Thermodynamic potentials are extremely useful tools, whose name derives from an analogy with mechanical potential energy: as we will later see, in certain circumstances the work obtainable from a macroscopic system is related to the change of an appropriately defined function, the thermodynamic potential. They are useful because they allow one to define quantities which are experimentally more easy to control and to rewrite the fundamental thermodynamic relations in terms of them.
Mathematically all the thermodynamic potentials are the result of a Legendre transformation of the internal energy, namely they are a rewriting of the internal energy so that a variable has been substituted with another.
For a system ; more in general we can write:
are called generalized displacements
is the number of the
-th type of particle, and so we have:
are called generalized forces
The thermodynamic potentials that are generally used are:
- Helmholtz free energy. It is defined by:
Let's see that it is indeed a function of instead of :
Let us note that from this we have:
We now show that is in effect a thermodynamic potential.
For a general infinitesimal process we have:
For a reversible transformation
, and if it is also isothermal then
; thus, for a reversible isothermal process
: the quantity
is the amount of work that can be obtained from a reversible isothermal process, and hence the name "thermodynamic potential".
However, if the process is isothermal but irreversible then
therefore in general
is the maximum work that can be extracted from a system at constant temperature.
We also see that if the process is spontaneous
: a spontaneous transformation can only decrease the Helmholtz free energy of a system, and thus we can conclude that equilibrium states of a system at fixed
are the global minima of
- Gibbs free energy. It is defined by:
and as we have done for
it can be shown that
is the thermodynamic potential for transformations at fixed temperature and pressure.
Note that in general, if a system can be characterised by a set
of generalized displacements (and
are the corresponding generalized forces) and is composed of different types of particles, then:
In order to show that, we must consider the Euler identity
associated tu the internal energy
. As a reminder,
is a homogeneous function of degree
if and only if we have:
as the internal energy
, since it is homogeneous of degree one we have:
Considering the general definition of the Gibbs free energy, we get precisely
- Entalpy. It is defined as:
and it is the thermodynamic potential for isobaric transformations.
- Grand potential. It is defined as:
and is useful for the description of open systems, namely systems that can exchange particles with their surroundings.