It is shown that the observed features of Hubble redshift can be explained within the framework of Einstein's general relativity. The observed Hubble redshift could be attributed to thus far unnoticed mechanism of time dilation coupled to curvature of space. Einstein's universe regains its status as a viable model predicting cosmological observations such as the (apparent) expansion of space and the observed acceleration of this expansion, without the necessity of introducing the cosmological constant. |
Derivation of Hubble constant of Einstein's universe
Consider Einstein's homogeneous universe filled with dust. Let photons move through this dust interacting with it only gravitationally. We will assume that energy conservation holds and that Newton's approximation can be applied. With these assumptions one can readily calculate energy transfer from photons to dust. To the observer at some distance from the light source this energy transfer will manifest itself as a change in wavelength, which is exactly what was observed by Hubble. The relativistic interpretation of this result allows the derivation of Hubble redshift (HR), including discovery that Hubble's constant depends on the distance between the place in deep space and the observer [1].
Let
d2E/dr2 = ΛE E | (1) |
E / Eo = exp( - r / RE ) | (2) |
dτ/dt = exp( - r / RE ) | (3) |
(d2τ/dtdr)2 - ΛE = 0 | (4) |
It follows from equation (2) or (3) equivalently, that the redshift, produced by HTD, is equal to
Z = (Eo - E) / E = exp( r / RE ) - 1 | (5) |
Ho = c / RE | (6) |
dH / dt = - Ho2 / 2 | (7) |
Conclusions
The analysis of Hubble redshift (HR) can be carried out using Einstein's general relativity and the law of conservation of energy. The observed HR can be attributed to the time dilation in the universe which remains stationary as predicted by Einstein in 1917.
In addition to reproducing the measured properties of HR, the approach outlined in this paper allows direct calculation of the important parameters of our universe such as the average density of space and the acceleration of its apparent expansion. While the formula for Hubble redshift, equation (5), can be derived directly from equation (2) obtained using Newtonian approximation, it is equation (3), which expresses the essential transition from Newtonian approach in which space and time are distinct, to a general relativistic spacetime.
The value of Einstein's cosmological constant turning out, seemingly accidentally, in eq. (1) allows to eliminate this constant from
Einstein's field equation (EFE) since as it was shown in the above
derivation of HR it has to add an additional energy term on the right
side of EFE to provide for apparent loss of photons energy due to the
Hubble time dilation as suggested by eq. (4).
Then EFE instead of Einstein's version of 1917
[5],
Rμν - (R / 2)gμν = 8πTμν + (H / 2)gμν | (8) |
Rμν = 8πTμν | (9) |
Acknowledgments
The author expresses his gratitude to Dr Halton Arp, Dr Helmut A. Abt, Dr Chris E. Adamson, Prof. John Baez, Prof. Tadeusz Balaban, Dr Krzysztof Bolejko, Prof. Michael Chodorowski, Dr Tom Cohoe, Prof. Marek Demianski, Dr Marijke Van Gans, Prof. Roy J. Glauber, Dr Mike Guillen, Prof. Alan Guth, Dr Martin J. Hardcastle, Dr Franz Haymann, Dr Chris Hillman, Dr Marek Kalinowski, Dr Alan P. Lightman, Prof. Krzysztof Meissner, Prof. Jozef M. Namyslowski, Dr Bjarne G. Nielsen, Prof. Bohdan Paczynski, Janina Pisera, BS, Dr Ramon Prasad, Dr Frank E. Reed, Dr Anrzej Szechter, Prof. Henryk Szymczak, Jerzy Tarasiuk, MS, Dr Michael S. Turner, Dr Slava Turyshev, Prof. Clifford M. Will, Prof. Ned Wright, and anonumous referees from various scientific journals, for the time they have spent discussing with the author the subject of the paper and related issues. The most thanks goes to Prof. Michael Chodorowski of CAMK-PAN (Copernican Astronomical Center of Polish Accademy of Science), without whose friendly critique the ideas expressed in this paper might have never developed to a legible state.
Bobliography
Appendix A: Detailed derivation of equation (1)
Let c be speed of light, G the Newtonian
gravitational constant, ρ the density of Einstein's
dust universe (while one galaxy corresponds to one dust
particle), the gravitational energy of dust gained through the
gravitational interaction of light with dust ("dynamical
friction") contained in the volume of a ball of dust of radius
r be Ed(r).
After photons of energy Eo are radiated out
from arbitrarily placed center of coordinate system called
"point zero" (point with radial coordinate
| (A.1) |
Integrating over all dust particles in a spherical layer of dust of radius r and thickness dr we get mass of this layer of dust at distance r from point zero as
| (A.2). |
Substituting (A.2) for mparticle in (A.1) the total force that is the source of gravitational energy of dust of this leyer becomes
| (A.3). |
Integrating both sides of (A.3) over all spherical layers between point zero and r to get total energy of dust, and differentiating both sides with respect to r to get rid of the integral on the right side of this equation, we get
| (A.4). |
Substitutig
| (A.5) |