Covariant derivative of stress-energy tensor

In summary, the speaker is trying to understand why the Christoffel symbols vanish for the equation Tab;b=0, and the other person clarifies that they do not. They explain that the equation can be derived from the second Bianchi identity and that it is locally equivalent to T^{\mu \nu }; _{\mu } = 0.
  • #1
solveforX
19
0
hi, I understand that Tab,b=0 because the change in density equals the negative divergence, but why do the christoffel symbols vanish for Tab;b=0?
 
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  • #2
They don't. Why would you think that?

I think your first equation came from flat space, because it is not true in curved space.
 
  • #3
[itex]\triangledown _{\mu }T^{\mu \nu } = 0[/itex] can be gotten from [itex]\triangledown_{\mu }G^{\mu \nu } = 0[/itex] which is a consequence of the second bianchi identity. You also know that [itex]T^{\mu \nu }, _{\mu } = 0[/itex] but what you can do is say that locally this is the same thing as [itex]T^{\mu \nu }; _{\mu } = 0[/itex] and if this is true for some coordinate system it will be true for all coordinate systems.
 
  • #4
thank you
 

1. What is the Covariant Derivative of Stress-Energy Tensor?

The covariant derivative of stress-energy tensor is a mathematical concept used in the field of general relativity to describe the rate of change of the stress-energy tensor with respect to a particular coordinate system. It is a tensor that takes into account both the curvature of spacetime and the energy-momentum distribution within that spacetime.

2. Why is the Covariant Derivative of Stress-Energy Tensor important?

The covariant derivative of stress-energy tensor is important because it allows us to describe how matter and energy interact with the curved spacetime described by Einstein's theory of general relativity. It is a crucial tool for understanding the behavior of matter and energy in the universe and for making precise predictions about gravitational phenomena.

3. How is the Covariant Derivative of Stress-Energy Tensor calculated?

The covariant derivative of stress-energy tensor is calculated using the mathematical framework of differential geometry. It involves taking the partial derivatives of the stress-energy tensor with respect to the coordinates of the spacetime manifold and then applying certain correction terms to account for the curvature of the manifold.

4. What are the applications of the Covariant Derivative of Stress-Energy Tensor?

The covariant derivative of stress-energy tensor has many applications in the field of general relativity. It is used to describe the behavior of matter and energy in the presence of strong gravitational fields, such as those found near black holes or in the early universe. It is also used in the study of cosmology and the evolution of the universe.

5. Can the Covariant Derivative of Stress-Energy Tensor be extended to other theories of gravity?

Yes, the concept of covariant derivative of stress-energy tensor can be extended to other theories of gravity beyond general relativity. In fact, it has been adapted for use in other theories such as scalar-tensor theories, which involve a scalar field in addition to the metric tensor. It remains an important tool for studying the behavior of matter and energy in various theories of gravity.

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