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Martin mpc 128 universes
Martin mpc 128 universes




Thus, although the pressure is not zero at the center of symmetry, r = 0, the effect of acceleration is nondetectable at the center, since the acceleration scalar vanishes there. This limit gives a value for the acceleration scalar u˙ of order |u˙|<~0.66×10 -10r Mpc -1, where r is the radial coordinate in the model. The choice of model parameters is quite robust: in order to obtain a good fit to the current data, one requires only that the non-uniform pressure parameter a in one of the models be negative and satisfy |a| <~ 3 km 2 s -2 Mpc -1. The Stephani models considered here could, therefore, significantly alleviate the conflict between recent cosmological and astrophysical age predictions. Our Stephani models, on the other hand, can give a good fit to the data with an age of up to 15 Gyr. Based on this value for H 0 and assuming Λ >= 0, the data would imply a Friedmann age of at most 13 Gyr and in fact a best-fit (for q 0 = 0.5) age of only 10 Gyr. Several recent calibrations of the Hubble parameter from the Hubble diagram of SN Ia's and other distance indicators indicate a value of H 0 ~= 65 and a Hubble time of ~15 Gyr. We claim that this paper is the first attempt to compare inhomogeneous models of the universe with real astronomical data.

martin mpc 128 universes

We show that this age increase is obtained for a wide range of the non-uniform pressure parameters of the Stephani models. By a particular choice of model parameters, we show that these models can give an excellent fit to the observed redshifts and (corrected) B-band apparent magnitudes of the data, but for an age of the universe that is typically about 2 Gyr-and may be more than 3 Gyr-greater than in the corresponding Friedmann model, for which nonnegative values of the deceleration parameter appear to be favored by the data. We use the redshift-magnitude relation, as derived by Dąbrowski, for the two exact non-uniform pressure spherically symmetric Stephani universes with the observer positioned at the center of symmetry in order to test the agreement of these models with recent observations of high-redshift Type Ia supernovae (SN Ia's).






Martin mpc 128 universes