c12 JWBS043-Rogers September 13, 2010 11:27 Printer Name: Yet to Come
192 SOLUTION CHEMISTRY
π
solvent solution
membrane
FIGURE 12.6 Osmotic pressure,π.
ambient pressureμ◦ 1 (p)plus the change resulting from the increase in pressure to
p+π:
μ◦ 1 (p+π)=μ◦ 1 (p)+
∫ p+π
p
(
∂μ 1
∂p
)
T
dp
The variation of a perfect differential of a thermodynamic function is
dμ=
(
∂μ
∂p
)
T
dp+
(
∂μ
∂T
)
p
dT
but the second term on the right drops out becauseT=const.We shall refer to the
molar volume of solvent asVm, 1 and note that (Klotz and Rosenberg, 2008)
(
∂μ 1
∂p
)
T
=Vm, 1
The Gibbs chemical potential of the pure solvent subjected to a pressure change from
ptop+πat constantVm, 1 is
μ◦ 1 (p+π)=μ◦ 1 (p)+
∫ p+π
p
Vm, 1 dp=μ◦ 1 (p)+πVm, 1