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7.2 USES OF THE THERMODYNAMIC RELATIONSHIPS             145





                  Thus, equating the two areas gives


                                               vT          vp
                                                   dv ds ¼      ds dv:                      (7.21)
                                               vv           vs
                                                   s           v
               and hence
                                                 vp        vT

                                                      ¼         :                          (7.19a)
                                                 vs  v     vv  s

               7.2 USES OF THE THERMODYNAMIC RELATIONSHIPS
               When performing certain types of calculation it is useful to have data on the values of the specific heat
               capacities of the substance under consideration and also the variation of these specific heat capacities
               with the other properties. The specific heat capacities themselves are first derivatives of the internal
               energy (u) and the enthalpy (h), and hence the variations of specific heat capacities are second de-
               rivatives of the basic properties.
                  By definition, the specific heat capacity at constant volume is

                                                 vu       vu    vs
                                           c v ¼      ¼             :                       (7.22)
                                                 vT       vs   vT
                                                     v       v     v
                  But

                                          vu                      vs
                                               ¼ T; and thus c v ¼ T   :                    (7.23)
                                          vs                      vT
                                              v                       v
                  Similarly

                                            vh       vh    vs        vs
                                      c p ¼      ¼              ¼ T      :                  (7.24)
                                            vT  p    vs  p  vT  p    vT  p
                  Consider the variation of the specific heat capacity at constant volume, c v , with specific volume, v,
               if the temperature is maintained constant. This can be derived in the following way.

                                                              2
                                    vc v     v    vs         v s     v  vs
                                          ¼    T        ¼ T      ¼ T         :
                                     vv     vv    vT        vvvT    vT vv
                                        T             v                     T
                  Now, from Eqn (7.19c),
                                                  vs      vp

                                                       ¼       ;
                                                  vv  T   vT  v
               giving

                                                        2         2
                                           vc v        v s       v p
                                                 ¼ T        ¼ T                             (7.25)
                                            vv  T     vTvv       vT 2  v
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