Bianchi type-I cosmological effective stiff fluid model in Saez and Ballester theory

2004 ◽  
Vol 291 (1) ◽  
pp. 75-83 ◽  
Author(s):  
G. Mohanty ◽  
S.K. Sahu
1998 ◽  
Vol 07 (05) ◽  
pp. 749-771 ◽  
Author(s):  
MATTHIAS WOLLENSAK

Maxwell's equations are rewritten with respect to anholonomic orthonormal frames and applied to the case when the background is described by a diagonal Bianchi Type I universe with line element [Formula: see text]. It is generally shown that solutions analogous to plane wave solutions in flat spacetime must obey two transversality conditions when the spacetime is anisotropic i.e., when at least one of the coefficients αj(t) differs from the others. Analytic solutions are presented for propagation along the respective coordinate axes and a special stiff fluid model. Furthermore, by use of a generally applicable ansatz the long- and short-time behavior of waves traveling in the axisymmetric Kasner universe have been investigated.


2018 ◽  
Vol 92 (6) ◽  
pp. 813-818 ◽  
Author(s):  
S. K. Sahu ◽  
T. T. Tole ◽  
M. Balcha

Pramana ◽  
2008 ◽  
Vol 71 (1) ◽  
pp. 15-22 ◽  
Author(s):  
S. D. Katore ◽  
S. V. Thakare ◽  
K. S. Adhao

2014 ◽  
Vol 92 (5) ◽  
pp. 365-369 ◽  
Author(s):  
Raj Bali ◽  
Swati Singh

Stiff fluid inflationary cosmological model with variable bulk viscosity in the frame work of locally rotationally symmetric (LRS) Bianchi type I space–time, is investigated. To get the deterministic solution, we have also assumed that σ is proportional to θ and ζθ = constant = α where σ is shear, θ the expansion, and ζ the coefficient of bulk viscosity. The ansatz ζθ = constant, was found to connect with the occurrence of Little Rip cosmology using Friedmann–Robertson–Walker metric given by Brevik et al. (Phys. Rev. D, 84, 103508 (2011)). We find that the model has constant expansion but represents accelerating phase. The model in general represents an anisotropic universe but in special case, it leads to an isotropic one. The spatial volume increases exponentially with time representing the inflationary scenario. The presence of bulk viscosity tends to increase the inflationary phase. Also, the model leads to the de Sitter model in a special case. The presence of bulk viscosity prevents the matter density to vanish at late time. The energy conditions as given by Kolassis et al. (Classical Quantum Gravity, 5, 1129 (1988)). Chatterjee and Banerjee (Gen. Relativ. Gravitation, 36, 303 (2004)) are also discussed. We find that the energy conditions are satisfied for stiff fluid inflationary universe with variable bulk viscosity.


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