Diffusion: Graham's
law
Principle
Graham's law is also
known as Graham's law of effusion. Effusion is the process where
individual molecules flow through a hole without collisions. This will occur if
the diameter of the hole is considerably smaller than the mean (collision-)free
path of the molecules. The free path is
v1/v2 = (m1/m2)0.5, (1)
where:
v1 is the rate of
effusion of the first gas;
v2 is the rate of
effusion for the second gas;
m1 is the molar mass of gas 1;
m2 is the molar mass of gas 2.
Graham's law is most accurate for molecular effusion
which involves the movement of one gas at a time through a hole. It is only
approximate for diffusion of one gas in another or in air, as these processes
involve the movement of more than one gas.
According to the kinetic theory of gases, the absolute temperature
T (Kelvin) is directly proportional to the average kinetic energy of the gas
molecules (0.5mv2). This
can be derived from:
<v2>
= 3RT/(
where <v2> the mean of the squared velocity of the
particles, R the molar gas constant (= 8315 J/kmol·K),
Thus, to have equal kinetic energies and so temperature,
the velocities of two different molecules would have to be in inverse
proportion to the square roots of their masses. Since the rate of diffusion is
determined by the average molecular velocity, Graham's law for diffusion could
be understood in terms of the molecular kinetic energies being equal at the
same temperature.
Application
The law is of important for processes of diffusion of a
gas into another gas or gas mixture (see Diffusion: general). For diffusion
across a liquid membrane, gas concentration should be low and the membrane
thin.
Graham's Law can also be used to find the approximate
molecular weight of a gas if the rates are measured and the molecular weight of
one of the gases is a known.
Graham's law was the basis for separating 235UF6
from 238UF6. Both isotopes of uranium, as element, are
found in natural uranium ore, but the 235-isotope about 100 times less. By repeated
diffusion through porous barriers the slightly lighter 235U isotope
is enriched.