Certain processes occur spontaneously - for example cooling of a
hot object to the temperature of the surroundings, and expansion of
a gas to fill the volume available to it. Though these processes can
be made to go the other way (heating an object up, confining a gas
to a smaller volume), they do not occur spontaneously, and can only
be brought about by doing work upon the system of interest.
It is useful to be able to predict whether or not a process will be
spontaneous, but to do so we need to find some property of a system
that will determine the direction of spontaneous change. Initially,
one might consider the internal energy, U, of a system and hypothesise
that it tends to a minimum. However, the First Law of Thermodynamics
states that total energy is conserved in any process. This means firstly
that the energy of an isolated system cannot change in any process,
in disagreement with our expectation.
There is a second, more fundamental problem with the hypothesis:
if the energy of a system decreases in a spontaneous change, then
by the First Law the energy of the surroundings must increase by the
same amount, but both processes are spontaneous. Thus it is
clear that changes in the internal energy of a system cannot be the
signpost of spontaneous change.
We shall see that in fact the direction
of change is related to the distribution of energy in the system -
a spontaneous change is always accompanied by a dispersal of energy
into a less ordered form.
We can use this idea to illustrate the two examples given above:
Objects do not spontaneously become warmer than their surroundings
because this would require the accumulation of excess thermal energy
(in the form of thermal motion) in the object. It is exceptionally
unlikely that this could occur by transmission of energy from randomly
vibrating atoms in the surroundings, so may be considered impossible.
The opposite process, dispersal of the object's thermal energy into
the random vibrational motion of the surroundings, is a consequence
of the tendency towards increased chaos.
Gases do not spontaneously contract because to do so requires the
chaotic motion of the gas particles to become ordered and localised
in one part of the container. This is also so overwhelmingly improbable
that it can be considered impossible. The opposite process, spontaneous
expansion, is a natural consequence of increasing disorder.
The distinction between spontaneous and non-spontaneous processes
is formalised in the Second Law of Thermodynamics.
|