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                218
               Chapter 7                 steepness of the slope of the P-versus-T fusion line (Fig. 7.1b) means that unless P   P 1
                                                                                                            2
               One-Component Phase Equilibrium  is very large, the change in melting-point temperature T  will be quite small. More-
               and Surfaces                                                              fus
                                         over, the properties of solids and liquids change only slowly with pressure (Sec. 4.4).
                                         Therefore, unless P   P is quite large, we can approximate   S,   H, and   V
                                                          2    1                               fus   fus      fus
                                         as constant. To integrate (7.23), we can assume either that   S/  V is constant or
                                                                                             fus  fus
                                         that   H/  V is constant. For small changes in freezing point, these two approxi-
                                              fus   fus
                                         mations give similar results and either can be used. For substantial changes in freez-
                                         ing point, neither approximation is accurate for solid–liquid transitions. However, the
                                         equilibrium lines for many solid–solid transitions (Sec. 7.4) on P-versus-T phase dia-
                                         grams are observed to be nearly straight over wide temperature ranges. The constant
                                         slope dP/dT    S/  V for such solid–solid transitions means that taking   S/  V
                                                       trs  trs                                           trs  trs
                                         is often a good approximation here.
                                             If we approximate   S/  V as constant, then (7.23) becomes
                                                              fus  fus
                                                    ¢ S               ¢ H
                                          P   P       fus   1T   T 2    fus   1T   T 2   solid–liq. eq., T   T  small
                                                1
                                                           2
                                           2
                                                                                   1
                                                                                                      2
                                                                1
                                                                              2
                                                                                                           1
                                                    ¢ V              T  ¢ V
                                                     fus              1  fus
                                                                                                            (7.24)
                                         If we approximate ¢ H  and ¢ V  as constant, Eq. (7.23) gives
                                                           fus
                                                                    fus
                                                                ¢ H    T
                                                     P   P       fus   ln   2      solid–liq. eq., T   T  small  (7.25)
                                                                                          2
                                                       2
                                                            1
                                                                                               1
                                                                ¢ V    T
                                                                 fus    1
                                         EXAMPLE 7.5 Effect of pressure on melting point
                                            Find the melting point of ice at 100 atm. Use data from Prob. 2.49.
                                               Since this is a solid–liquid equilibrium, Eq. (7.24) applies. [Afrequent student
                                            error is to apply Eq. (7.19) to solid–liquid equilibria.]For1gof ice,   H
                                                                                                         fus
                                                                                                3
                                                                                                            3
                                            333.6 J and the densities give   V   V   V    1.000 cm   1.091 cm
                                                                      fus    liq   solid
                                                     3
                                             0.091 cm . Let state 1 be the normal melting point. Then P   P   100 atm
                                                                                              2   1
                                            1atm   99 atm, and (7.24) becomes
                                                                               333.6 J
                                                              99 atm                          ¢T
                                                                                           3
                                                                       1273.15 K21 0.091 cm 2
                                                                                    3
                                                                    ¢T   7.38 K cm  atm>J
                                                                                 3
                                            We now use two values of R to convert cm atm to joules, so as to eliminate
                                              3
                                            cm atm/J.
                                                                    3
                                                                                        1
                                                                  cm  atm    8.314 J mol  K  1
                                                    ¢T   7.38 K                                   0.75 K
                                                                                           1
                                                                                  3
                                                                     J    82.06 cm  atm mol  K  1
                                            Hence, T   273.15 K   0.75 K   272.40 K. The pressure increase of 99 atm
                                                   2
                                            has lowered the melting point by only 0.75 K to  0.75°C.
                                            Exercise
                                            Repeat this problem assuming that   H/  V is constant. (Answer: 272.40 K.)
                                                                           fus
                                                                                fus
                                            Exercise
                                            At the normal melting point of NaCl, 801°C, its enthalpy of fusion is 28.8 kJ/mol,
                                                                                                              3
                                                                          3
                                            the density of the solid is 2.16 g/cm , and the density of the liquid is 1.73 g/cm .
                                                                    5
                                                                                                        3
                                            What pressure increase is needed to raise the melting point by 1.00°C?
                                            (Answer: 39 atm.)
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