Thermodynamics, Statistical Physics, and Quantum Mechanics

(Axel Boer) #1
113

On the other hand, at equilibrium, there is no net force acting on the piston
(seeFigure S.4.23), and we have

Substituting(S.4.23.2)into(S.4.23.1)gives

We can also use energyconservation in this thermally insulatedsystem.
Then thework done to the gas equals its energy change For an ideal
gas

where is theheat capacity of one mole of the gas (for amonatomic gas,
The work done to the gas


where is the distance thepiston moves,wheredownward
is positive. From(S.4.23.4) and(S.4.23.5), wehave


Solving (S.4.23.3) and(S.4.23.6) yields

We may checkthat if i.e.,that the piston was initially
balanced,(S.4.23.7)gives and

4.24 Spring Cylinder (Moscow Phys-Tech)


For athermallyinsulatedsystem (no heattransfer), theenergy change
is given by


THERMODYNAMICS AND STATISTICAL PHYSICS
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