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140    REACTION SPONTANEITY AND THE DIRECTION OF THERMODYNAMIC CHANGE

                                        Sections 3.1 and 3.2 describe heat capacity and explain how it
              The heat capacity
              C p(ice) = 39 J K −1  mol −1  may be determined at constant pressure C p or at constant volume
              tells us that adding 39 J  C V . Most chemists need to make calculations with C p , which repre-
              of energy increases the  sents the amount of energy (in the form of heat) that can be stored
              temperature of 1 mol    within a substance – the measurement having been performed at
              of water by 1 K.        constant pressure p. For example, the heat capacity of solid water
                                                        −1
                                      (ice) is 39 J K −1  mol . The value of C p for liquid water is higher,
                                    −1
                      at 75 J K −1  mol , so we store more energy in liquid water than when it is solid;
                      stated another way, we need to add more energy to H 2 O (l) if its temperature is to
                                                               −1
                      increase. C p for steam (H 2 O (g) ) is 34 J K −1  mol . C p for solid sucrose (II) – a major
                                                                               −1
                      component of any jam – is significantly higher at 425 J K −1  mol .


                                                      OH
                                                    H
                                                            H
                                                OH            O
                                                  OH    H
                                                      H     OH

                                                   CH 2 OH    O

                                                        H OH
                                                    H          CH 2 OH

                                                     OH       H
                                                           (II)


                        The heat capacity of a liquid is always greater than the heat capacity of the respec-
                      tive solid because the liquid, having a greater amount of energetic disorder, has a
                      greater entropy according to


                                                                T 2

                                                                  C p
                                                S = S 2 − S 1 =      dT                     (4.9)
                                                                   T
                                                               T 1
                      More energy is ‘stored’ within a liquid than in its respective solid, as gauged by
                      the relative values of C p implied by the connection between the heat capacity and
                      entropy S (of a pure material). This is to be expected from everyday experience:
                      to continue with our simplistic example, when a freshly baked jam tart is removed
                      from the oven, the jam burns the mouth and not the pastry, because the (liquid)
                      jam holds much more energy, i.e. has a higher C p than does the solid pastry, even
                      though the two are at the same temperature. The jam, in cooling to the same tem-
                      perature as the tongue, gives out more energy. The tongue cannot absorb all of this
                      energy; the energy that is not absorbed causes other processes in the mouth, and hence
                      the burn.
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