Two questions on the Stress-Energy Tensor

Click For Summary
SUMMARY

The discussion centers on the Stress-Energy tensor, specifically its derivation for a perfect fluid and the implications of its trace. The participant derives the 00 entry of the tensor as \(T^{00} = \rho_0 + 3P\), where \(\rho_0\) is the rest-mass density and \(P\) is the pressure, confirming its validity for non-photon fluids. However, confusion arises regarding the Lorentz scalar \({T^\alpha}_\alpha\), which yields \(-\rho + 3P\) instead of the expected \(+\rho + 3P\). This discrepancy is attributed to the choice of metric convention.

PREREQUISITES
  • Understanding of the Stress-Energy tensor in General Relativity
  • Familiarity with perfect fluid models in relativistic physics
  • Knowledge of Lorentz transformations and their implications
  • Basic concepts of isotropy and pressure in fluid dynamics
NEXT STEPS
  • Study the derivation of the Stress-Energy tensor for various fluid types
  • Explore the implications of the Trace Energy Condition in General Relativity
  • Learn about different metric conventions in General Relativity
  • Investigate the behavior of the Stress-Energy tensor for photon gases
USEFUL FOR

Physicists, particularly those specializing in General Relativity, fluid dynamics, and cosmology, will benefit from this discussion, as well as students seeking to deepen their understanding of the Stress-Energy tensor and its applications.

zenmaster99
Messages
29
Reaction score
6
I am trying to get a good feel for the Stress-Energy tensor, but I seem to be hung up on a few concepts and I was wondering if anyone could clear up the issues.

First, when I look at the derivation of the Stress-Energy tensor for a perfect fluid (of one species, say), the 00 entry can be written as a sum over each "particle" in the fluid:
$$T^{00}=\sum_kmu_k^0u_k^0=m\sum_k\gamma_k^2=m\sum_k\left(1+{v_k^2\over1-v_k^2}\right)=m\sum_k\left(1+\gamma_k^2v_{k,x}^2+\gamma_k^2v_{k,y}^2+\gamma_k^2v_{k,z}^2\right)$$
$$=\sum_km+\sum_kmu_k^1u_k^1+\sum_kmu_k^2u_k^2+\sum_kmu_k^3u_k^3$$
In the rest frame of the bulk, I can divide by a small 3-volume element and, assuming things are isotropic, I find
$$T^{00}=\rho_0+3P$$
where ##\rho_0## is the rest-mass density and ##P## is the pressure. Is this correct? If so, is it useful? Clearly, I can't use this for photons.

My second question involves the Lorentz scalar ##{T^\alpha}_\alpha##. Setting ##T^{00}\equiv\rho##, when I actually find this using ##T^{\alpha\nu}\eta_{\nu\alpha}##, I get ##-\rho+3P## instead of ##+\rho+3P##. What am I doing wrong?

I ask this because I'm guessing that this scalar ##T## must be a useful quantity, but I don't know what, exactly. It's implicated in the Trace Energy Condition... but if I'm getting a negative value for a dust (##P=0##), then I can't possibly satisfy ##T\ge0##.

Any and all insight is greatly appreciated. Much thanks in advance.

ZM
 
Physics news on Phys.org
zenmaster99 said:
Clearly, I can't use this for photons.
For a photon gas, ##T^{00}=3p## in the rest frame, so the expression has the correct limiting behaviour.

The sign in the trace condition depends on your metric convention.
 

Similar threads

  • · Replies 38 ·
2
Replies
38
Views
2K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 21 ·
Replies
21
Views
4K
  • · Replies 21 ·
Replies
21
Views
3K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 33 ·
2
Replies
33
Views
5K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 3 ·
Replies
3
Views
1K