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Conditions of Multiphase Equilibrium

Below it will be shown, for a multiphase system, that the chemical potential in each phase must be uniform and equal.

Consider the following simple multiphase system:

Figure 25-1: An example of a multiphase system. $ P$ and $ T$ are constant and equilibrium with a reservoir.
\begin{figure}\resizebox{6in}{!}
{\epsfig{file=figures/brine.eps}}
\end{figure}


Application of the conditions of internal equilibrium to the entire system considering that it is composed of \bgroup\color{blue}$ f$\egroup phases:

$\displaystyle \input{equations/19-1A}$ (25-10)

\bgroup\color{blue}$ \mu^j_i$\egroup is the chemical potential of chemical species \bgroup\color{blue}$ i$\egroup in phase \bgroup\color{blue}$ j$\egroup.

Write this out for a three ( \bgroup\color{blue}$ f=3$\egroup) phase system composed of two ( \bgroup\color{blue}$ C=2$\egroup) species \bgroup\color{blue}$ W$\egroup and \bgroup\color{blue}$ B$\egroup:


For a closed system,

$\displaystyle \input{equations/19-2A}$ (25-11)

this follows for each possible species \bgroup\color{blue}$ i$\egroup, therefore:

$\displaystyle \input{equations/19-2Abis}$ (25-12)


In other words, the chemical potentials of any chemical species is equal in all the present phases.

Or if we number the species \bgroup\color{blue}$ i=1,2,\ldots,C$\egroup and the number of phases \bgroup\color{blue}$ j=I,II,\ldots,f$\egroup:

$\displaystyle \input{equations/19-4A}$ (25-13)

Each row has \bgroup\color{blue}$ f-1$\egroup equal signs; i.e. \bgroup\color{blue}$ f-1$\egroup equations. So in the above there are \bgroup\color{blue}$ C(f-1)$\egroup equations.


In addition we have, via the Gibbs-Duhem equation for each phase, another relation between the variables:

$\displaystyle \input{equations/19-3A}$ (25-14)

that gives us another \bgroup\color{blue}$ f$\egroup equations. Therefore,

Let the number of free variables be \bgroup\color{blue}$ D$\egroup (degrees of freedom). Then,


$\displaystyle \input{equations/19-3B}$ (25-15)

or:

$\displaystyle \input{equations/gibbs-phase-rule}$ (25-16)

This is a relation between the number of degrees of freedom in a system and the number of components. Commonly, one can think of the number of degrees of freedom in a system as the number of phases that can co-exist, or \bgroup\color{blue}$ D = P$\egroup.

And this brings to mind the following..... limerick:

There was a recent graduate from MIT
Who was forced to send back her course three degree
she couldn't make a phase plot
Because she had simply forgot
that P + F = 2 + C

next up previous
Next: About this document ... Up: Lecture_25_web Previous: Further Restrictions on Material
W. Craig Carter 2002-11-21