Entropy and InformationFor over sixty years, since I first read Arthur Stanley Eddington's The Nature of the Physical World, as the "information philosopher" I have been struggling to understand and to find simpler ways to explain the concept of entropy. Even more challenging has been to find the best way to teach the mathematical and philosophical connections between entropy and information. A very strong connection is obvious because Ludwig Boltzmann's formula for entropy S is mathematically identical to Claude Shannon's expression for information I, but with a minus sign and different dimensions. Boltzmann entropy: S = k ∑ pi ln pi. Shannon information: I = - ∑ pi ln pi. Boltzmann entropy and Shannon entropy have different dimensions (S = joules/°K,
I = dimensionless "bits"), but they share the "mathematical isomorphism" of a logarithm of probabilities, which is the basis of both Boltzmann's and Gibbs' statistical mechanics.. The first entropy is material, the latter mathematical - indeed purely immaterial information. But they have deeply important connections which information philosophy must sort out and explain. First, both Boltzmann and Shannon expressions contain probabilities and statistics. Many philosophers and scientists deny any ontological indeterminism, such as the chance in quantum mechanics discovered by Albert Einstein in 1916. They may accept an epistemological uncertainty, as proposed by Werner Heisenberg in 1927. Today many thinkers propose chaos and complexity theories (both theories are completely deterministic) as adequate explanations, while they deny ontological chance. Ontological chance is the basis for creating any information structure. It explains the variation in species needed for Darwinian evolution. It underlies human freedom and the creation of new ideas. In statistical mechanics, the summation ∑ is over all the possible distributions of gas particles in a container. If the number of distributions is W , and the probability of all distributions is the same, the pi are all equal to 1/W and entropy is maximal: S = k ∑ 1/W ln 1/W, so S = k ln W. In the communication of information, W is the number of possible messages. If the probability of all messages is the same, pi are identical, I = - lnW. If there are N possible messages, then N bits of information are communicated by receiving one of them. On the other hand, if there is only one possible message, its probability is unity, and the information content is 1 ln 0 = zero. If there is only one possible message, no new information is communicated. This is the case in a deterministic universe, where past events completely cause present events. The information in a deterministic universe is a constant of nature. Religions that include an omniscient god often believe all that information is in God's mind. Note that if there are no alternative possibilities in messages, Shannon (following his Bell Labs colleague Ralph Hartley) says there can be no new information. We conclude that the creation of new information structures in the universe is only possible because the universe is in fact indeterministic and our futures are open and free. Thermodynamic entropy involves matter and energy, Shannon entropy is entirely mathematical, on one level purely immaterial information, though it cannot exist without "negative" thermodynamic entropy. It is true that information is neither matter nor energy, which are conserved constants of nature (the first law of thermodynamics). But information needs matter to be embodied in an "information structure." And it needs ("free") energy to be communicated over Shannon's information channels. Boltzmann entropy is intrinsically related to "negative entropy." Without pockets of negative entropy in the universe (and out-of-equilibrium free-energy flows), there would no "information structures" anywhere. Pockets of negative entropy are involved in the creation of everything interesting in the universe. It is a cosmic creation process without a creator.
Visualizing InformationThere is a mistaken idea in statistical physics that any particular distribution or arrangement of material particles has exactly the same information content as any other distribution. This is an anachronism from nineteenth-century deterministic statistical physics.