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2.10 CALCULATING q, w, ¢U , AND ¢H  FOR PROCESSES INVOLVING IDEAL GASES  37


               EXAMPLE PROBLEM 2.5                                                       1                        2
                                                                           -1
              A system containing 2.50 mol of an ideal gas for which C V,m  = 20.79 J mol  K -1  is  16.6 bar,   16.6 bar,
                                                                                                                25L
                                                                                             1.00L
              taken through the cycle in the following diagram in the direction indicated by the
              arrows. The curved path corresponds to PV = nRT , where T = T = T 3 .    P/bar
                                                                   1
               a. Calculate q, w, ¢U , and ¢H  for each segment and for the cycle assuming that
                 the heat capacity is independent of temperature.
                                                                                                                 3
              b. Calculate q, w, ¢U , and ¢H  for each segment and for the cycle in which the
                 direction of each process is reversed.                                            V/L
              Solution
              We begin by asking whether we can evaluate q, w, ¢U , or ¢H  for any of the
              segments without any calculations. Because the path between states 1 and 3 is
              isothermal, ¢U  and ¢H  are zero for this segment. Therefore, from the first law,
              q 3:1  =-w 3:1 . For this reason, we only need to calculate one of these two quan-
              tities. Because ¢V = 0  along the path between states 2 and 3, w 2:3  =  . 0
              Therefore, ¢U 2:3  = q 2:3 . Again, we only need to calculate one of these two
              quantities. Because the total process is cyclic, the change in any state function is
              zero. Therefore, ¢U =¢H = 0  for the cycle, no matter which direction is cho-
              sen. We now deal with each segment individually.

              Segment 1 : 2
              The values of n, P and V , and P and V are known. Therefore, T and T can be cal-
                            1
                                                                         2
                                        2
                                              2
                                                                   1
                                  1
              culated using the ideal gas law. We use these temperatures to calculate ¢U  as follows:
                                                    nC V,m
                           ¢U 1:2  = nC V,m (T - T ) =     (P V - P V )
                                           2
                                                                   1 1
                                                1
                                                            2 2
                                                      nR
                                                -1
                                      20.79 J mol  K -1
                                 =
                                                 -1
                                   0.08314 L bar K  mol -1
                                     * (16.6 bar * 25.0 L - 16.6bar * 1.00 L)
                                 = 99.6kJ
              The process takes place at constant pressure, so
                                                                5
                                                              10  Nm -2
                            w =-P external (V - V ) =-16.6bar *
                                         2
                                               1
                                                                 bar
                                                           -3
                                              3
                                                               3
                                           -3
                               * (25.0 * 10  m - 1.00 * 10  m )
                              =-39.8kJ
              Using the first law,
                             q =¢U - w = 99.6 kJ + 39.8 kJ = 139.4 kJ
              We next calculate T :
                             2
                         P V             16.6bar * 25.0L
                           2 2
                                                                          3
                    T =       =                                 = 2.00 * 10  K
                     2
                                                       -1
                          nR     2.50mol * 0.08314LbarK  mol -1
              We next calculate T = T 1  and then ¢H 1:2 :
                              3
                               P V            16.6bar * 1.00L
                                1 1
                           T =      =                               = 79.9 K
                           1
                                                            -1
                               nR     2.50mol * 0.08314LbarK mol -1
                      ¢H 1:2  =¢U 1:2  +¢(PV) =¢U   1:2  + nR(T - T )
                                                              2
                                                                   1
                                       3
                              = 99.6 * 10  J + 2.5mol * 8.314Jmol -1 K -1
                                 * (2000K - 79.9K) = 139.4kJ
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