2 ##
(I) Calculate ##\Gamma^{0}_{12}##

Now assume the following values for the connection coefficients: ##\Gamma^{0}_{12}=\Gamma^{0}_{21}=\Gamma^{0}_{10}=\Gamma^{0}_{01}=1##, ##\Gamma^{1}_{22}=\frac{e^{2x}}{2}$, $\Gamma^{2}_{10}=-e^{-x}##, ##\Gamma^{1}_{02}=\Gamma^{1}_{20}=\frac{e^{x}}{2}## and all others are zero.

(II) Calculate ##R_{22}##


I am currently working through an exercise to calculate the component ##R_{22}## of the Ricci tensor for the line element ##ds^2=a^2dt^2 -a^2dx^2 - \frac{a^2e^{2x}}{2}dy^2 +2a^2e^xdydt -a^2dz^2##. The question first asks for the value of ##\Gamma^{0}_{12}##, which I calculate to be ##\frac{e^{x}}{2}##. I am told to assume the following values for the connection coefficients: ##\Gamma^{0}_{12}=\Gamma^{0}_{21}=\Gamma^{0}_{10}=\Gamma^{0}_{01}=1##, ##\Gamma^{1}_{22}=\frac{e^{2x}}{2}$, $\Gamma^{2}_{10}=-e^{-x}##, ##\Gamma^{1}_{02}=\Gamma^{1}_{20}=\frac{e^{x}}{2}## and all others are zero.

Using the relation for the Ricci tensor, I find that the only non-zero components are: ##R_{22}=\partial_1(\Gamma^{0}_{12})+\Gamma^{0}_{10}\Gamma^{1}_{22}-\Gamma^{0}_{21}\Gamma^{1}_{02}-\Gamma^{1}_{20}\Gamma^{0}_{12}##. This is where the problem arises: using the assumed values for the connection coefficients (with ##\Gamma^{0}_{12}=\Gamma^{0}_{21}=1##) I find that ##R_{22}=e^{2x}-e^{x}##, while using the values ##\Gamma^{0}_{12}=\Gamma^{0}_{21}=\frac{e^{x}}{2}## (the rest being those assumed) I find that ##R_{22}=e^{2x}##. I am told that the second result is correct. It seems to be the case that the assumed value for ##\Gamma^{0}_{12}## is incorrect.

Could someone provide clarification as to whether there is indeed a mistake in the question? As a beginner in GR, I find myself questioning the basics.
Relevant Equations
##R_{ab}=\Gamma^{d}_{ab,d}-\Gamma^{d}_{da,b}+\Gamma^{d}_{de}\Gamma^{e}_{ab}-\Gamma^{d}_{ae}\Gamma^{e}_{db}##

##\Gamma^{a}_{bc}=\frac{1}{2}g^{ad}(g_{bd,c}+g_{cd,b}-g_{bc,d}##
(I) Using the relevant equation I find this to be ## \frac{e^{x}}{2} ##.

(II) Using the relation for the Ricci tensor, I find that the only non-zero components are: ##R_{22}=\partial_1(\Gamma^{0}_{12})+\Gamma^{0}_{10}\Gamma^{1}_{22}-\Gamma^{0}_{21}\Gamma^{1}_{02}-\Gamma^{1}_{20}\Gamma^{0}_{12}##. This is where the problem arises: using the assumed values for the connection coefficients (with ##\Gamma^{0}_{12}=\Gamma^{0}_{21}=1##) I find that ##R_{22}=e^{2x}-e^{x}##, while using the values ##\Gamma^{0}_{12}=\Gamma^{0}_{21}=\frac{e^{x}}{2}## (the rest being those assumed) I find that ##R_{22}=e^{2x}##.

Could someone provide clarification as to whether there is indeed a mistake in the question? As a beginner in GR, I find myself questioning the basics.
 
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  • #2
I could have slipped up, but I'm getting ##\Gamma^0_{1 2} = -\large\frac{e^x} 6##.

Please double-check that there are no typos in your expression for ##ds^2##. It will also help if you list the expressions you used for the nonzero ##g_{\mu \nu}## and the nonzero ##g^{\mu \nu}##.
 
  • #3
Yes, I mistyped the metric should be: ##ds^2=a^2dt^2 -a^2dx^2 + \frac{a^2e^{2x}}{2}dy^2 +2a^2e^xdydt -a^2dz^2##

This then gives: ##g_{ab} = \left[\begin{matrix}a^{2} & 0 & a^{2} e^{x} & 0\\0 & - a^{2} & 0 & 0\\a^{2} e^{x} & 0 & + \frac{a^{2} e^{2 x}}{2} & 0\\0 & 0 & 0 & - a^{2}\end{matrix}\right]##

and ##g^{ab} = \frac{1}{a^2}\left[\begin{matrix}-1 & 0 & 2 e^{-x} & 0\\0 & - 1 & 0 & 0\\ 2e^{-x} & 0 & -2e^{-2x} & 0\\0 & 0 & 0 & - 1\end{matrix}\right]##

Apologies for the mistake.
 
Last edited:
  • #4
jore1 said:
the metric should be: ##ds^2=a^2dt^2 -a^2dx^2 + \frac{a^2e^{2x}}{2}dy^2 +2a^2e^xdydt -a^2dz^2##
Ok. I agree with you, ##\Gamma^0_{12} = \large \frac{e^x} 2##.
 
  • #5
Thanks for the response. So is my conclusion correct that there is a mistake in the question? I think the idea was that the component ##R_{22}## was supposed to be ##e^{2x}## either way. Though this doesn't seem to be work.
 
  • #6
jore1 said:
So is my conclusion correct that there is a mistake in the question?
Yes, I think there must be a mistake in the question. Here's what I find for the nonzero connection coefficients, $$\Gamma^0_{10} = \Gamma^0_{01} = 1$$ $$\Gamma^0_{12} = \Gamma^0_{21} = \frac {e^x} 2$$ $$\Gamma^2_{10} = \Gamma^2_{01} = -e^{-x}$$ $$\Gamma^1_{22} = -\frac{e^{2x}}{2}$$ $$\Gamma^1_{02} = \Gamma^1_{20} = -\frac{e^{x}}{2}$$ The last two differ in sign from the problem statement.
 
  • #7
R_11 = e^-2x

R_12 = 1 - e^2x

R_21 = 1 + e^2x

R_22 = e^2x
 

FAQ: Calculating the components of the Ricci tensor

What is the Ricci tensor and why is it important in general relativity?

The Ricci tensor is a mathematical object that represents the degree to which the geometry of a space-time deviates from being flat. It is derived from the Riemann curvature tensor and is used in the Einstein field equations to describe how matter and energy influence the curvature of space-time. This curvature, in turn, affects the motion of objects, making the Ricci tensor crucial for understanding gravitational phenomena in the framework of general relativity.

How do you obtain the Ricci tensor from the Riemann curvature tensor?

The Ricci tensor is obtained by contracting the Riemann curvature tensor. Specifically, you sum over the first and third indices of the Riemann tensor. Mathematically, this is expressed as \( R_{ij} = R^{k}_{ikj} \), where \( R_{ij} \) is the Ricci tensor and \( R^{k}_{ikj} \) are the components of the Riemann tensor.

What are the steps involved in calculating the components of the Ricci tensor?

Calculating the components of the Ricci tensor involves several steps: 1. Compute the Christoffel symbols from the metric tensor.2. Use the Christoffel symbols to calculate the Riemann curvature tensor.3. Contract the Riemann curvature tensor to obtain the Ricci tensor. Each of these steps requires careful application of differential geometry and tensor calculus.

What role do the Christoffel symbols play in the calculation of the Ricci tensor?

The Christoffel symbols, also known as the connection coefficients, are essential for calculating the Riemann curvature tensor. They describe how the coordinate basis vectors change from point to point in a curved space-time. These symbols are derived from the metric tensor and are used to express the Riemann tensor, which is then contracted to find the Ricci tensor.

Can software tools be used to calculate the Ricci tensor, and if so, which ones are commonly used?

Yes, various software tools can be used to calculate the Ricci tensor. Commonly used tools include symbolic computation software like Mathematica, Maple, and SageMath, as well as specialized packages for general relativity such as GRtensor for Maple and xAct for Mathematica. These tools can handle the complex algebraic manipulations involved in deriving the Ricci tensor from the metric tensor.

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