Page 45 - Bruno Linder Elementary Physical Chemistry
P. 45

August 18, 2010 11:36      9in x 6in     b985-ch04     Elementary Physical Chemistry





                               30                   Elementary Physical Chemistry
















                                                          Variation of S with T.
                                                  Fig. 4.1

                                  Still, because there are exceptions, some individuals are reluctant to
                               call the Third Law a Law on par with the First and Second Laws. But
                               most chemists accept the law, and use it as the basis for absolute entropies.
                                  Suppose one wants to determine the entropy change ∆S = S(T )−S(0).
                               Since S(0) is assumed to be zero, one obtains
                                                                    T
                                                 ∆S(T )= S(T )=     (C P /T )dT            (4.1)
                                                                  0
                               A schematic representation of the variation of S with T is shown in Fig. 4.1.


                               4.1. Standard Entropy
                                                               o
                                                                                              o
                               Just as with standard enthalpy, H , there is a standard entropy, S ,
                               defined as the entropy of one mole of a substance at 1 bar and a specified
                               temperature, normally 25 C.
                                                     ◦
                               4.2. Molecular Interpretation of Entropy
                               We have seen that when a system changes from a solid to a gas, from a solid
                               to a liquid or from a liquid to a gas, there is an increase in entropy. We have
                               also seen that in an irreversible isothermal change, as in the expansion into
                               a vacuum of a gas at constant temperature, the entropy increases. Also,
                               when there is an increase in temperature, the entropy increases.
                                  Evidently, in all these cases, the increase in entropy seems to be
                               accompanied from a microscopic (molecular) point of view by an increase
                               in disorder, greater randomness in the distribution of the molecules, and
                               more chaotic motion.

                               Example 4.1. Suppose you are dealing with a system consisting of
                               particles, distributed among the energy levels shown in Fig. 4.2. The total
   40   41   42   43   44   45   46   47   48   49   50