6.4 The Activities of Nonvolatile Solutes 269
and themean ionic molalitym±(
mν++mν−−) 1 /ν
(6.4-7)These are examples ofgeometric means. For a 1-3 electrolyte such as CrCl 3 ,m±is
equal to (27)^1 /^4 m 2 2. 2795 m 2 , wherem 2 is thestoichiometric molalityof the solute
(the molality that would occur if no dissociation occurred). The chemical potential of
the neutral electrolyte solute is given byμ 2 ν+μ◦++ν−μ◦−+RTln(γ±ν(
m±/m◦)ν
)
ν+μ◦++ν−μ◦−+νRTln(
γ±m±/m◦)
(6.4-8)
The activity of the solvent can be expressed in terms of theosmotic coefficientφ,
defined byφ−ln(a 1 )
M 1 vm 2μ◦ 1 −μ 1
RTM 1 vm 2(definition) (6.4-9)wherea 1 is the activity of the solvent, andM 1 is the molar mass of the solvent. If the
solute dissociates completely,νm 2 is equal to the sum of the molalities of the ions.
From Eq. (6.4-9)μ 1 μ◦ 1 −RTM 1 vm 2 φ (6.4-10)The chemical potential of the solute can be writtenμ 2 μ◦ 2 +νRTln(γ±ν±m 2 /m◦) (6.4-11)whereγ±(
γ
v+
+γv−
−) 1 /v
(6.4-12)For constant pressure and temperature, the Gibbs–Duhem relation for a two-
component system is written in the formn 1 dμ 1 +n 2 dμ 2 0 (6.4-13)Since the molalitym 2 is equal to the amount of substance 2 divided by the mass of the
solvent (substance 1),n 2 m 2 n 1 M 1 (6.4-14)whereM 1 is the molar mass of the solvent. Use of Eqs. (6.4-10), (6.4-11), and (6.4-14)
in Eq. (6.4-13) gives−n 1 νRTM 1 m 2 dφ+φdm 2 +m 2 n 1 M 1 νRTdln(γ 2 )+dln(m 2 /m◦) 0Cancellation of the common factor and use of the identitydln(m)(1/m)dmgives−m 2 dφ−φdm 2 +m 2 dln(γ 2 )+dm 2 0 (6.4-15)