Grahams Law Of Diffusion
December 9, 2009According to the Graham’s Law of diffusion, the rate of diffusion of a gas is inversely proportional to the square root of it’s density or molecular weights. If r1 and r2 are the rates of diffusion of two gases, whose densities under the given conditions are d1 and d2 respectively, then we have

(M1 and M2 are the respective molecular weights of the two gases) and d1 and d2 are their respective vapour densities.)
Knowing the experimental gas laws, it is of interest to develop a theoretical model based on the structure of gases, which can co-relate the experiment. Fortunately, such a theory has been developed and is known as kinetic theory of gases.
Kinetic Theory of Gases
The word ‘Kinetic’ means ‘Motion’. Gaseous molecules are assumed to be in constant motion. A theory with the help of which the various gas laws can be derived mathematically is known as the kinetic theory of gases.
The main postulates of the theory are as follows:
Þ A gas is made of extremely tiny particles called molecules. The molecules of any given gas are identical and have the same mass,
and the molecules are assumed to be dispersed in a lot of vacant space.
Þ The individual molecules are relatively far apart from each other and they exert very little attraction for each other except under collision of molecules and near the liquification point. The real volume of the gas molecules at ordinary temperatures and pressures is very small in comparison to the total volume of the gas. Here we are talking about real gases or non-ideal gases since ideal gases cannot be liquefied.
Þ The gaseous molecules are in continuous random, straight line motion with very high speeds in all directions. They collide frequently and this may bring about a change in the direction of movement and a redistribution of energy between the colliding molecules. The collisions are perfectly elastic (i.e. no loss of energy) but only redistribution of energy may occur.
Þ The force of gravity has negligible effect on the speed of the gas molecules.
Þ The pressure exerted by a gas is due to collisions made by gas molecules on the walls of the container. Gases not only distribute themselves throughout the total volume of the container but also exert uniform pressure on every point of the container.
Þ The average K.E. of the molecules is directly proportional to the absolute temperature of the gas.


