214 SOLUTIONS
The converse is also true: If the variables and are statis-
tically independent. Now for a closed system we can write
where is the total entropy of the system and is the entropy change
due to the fluctuation. On the other hand,
where is the minimum work to change reversibly the thermodynamic
variables of a small part of a system (the rest of the system works as a heat
bath), and is the average temperature of the system (and therefore the
temperature of the heat bath). Hence,
However,
where and are changes of a small part of a system due to
fluctuations and P are the average temperature and pressure. So,
Expanding (for small fluctuations) gives
Substituting (S.4.93.16) into (S.4.93.14), we obtain