Appendix A. How Did the Thermal Radiation of the Decoupled Fire Ball Fly Off and Eject Freely into the Vast Cosmic Space, and Their Final Destination
As mentioned above, in our opinion, the 2.73K background radiation is an immense heat ocean, a natural and intrinsic existence in the closed universe.
Some researchers’ opinions are different from ours. They believe that the 2.73K background radiation is produced by the big bang. And they believe further that the 2.73K background radiation is the afterglow of the thermal radiation in the decoupled fire ball, 380,000 years after the big bang. From the decoupled thermal radiation to the 2.73K background radiation, there was an “adiabatic expansion” of a long, long duration.
We have explained above that their idea of the “adiabatic expansion” is not correct, the actual process should be a free ejection.
Figure 1.
The radius of the decoupled fire ball was about ao ≈ 5×105 light years, 380,000 years after the big bang. The diameter is ab ≈ 106 light years. once decoupled. all the thermal radiation within the whole decoupled fire ball aob began to fly off at the speed of light to leave it in all the directions. 5×106 years later, the radiations from the whole sphere aob in the direction of oo′ reached a new place of a sphere a′o′b′, within the spherical layer a′b′ ≈ 106 light years′. And all the thermal radiation from the decoupled fire ball in all the directions in the 4π solid angle all reached the spherical layer a′b′ with a width of a′b′ = 106 light years, the big blue spherical layer in this figure.
Figure 1.
The radius of the decoupled fire ball was about ao ≈ 5×105 light years, 380,000 years after the big bang. The diameter is ab ≈ 106 light years. once decoupled. all the thermal radiation within the whole decoupled fire ball aob began to fly off at the speed of light to leave it in all the directions. 5×106 years later, the radiations from the whole sphere aob in the direction of oo′ reached a new place of a sphere a′o′b′, within the spherical layer a′b′ ≈ 106 light years′. And all the thermal radiation from the decoupled fire ball in all the directions in the 4π solid angle all reached the spherical layer a′b′ with a width of a′b′ = 106 light years, the big blue spherical layer in this figure.
Now, let us show how the remnant 3,000K thermal radiation in the decoupled fire ball ejected freely to the exterior vast cosmic space, and their final destination.
First, as shown in Figure 1, the small ball with the diameter ab in the central part of the figure represents the decoupled fireball, 380,000 years after the big bang. Its radius is approximately oa ≈ 10 22 m = 5×105 light years. (For convenience of discussion, we make up a round number for the radius here, oa ≈ 5×105 light years, and the diameter is ab ≈ 1×106 light years.)
When the decouple happened, the fire ball became transparent. All the thermal radiation in the fireball immediately started to fly off in all the directions at the speed of light to the exterior vast cosmic space, and travels straight forward farther and farther. Obviously, it is just a free ejection, not an “adiabatic expansion”.
Let us see how the thermal radiation flied freely to the infinitively vast space.
5×106 years later, the thermal radiation from point o, and in the direction of oo', reached point o', oo' = 10 oa = 5×106 light years, as shown in Figure 1. The thermal radiation from point a reached point a', the thermal radiation from point b reached point b'. All the thermal radiations in the direction of oo' from all the points of the decoupled fire ball aob now reached the corresponding points of an equal ball a'o'b', which lay in the spherical layer a'b', obviously a'b' = 106 light years.
And all the thermal radiations ejected from the decoupled fireball aob
in all the different directions in the 4π solid angle now all reached points within the whole spherical layer a′b′, as shown in Figure 1. The thickness of the spherical layer a′b′ equals the diameter of the small ball ab,
5 ×10
7 years after the decouple, all the thermal radiation from point o arrived at the spherical surface of the radius of oo'' = 5 ×10
7 light years (oo'' = 100 oa), as shown in Figure 2. And in the direction of oo'', the thermal radiation from point a reached point a'', the thermal radiation from point o reached point o'', the thermal radiation from point b reached point b''. All the thermal radiations in the direction of oo'' from all the points of the decoupled fire ball aob now reached the corresponding points of an equal ball a''o''b'', which lay in the spherical layer a''b''. And, all the thermal radiations from all the points of the small ball aob
in all the different directions in the 4π solid angle now all reached the points within the whole spherical layer a'' b''. Obviously,
Figure 2.
5 ×107 years after the decoupling, in the direction of oo'', the radiation from o reached point o'',and the radiation from a reached a'', the radiation from b reached b''. The radiation from all the points of the decoupling ball aob reached the corresponding points of ball a''o''b'', laying in the spherical layer a''b''. And, the radiation from all the points of the ball aob in all the directions in the 4π solid angle reached the spherical layer a''b'',.
Figure 2.
5 ×107 years after the decoupling, in the direction of oo'', the radiation from o reached point o'',and the radiation from a reached a'', the radiation from b reached b''. The radiation from all the points of the decoupling ball aob reached the corresponding points of ball a''o''b'', laying in the spherical layer a''b''. And, the radiation from all the points of the ball aob in all the directions in the 4π solid angle reached the spherical layer a''b'',.
Similarly, 5 ×10
8 years later,all the radiations from all the points of the small ball aob (i.e., from the whole decoupled fire ball at
t = 380,000 years) and
in all the different directions in the 4π solid angle, all reached the correspondent points within the whole spherical layer a'''b''',
And, 5 ×10
9 years later, 5 ×10
10 years later,and so on, as the thermal radiation ejected freely from the decoupled fireball aob, flied outward continuously at the speed of light, it always keeps within a spherical layer with a thickness of 10
6 light years,
The expanding of this spherical layer of the thermal radiation of a thickness of 106 light years, (ab), a′b′, a''b'', a'''b''', a''''b'''', a'''''b''''' ……, and so on, should not go on and on at the light speed to the farther and farther space without an end. Because the space of the universe is closed, when some utmost possible position is reached, the thermal radiation layer of a thickness of 106 light years will no longer fly away further. It will return back to the central region of the universe, and passing through the central region, travel to their far most positions on the other side of the central region. In such away, the layer of the 106 light years will keep shuttling in the closed universe ceaselessly, meanwhile, getting more and more dispersive.
Finally, after an extremely long relaxation time, by interactions (exchange heat) with the cosmic atoms, molecules, dusts or rocks (these matter are all at 2.73K) and so on in the metagalaxy region. And all the thermal radiation from the decoupled fire ball will eventually mingle into the 3K heat ocean, That is their final destination.
So, the authors behold that, the 2.73K background radiation discovered by Penzias and Wilson in 1965 is not the afterglow of the decoupled fire ball. It is not produced by the big bang. It itself is just an extremely immense intrinsic 3K vast heat ocean in the closed universe. It existed before the big bang, it exists now, and it will exist in the future.
In the above discussion, for the sake of concise, we postponed a detail about the process of the light and heat ejected from the surface of the expanding fireball from the time of the big bang to the decouple time, i.e., from t1 = 0 to t2 = 380,000 years. Now we make it up as follows.
Please have a look at Figure 3.
After the big bang, the expanding fireball was initially at an extremely high temperature. The temperature descended very rapidly as it expanded. In this process, the whole interior of the fireball was plasma at extremely high temperature, which was totally opaque for the interior thermal radiation. So, the thermal radiation within the expanding fireball could not eject outward freely to leave the fireball.
Figure 3.
Another spherical layer with a width of c'a' = 380,000 light years (shown as a “yellow” one in the figure) just out the spherical layer of 106 light years (the “blue” ones a′b′, a''b'', a'''b''', ……).
Figure 3.
Another spherical layer with a width of c'a' = 380,000 light years (shown as a “yellow” one in the figure) just out the spherical layer of 106 light years (the “blue” ones a′b′, a''b'', a'''b''', ……).
However, in the same duration, the surface of the expanding fire ball was also plasma at a lower and also descending temperature, but its temperature still kept very high. This surface of the expanding fire ball should eject thermal radiation ceaselessly, from t1= 0 to t2= 380,000 years.
Let us make a compare: as is well known, the temperature at the central part of the sun is about 15000K, and the temperature at the surface of the sun is about 6000K. The interior thermal radiation of the sun cannot fly off the sun, because the interior plasma is totally opaque for the thermal radiation. Only the surface of the sun, which is exposed to the exterior space, would eject light and heat ceaselessly. And the temperature of the ejected light and heat is about 6000K.
Similarly, the descending temperature at the surface of the expanding fire ball in the duration from the big bang to the decouple time was also still be extremely high. The surface kept being plasma until the decouple happened, and it was exposed to the vast exterior space. Like the surface of the sun, the surface of the expanding primitive fire ball should eject thermal radiation continuously, from
t1 = 0 to
t2 = 380,000 years. Hence, just out the expanding spherical layer with a width of 10
6 light years (the expanding “blue” spherical layer as shown in Figure 1 and Figure 2),
there is another spherical layer of a width of 380,000 light years, the “yellow” one spherical layer in Figure 3.
The two layers both ejected outward at light speed, one after the other, the yellow one progresses ahead and the blue one follows. After reaching their far-most positions in the closed universe, they will both return back, still one after the other.
Then they will keep shuttering in the closed universe, becoming more and more dispersive. After a long, long relaxation time, finally, both the “blue” and “yellow” thermal radiations should mingle into the stable immense 2.73K heat ocean.