CHAPTER 9 MIXTURES
9.6 EVALUATION OFACTIVITYCOEFFICIENTS 266
coefficient of a solution of nonelectrolyte solutes is defined by
mdefDA A
RTMA
X
i§Ami(9.6.11)
(nonelectrolyte solution)The definition ofmin Eq.9.6.11has the following significance. The sum
P
i§Amiis
the total molality of all solute species. In an ideal-dilute solution, the solvent chemical
potential isADACRTlnxA. The expansion of the function lnxAin powers of
.1 xA/gives the power series lnxAD .1 xA/ .1 xA/^2 =2 .1 xA/^3 =3 .
Thus, in a very dilute solution we have lnxA .1 xA/D
P
i§Axi. In the limit
of infinite dilution, the mole fraction of soluteibecomesxiDMAmi(see Eq.9.1.14).
In the limit of infinite dilution, therefore, we havelnxAD MAXi§Ami (9.6.12)
(infinite dilution)
and the solvent chemical potential is related to solute molalities byADA RTMAXi§Ami (9.6.13)
(infinite dilution)
The deviation ofmfrom unity is a measure of the deviation ofAfrom infinite-
dilution behavior, as we can see by comparing the preceding equation with a rear-
rangement of Eq.9.6.11:ADA mRTMAXi§Ami (9.6.14)The reasonmis called the osmotic coefficient has to do with its relation to the osmotic
pressureof the solution: The ratio=mBis equal to the product ofmand the
limiting value of=mBat infinite dilution (see Sec.12.4.4).Evaluation ofm
Any method that measuresA A, the lowering of the solvent chemical potential caused
by the presence of a solute or solutes, allows us to evaluatemthrough Eq.9.6.11.
The chemical potential of the solvent in a solution is related to the fugacity in an equili-
brated gas phase byADrefA(g)CRTln.fA=p/(from Eq.9.5.11). For the pure solvent,
this relation isADrefA(g)CRTln.fA=p/. Taking the difference between these two
equations, we obtain
A ADRTlnfA
fA(9.6.15)
which allows us to evaluatemfrom fugacity measurements.
Osmotic coefficients can also be evaluated from freezing point and osmotic pressure
measurements that will be described in Sec.12.2.