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.
Observed surface forms (5)
| Surface form | Occurrences |
|---|---|
| Boltzmann–Gibbs entropy | 0 |
| Boltzmann entropy | 5 |
| Boltzmann entropy formula | 4 |
| Gibbs entropy | 3 |
| Gibbs paradox | 1 |
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 ⓘ |
Referenced by (14)
Full triples — surface form annotated when it differs from this entity's canonical label.
this entity surface form:
Boltzmann entropy formula
Boltzmann–Gibbs entropy in statistical mechanics
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Boltzmann–Gibbs entropy in statistical mechanics
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subject surface form:
Boltzmann–Gibbs entropy
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Gibbs entropy
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Gibbs paradox
this entity surface form:
Boltzmann entropy formula
this entity surface form:
Boltzmann entropy formula
this entity surface form:
Boltzmann entropy formula
this entity surface form:
Gibbs entropy
Maxwell's demon thought experiment
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relatedConcept
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Boltzmann–Gibbs entropy in statistical mechanics
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this entity surface form:
Boltzmann entropy
this entity surface form:
Boltzmann entropy
Boltzmann–Gibbs entropy in statistical mechanics
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relatedTo
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Boltzmann–Gibbs entropy in statistical mechanics
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subject surface form:
Boltzmann–Gibbs entropy
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Gibbs entropy
Boltzmann–Gibbs entropy in statistical mechanics
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relatedTo
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Boltzmann–Gibbs entropy in statistical mechanics
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subject surface form:
Boltzmann–Gibbs entropy
this entity surface form:
Boltzmann entropy
this entity surface form:
Boltzmann entropy
this entity surface form:
Boltzmann entropy