| 1. | In that case, the equipartition theorem for the canonical ensemble follows immediately
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| 2. | Where Q is the partition function for the canonical ensemble.
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| 3. | It is also possible to derive Fermi Dirac statistics in the canonical ensemble.
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| 4. | It has been extended to include the grand canonical ensemble
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| 5. | It is derived in the same way as the partition function for the canonical ensemble.
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| 6. | In the canonical ensemble, the partition function of the system can be written as:
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| 7. | It is widely satisfied in common statistical ensembles-e . g . the canonical ensemble.
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| 8. | In quantum mechanics, the canonical ensemble affords a simple description since microstates with specific energies.
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| 9. | Boltzmann's entropy is the expression of entropy at thermodynamic equilibrium in the canonical ensemble.
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| 10. | It generalizes the narrower concepts of the grand canonical ensemble and canonical ensemble in statistical mechanics.
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