Quantum redactiones paginae "Physica statistica" differant
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Probabilitas macrostatui cuidam k est <math>\;\rho = \frac {e^{-\beta E_k}}{Z} </math>, ubi constans normalizationis (appellatus functio partitionis) <math>Z = \sum_{k} e^{-\beta E_k}</math>, <math>E_k</math> est energia tota microstatus k, et <math>\beta = {1 \over k_B T}</math>.
Partitionis functione utentes possumus calculare omnes quantitates thermodynamicas per [[derivativum|derivativa]] huius functionis, sic ut in tabula infera
: <math>E = \langle E\rangle={\sum_i E_i e^{-\beta E_i}\over Z}=-{1 \over Z} {dZ \over d\beta}= -\left( \frac{\partial\ln Z}{\partial\beta} \right)_{N,V}</math>
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