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238   CHAPTER 8.  STEADY MICROSCOPIC BALANCES  WITHOUT GEN.

             8.1  MOMENTUM TRANSPORT


             Momentum per unit mass, by definition, is the fluid velocity and changes in velocity
             can result  in momentum transport.  For fully developed flow'  through  conduits,
             velocity variations take place in the direction perpendicular to the flow since nG
             slip boundary conditions must be satisfied at the boundaries of  the conduit.  This
             results  in  the transfer  of  momentum in the direction perpendicular  to the flow
             direction.
                The inventory rate equation for momentum at the microscopic level is called
             the equation of motion.  It is a vector equation with three components. For steady
             transfer of momentum without generation, the conservation statement for momen-
             tum reduces to

                     (Rate of momentum in) - (Rate of momentum out) = 0       (8.1-1)


             When there is no generation of  momentum, this implies that both pressure and
             gravity terms are zero.  Hence, flow  can only be generated by  the movement of
             surfaces enclosing the fluid and the resulting flow is called  Couette flow. We will
             restrict our analysis to cases in which the following assumptions hold:


               1. Incompressible Newtonian fluid,

               2.  One-dimensional2 , fully developed laminar flow,

               3.  Constant physical properties.


             The last assumption comes from the fact that temperature rise as a result of viscous
             dissipation during fluid motion, i.e., irreversible degradation of mechanical energy
             into thermal energy, is very small and cannot be detected by ordinary measuring
             devices in most of  the cases.  Hence, for all practical purposes the flow is assumed
             isothermal.


             8.1.1  Plane Couette Flow

             Consider a Newtonian fluid between two parallel plates that are separated by a
             distance B  as shown in Figure  8.1.  The lower  plate  is  moved  in  the positive
             z-direction  with a constant velocity of V while the upper plate is held stationary.


                Fully developed flow means there is no variation of velocity in the axial direction, In this way,
             the flow development regions near  the entrance and exit are not taken into consideration.
                One-damensional flow indicates that there is only one non-zero velocity component.
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