Page 164 - Physical chemistry understanding our chemical world
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THE DIRECTION OF PHYSICOCHEMICAL CHANGE: ENTROPY      131


              Why, when one end of the bath is hot and the other
              cold, do the temperatures equalize?

             Entropy and the second law of thermodynamics

             Quite often, when running a bath, the water is initially quite cold. After the hot
             water from the tank has had time to travel through the pipes, the water from the tap
             is hot. As a result, one end of the bath is hotter than the other. But a short time
             later, the temperature of the water is the same throughout the bath, with the hot
             end cooler and the cold end warmer. Temperature equilibration occurs even without
             stirring. Why?
               We saw in Chapter 1 how the simplest way to gauge how much energy a molecule
             possesses is to look at its temperature. We deduce through a reasoning process such as
             this that molecules of water at the cold end of the bath have less energy than molecules
             at the hot end. Next, by combining the minus-oneth and zeroth laws of thermody-
             namics, we say that energy (in the form of heat) is transferred from molecules of
             water at the hot end of the bath to molecules at the cold end. Energy transfers until
             equilibrium is reached. All energy changes are adiabatic if the bath
             is lagged (to prevent energy loss), in accordance with the first law  The word ‘entropy’
             of thermodynamics.                                           comes from the Greek
               As no chemical reactions occur, we note how these thermo-  en tropa, meaning
                                                                          ‘in change’ or ‘during
             dynamic changes are purely physical. But since no bonds form or
                                                                          transformation’.
             break, what is the impetus – the cause – of the transfer of energy?
             We have already seen the way processes occur with an attendant
             increase in disorder. We now introduce the concept of entropy.The
             extent of energetic disorder is given the name entropy (and has the
                                                                          The ‘second law of ther-
             symbol S). A bigger value of S corresponds to a greater extent of  modynamics’ says a
             energetic disorder.                                          process occurs sponta-
               We now introduce the second law of thermodynamics: a physic-  neously only when the
             ochemical process only occurs spontaneously if accompanied by  concomitant energetic
             an increase in the entropy S. By corollary, a non-spontaneous  disorder increases. We
             process – one that we can force to occur by externally adding  can usually approxi-
             energy – would proceed concurrently with a decrease in the ener-  mate, and talk in terms
             getic disorder.                                              of ‘disorder’ alone.
               We can often think of entropy merely in terms of spatial disorder,
             like the example of the sugar grains above; but the entropy of a
             substance is properly the extent of energetic disorder. Molecules of  The energy is trans-
             hot and cold water in a bath exchange energy in order to maximize  ferred via random,
                                                                          inelastic collisions bet-
             the randomness of their energies.
                                                                          ween the molecules of
               Figure 4.1 depicts a graph of the number of water molecules
                                                                          water. Such molecular
             having the energy E (as y) against the energy of the water mole-
                                                                          movement is some-
             cules E (as x). Trace (a) in Figure 4.1 shows the distribution of  times called Brownian
             energies in a bath where half the molecules have one energy while
                                                                          motion; see p. 139.
             the other half has a different energy, which explains why the graph
             contains two peaks. A distribution of energies soon forms as energy
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