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132    REACTION SPONTANEITY AND THE DIRECTION OF THERMODYNAMIC CHANGE


                                            Colder end             Hotter end
                                             of bath                of bath

                                      n(E)




                                                  Energy of water molecules E
                                                           (a)




                                      n(E)



                                                   Energy of water molecules E
                                                           (b)

                      Figure 4.1 Graph of the number of water molecules of energy E against energy. (a) Soon after
                      running the bath, so one end is hotter and the other cooler; and (b) after thermal equilibration. The
                      (average) energy at the peak relates to the macroscopic temperature


                      is transferred from one set of water molecules to other. Trace (b) in Figure 4.1 shows
                      the distribution of energies after equilibration. In other words, the energetic disorder
                      S increases. The reading on a thermometer placed in the bath will represent an
                      average energy.
                        The spread of energies in Figure 4.1 is a direct indication of entropy, with a wider
                      spread indicating a greater entropy. Such energetic disorder is the consequence of
                      having a range of energies. The spread widens spontaneously; an example of a non-
                      spontaneous process would be the reverse process, with the molecules in a bath at,
                             ◦
                                                                               ◦
                      say, 50 C suddenly reverting to one having a temperature of 30 C at one end and a
                                      ◦
                      temperature of 70 C at the other.
                                        The German scientist Rudolf Clausius (1822–1888) was the
              In the thermodynamic    first to understand the underlying physicochemical principles dic-
              sense, an ‘engine’ is a  tating reaction spontaneity. His early work aimed to understand
              device or machine for   the sky’s blue colour, the red colours seen at sunrise and sun-
              converting energy into
                                      set, and the polarization of light. Like so many of the ‘greats’
              work. Clausius himself  of early thermodynamics, he was a mathematician. He was inter-
              wanted to devise an effi-
              cient machine to con-   ested in engines, and was determined to improve the efficiency of
              vert heat energy (from  steam-powered devices, such as pumping engines used to remove
              a fuel) into mechani-   water from mines, and locomotives on the railways. Clausius was
              cal work.               the first to introduce entropy as a new variable into physics and
                                      chemistry.
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