Page 201 - Essentials of physical chemistry
P. 201

More Kinetics and Some Mechanisms                                           163

            but it is better to use the slope from a graph fitted to several points as shown above ( 10,864) or use
            two rates far apart in temperature. The best two-point slope would be over the full range of the data
            that spans from 08Cto458C here, and we would obtain a slope from those two points as

                                         5
                          3
              ln (2:92   10 )   ln (1:06   10 )    2:93   10  3    (318:15)(273:15)
                                           ¼ ln                             ¼ 10,856:85:

                       1         1              1:06   10  5       45
                    318:15     273:15
            We will use the slope of the graph here ( 10,864) since it is available from a least-squares fit:

                     DH (25 C) ¼ ( R)[(slope) þ T] ¼ ( 8:314 J=mol K)[ 10,864 þ 298:15],


                       z
            so we find
                                DH ¼þ87:844 kJ=mol ¼þ20:995 kcal=mol,
                                   z

                                                K rate h  slope
                                  DS (T) ¼ R ln                   1 ,
                                    z
                                                k B T      T
                                                    4               34
                                          (3:19   10 )(6:6260693   10  )    10,864
             DS (25 C) ¼ (8:314 J=mol K) ln                                           1 ,

                z

                                            (1:3806505   10  23 )(298:15)   298:15
                         DS (25 C) ¼ 17:208822 J=deg mol ¼ 4:1130072 cal=deg mol:
                           z

            We can calculate DG in two ways. First,
                             y
                                                                  4               34
                                                        (3:19   10 )(6:6260693   10  )
                 DG (25 C) ¼ (8:314 J=mol K)(298:15 K) ln



                    z
                                                          (1:3806505   10  23 )(298:15)
            or
                                      DG (25 C) ¼þ92:975 kJ=mol:
                                         z

            And so finally, DG ¼ DH   TDS ¼þ87, 844   (298:15)( 17:208822) ¼þ92:975 kJ=mol.
                                        z
                           z
                                 z
              While it is comforting that we get the same answer for DG in two different ways and that is a
                                                              z
            check on the calculations for DH and DS , the opportunities for error in these calculations are
                                       z
                                               z
            many. Assuming you might be tested on these equations (hint), it would be best to ‘‘practice’’ doing
            these calculations several times when you are rested with a clear head.
            SUMMARY OF GRAPHICAL METHOD RESULTS AT T ¼ 258C
                             DH (25 C) ¼þ87:844 kJ=mol ¼þ20:995 kcal=mol,
                                z

                        DS (25 C) ¼ 17:208822 J=8 mol ¼ 4:1130072 cal=8 mol,  and
                           z

                              DG (25 C) ¼þ92:975 kJ=mol ¼þ22:222 kcal=mol:
                                z

            One conclusion from this study of the simple form of Eyring’s absolute reaction rate theory is that
            we can obtain DH and DS using two equations in two unknowns over a limited temperature range.
                                 z
                          z
            However, the more general analytical formulas show that the values are definitely dependent on the
            temperature. Considering the many ways to make errors in these calculations, it might occur to a
   196   197   198   199   200   201   202   203   204   205   206