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forces  arising  from  pressure  differences.  If  every  element  passing
                  through a given point follows the same line of flow as that of preceding
                  elements, the flow is said to be steady or stationary
                         In steady flow, the velocity at each point of space remains constant

                  in time, although the velocity of a particular particle of the fluid may
                  change as it moves from one point to another. A streamline  or line of
                  flow.    is  defined  as  a  curve  whose  tangent,  at  any  point,  is  in  the

                  direction of the fluid velocity at that point as shown in fig 7.1.
                        If we construct all of the streamlines passing through the periphery
                  * of an element of area, such as the area A in fig. 7.2, these lines enclose
                  a  tube  called  a.  flow  tube  or  tube  of  flow.  From  the  definition  of  a

                  streamline, no fluid can cross the side walls of a tube of flow; in steady
                  flow there can be no mixing of the fluids in different flow tubes.


                                          7.2 The Equation of Continuity

                            Let us consider any stationary, closed surface in a moving fluid; in

                  general,  fluid  flows  into  the  volume  enclosed  by  the  surface  at  some
                  points  and  flows  out  at  other  points.  The  equation  of  continuity  is  a
                  mathematical  statement  of  the  fact  that  the  net  rate  of  flow  of  mass

                  inward across any closed surface is equal to the rate of increase of the
                  mass within the surface.
                          Figure 7.2 represents a part of a tube of flow, between two fixed
                                                                            cross  sections  of  areas  S
                                                                                                              1
                                                                            and  S .  Let    v and  v   be
                                                                                    2
                                                                                                          2
                                                                                                1
                                                                            the speeds at these sections.
                                                                            There is no flow across the
                                                                            side  wall  of  the  tube
                                                                            because  at  every  point  on

                                       Figure 7.2                           the  wall  the  velocity  is
                                                                            tangent  to  the  wall.  The

                  volume of fluid that flows into the tube across S  in a time interval  t  is
                                                                                1
                  that  contained  in  the  short  cylindrical  element  of  base  S   and  height
                                                                                               1
                   l    v 1  t  ,  that  is vS 1  1  t  .  If  the  density  of  the  fluid  is   ,  the  mass
                     1
                  flowing  in  is        S   1 v 1  t  .    Similarly,  the  mass  that  flows  out  across

                  S 1 v 1  t   in the same time is     S 2 v 2  t  . The volume between  S  and  S
                                                                                                              2
                                                                                                    1
                  is constant, and since the flow is steady, the mass flowing out equals that
                  flowing in.



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