A Level Physics Notes: Thermal Physics and Gases – The Kinetic Theory of Gases
The kinetic theory of gases is a model that explains gas behaviour
– pressure, temperature and volume – using a model of the gas as
hard little particles of no volume which exert no forces on each
other. For many everyday situations these are very good
approximations. Classical Newtonian mechanics is used to derive the
equation of state which describes the relationship between Pressure
Volume
and
Temperature
for
an 'ideal gas'.
Suppose we have a cube full of N identical gas molecules of mass m inside a cube of side l. Imagine a gas molecule moving backwards and forwards between the walls 1 and 2. The collisions of the molecule with the walls of the box are perfectly elastic so no kinetic energy is lost, and the molecule always has speed v. We assume the wall to be fixed – this is not true, but they are so much heavier than the gas molecules that it is a very good approximation.
Each time the gas molecule collides with the wall (1) it's
momentum changes by![]()
Between each collision with wall 1 the molecule travels a
distance
so
takes
seconds
to travel from 1 to 2 and back, hence the molecule collides with wall
1
times
per second.
This means that the rate of change of momentum of the molecule is
because of it's collisions with wall 1 is
and
we can equate this to the impulse exerted by the wall on the molecule
and hence using Newton's Third Law, to the impulse exerted by the
molecule on the wall.
(1)
since![]()
We add up terms such as (1) obtaining
where
N is the total number of molecules in the box, but now we have to
take into account that not all the gas molecules are bouncing between
walls 1 and 2: on average, only one third are, so we can introduce a
factor of
to
take account of this then
becomes![]()
![]()
using![]()
![]()
![]()
The mean kinetic energy of gas molecules is given by![]()
![]()
number
of mols*number of molecules in each mol
where
is
Avagadro's number.
![]()
Finally
the
Universal Gas constant:
![]()
This is the usually stated form of the ideal gas equation.