Equilibrium and Thermodynamics problem: For the reaction NH4Cl (s) ----> NH3 (g) + HCl (g) delta H = 176 kJ and delta G = 91.2 kJ at 298 K. What is the value of delta G at 1000 K? A. -109 kJ B. -64 kJ C. 64 kJ D. 109 kJ You don't have to explain it completely, I just want to see someone else's answer. I keep getting -705 kJ.
We are interested in the following expression which you can show: \[\left( \frac{ \partial G }{ \partial T } \right)_{p}=-S\] The entropy can be written as: \[S=\frac{ (H-G) }{ T }\] We therefor get: \[\left( \frac{ \partial G }{ \partial T } \right)_{p}=\frac{ (G-H) }{ T }\] \[\left( \frac{ \partial G }{ \partial T } \right)_{p}-\frac{ G }{ T }=-\frac{ H }{ T }\] Combine the two terms on the left side: \[\left( \frac{ \partial }{ \partial T } \frac{ G }{ T } \right)_{p}=\frac{ 1 }{ T } \left( \frac{ \partial G }{ \partial T } \right)_{p}+G \frac{ d }{ dT }\frac{ 1 }{ T }=\frac{ 1 }{ T } \left( \frac{ \partial G }{ \partial T } \right)_{p}-\frac{ G }{ T ^{2} }\]
We therefor get: \[\left( \frac{ \partial }{ \partial T } \frac{ G }{ T } \right)_{p}=\frac{ 1 }{ T }\left\{ \left( \frac{ \partial G }{ \partial T } \right)_{p}-\frac{ G }{ T } \right\}\]
We use the very first partial differential and substitute: \[\left( \frac{ \partial }{ \partial T } \frac{ G }{ T } \right)_{p}=\frac{ 1 }{ T }\left\{ -S -\frac{ G }{ T } \right\}=\frac{ 1 }{ T }\left\{ -S-\frac{ H-TS }{ T } \right\}=-\frac{ H }{ T ^{2} }\] Integreate the expression below using separation of the variables and you have your equation. \[\left( \frac{ \partial }{ \partial T } \frac{ G }{ T } \right)_{p}=-\frac{ H }{ T ^{2} }\]
As we do not have a heat capacity at constant pressure we approximate and assume that the enthalpy is independent of the change in temperature.
Doing so and using that Delta G is proportional to Delta H we get (tell me if you want to see the integral: \[\large \Delta H \left( \frac{ 1 }{ T _{2} }-\frac{ 1 }{ T _{1} } \right)=\frac{ \Delta G _{2} }{ T _{2} }-\frac{ \Delta G _{1} }{ T _{1} }\] Solve for Delta G_2: \[\large \Delta G _{2}=\Delta H \left( \frac{ T _{2} }{ T _{2} }-\frac{ T _{2} }{ T _{1} } \right)+\frac{ \Delta G _{1} ~ T _{2} }{ T _{1} }=\Delta H \left( 1-\frac{ T _{2} }{ T _{1} } \right)+\frac{ \Delta G _{1} ~ T _{2} }{ T _{1} }\] For evaluation see attachment.
Wow, this is very in depth, thank you!
No problem. The equation before I solve for Delta G_2 is called the Gibbs–Helmholtz equation. :)
Or perhaps more the partial derivative as you can approximate depending on how accurate you want the answer.
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