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               Chapter 5                  T  and calculation of   U  from the known  U of combustion of benzoic acid then
                                                                298
                                                              r
               Standard Thermodynamic    gives us the heat capacity C  . The temperature ranges over which the two combus-
               Functions of Reaction                             K P
                                         tions are carried out are very similar. Also, the main contribution to C K P   and C K P
                                         comes from the bomb walls and the water bath. For these reasons, it is an excellent ap-
                                         proximation to take C K P     C K P . (In precise work, the difference between the two
                                         is calculated using the known heat capacities of the combustion products.) Knowing
                                         C    , we find   U  from Eq. (5.8).
                                           K P         r  298
                                             To find the standard internal energy change  U° for the reaction, we must allow
                                                                                     298
                                         for the changes in U and U that occur when the reactants and products are brought
                                                           R     P
                                         from the states that occur in the calorimeter to their standard states. This correction is
                                         typically about 0.1 percent for combustion reactions.
                                             (An analysis similar to Fig. 5.4b enables one to estimate the temperature of a
                                         flame. See Prob. 5.60.)
                                             For reactions that do not involve gases, one can use an adiabatic constant-pressure
                                         calorimeter. The discussion is similar to that for the adiabatic bomb calorimeter, ex-
                                         cept that P is held fixed instead of V, and  H of reaction is measured instead of  U.


                                         EXAMPLE 5.2 Calculation of   U°from calorimetric data
                                                                               c
                                            Combustion of 2.016 g of solid glucose (C H O ) at 25°C in an adiabatic bomb
                                                                               6  12  6
                                            calorimeter with heat capacity 9550 J/K gives a temperature rise of 3.282°C.
                                            Find   U° of solid glucose.
                                                 c  298
                                               With the heat capacity of the products neglected, Eq. (5.8) gives   U
                                             (9550 J/K)(3.282 K)   31.34 kJ for combustion of 2.016 g of glucose. The
                                            experimenter burned (2.016 g)/(180.16 g/mol)   0.01119 mol. Hence  U per
                                            mole of glucose burned is ( 31.34 kJ)/(0.01119 mol)   2801 kJ/mol, and this
                                            is   U° if the difference between conditions in the calorimeter and standard-
                                               c  298
                                            state conditions is neglected.
                                            Exercise

                                            If 1.247 g of glucose is burned in an adiabatic bomb calorimeter whose heat
                                            capacity is 11.45 kJ/K, what will be the temperature rise? (Answer: 1.693 K.)



                                         Relation between  H° and  U°
                                         Calorimetric study of a reaction gives either   U° or   H°. Use of  H   U   PV
                                         allows interconversion between   H°and   U°. For a process at constant pressure,
                                          H   U   P  V. Since the standard pressure P° [Eq. (5.2)] is the same for all sub-
                                         stances, conversion of pure standard-state reactants to products is a constant-pressure
                                         process, and for a reaction we have
                                                                   ¢H°   ¢U°   P° ¢V°                        (5.9)
                                             Similar to  H°     n H° [Eq. (5.3)], the changes in standard-state volume and
                                                              i  i  m,i
                                         internal energy for a reaction are given by  V°     n V° and  U°     n U° . A
                                                                                      i  i  m,i         i  i  m,i
                                         sum like   n U° looks abstract, but when we see   n     , we can translate this into
                                                  i  i  m,i                          i  i
                                         “products minus reactants,” since the stoichiometric number n is positive for products
                                                                                             i
                                         and negative for reactants.
                                             The molar volumes of gases at 1 bar are much greater than those of liquids or
                                         solids, so it is an excellent approximation to consider only the gaseous reactants and
                                         products in applying (5.9). For example, consider the reaction
                                                           aA1s2   bB1g2 S cC1g2   dD1g2   eE1l2
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