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Equilibrium for a System with Internal Degrees of Freedom

For the case of an ideal fluid that has ``internal degrees of freedom,'' new terms must be added to the internal energy. To illustrate this, we considered that particular case numbers of molecules of each type (of a possible number of \bgroup\color{blue}$ C$\egroup types) was variable in each of the \bgroup\color{blue}$ j$\egroup possible phases.

$\displaystyle \input{equations/13-1A}$ (19-1)


or in general

$\displaystyle \input{equations/13-1B}$ (19-2)


The condition that we applied to find the conditions of equilibrium [( \bgroup\color{blue}$ \ensuremath{\delta}S )_{\ensuremath{\delta}U = 0 , \; \ensuremath{\delta}V = 0} \leq 0$\egroup, or, equivalently ( \bgroup\color{blue}$ \ensuremath{\delta}U )_{\ensuremath{\delta}S = 0 , \; \ensuremath{\delta}V = 0} \geq 0$\egroup] previously were not practical. It is difficult to arrange to do experiments where \bgroup\color{blue}$ U =$\egroup constant and \bgroup\color{blue}$ V =$\egroup constant. They are difficult to arrange in the lab.

Question: Consider that you are doing an experiment to determine the equilibrium properties of a material? What kinds of experimental conditions would be the most straightforward to implement?



next up previous
Next: Equilibrium with constraints that Up: Lecture_19_web Previous: Lecture_19_web
W. Craig Carter 2002-10-22