Zipsey,

If you care to understand how black communicate with each other, read
http://arxiv.org/pdf/1308.0289v1.pdf.
clem

On Sat, Nov 15, 2014 at 4:46 PM, <[email protected]> wrote:

>
>
> On Saturday, November 15, 2014 9:36:57 PM UTC, [email protected] wrote:
>>
>>
>>
>> On Saturday, November 15, 2014 4:57:14 PM UTC, John Clark wrote:
>>>
>>>
>>>
>>> On Fri, Nov 14, 2014 at 5:23 PM, meekerdb <[email protected]> wrote:
>>>
>>> > "The numbers of ways the system could have gotten to the way it is"
>>>> isn't the usual formulation
>>>
>>>
>>> If you want to say that Entropy is proportional to the number of
>>> microstates that produce the same macrostate then it's also proportional to
>>> the number of precursor states.
>>>
>>> > and I think it's ambiguous.  In general there are arbitrarily many
>>>> possible histories and different possible starting points.
>>>>
>>>
>>> Unless you're talking about hypothetical new physics there are not
>>> arbitrarily many previous states that could have produced the present
>>> state, just a astronomical number.
>>>
>>> > Boltzmann's formulation was the logarithm of the numbers of possible
>>>> states consistent with constraints defining the system, e.g. its total
>>>> kinetic energy
>>>>
>>>
>>> Entropy is inversely proportional to work not kinetic energy. A box of
>>> gas may have a lot of kinetic energy because all the atoms in it are moving
>>> around  at high speed, but they're all moving in different directions,
>>> Entropy is a measure of how well all that activity can be translated into
>>> moving something in just one direction (work). The higher the Entropy the
>>> less work you can get out of it with the same heat sink
>>>
>>> > In the case of a BH the constraints are its classical defining
>>>> parameters: mass, angular momentum, and electric charge.
>>>>
>>>
>>> Yes, a Black Hole is the simplest macroscopic thing in the universe,
>>> just 3 numbers tells you all there is to know about a particular one; but
>>> there are a gargantuan number of ways that Black Hole could have formed,
>>> perhaps it was made by putting a lot of sand together in one place, or
>>> encyclopedias or too many puppy dogs, it doesn't matter. And that's why
>>> Black Holes have such a enormous Entropy.
>>>
>>
>>  Would you help me to understand this?
>>
>> It's just that I'm seeing the number of ways a black hole could have
>> formed as a non-physical conception that depends ....some kind of
>> information deficit across the event horizon.
>>
>> Like, if I have special information...like maybe a theory....that
>> eliminates 50 percent of the ways a specific black hole could have formed,
>> by some process of elimination. The entropy should now physically read half
>> what it did to start with.
>>
>
> Isn't this an approach on what Susskind contributes as the holographic
> principle (or as what then leads to that)
>
> Along with the time invariant term in that equation...that has the outside
> observer see the falling man freeze at the event horizon as a badly mangled
> splodge of subatomic fragmentation.
>
> That then acts as the informational record of everything that goes inside.
> Which makes Hawking look like a right plum circa 1985
>
>
>
>>
>>
>>
>>
>>
>>   John K Clark
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>
>>>  Classically there is no finer grained description, so that's what seems
>>> to make BH entropy more fundamental that the usual thermodynamic system.
>>>
>>>>
>>>> Brent
>>>>
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>>>
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