Boltzmann–Gibbs entropy in statistical mechanics
E45253
Boltzmann–Gibbs entropy in statistical mechanics is the standard measure of disorder or uncertainty in a system, quantifying how many microscopic configurations correspond to a given macroscopic state and forming the basis of classical equilibrium statistical mechanics.
All labels observed (6)
| Label | Occurrences |
|---|---|
| Boltzmann entropy | 7 |
| Boltzmann entropy formula | 4 |
| Gibbs entropy | 4 |
| Boltzmann–Gibbs entropy in statistical mechanics canonical | 1 |
| Boltzmann–Gibbs statistical mechanics | 1 |
| Gibbs paradox | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T356724 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
Target entity: Boltzmann–Gibbs entropy in statistical mechanics Context triple: [Shannon–Khinchin axioms, characterizes, Boltzmann–Gibbs entropy in statistical mechanics]
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A.
Tsallis entropy
Tsallis entropy is a generalized, nonadditive entropy measure in statistical mechanics and information theory that extends Shannon entropy to better describe complex, nonextensive systems.
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B.
Rényi entropy
Rényi entropy is a generalized measure of information and uncertainty that extends Shannon entropy by introducing a tunable order parameter to emphasize different aspects of a probability distribution.
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C.
Maxwell–Boltzmann statistics
Maxwell–Boltzmann statistics is a classical statistical framework in physics that describes the distribution of speeds or energies among distinguishable, non-quantum particles in thermal equilibrium.
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D.
Shannon–Khinchin axioms
The Shannon–Khinchin axioms are a set of fundamental conditions that uniquely characterize Shannon entropy as the standard measure of information and uncertainty in probability theory and information theory.
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E.
Bekenstein–Hawking entropy
Bekenstein–Hawking entropy is the thermodynamic entropy associated with a black hole, proportional to the area of its event horizon and fundamental in linking gravity, quantum theory, and thermodynamics.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Boltzmann–Gibbs entropy in statistical mechanics Target entity description: Boltzmann–Gibbs entropy in statistical mechanics is the standard measure of disorder or uncertainty in a system, quantifying how many microscopic configurations correspond to a given macroscopic state and forming the basis of classical equilibrium statistical mechanics.
-
A.
Tsallis entropy
Tsallis entropy is a generalized, nonadditive entropy measure in statistical mechanics and information theory that extends Shannon entropy to better describe complex, nonextensive systems.
-
B.
Rényi entropy
Rényi entropy is a generalized measure of information and uncertainty that extends Shannon entropy by introducing a tunable order parameter to emphasize different aspects of a probability distribution.
-
C.
Maxwell–Boltzmann statistics
Maxwell–Boltzmann statistics is a classical statistical framework in physics that describes the distribution of speeds or energies among distinguishable, non-quantum particles in thermal equilibrium.
-
D.
Shannon–Khinchin axioms
The Shannon–Khinchin axioms are a set of fundamental conditions that uniquely characterize Shannon entropy as the standard measure of information and uncertainty in probability theory and information theory.
-
E.
Bekenstein–Hawking entropy
Bekenstein–Hawking entropy is the thermodynamic entropy associated with a black hole, proportional to the area of its event horizon and fundamental in linking gravity, quantum theory, and thermodynamics.
- F. None of above. chosen
Statements (48)
| Predicate | Object |
|---|---|
| instanceOf |
information measure
ⓘ
statistical mechanical entropy ⓘ thermodynamic entropy ⓘ |
| additivityProperty | additive for statistically independent subsystems ⓘ |
| appearsOn | Boltzmann’s tombstone formula S = k_B ln W ⓘ |
| appliesTo |
canonical ensemble
ⓘ
classical systems in equilibrium ⓘ grand canonical ensemble ⓘ microcanonical ensemble ⓘ |
| assumes |
ergodic hypothesis
ⓘ
short-range interactions in typical applications ⓘ |
| basisOf | classical equilibrium statistical mechanics ⓘ |
| concavityProperty | concave functional of the probability distribution ⓘ |
| continuousVersionName |
Boltzmann–Gibbs entropy in statistical mechanics
self-linksurface differs
ⓘ
surface form:
Gibbs entropy
|
| contrastedWith |
Rényi entropy
ⓘ
Tsallis entropy ⓘ |
| domain |
continuous probability densities
ⓘ
discrete probability distributions ⓘ |
| field |
information theory
ⓘ
statistical mechanics ⓘ thermodynamics ⓘ |
| historicalOrigin | late 19th century ⓘ |
| increasesWith | irreversible processes ⓘ |
| maximizationYields | Boltzmann distribution ⓘ |
| maximizedUnder |
constraints on average energy
ⓘ
normalization of probabilities ⓘ |
| monotonicWith | number of accessible microstates ⓘ |
| namedAfter |
Josiah Willard Gibbs
ⓘ
Ludwig Boltzmann ⓘ |
| quantifies |
disorder
ⓘ
number of microscopic configurations compatible with a macroscopic state ⓘ uncertainty ⓘ |
| relatedTo |
Boltzmann–Gibbs entropy in statistical mechanics
self-linksurface differs
ⓘ
surface form:
Boltzmann entropy
Boltzmann–Gibbs entropy in statistical mechanics self-linksurface differs ⓘ
surface form:
Gibbs entropy
H-theorem ⓘ Maxwell–Boltzmann statistics ⓘ
surface form:
Maxwell–Boltzmann distribution
Shannon entropy ⓘ canonical partition function ⓘ second law of thermodynamics ⓘ |
| standardFormula |
S = -k_B \sum_i p_i \ln p_i
ⓘ
S = k_B \ln W ⓘ |
| symbol | S ⓘ |
| unit | joule per kelvin ⓘ |
| usedFor |
characterizing equilibrium states
ⓘ
defining free energy ⓘ defining temperature in statistical mechanics ⓘ deriving thermodynamic relations ⓘ |
| usesConstant | Boltzmann constant ⓘ |
How these facts were elicited
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Subject: Boltzmann–Gibbs entropy in statistical mechanics Description of subject: Boltzmann–Gibbs entropy in statistical mechanics is the standard measure of disorder or uncertainty in a system, quantifying how many microscopic configurations correspond to a given macroscopic state and forming the basis of classical equilibrium statistical mechanics.
Referenced by (18)
Full triples — surface form annotated when it differs from this entity's canonical label.