Helmholtz free energy


The Helmholtz free energy AA or FF is a measure of the energy of a system. It is defined as

A=UTSA=U-TS

where UU is the internal energy, TT is the temperature and SS is the entropy. Helmholtz free energy is particularly useful in systems that a constant temperature.

Mechanically isolated system

For a mechanically isolated system at constant temperature, AA never increases. In fact, from the second law of thermodynamics we get

ABdQTS(B)S(A)ΔSΔQTΔS\int_{A}^{B} \frac{dQ}{T}\leq S(B)-S(A)\equiv \Delta S\quad\Rightarrow \quad \frac{\Delta Q}{T}\leq \Delta S

(to pull TT out of the integral it must be constant). From the first we get

ΔQ=ΔU+WWΔU+TΔS=ΔA\Delta Q=\Delta U+W\quad\Rightarrow \quad W\leq-\Delta U+T\Delta S=-\Delta A

For a reversible transformation we get W=ΔAW=-\Delta A. But in a mechanically isolated system we have W=0W=0, therefore

0ΔAΔA00\leq-\Delta A \quad\Rightarrow \quad \Delta A\leq 0

In other words, for a system of constant temperature, AA can only decrease. Thus the most stable state (i.e. lowest energy state) is the one where AA is lowest. The equilibrium is reached because the internal energy has a tendency to stabilize the system, whereas entropy tends to make it more disorderly and eventually balance each other out.