Are $\Delta G = RT \ln{\frac{Q}{K}}$ and $\Delta S = -\frac{RT\ln{\frac{Q}{K}}-q_p}{T}$ legitimate relations?
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While messing around with ΔG=ΔG⊖+RTlnQΔG=ΔG⊖+RTlnQ and ΔG⊖=−RTlnKΔG⊖=−RTlnK, I found this relation:
ΔG=RTlnQKΔG=RTlnQK
which helped me clarify how ΔGΔG is affected by changes in QQ, but I wanted to make sure that it is actually true before I rely on it for such things.
Also, would this mean that:
ΔS=−RTlnQK−ΔHTΔS=−RTlnQK−ΔHT
and therefore, at constant pressure:
ΔS=−RTlnQK−qpTΔS=−RTlnQK−qpT
holds true? That is, that change in entropy can be increased by essentially adding product, or is that cancelled out by the heat exchange
ΔG=RTlnQKΔG=RTlnQK
which helped me clarify how ΔGΔG is affected by changes in QQ, but I wanted to make sure that it is actually true before I rely on it for such things.
Also, would this mean that:
ΔS=−RTlnQK−ΔHTΔS=−RTlnQK−ΔHT
and therefore, at constant pressure:
ΔS=−RTlnQK−qpTΔS=−RTlnQK−qpT
holds true? That is, that change in entropy can be increased by essentially adding product, or is that cancelled out by the heat exchange
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Let's consider the special case of an ideal gas. If your development is valid in general, then it must work for that special case. In your equation ΔG=RTlnQKΔG=RTlnQK, what are the initial and final thermodynamic equilibrium states, according to your understanding....
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