The experiment uses a semipermeable membrane between pure solvent on one side, and a dilute solution of the polymer in the same solvent on the other side, PC Fig. 10.1. The membrane is permeable to the solvent, but impermeable to the polymer. At constant T, the chemical potential of the solvent, mu, is
For equilibrium in a two-component ideal solution,
mu (pure solvent, pressure P) = mu (solution, pressure P + pi)
The right-hand side can be replaced by
mu (pure solvent, pressure P) + RT ln x1 + integralPP + pi (d mu / d P)T dP
where the second term accounts for the effect of concentration (ideality assumed, mole fraction of solvent used as the concentration variable) and the last term accounts for the effect of pressure. If the solution is incompressible,
Vm pi / RT = - ln x1
where Vm is the molar volume of the solvent. Assuming dilute solution (so that x1 is close to 1), the right hand side is well approximated as
- ln x1 = x2 = N2/N1
which leads to the van't Hoff equation
pi = m2RT
Conversion to concentration in units of mass/volume, c, and introduction of solution nonideality via a virial equation, leads to
pi / c = RT/M + Bc + Cc2 + ...
If the osmotic pressure is to be expressed in terms of the height, h, of a column of liquid with density rho, the conversion to pressure is via pi = rho g/h, where g is the acceleration due to gravity.
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