On Saturday, September 14, 2019 at 10:07:28 AM UTC-5, Alan Grayson wrote:
>
>
>
> On Saturday, September 14, 2019 at 7:12:34 AM UTC-6, Alan Grayson wrote:
>>
>> If the early universe, say before the emergence of the CMBR, consisted of 
>> a random collection of electrons and photons, wouldn't this correspond to a 
>> *high*, not low entropy? Wouldn't it be analogous to gas with many 
>> possible states? Yet cosmologists seem hard pressed to explain an initial 
>> or early state assuming the entropy is low. AG
>>
>
> Here's an easier question: when Boltzmann defined entropy as S = k * log 
> N, why the log; why not just k*N? AG
>

 Think of the case where you have binary strings of length n. How many 
possible binary string are there with that length? There are N = 2^n. The 
Boltzman log(N) is just the size of the macrostate, where there are 2^n 
possible microstates. This is where the entropy S = kn comes from, for the 
units of Planck area on the horizon count microstates. We have 

S = k ln(N) = k ln(2^n) = k n ln(2).

With the black hole horizon or any horizon this linear chain is replaced by 
a two dimensional table or matrix. The same argument carries over.

LC

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