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McKay, Donald. "Front matter" Multimedia Environmental Models ...

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We are concerned with systems in which a chemical migrates from phase to<br />

phase. These phase changes involve input or output of energy, thus this energy<br />

exchange can compensate for entropy loss or gain. It can be shown that, whereas<br />

entropy maximization is the criterion of equilibrium for a system containing constant<br />

energy at constant volume, the criterion at constant temperature and pressure (the<br />

environmentally relevant condition) is minimization of the related function, the<br />

Gibbs free energy, which serves to combine energy and entropy in a common<br />

currency.<br />

Return to the example presented in Figure 5.1, of benzene diffusing from water<br />

into an air bubble and striving to achieve equilibrium. The basic concept is that, if<br />

we start with a benzene concentration in the water and none in air, the free energy<br />

of the system will decrease as benzene migrates from water to air, because the<br />

increase in free energy associated with the rise in benzene concentration in the air<br />

is less that of the decrease associated with benzene loss from the water. The process<br />

is thus spontaneous and irreversible. Benzene continues to diffuse from water into<br />

the air until it reaches a point at which the free energy increase in the air is exactly<br />

matched by the free energy decrease in the water. At this point, the system comes<br />

to rest or equilibrium.<br />

Likewise, if the system started with a higher benzene concentration<br />

in the air phase and approached equilibrium, it would reach exactly the<br />

same point of equilibrium with a particular ratio of concentrations in each phase.<br />

The system thus seeks a minimum in free energy at which its derivative with<br />

respect to moles of benzene is equal in both air and water phases. This derivative<br />

is of such importance that it is called the chemical potential. The underlying principle<br />

of phase equilibrium thermodynamics is that, when a solute such as benzene achieves<br />

equilibrium between phases such as air, water, and fish, it seeks to establish an equal<br />

chemical potential in all phases. The net diffusion flux will always be from high to<br />

low chemical potential. Thus, we can use chemical potential for deductions of mass<br />

diffusion in the same way that we use temperature in heat transfer calculations.<br />

5.1.3 Fugacity<br />

Unfortunately, chemical potential is logarithmically related to concentration,<br />

thus doubling the concentration does not double the chemical potential. A further<br />

complication is that a chemical potential cannot be measured absolutely, therefore<br />

it is necessary to establish some standard state at which it has a reference value. It<br />

was when addressing this problem that G.N. Lewis introduced a new equilibrium<br />

criterion in 1901, which he termed fugacity, and which has units of pressure and is<br />

assigned the symbol f. The term fugacity comes from the Latin root fugere, describing<br />

a “fleeing” or “escaping” tendency. It is identical to partial pressure in ideal<br />

gases and is logarithmically related to chemical potential. It is thus linearly or nearly<br />

linearly related to concentration. Absolute values can be established because, at low<br />

partial pressures under ideal conditions, fugacity and partial pressure become equal.<br />

Thus, we can replace the equilibrium criterion of chemical potential by that of<br />

fugacity. When benzene migrates between water and air, it is seeking to establish<br />

an equal fugacity in both phases; its escaping tendency, or pressures, are equal in<br />

both phases.<br />

©2001 CRC Press LLC

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