Gravitational Energy Equation of State Parameter

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Discussion Overview

The discussion revolves around the concept of the equation of state parameter for gravitational energy in the context of General Relativity, particularly in comparison to the equation of state parameter for dark energy, which is known to be -1. Participants explore whether a similar parameter can be defined for gravitational energy and how it relates to pressure and energy density.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants assert that there is no equation of state parameter for gravitational energy within the standard formulation of General Relativity.
  • Others propose that while gravitational energy does not exist in the conventional sense, a relation could be constructed between positive pressure and gravitational energy density through the conservation of the stress-energy tensor.
  • A participant suggests that a new "total energy density" could be defined to account for gravitational potential energy in curved spacetime, although this idea is met with skepticism regarding its implications.
  • There is a discussion about whether introducing a new quantity for gravitational potential energy would alter the stress-energy tensor, with some arguing it would not change the tensor conceptually.
  • Concerns are raised about the implications of negative energy concepts and how they relate to dark energy and gravitational energy.

Areas of Agreement / Disagreement

Participants do not reach a consensus on whether an equation of state parameter for gravitational energy can be defined or how it would relate to dark energy. Multiple competing views remain regarding the implications of introducing new quantities and the nature of gravitational energy.

Contextual Notes

The discussion highlights limitations in defining gravitational energy within the framework of General Relativity and the complexities introduced by curved spacetime. There are unresolved questions about the mathematical formulation and the physical implications of proposed concepts.

Ranku
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Cosmological constant dark energy has equation of state parameter = -1. What is the equation of state parameter of gravitational energy?
 
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Ranku said:
Cosmological constant dark energy has equation of state parameter = -1. What is the equation of state parameter of gravitational energy?
There isn't one. In the standard formulation of General Relativity, there is no such thing as gravitational energy.
 
Chalnoth said:
There isn't one. In the standard formulation of General Relativity, there is no such thing as gravitational energy.

Since dark energy density is related to negative pressure, is there no way to construct a relation between 'positive pressure' and 'gravitational energy density', even though gravitational energy does not occur in general relativity?
 
Ranku said:
Since dark energy density is related to negative pressure, is there no way to construct a relation between 'positive pressure' and 'gravitational energy density', even though gravitational energy does not occur in general relativity?
No, I don't think so.

One way you could do it, though, is through the conservation of the stress-energy tensor. The stress-energy tensor is a 2nd-rank tensor (sort of like a matrix) that includes components such as energy, momentum, pressure, and shear (shear includes things like twisting forces). This tensor is always conserved in a very particular way: its so-called covariant derivative is zero.

If you examine this conservation law in flat space-time, you get an energy transport equation: the time rate of change of energy in a region of space is equal to the flow of energy into/out of that region.

However, in curved space-time things get a little bit more complicated. What you could do is make up a new "total energy density" which is always conserved: as in the flat space-time example, the total energy density within a region of space-time only changes if it flows from one place to another. You could do this by adding an extra term to the equations that exactly cancels the extra terms you get from curved space-time, and call this your gravitational potential energy.
 
Chalnoth said:
No, I don't think so.

One way you could do it, though, is through the conservation of the stress-energy tensor. The stress-energy tensor is a 2nd-rank tensor (sort of like a matrix) that includes components such as energy, momentum, pressure, and shear (shear includes things like twisting forces). This tensor is always conserved in a very particular way: its so-called covariant derivative is zero.

If you examine this conservation law in flat space-time, you get an energy transport equation: the time rate of change of energy in a region of space is equal to the flow of energy into/out of that region.

However, in curved space-time things get a little bit more complicated. What you could do is make up a new "total energy density" which is always conserved: as in the flat space-time example, the total energy density within a region of space-time only changes if it flows from one place to another. You could do this by adding an extra term to the equations that exactly cancels the extra terms you get from curved space-time, and call this your gravitational potential energy.

Hmm...interesting. Well it's good to know that a positive pressure:gravitational energy relation could at least be considered, whether it works or not.
Thanks.
 
Would't that leave you with a completely new stress-energy tensor with two components(simplifying a lot): one negative "dark" energy (pressure) and one "gravitational" positive energy pressure?
It's interesting, if a bit radical. In the past there have been attempts along those lines with negative and positive gravity or with inertia versus gravity(de Sitter) but they were all turned down because they seemed to bring up unphysical concepts like "negative energy".Since 1998 with the accelerated expansion surprise and "dark energy" there is more going in that direction.
 
AWA said:
Would't that leave you with a completely new stress-energy tensor with two components(simplifying a lot): one negative "dark" energy (pressure) and one "gravitational" positive energy pressure?
Hmm, that's not what I was talking about. The basic idea is this. If we have massless particles in flat space-time, we can write energy conservation as:

[tex]\frac{d\rho}{dt} = -\bigtriangledown \vec{p}c[/tex]

That is, for the energy density in a region of space can only change if some of that energy flows into or out of the region. When we have curved space-time, we instead have:

[tex]\frac{d\rho}{dt} = -\bigtriangledown \vec{p}c +[/tex]curvature-related terms

I won't bother to look up the precise form of the curvature-related terms on the right hand side. But suffice it to say it's always possible to write energy conservation in this way. So I could simply make up "gravitational potential energy" and set it to the negative of those curvature-related terms. Then I would have conservation of total energy again.

This has nothing to do with making up a new tensor, just making up a new quantity.

AWA said:
It's interesting, if a bit radical. In the past there have been attempts along those lines with negative and positive gravity or with inertia versus gravity(de Sitter) but they were all turned down because they seemed to bring up unphysical concepts like "negative energy".Since 1998 with the accelerated expansion surprise and "dark energy" there is more going in that direction.
Er, dark energy must have a positive energy density to produce an accelerated expansion.
 
Ok, and wouldn't adding that new made up quantity change anything in the tensor,at least conceptually?
About dark energy sign, I know itis supposed to have conventionally positive density to attain
accelaration, but as the OP spoke in terms of negative pressure and we were calling "gravitational energy" positive I switched the signs,but I coul have made the gravitational energy negative and dark energy positive since the point seeemed to be that they are opposite and cancel each other out. Let's not get hung up about the signs here.
 
AWA said:
Ok, and wouldn't adding that new made up quantity change anything in the tensor,at least conceptually?
No, the tensor remains exactly the same. This would just be a way of talking about gravitational potential energy.
 

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