Gibbs free energy and equilibrium constant at a high T

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In a system where ΔG is negative and ΔS is positive, increasing temperature makes ΔG more negative, favoring product formation. However, the equilibrium constant (Keq) approaches 1 at high temperatures, suggesting equal amounts of products and reactants, which appears contradictory. The relationship between ΔG and Keq is clarified through the equation Keq = e^(-ΔG/TR), indicating that Keq's behavior is influenced by ΔH and ΔS. The discussion highlights that the change in Keq with temperature depends on the sign of ΔH, aligning with established thermodynamic principles. Overall, the apparent contradiction arises from the interplay between Gibbs free energy and the equilibrium constant at varying temperatures.
gmianosi
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I posted this earlier, but I just realized it might have been in the wrong section. Sorry

Okay, so consider you have system in which ΔG<0 and ΔS>0. Using Gibbs free energy (ΔG=ΔH-TΔS), you'll know that it will always be negative. As the temperature increases, it will actually become more and more negative. This means that as the temperature increases to a higher T, ΔG will become even more negative. making the system favor products much more than reactants.

Now consider the equation for the equilibrium constant, Keq=e^-ΔG/TR. Using this definition, as T gets very high, Keq seems to be going to 1, meaning that there will be an equal amount of product and reactants at a very high temperature.

These two definitions are both correct, yet they seem to contradict one another. Why is that? I feel like I'm missing something very definition based.

Thanks in advance to anyone who helps :)
 
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Without getting into any other arguments - Keq doesn't go to 1.

K_{eq} = e^{\frac {-\Delta G}{TR}} = e^{\frac {-(\Delta H - T\Delta S)}{TR}} = e^{\frac {-\Delta H}{TR}}e^{\frac {\Delta S}{R}}
 
Borek said:
Without getting into any other arguments - Keq doesn't go to 1.

K_{eq} = e^{\frac {-\Delta G}{TR}} = e^{\frac {-(\Delta H - T\Delta S)}{TR}} = e^{\frac {-\Delta H}{TR}}e^{\frac {\Delta S}{R}}
Oh wow, I can't believe I did that. Thank you.
But still, Keq seems to be going to a smaller value, while ΔG is becoming more negative, which doesn't make sense.
 
It shows that the change of K with T depends on the sign of ##\Delta H##. This is in line with the argument of Borek.
 
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