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on_phenomenological_thermodynamics_._note [2015/11/07 19:49]
nikolaj
on_phenomenological_thermodynamics_._note [2015/11/08 14:46]
nikolaj
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 $(\Delta G)_{T,​\{N_i\}}:​=\int_{p_2}^{p_1}V(T,​p)\,​{\mathrm d}p=c^S T\ln(\frac{p_2}{p_1})$ $(\Delta G)_{T,​\{N_i\}}:​=\int_{p_2}^{p_1}V(T,​p)\,​{\mathrm d}p=c^S T\ln(\frac{p_2}{p_1})$
  
-$\implies ​p_2 = p_1\cdot\exp\left(\dfrac{(\Delta G)_{T,​\{N_i\}}}{c^S T}\right)$.+$\implies p_1 = p_2\cdot\exp\left(-\dfrac{(\Delta G)_{T,​\{N_i\}}}{c^S T}\right)$.
  
 This sort of "​concentration varies with $\exp(-E/​k_BT)$"​ equation also pops up often in chemistry and electronics (Goldmann equation, Nernst equation, diode current-voltage-characteristics,​...) This sort of "​concentration varies with $\exp(-E/​k_BT)$"​ equation also pops up often in chemistry and electronics (Goldmann equation, Nernst equation, diode current-voltage-characteristics,​...)
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 === Related === === Related ===
 +[[Notes on physical theories . note]],
 [[Statistical internal energy]] [[Statistical internal energy]]
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