Osmotic Pressure and Diffusion (the solute dissociates into two monovalent ions)
Let the velocities of the cation (+) and anion (-) in unit electric field (i.e. the mobilities of the ions) be (U) and (V) cm per second respectively. Now, each ion will be driven by the osmotic pressure, thus for the cation (F1),
where (n) is the concentration per cc. of each kind of ion and (P) is the osmotic pressure of the solution.
The velocity of a cation due to
the osmotic pressure is
, that is,
and
for the anion ![]()
In most cases
and as a consequence
if the osmotic pressure alone were the driving force the two ions would become
separated and as this is not possible another force must be active. Consider
some hydrochloric acid placed at the bottom of a tube of water.
The hydrogen ions would have a mobility (U), which would exceed the mobility of the chlorine ions (V). Under such circumstances the liquid at the top would be positively charged and that at the bottom negatively charged due to the more rapids movement of the hydrogen ions. An electric field would be set up which would reduce the velocity of the faster ions and increase the velocity of the slower ions. The final state would be reached where both ions traveled at the same rate. Assuming this state to occur the coefficient of diffusion can be calculated.
In the direction Ox, at any point let the let the
electric field be (X) and the derivative
where E is the
potential at that point. Now, a monovalent ion
situated at that point would experience a force
dynes according to the sign of its charge. Now, as the
cation velocity under unit force is (U) cm per
second, a force
will result in a
terminal velocity of
cm per second. In the
same way the terminal velocity
of an anion will be
cm per second.
The total velocity of a cation due to both osmotic pressure and the electric field will be,
and
for the anion ![]()
Now, it would be fair to assume that the number of ions
of each kind crossing unit area per unit time would be the same
which will be equal to
the product of their velocity and their concentration,
Thus,
![]()
Eliminating
, ![]()
Now although the osmotic pressure (Pa) according to Van’t
Hoff is given by
, in practice the actual osmotic pressure is less i.e.,
.
Differentiating,
![]()
substituting for
Now if the mass of each ion is (m1) and (m2), then the total mass crossing unit area per unit time will be,

and as (m) the mass of a
molecule will be
then the total mass
crossing unit area per unit time will be,
![]()
Now according to Fick’s law the
total mass crossing unit area per unit time is,![]()
Consequently, the Diffusivity (D)
is given by, ![]()