Treatment originally used to discard inverse square law as solution to Olbers' paradox was not set up correctly. If we include sensor (camera) in the treatment and model light as photons the result describes what we actually see.

Treatment originally used to discard inverse square law as solution to Olbers' paradox was not set up correctly. If we include sensor (camera) in the treatment and model light as photons the result describes what we actually see.
Sure. I'd prefer to give you some more "official" reference, like Wikipedia, but they don't even mention it. There are papers about it of course, but overall I found the subject is quite overlooked, which is what inspired my curiosity in the first place. It seems as if conclusion was made few hundred years ago by some famous names and since then it's like no one bothered to seriously reconsider it. In any case this how it goes:
http://www.asterism.org/tutorials/tut091.htm
Since the area of a sphere of radius r is
A = 4p r2 (1)
the volume of such a shell is
V = 4p r2t (2)
If the density of each of the luminous objects within the shell is "n", then the total number of these objects in the shell must be
N = 4p r2nt (3)
Now let us ask just what amount of energy such a shell will send to the Earth. Since the shell's thickness is small, it is reasonable to assume that the entire shell is at a distance "r" from the earth. The energy, E, emitted by any source at distance r, produces an intensity, "I", over a given area, A, on the Earth of (inverse square law)
I = E/4p r2 (4)
The total intensity received on the Earth from all the sources in the shell r units away must then be the intensity produced by each source times the total number of sources or
T = IN (5)
Substituting the value of N previously calculated into the above, we find that
T = tnE (6)
We notice at once that the total energy received from any chosen shell does not depend upon its distance from us (no r in the above equation). The total energy received from all the shells is the sum of the contributions of each shell. If there are M shells this total is
S = tnEM (7)
But there is an infinite number of shells and so the total intensity on the earth must be infinite. Therefore, the nighttime sky should be blindingly bright!
Pardon me, Wikipedia actually does mention it. It seems that's what this paradox is all about. I suppose it was natural to expect inverse square law is the solution, but when they found that it is not, that's when they started calling it a paradox.
Olbers' paradox  Wikipedia, the free encyclopedia
 The paradox is that a static, infinitely old universe with an infinite number of stars distributed in an infinitely large space would be bright rather than dark. To show this, we divide the universe into a series of concentric shells, 1 light year thick (say). Thus, a certain number of stars will be in the shell 1,000,000,000 to 1,000,000,001 light years away, say. If the universe ishomogeneous at a large scale, then there would be four times as many stars in a second shell between 2,000,000,000 to 2,000,000,001 light years away. However, the second shell is twice as far away, so each star in it would appear four times dimmer than the first shell. Thus the total light received from the second shell is the same as the total light received from the first shell. Thus each shell of a given thickness will produce the same net amount of light regardless of how far away it is. That is, the light of each shell adds to the total amount. Thus the more shells, the more light. And with infinitely many shells there would be a bright night sky.
Well, these classical treatments are all based on the assumption that the universe is static  we know now that it isn't.
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