2.1 Work and the State of a System 43
(T 2 ,V 2 )
V 1 (T 1 ,V 1 )
V 2
T 1 T 2
T
V
Figure 2.3 A Curve in State Space.
Work Done on an Ideal Gas in a Reversible Process
The ideal gas is a convenient system for example calculations, since it has simple
properties but illustrates the principles involved. However, you should be careful not
to apply ideal gas equations to other systems. For a finite reversible change in volume
ofnmoles of an ideal gas,
wrev
∫
c
dwrev−
∫
c
PdV−nR
∫
c
T
V
dV (ideal gas) (2.1-12)
Because the integrand in this integral depends onTandVwe must specify howT
depends onVin order to carry out the integration. This dependence corresponds to a
curve in state space, and the lettercunder the integral stands for this curve. This kind
of integral is called aline integral.
If the temperature is constant the process is calledisothermal. For an isothermal
process,
wrev
∫
c
dwrev−
∫V 2
V 1
nRT
V
dV−nRT
∫V 2
V 1
1
V
dV
wrevnRTln
(
V 2
V 1
)
(closed ideal gas,
isothermal process)
(2.1-13)
whereV 1 is the initial value of the volume andV 2 is the final value.