Gibbs energy function: Difference between revisions

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m (New page: Definition: :<math>\left.G\right.=A+pV</math> :<math>\left.G\right.=U-TS+pV</math> Taking the total derivative :<math>\left.dG\right.=dU-TdS-SdT+pdV+Vdp</math> but from equation \ref...)
 
m (Added internal link)
 
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:<math>\left.G\right.=A+pV</math>
:<math>\left.G\right.=A+pV</math>


where ''p'' is the [[pressure]], ''V'' is the volume, and  ''A'' is the [[Helmholtz energy function]], i.e.


:<math>\left.G\right.=U-TS+pV</math>
:<math>\left.G\right.=U-TS+pV</math>
Line 10: Line 11:
:<math>\left.dG\right.=dU-TdS-SdT+pdV+Vdp</math>
:<math>\left.dG\right.=dU-TdS-SdT+pdV+Vdp</math>


but from equation \ref{secondlaw} we obtain
From the [[Second law of thermodynamics]]  one obtains


:<math>\left.dG\right.=TdS -pdV-TdS-SdT+pdV+Vdp</math>
:<math>\left.dG\right.=TdS -pdV-TdS-SdT+pdV+Vdp</math>
Line 16: Line 17:
thus one arrives at
thus one arrives at


 
:<math>\left.dG\right.=-SdT+Vdp</math>
<math>\left.dG\right.=-SdT+Vdp</math>


For ''G(T,p)'' we have the following ''total differential''
For ''G(T,p)'' we have the following ''total differential''


:<math>dG=\left(\frac{\partial G}{\partial T}\right)_p dT + \left(\frac{\partial G}{\partial p}\right)_T dp</math>
:<math>dG=\left(\frac{\partial G}{\partial T}\right)_p dT + \left(\frac{\partial G}{\partial p}\right)_T dp</math>
 
[[Category: Classical thermodynamics]]
Good for $NpT$

Latest revision as of 17:17, 29 January 2008

Definition:

where p is the pressure, V is the volume, and A is the Helmholtz energy function, i.e.

Taking the total derivative

From the Second law of thermodynamics one obtains

thus one arrives at

For G(T,p) we have the following total differential

Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle dG=\left({\frac {\partial G}{\partial T}}\right)_{p}dT+\left({\frac {\partial G}{\partial p}}\right)_{T}dp}