Thermodynamics MOC

Thermodynamic potential

A thermodynamic potential is an extensive quantity which is naturally1 a function of the natural2 independent variables and whose minimization or maximization follows from the ^P4 when these independent variables are held constant.

Equations of state

To show that a quantity 𝑀 is naturally a function of parameters (π‘₯𝑖)𝑛𝑖=1, one takes the Exterior derivative 𝑑𝑀 and shows 𝑑𝑀 =βˆ‘π‘›π‘–=1𝑓𝑖𝑑π‘₯𝑖, where 𝑓𝑖 are 0-forms. One then arrives at the equations of state

πœ•π‘€πœ•π‘₯𝑖=𝑓𝑖

Examples


tidy | en | SemBr

Footnotes

  1. i.e. by the First law of thermodynamics. ↩

  2. a natural choice of variables for the situation at hand, i.e. the intensive or extensive parameters that can be controlled directly. ↩