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GE-Modelle
ββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββ
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Unter gE-Modellen versteht man Methoden zur Vorhersage von AktivitΓ€tskoeffizienten Ξ³ Ξ³ {\displaystyle \gamma } mit Hilfe der freien Exzessenthalpie g E {\displaystyle g^{E}} (ExzessgrΓΆΓe bezΓΌglich der freien Enthalpie g {\displaystyle g} ). Hierbei bedient man sich des Zusammenhangs:
g E = R β
β
T β β i x i ln β‘ β‘ Ξ³ Ξ³ i {\displaystyle g^{E}=R\cdot T\sum _{i}\ x_{\text{i}}\ln \gamma _{\text{i}}\ }
Es stehen
β’ R {\displaystyle R} fΓΌr die universelle Gaskonstante
β’ T {\displaystyle T} fΓΌr die absolute Temperatur
β’ x i {\displaystyle x_{\text{i}}} fΓΌr den Stoffmengenanteil des Stoffes i und
β’ Ξ³ Ξ³ i {\displaystyle \gamma _{\text{i}}\ } fΓΌr den AktivitΓ€tskoeffizienten des Stoffes i.
Contents
β’ Gibbs-Helmholtz
β’ Beispiele
ββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββ
Gibbs-Helmholtz
Hoch parametrisierte gE-Modelle lassen sich robuster nach T extrapolieren, wenn Daten zur molaren Exzessenthalpie h E {\displaystyle h^{E}} vorliegen:
( β β ( g E T ) β β T ) p , n j = β β h E T 2 {\displaystyle \left({\frac {\partial \left({\frac {g^{E}}{T}}\right)}{\partial T}}\right)_{p,n_{j}}=-{\frac {h^{E}}{T^{2}}}}
Die Herleitung erfolgt analog zur Herleitung der Gibbs-Helmholtz-Gleichung.
Beispiele
β’ NRTL (Non-Random-Two-Liquid)
β’ UNIQUAC (Universal Quasichemical)
β’ UNIFAC (Universal Quasichemical Functional Group Activity Coefficients)
β’ COSMO-RS (Conductor-like Screening Model for Real Solvents)
β’ Wilson-Gleichung
β’ Porter-Ansatz