kent davidge
- 931
- 56
Is it true that the Einstein Field Equations have an infinite number of solutions when the pressure is zero?
The Einstein Field Equations (EFE) can have an infinite number of solutions when the pressure is zero, but this is contingent on the frame of reference. Solutions described as "vacuum" are more appropriate than those labeled as "zero pressure." Metrics with Weyl curvature and no Ricci curvature exhibit vanishing stress-energy tensors (SET), leading to configurations of pressureless dust. However, these configurations are only pressureless in specific coordinate charts and may vary for different observers.
PREREQUISITESPhysicists, mathematicians, and students of general relativity seeking to deepen their understanding of the Einstein Field Equations and their solutions, particularly in cosmological contexts.
PAllen said:All metrics with Weyl curvature and no Ricci curvature have vanishing SET
PAllen said:there would be an infinite number of configurations of pressureless dust
But there is an invariant definition of a pressureless dust solution. See, for example, the criterion of contractions of the Einstein tensor given here: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.
PAllen said:there is an invariant definition of a pressureless dust solution
Even more trivially, it is true for any differential equation for which a sufficient number of boundary conditions have not been specified.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.
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.Orodruin said:Even more trivially, it is true for any differential equation for which a sufficient number of boundary conditions have not been specified.
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?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.
See the earlier link I gave to Wikipedia.martinbn said:Hm, not sure. Are these independent? What are the 4 conditions for dust?
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?PAllen said:See the earlier link I gave to Wikipedia.
I’m reasoning directly from the SET as a symmetric tensor field. 4 conditions are given on T itself.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 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.martinbn said:Oh, I see. But why do you say 4, the condition for no pressure should be 3 conditions, no?