Page 202 - Physical Chemistry
P. 202

lev38627_ch06.qxd  3/3/08  10:07 AM  Page 183





                                                                                                                 183
                  Since  G°   H°   T  S°, we end up with                                                      Section 6.3
                                                                                                  Temperature Dependence of the
                                                d ln K°  ¢H°                                            Equilibrium Constant
                                                     P                              (6.36)*
                                                  dT     RT  2
                  This is the van’t Hoff equation. [Since ln K°    G°/RT, Eq. (6.36) follows from
                                                         P
                  the Gibbs–Helmholtz equation (Prob. 4.13) (
(G/T)/
T)   H/T .] In (6.36),  H°
                                                                          2
                                                                 P
                   H° is the standard enthalpy change for the ideal-gas reaction at temperature  T
                     T
                  [Eq. (5.3)]. The greater the value of    H° , the faster the equilibrium constant  K°
                                                                                          P
                  changes with temperature.
                      The degree superscript in (6.36) is actually unnecessary, since H of an ideal gas is
                  independent of pressure and the presence of other ideal gases. Therefore,  H per mole
                  of reaction in the ideal gas mixture is the same as  H°. However, S of an ideal gas de-
                  pends strongly on pressure, so  S and  G per mole of reaction in the mixture differ
                  quite substantially from  S° and  G°.
                      Multiplication of (6.36) by dT and integration from T to T gives
                                                                   1    2
                                                        ¢H°
                                              d ln K°         dT
                                                   P
                                                        RT 2
                                             K°1T 2    T 2 ¢H°1T2
                                              P
                                                 2
                                           ln                2  dT                   (6.37)
                                             K°1T 2   T 1  RT
                                              P
                                                 1
                  To evaluate the integral in (6.37), we need  H° as a function of T.  H°(T) can be
                  found by integration of  C° (Sec. 5.5). Evaluation of the integral in Eq. (5.19) leads
                                          P
                  to an equation with the typical form (see Example 5.6 in Sec. 5.5)
                                                                3
                                                          2
                                      ¢H°   A   BT   CT   DT   ET     4              (6.38)
                                         T
                  where A, B, C, D, and E are constants. Substitution of (6.38) into (6.37) allows K° at
                                                                                       P
                  any temperature T to be found from its known value at T .
                                  2                                1
                       H° for gas-phase reactions usually varies slowly with T, so if T   T is reason-
                                                                            2    1
                  ably small, it is generally a good approximation to neglect the temperature dependence
                  of  H°. Moving  H° outside the integral sign in (6.37) and integrating, we get
                                           K°1T 2    ¢H°   1    1
                                                2
                                             P
                                         ln               a       b                  (6.39)
                                           K°1T 2     R    T 1  T 2
                                             P
                                                1
                  EXAMPLE 6.2 Change of K° with T
                                                    P
                     Find K° at 600 K for N O (g) ∆ 2NO (g) (a) using the approximation that  H°
                           P            2  4         2
                     is independent of T; (b) using the approximation that  C° is independent of T;
                                                                     P
                     (c) using the NIST-JANAF tables (Sec. 5.9).
                        (a) If   H° is assumed independent of  T, then integration of the van’t
                     Hoff equation gives (6.39). Appendix data for NO (g) and N O (g) give
                                                                    2         2  4
                      H°   57.20 kJ/mol and  G°   4730 J/mol. From  G°   RT ln K°, we
                        298                    298                                  P
                     find K°    0.148. Substitution in (6.39) gives
                          P,298
                               K°       57200 J>mol      1         1
                                P,600
                            ln                      a                 b   11.609
                               0.148   8.314 J>mol-K  298.15 K   600 K
                                              K°     1.63 	 10 4
                                               P,600
   197   198   199   200   201   202   203   204   205   206   207