Gibbs-Helmholtz equation

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The Gibbs-Helmholtz equation is a thermodynamic equation useful for calculating changes in the Gibbs energy of a system as a function of temperature. It is named after Josiah Willard Gibbs and Hermann von Helmholtz:

\left( \frac{\partial ( \frac{G} {T} ) } {\partial T} \right)_{p\,} = - \frac {H} {T^2}

With:

H\, the enthalpy
T\, the absolute temperature
G\, the Gibbs free energy

at constant pressure P\,. The equation states that the change in the G/T ratio at constant pressure as a result of an infinite small change in temperature is a factor (H/T2).

For a chemical reaction the equation reads:

\left( \frac{\partial ( \frac{\Delta G} {T} ) } {\partial T} \right)_{p\,} = - \frac {\Delta H} {T^2}

with \Delta G\, as the change in Gibbs energy and \Delta H\, as the enthalpy change (which is considered independent of temperature).

which can rearrange to:

\frac{\Delta G,T_2}{T_2} - \frac{\Delta G^\circ,T_1}{T_1} = \Delta H^\circ(P)*(\frac{1}{T_2} - \frac{1}{T_1})

This equation quickly enables the calculation of the Gibbs free energy change for a chemical reaction at any temperature T2 with knowledge of the just the Standard Gibbs free energy change of formation and the Standard enthalpy change of formation for the individual components at 25°C and 1 bar.

Through:

\ \Delta G^\circ = -RT \ln K

which relates Gibbs energy to an equilibrium constant, the Van't Hoff equation is derived.


The Gibbs free energy for an open system


dG =  - SdT + VdP \,


at constant pressure P\, (dP = 0) reduces to


dG_{p\,} =  - SdT \,


or

\left(\frac{\partial G}{\partial T}\right)_{p\,} =  - S \,


As the Gibbs energy for a closed system is


G = H - TS \,


it follows that


\left(\frac{\partial G}{\partial T}\right)_{P\,} =  \frac{G - H}{T} \,


The dependence of the G/T ratio on T is found with the aid of the quotient rule:


\left( \frac{\partial ( \frac{G} {T} ) } {\partial T} \right)_{p\,} =  \frac{\frac{\partial g}{\partial T}}{\frac{\partial}{\partial T}}   =  \frac{T\left(\frac{\partial G}{\partial T}\right)_{P\,} - G\left(\frac{\partial T}{\partial T}\right)_{P\,} }{T^2}   =  \frac{1}{T}\left(\frac{\partial G}{\partial T}\right)_{P\,}  - \frac {G} {T^2}


and with substitution:


\left( \frac{\partial ( \frac{G} {T} ) } {\partial T} \right)_{p\,} =  \frac{1}{T}\frac{G - H}{T}- \frac {G} {T^2}


the result is


\left( \frac{\partial ( \frac{G} {T} ) } {\partial T} \right)_{p\,} = - \frac {H} {T^2}

  • Gibbs-Helmholtz equation @ www.chem.arizona.edu Link
  • Gibbs-Helmholtz equation @ www.owlnet.rice.edu Link
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