On 23.01.2012 01:26 Russell Standish said the following:
On Sun, Jan 22, 2012 at 07:16:23PM +0100, Evgenii Rudnyi wrote:
On 20.01.2012 05:59 Russell Standish said the following:
On Thu, Jan 19, 2012 at 08:03:41PM +0100, Evgenii Rudnyi wrote:
and since information is measured by order, a maximum of order
is conveyed by a maximum of disorder. Obviously, this is a
Babylonian muddle. Somebody or something has confounded our
I would say it is many people, rather than just one. I wrote "On
Complexity and Emergence" in response to the amount of
unmitigated tripe I've seen written about these topics.
I have read your paper
It is well written. Could you please apply the principles from
your paper to a problem on how to determine information in a book
(for example let us take your book Theory of Nothing)?
Also do you believe earnestly that this information is equal to
the thermodynamic entropy of the book?
These are two quite different questions. To someone who reads my
book, the physical form of the book is unimportant - it could just as
easily be a PDF file or a Kindle e-book as a physical paper copy. The
PDF is a little over 30,000 bytes long. Computing the information
content would be a matter of counting the number 30,000 long byte
strings that generate a recognisable variant of ToN when fed into
Acrobat reader. Then subtract the logarithm (to base 256) of this
figure from 30,000 to get the information content in bytes.
This is quite impractical, of course, not to speak of expense in
paying for an army of people to go through 256^30,000 variants to
decide which ones are the true ToN's. An upper bound can be found by
compressing the file - PDFs are already compressed, so we could
estimate the information content as being between 25KB and 30KB
Yet, this is already information. Hence if take the equivalence between
the informational and thermodynamic entropies literally, then even in
this case the thermodynamic entropy (that should be possible to measure
by experimental thermodynamics) must exist. What it is in this case?
To a physicist, it is the physical form that is important - the fact
that it is made of paper, with a bit of glue to hold it together.
The arrangement of ink on the pages is probably quite unimportant - a
book of the same size and shape, but with blank pages would do just
as well. Even if the arrangement of ink is important, then does
typesetting the book in a different font lead to the same book or a
It is a good question and in my view it again shows that thermodynamic
entropy and information are some different things, as for the same
object we can define the information differently (see also below).
To compute the thermodynamic information, one could imagine
performing a massive molecular dynamics simulation, and then count
the number of states that correspond to the physical book, take the
logarithm, then subtract that from the logarithm of the total
possible number of states the molecules could take on (if completely
Do not forget that molecular dynamics simulation is based on the Newton
laws (even quantum mechanics molecular dynamics). Hence you probably
mean here the Monte-Carlo method. Yet, it is much simpler to employ
experimental thermodynamics (see below).
This is, of course, completely impractical. Computing the complexity
of something is generally NP-hard. But in principle doable.
Now, how does this relate to the thermodynamic entropy of the book?
It turns out that the information computed by the in-principle
process above is equal to the difference between the maximum entropy
of the molecules making up the book (if completely disassociated) and
the thermodynamic entropy, which could be measured in a calorimeter.
If yes, can one determine the information in the book just by means
of experimental thermodynamics?
One can certainly determine the information of the physical book
(defined however you might like) - but that is not the same as the
information of the abstract book.
Let me suggest a very simple case to understand better what you are
saying. Let us consider a string "10" for simplicity. Let us consider
the next cases. I will cite first the thermodynamic properties of Ag and
Al from CODATA tables (we will need them)
S ° (298.15 K)
J K-1 mol-1
Ag cr 42.55 ą 0.20
Al cr 28.30 ą 0.10
In J K-1 cm-3 it will be
Ag cr 42.55/107.87*10.49 = 4.14
Al cr 28.30/26.98*2.7 = 2.83
1) An abstract string "10" as the abstract book above.
2) Let us make now an aluminum plate (a page) with "10" hammered on it
(as on a coin) of the total volume 10 cm^3. The thermodynamic entropy is
then 28.3 J/K.
3) Let us make now a silver plate (a page) with "10" hammered on it (as
on a coin) of the total volume 10 cm^3. The thermodynamic entropy is
then 41.4 J/K.
4) We can easily make another aluminum plate (scaling all dimensions
from 2) to the total volume of 100 cm^3. Then the thermodynamic entropy
is 283 J/K.
Now we have four different combinations to represent a string "10" and
the thermodynamic entropy is different. If we take the statement
literally then the information must be different in all four cases and
defined uniquely as the thermodynamic entropy is already there. Yet in
my view this makes little sense.
Could you please comment on this four cases?
P.S. Why it is impossible to state that a random string is
generated by some random generator?
Not sure what you mean, unless you're really asking "Why it is
impossible to state that a random string is generated by some
In which case the answer is that a pseudorandom generator is an
algorithm, so by definition doesn't produce random numbers. There is
a lot of knowledge about how to decide if a particular PRNG is
sufficiently random for a particular purpose. No PRNG is
sufficiently random for all purposes - in particular they are very
poor for security purposes, as they're inherently predictable.
I understand. Yet if we take a finite random string, then presumably
there should be some random generate with some seed that produces it.
What would be wrong with this?
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