Number of Solutions of Einstein Field Equations w/ Zero Pressure

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Discussion Overview

The discussion centers around the number of solutions to the Einstein Field Equations (EFE) when the pressure is considered to be zero. Participants explore the implications of this condition, the definitions involved, and the nature of solutions in various contexts, including theoretical and mathematical reasoning.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that the EFE have an infinite number of solutions when pressure is zero, citing metrics with Weyl curvature and no Ricci curvature as examples.
  • Others argue that "pressure is zero" is not an invariant criterion, as the pressure can vary across different frames of reference, making the question poorly defined.
  • A participant mentions that while metrics with Weyl curvature can be described as having vanishing stress-energy tensor (SET), they should be referred to as "vacuum" solutions rather than "zero pressure" solutions.
  • There is a discussion about the nature of pressureless dust solutions, with some noting that these solutions are only pressureless in specific coordinate charts or for comoving observers.
  • One participant raises a point about the constraints imposed by the SET and how they relate to the uniqueness of cosmological solutions for dust, suggesting that initial data can be chosen in infinitely many ways.
  • Another participant questions the independence of the conditions imposed by the SET and discusses the implications of differential conditions being weaker, leading to potential overdetermination issues.
  • There is a debate over the number of conditions required for a pressureless solution, with differing opinions on whether it should be three or four conditions.

Areas of Agreement / Disagreement

Participants express differing views on the definition and implications of "zero pressure" solutions, with no consensus reached on the nature of these solutions or the conditions that govern them. The discussion remains unresolved regarding the independence of constraints and the implications for the uniqueness of solutions.

Contextual Notes

Limitations include the dependence on definitions of pressure and the context in which solutions are considered. The discussion highlights the complexity of the relationships between different coordinate systems and observer frames.

kent davidge
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Is it true that the Einstein Field Equations have an infinite number of solutions when the pressure is zero?
 
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"Pressure is zero" is not an invariant criterion; a solution that has zero pressure in one frame can have nonzero pressure in other frames. So your question as you state it is not well-defined.

It might help if you gave some more context about why you are asking the question.
 
Seems trivially true. All metrics with Weyl curvature and no Ricci curvature have vanishing SET, thus vanishing pressure. In addition to this, there would be an infinite number of configurations of pressureless dust.
 
PAllen said:
All metrics with Weyl curvature and no Ricci curvature have vanishing SET

Yes; but I would expect these to be described as "vacuum" solutions, not "zero pressure" solutions.

PAllen said:
there would be an infinite number of configurations of pressureless dust

These are only pressureless in one coordinate chart; in other coordinate charts they are not. Or, for a more physical description, they are only pressureless to comoving observers; they are not pressureless to non-comoving observers. This is the kind of thing I was referring to in my previous post.
 
PeterDonis said:
Yes; but I would expect these to be described as "vacuum" solutions, not "zero pressure" solutions.
These are only pressureless in one coordinate chart; in other coordinate charts they are not. Or, for a more physical description, they are only pressureless to comoving observers; they are not pressureless to non-comoving observers. This is the kind of thing I was referring to in my previous post.
But there is an invariant definition of a pressureless dust solution. See, for example, the criterion of contractions of the Einstein tensor given here:

https://en.m.wikipedia.org/wiki/Dust_solution#Dust_model
 
PAllen said:
there is an invariant definition of a pressureless dust solution

I'm not disputing that the solution has an invariant definition. I'm just pointing out, for the OP's benefit, that "pressureless" only correctly describes that solution with respect to comoving observers. That's because the OP did not ask specifically about "pressureless dust" solutions defined as you say; he asked about "pressure zero" solutions, and he probably does not realize the limitations of that description.
 
PAllen said:
Seems trivially true. All metrics with Weyl curvature and no Ricci curvature have vanishing SET, thus vanishing pressure. In addition to this, there would be an infinite number of configurations of pressureless dust.
Even more trivially, it is true for any differential equation for which a sufficient number of boundary conditions have not been specified.
 
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Orodruin said:
Even more trivially, it is true for any differential equation for which a sufficient number of boundary conditions have not been specified.
This case is not so obvious by that type of criteria, which is why I made a physical argument. One can sort of argue the SET is over constrained for a pressureless dust solution. You start with arbitrary symmetric tensor fields with 10 functional degrees of freedom. First, by coordinate invariance, they form equivalence classes leaving only 6. Then, vanishing divergence is 4 more conditions. But then 4 conditions need to be satisfied for a pressureless dust solution. Of course, vanishing divergence are differential conditions, which are weaker.

I would be interested if you can add anything in this area.
 
A cosmological solution for dust is not unique, you can choose the initial data in infinitely many ways. The Friedman equations are not overditermined.
 
  • #10
martinbn said:
A cosmological solution for dust is not unique, you can choose the initial data in infinitely many ways. The Friedman equations are not overditermined.
I know that, but I am a little bothered by the counting argument I just gave. Is the flaw just that differential conditions are very weak?
 
  • #11
Hm, not sure. Are these independent? What are the 4 conditions for dust?
 
  • #12
martinbn said:
Hm, not sure. Are these independent? What are the 4 conditions for dust?
See the earlier link I gave to Wikipedia.
 
  • #13
PAllen said:
See the earlier link I gave to Wikipedia.
I guess what I am confused about is what 4 conditions need to be satisfied? The SET is ##T_{\mu\nu}=\rho u_\mu u_\nu##, why does this impose any restriction on the metric other than the EFE?
 
  • #14
martinbn said:
I guess what I am confused about is what 4 conditions need to be satisfied? The SET is ##T_{\mu\nu}=\rho u_\mu u_\nu##, why does this impose any restriction on the metric other than the EFE?
I’m reasoning directly from the SET as a symmetric tensor field. 4 conditions are given on T itself.
 
  • #15
Oh, I see. But why do you say 4, the condition for no pressure should be 3 conditions, no?
 
  • #16
martinbn said:
Oh, I see. But why do you say 4, the condition for no pressure should be 3 conditions, no?
I was looking at the conditions involving G and R. But you are right, in terms of T there are only 3, but that still leads to over determination except for the idea that differential conditions are weaker.
 
  • #17
I might be wrong, but my guess is that these constraints are not independent. If I have 5 equations for 4 unknowns, it doesn't mean that the system is overdertermined, say equation 5 might be a consequence of the other 4.

When you say, that the differential conditions are weaker, do you mean that they can have many solutions. One differential equation for one unknown has infinitely many solutions, unless more information is specified, say boundary conditions.
 

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