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134                               CHAPTER 5.  RATE OF GENERATION

            momentum into and out of  the volume element, i.e.,

                    Rate of             Rate of          Summation of  forces
               ( momentum in ) - ( momentum out           acting on a system
                                                     Time rate of  change of
                                                     momentum of  a system   )  (5.1-2)
            On the other hand, for a given system, the inventory rate equation for momentum
            can be expressed as
                    Rate of             Rate of  ) + ( Rate of  momentum
               ( momentum in ) - ( momentum out              generation
                                                    = ( Rate of  momentum   )  (5.1-3)
                                                           accumulation

            Comparison of  Eqs.  (5.1-2) and (5.1-3) indicates that
                           Rate of  momentum       Summation of  forces  )    (5.1-4)
                               generation           acting on a system
            in which the forces acting on a system are the pressure force (surface force) and
            the gravitational force (body force).

            5.1.1  Momentum Generation As a Result  of  Gravitational
                    Force

            Consider a basketball player holding a ball in his hands.  When he drops the ball,
            it starts to accelerate as a result of  gravitational force.  According to Eq.(5.1-4),
            the rate of  momentum generation is given by
                                Rate of  momentum generation = Mg             (5.1-5)
            where M  is the mass of  the ball and g is the gravitational acceleration. Therefore,
            the rate of  momentum generation per unit volume, R, is given by
                                                                              (5.1-6)


            5.1.2  Momentum Generation As a Result of Pressure Force
            Consider the steady flow of  an incompressible fluid in a pipe as shown in Figure 5.1.
            The rate of  mechanical energy required to pump the fluid is given by  Eq.  (4.53)
            as
                                      I&’  = F’(v) = & IAP(                   (5.1-7)
            Since the volumetric flow rate, &, is the product of  average velocity, (v), with the
            cross-sectional area, A, Eq.  (5.1-7) reduces to
                                        AlAPl-3’0  =O                         (5.1-8)
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