We are all familiar with phase transitions where a substance transforms from one stable phase to another at an equilibrium temperature. For example, ice will be in equilibrium with liquid water at 273.15 K and 1 atmosphere pressure, or liquid water will be in equilibrium with water vapor at 373.15 K and one atmosphere. We will now take a look at the thermodynamic principles involved in phase transitions.
I will assume at the beginning that we know nothing about the conditions under which two phases can be in equilibrium. The only things we know are the criteria for equilibrium under certain conditions. That is, we know that
(1)for a closed isolated system (that is, the entropy seeks a maximum), and
(2)for a system as constant temperature and volume (that is,the Helmholtz free energy seeks a minimum), and
(3)for a system at constant temperature and pressure (the Gibbs free energy seeks a minimum).
We will do a series of three thought experiments under different sets of conditions and use the above criteria to tell us things about the temperature, pressure, and chemical potential of a system of two phases in equilibrium.
I. A closed isolated system.
Consider a closed isolated system consisting of two phases, phase α in equilibrium with phase β . We will call the temperature of the α phase Tαand the temperature of the β phase Tβ.
We do not know, yet, what is the relationship between Tα and Tβ. We do know that in this system entropy seeks a maximum. That is,
(4)Let us transfer a small amount of heat, dq, reversibly from phase α to phase β . For definiteness we will set dq > 0. So
(6a, b)The total entropy change for the system is
(7)Since dq is positive by construction we conclude that
(9)If the system is not at equilibrium then which makes sense because heat flows spontaneously from a higher temperature to a lower temperature.
If the system is at equilibrium then There is only one temperature defined and there in no need to distinguish between the temperatures of the two phases.
II. A system at constant volume and temperature
Since we now know that at equilibrium there is only one temperature defined for the two phases let us now remove the system from isolation and place it in a heat bath at temperature, T. We will still hold the volume constant. Under conditions of constant temperature and volume we know that the criterion for equilibrium is that the Helmholtz free energy seeks a minimum. That is,
Our system now looks like,
Let us now transfer a small amount of volume, dV > 0, from phase α to phase β .
We know that dA = − SdT − pdV = − pdV for a constant temperature system. So,
(10)The change in Helmholtz free energy for the entire system is,
(11)Since dV is positive we conclude that
If the system is at equilibrium then so that there is only one pressure defined for the system.
III. The system at constant pressure and temperature
Since we now know that at equilibrium both phases are at the same temperature and pressure, let us remove the constant volume restriction and place our system in a heat bath at temperature, T, and a pressure bath at pressure, p. (The atmosphere is a good example of a pressure bath at approximately one atmosphere pressure. You can make chambers to hold different pressures if you wish.) Our system looks like,
but we do not know the relationship between the chemical potentials in the two phases.
At constant temperature and pressure we know that
(13)We also know that,
which at constant temperature and pressure becomes,
(14)Let us now move a small amount of material, dn, from phase α to phase β (with dn > 0). Then,
(16a, b)The change in Gibbs free energy for the entire system is then
(17)Since dn is positive by construction we conclude that,
(19)If the system is not in equilibrium then which makes sense since material wants to move from a region of higher chemical potential to a region of lower chemical potential.
If the system is in equilibrium then,
(20)so that there is only one chemical potential defined for the system.
Our conclusion, then, is that two phases in equilibrium must have the
same temperature, pressure and chemical potential. The above sequence of
derivations can easily be extended to include more phases and/or extended
to include mixtures, where we would find that the temperature, pressure, and
the chemical potential of each component must be the same in every phase. We will use these facts a little later
in our derivation of the Gibbs phase rule.
From here you can:
Copyright 2004, W. R. Salzman
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