Abstract

A Minkowskian solution of the equation of General Relativity (as written by Einstein in 1915) is trivial because it simply means that both members of the equation are equal to zero. However, if alternatively, one considers the complete equation with a non-zero constant Λ (Einstein 1917), a Minkowskian solution is no longer trivial because it amounts to impose a constraint on the right hand side of the equation (i.e. a non-null stress-energy tensor). If furthermore one identifies (as usual) this tensor to the one of a perfect fluid, one finds that this fluid has a positive energy density and a negative pressure that depend on the three constants of the equation (i.e. gravitational constant G, cosmological constant Λ and velocity of light c). When doing that (§1), one has to consider the “Minkowskian Vacuum” as a physical object of GR (an enigmatic non-baryonic Minkowskian fluid). Can one build a model of this object on the basis of a dynamical equilibrium between the effective gravitational attraction due to the positive energy density versus the negative pressure repulsion? We propose to study such a model, where the (enigmatic) fluid is assumed to exist only in a limited sphere whose surface acts like a “test body” sensitive to the gravitational field created by the fluid. No static equilibrium exists, but a pseudoNewtonian “dynamical equilibrium” (§2) can be reached if the pseudoEuclidean fluid is in state of expansion. Up to there, we have simply constructed a model of an “abstract Universe” (i.e. the limited sphere: There is no fluid outside this sphere!) that gives to a (purely mathematical) constant Λ a concrete physical meaning. We discover finally that our expanding fluid has not only dynamical (gravitational) properties (§3) but also optical properties that are connected with Doppler Redshift (§4). Remembering that recent observations in Cosmology indicate that the “real Universe” seems to be “Flat” and in “Accelerated Expansion”; remembering also (after all) that the archetypal Flat Universe is simply a Minkowskian Universe, we logically wonder if the unexpected Minkowskian global solution, could not be also a significant cosmological model (conclusion).

Highlights

  • Let us consider Einstein’s basic equation [1] of General Relativity (GR) completed by a positive mathematical constant Λ > 0 [2], that has a priori nothing to do with Cosmology: Gμν

  • In order to discover the physical meaning of this constant Λ > 0, let us simplify with Gμν = 0 the Equation (1)

  • Our enigmatic Minkowskian fluid becomes a physical object in the framework of GR

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Summary

Enigmatic Minkowskian Fluid Deduced from Complete Einstein’s Equation

Let us consider Einstein’s basic equation [1] of General Relativity (GR) completed by a positive mathematical constant Λ > 0 [2], that has a priori nothing to do with Cosmology (with gμν Riemanian metric, Gμν Einstein’s curvature tensor, Tμν stress-energy tensor, G gravitational constant and c light velocity): Gμν. REMARK 1 Our non-usual fluid (4) cannot be confused with usual perfect fluid (4-SR) in the framework of standard Special Relativity (SR). In this case, we have uμuν = 0 in proper system for all components except for purely temporal components u0u=0 c=2 1. REMARK 2 Our non-usual (classical) fluid (2) cannot be confused with usual (quantum) black energy (2bis) in the framework of Cosmology. By associating Tμν stress-energy tensor to the one of a perfect relativistic fluid TμΛν = ( p + ρ )uμuν − pgμν we usually obtain a fluid (black energy of “quantum vacuum”3) characterized by an unknown Riemanian metric gμν (2-Riemann) whilst in (2) the metric is determined a priori Minkowskian.

Thermodynamical Properties of Minkowskian Fluid and Unstable Static Model
Optical Properties of Fluid of Photons and Bondi’s Doppler Redshift Factor
Findings
Conclusion
Full Text
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