Example 1.8
Use the cyclic rule to determine an alternate expression for
V
P
T
Solution
Using Figure 1.11, it should be easy to see that
V
p
T
You should verify that this is correct.
1.8 A Few Partial Derivatives Defined
Many times, gaseous systems are used to introduce thermodynamic concepts.
That’s because generally speaking, gaseous systems are well behaved. That is,
we have a good idea how they will change their state variables when a certain
state variable, controlled by us, is changed. Therefore gaseous systems are an
important part of our initial understanding of thermodynamics.
It is useful to define a few special partial derivatives in terms of the state
variables of gaseous systems, because the definitions either (a) can be consid-
ered as basic properties of the gas, or (b) will help simplify future equations.
The expansion coefficientof a gas, labeled , is defined as the change in vol-
ume as the temperature is varied at constant pressure. A 1/Vmultiplicative fac-
tor is included:
V
1
V
T
p
(1.27)
For an ideal gas, it is easy to show that R/pV.
The isothermal compressibilityof a gas, labeled , is the change in volume as
the pressure changes at constant temperature (the name of this coefficient is
more descriptive). It too has a 1/Vmultiplicative factor, but it is negative:
V
1
V
p
T
(1.28)
Because ( V/ p)Tis negative for gases, the minus sign in equation 1.28 makes
a positive number. Again for an ideal gas, it is easy to show that RT/p^2 V.
For both and , the 1/Vterm is included to make the quantities intensive
(that is, independent of amount*).
Since both of these definitions use p,V, and T, we can use the cyclic rule to
show that, for example,
T
p
V
T
p
V
V
T
p
20 CHAPTER 1 Gases and the Zeroth Law of Thermodynamics
*Recall that intensive properties (like temperature and density) are independent of
amount of material, whereas extensive properties (like mass and volume) are dependent on
the amount of material.