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Entropy
Entropy is a technical quantity in at least a dozen fields, and the question of whether they are all measuring the same thing has an answer more interesting than either yes or no.
This page gathers the homes of the word. The thermodynamic side — where it began, and where its interpretation is most contested — is treated at length in the thermodynamics bundle and is not restated here.
The name
Rudolf Clausius coined it in 1865, and explained his reasoning in the paper:
If we wish to designate S by a proper name we can say of it that it is the transformation content of the body… However, since I think it is better to take the names of such quantities as these, which are important for science, from the ancient languages, so that they can be introduced without change into all the modern languages, I proposed to name the magnitude S the entropy of the body, from the Greek word ἡ τροπή, a transformation. I have intentionally formed the word entropy so as to be as similar as possible to the word energy, since both these quantities… are so nearly related to each other in their physical significance that a certain similarity in their names seemed to me advantageous.
Shannon’s adoption of the same word in 1948 has no comparable record, and the story that fills the gap is doubtful. In the familiar telling, von Neumann advised him to use it because “nobody knows what entropy really is, so in a debate you will always have the advantage” — recorded by Myron Tribus and Edward McIrvine in Scientific American in 1971. When Robert Price put it to Shannon directly in 1985, noting that Shannon’s classified 1945 cryptography report already used the word and that he had not been in contact with von Neumann then, Shannon answered: “No, I don’t think he did… I’m quite sure that it didn’t happen between von Neumann and me.” He added that he had known entropy from thermodynamics, “that goes way back”, and recalled having been told the same story about himself by a physicist — whom Price identified as Jaynes. The anecdote had circulated back to its own supposed source.
The family, and its outsiders
The most direct treatment of the question is Roman Frigg and Charlotte Werndl’s “Entropy — A Guide for the Perplexed” (2011), which surveys the thermodynamic, information-theoretic, statistical-mechanical, dynamical-systems and fractal entropies. Their conclusion is that all of them except the thermodynamic and the topological can be understood as variants of some information-theoretic notion — while insisting that “different notions of entropy have different meanings and play different roles.”
They also supply the instrument for asking the question, borrowed from Mary Hesse: the distinction between formal and material analogy. Two quantities are formally analogous when the same mathematical expressions describe them, and materially analogous when they share intrinsic properties beyond the mathematics. The distinction does real work — they judge the dynamical-systems entropies formally but not materially analogous to the information-theoretic ones, and conclude that claims of analogy in the literature are to that extent misleading.
Whether the recurrence amounts to unity is disputed. On the systematising side, the Shannon–Khinchin axioms pin the functional form tightly: continuity, maximality, expansibility and separability, with “generalized entropies” being those that relax the last. Anything measuring uncertainty over a distribution lands near Shannon’s expression because very little else satisfies the constraints. Against this, a line of argument running through David Feldman and James Crutchfield’s “Measures of statistical complexity: Why?” (1998) and their comment with Cosma Shalizi on a proposed complexity measure (2000) holds that a quantity of this kind means something only relative to the question asked and the structure being asked about — and that a measure which appears to apply universally is for that reason suspect rather than reassuring. A related point arrives from the other side of the same exchange: Mark Davison and J. S. Shiner’s “Many Entropies, Many Disorders” (2003) argues that which maximum entropy serves as the right reference depends on the constraints in play — the equiprobable distribution for one question, the corresponding equilibrium system for another — so that there are as many disorders as there are defensible choices of normaliser. They make the point to refine the measure rather than to doubt it.
Where the word does technical work
Information theory. Shannon’s entropy (1948) measures the average surprise of a source. The descendants are genuinely connected rather than merely named alike: Rényi entropy (1961) generalises it with a uniqueness theorem, Shannon being the limiting case; relative entropy, or Kullback–Leibler divergence, is arguably the more primitive quantity, since Shannon entropy can be written in terms of it and it survives to continuous spaces where differential entropy does not; and cross entropy is the quantity minimised by most of contemporary machine learning, where it coincides with maximum likelihood. Tsallis entropy is a well-defined functional, but the non-extensive statistical mechanics programme built on it is contested — the constraint choices have been argued to be unmotivated, and critics note that varying them can produce whichever distribution is wanted.
Algorithmic information theory. Kolmogorov complexity measures the length of the shortest program producing a string — a property of an individual object rather than of a distribution. Its relation to Shannon entropy is a theorem rather than an analogy: expected complexity and entropy agree to within a constant. The constant is the complexity of the distribution itself and is unbounded across distributions, which popular accounts tend to drop.
Dynamical systems. Kolmogorov–Sinai entropy applies Shannon’s functional to the measures of a partition, and for Bernoulli shifts returns Shannon’s own number — the tightest link in the family. It was introduced for the isomorphism problem rather than for chaos, and Ornstein proved in 1970 that it is a complete invariant for that class. Topological entropy was built by imitating the construction with open covers, and is connected to the measure-theoretic version by a variational principle; it is also the quantity Frigg and Werndl place outside the information-theoretic family.
The deepest connection back to physics runs through the thermodynamic formalism of Sinai, Ruelle and Bowen, where pressure corresponds to free energy, Gibbs states to Gibbs states, and the variational principle takes the form of a free-energy principle. A one-dimensional lattice gas and a subshift of finite type are the same mathematical object. What transfers is mathematical structure: the “energy” is an arbitrary potential and the “temperature” a formal parameter.
Ecology. The Shannon diversity index applies Shannon entropy unmodified to species abundances — introduced by Ramon Margalef in 1957, and commonly miscredited to “Shannon–Weaver” after the 1949 book whose second author wrote an expository essay rather than the measure. The field has since largely moved past the raw index: Lou Jost argued in 2006 that entropies are not diversities, since they fail the replication principle, and that the fix is to exponentiate into effective numbers of species — the Hill numbers, which are the effective-number transforms of the Rényi entropies. Ecology adopted the conversion. An earlier eliminativist position, Stuart Hurlbert’s “The nonconcept of species diversity” (1971), argued instead for abandoning the information-theoretic apparatus; his rarefaction methods survived, his eliminativism did not.
Molecular biology. Sequence logos, following Thomas Schneider and Michael Stephens (1990), measure position-wise information content in bits with an operational reading in substitution tolerance. Methylation entropy is a genuine Shannon computation that predicts chronological age out of sample.
Economics. The Theil index of inequality is redundancy in Shannon’s exact sense — the gap between maximum and observed entropy of income shares, equivalently a divergence of income shares from population shares. It belongs to the generalized entropy family, which is the only class both additively decomposable by subgroup and satisfying the Pigou–Dalton condition, and that characterisation is why it persists where the Gini coefficient cannot decompose. Nicholas Georgescu-Roegen’s The Entropy Law and the Economic Process (1971) is a different kind of contribution — a methodological critique of economics for modelling production as a circular flow blind to irreversibility, and the founding text of ecological economics. His proposed “fourth law of thermodynamics”, holding that material entropy must also increase irreversibly, was rejected by the field he founded, on the grounds that the Earth is closed to matter but open to energy, so material entropy can be reduced indefinitely by exporting heat.
Contested uses
Some applications of the word are disputed within their own fields, and the disputes are worth separating from the settled uses above.
The proposal that ageing is driven by a loss of epigenetic information — David Sinclair’s information theory of ageing, set out in Cell in 2023 — has been challenged in the same journal, in a 2024 correspondence titled “The information theory of aging has not been tested”, which attributes the reported phenotype to the cytotoxicity of the experimental system rather than to information loss. Methylation entropy, a distinct and narrower quantity, is a Shannon computation over methylation states that predicts chronological age out of sample. The looser claim that ageing is entropy increase in the thermodynamic sense sits outside both: organisms exchange energy with their surroundings, and the second law constrains isolated systems.
“Network entropy” names several non-equivalent quantities — degree-distribution, von Neumann, Körner, random-walk and ensemble versions — and their relations are not settled. Whether entropy is a good measure of network complexity has been questioned directly in the complexity literature, where it has been argued to be easily misled by structures it was not designed for. The maximum-entropy ensemble methods, including exponential random graph models, stand on firmer ground.
Frigg and Werndl’s instrument applies to these cases as it does to the others. Where a use is materially analogous — sharing intrinsic properties with the information-theoretic quantity, not only its expression — the mathematics carries the argument. Where the analogy is formal only, the shared name can suggest a connection the derivation has not established, and their judgement on the dynamical-systems entropies shows this can happen in the technical core of a field as easily as at its edges.
See also: Thermodynamics — and what entropy is for the thermodynamic quantity and its competing readings · Shannon · Boltzmann · Gibbs · Emergence — a word in a comparable situation