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20     CHAPTER 2 Heat, Work, Internal Energy, Enthalpy, and the First Law of Thermodynamics


          TABLE 2.1   Types of Work
         Types of Work        Variables                               Equation for Work    Conventional Units
                                                                              V f
                                                                                               3
         Volume expansion     Pressure (P), volume (V)                w =-      P external  dV  Pa m = J
                                                                            L V i
                                                                            x f  #
         Stretching           Force (F), length (l)                   w =     F dl         N m = J
                                                                           x
                                                                          L i
                                                                            s f  #
                                                                                                    2
                                                                                                -1
         Surface expansion    Surface tension (g) , area (s)          w =      G dS        (N m )(m ) = J
                                                                          Ls i
                                                                            Q
         Electrical           Electrical potential (f) , electrical charge (Q)  w =  fdQ¿  V C = J
                                                                          L 0

                                          EXAMPLE PROBLEM 2.1
                                          a. Calculate the work involved in expanding 20.0 L of an ideal gas to a final volume
                                             of 85.0 L against a constant external pressure of 2.50 bar.
                                          b. An air bubble in liquid water expands from a radius of 1.00 cm to a radius of
                                                                                   –1
                                             3.25 cm. The surface tension of water is 71.99 N m . How much work is done in
                                             increasing the area of the bubble? Assume that the system is the contents of the bubble.
                                          c. A current of 3.20 A is passed through a heating coil for 30.0 s. The electrical
                                             potential across the resistor is 14.5 V. Calculate the work done on the coil.
                                          d. If the force to stretch a fiber a distance x is given by F =-kx  with
                                             k = 100. N cm -1 , how much work is done to stretch the fiber 0.15 cm?

                                         Solution
                                                     V f
                                          a.  w =-      P external  dV =-P external (V - V )
                                                                                   i
                                                                              f
                                                   LV i
                                                                                         -3
                                                              5
                                                            10  Pa                    10  m  3
                                                =-2.50 bar *       * (85.0 L - 20.0 L) *      =-16.3 kJ
                                                              bar                        L
                                          b. A factor of 2 is included in the following calculation because a bubble has an
                                             inner and an outer surface. We consider the bubble and its contents to be the sys-
                                                                  point in opposite directions, giving rise to the negative
                                             tem. The vectors  and S
                                                           G
                                             sign in the second integral.
                                                             #
                                                         s f           s f
                                                                                           2
                                                                                      2
                                                    w =     G dS =-       gds = 2g4p(r - r )
                                                                                           i
                                                                                      f
                                                       Ls i          Ls i
                                                                                               10 -4  m 2
                                                                                2
                                                                                       2
                                                                      -1
                                                                            2
                                                                                           2
                                                      =-4p * 71.99 Nm   (3.25  cm - 1.00  cm ) *   2
                                                                                                 cm
                                                      =-0.865 J
                                                    Q
                                          c. w =     fdQ¿= fQ = Ift = 14.5 V * 3.20 A * 30.0 s = 1.39 kJ
                                                 L 0
                                          d. We must distinguish between F, the restoring force on the fiber, and F œ , the force
                                                                            œ #
                                             exerted by the person stretching the fiber. They are related by F =-F œ . If we
                                             calculate the work done on the fiber, F  dl = F¿dl  because the vectors F œ  and
                                             dl point in the same direction
                                                     œ #     x f        kx 2 x f  100. N m -1  * x 2  0.15
                                             w =    F   dl =   kxdx = B    R   = B               R   = 1.1 J
                                                  L         3           2   x 0          2        0
                                                             x 0
                                         If we calculate the work done by the fiber, the sign of w is reversed because F and
                                         dl point in opposite directions.
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