Linked from

The 15 pages that link to Canonical ensemble, each with the reason it gives.

• Statistical mechanicsBroader topic: It is the standard alternative to the isolated-system microcanonical description.

• Thermodynamic equilibriumRelated: It describes equilibrium under thermal contact with a reservoir.

• Boltzmann distributionNarrower topic: The distribution gives state probabilities for this ensemble.

• Transition state theoryRelated: The usual derivation counts activated complexes using a thermal distribution.

• Equipartition theoremRelated: Equipartition is derived by averaging energy over this fixed-temperature ensemble.

• Maxwell–Boltzmann distributionRelated: Its energy probabilities follow the Boltzmann weighting used in the classical distribution.

• Grand canonical ensembleCompared with: It permits energy exchange but keeps particle number fixed.

• Helmholtz free energyRelated: Its partition function determines the Helmholtz free energy directly.

• Microcanonical ensembleCompared with: Unlike the microcanonical ensemble, it permits energy fluctuations and weights states by the Boltzmann factor.

• Thermodynamic limitRelated: It defines finite-volume quantities whose large-system behavior can be studied.

• Thermal fluctuationsRelated: It provides the standard probability framework for equilibrium energy fluctuations.

• Gibbs paradoxNarrower topic: Its partition function makes the particle-counting correction explicit.

• Virial expansionRelated: Partition functions in this ensemble provide a route to deriving the gas’s density expansion.

• Classical statistical mechanicsBroader topic: It models thermal equilibrium when a system exchanges energy with a reservoir.

• Bohr–van Leeuwen theoremRelated: The theorem is commonly derived from the classical canonical ensemble’s field-independent partition function.