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Governing equations of fluid mechanics  89
                                 -vi
                               Y


                               y2   ------













         Fig. 2.28



         Example 2.2  For the rectangular region of a two-dimensional flow field depicted in Fig. 2.28,
         starting with the definition Eqn (2.81) of  circulation,  show that it can also be evaluated  by
         means of the integral around the closed circuit appearing as the last term in Eqn (2.83).
           From Eqns (2.76) and (2.81) it follows that







         Therefore








          But along the lines:  C1,  q = ui,  t = i, ds = dx; C2, q = vj,  t = j, ds = dy; C,,  q = ui,  t = -i,
         ds = -dx;  and Cq, q = uj, t = -j,  ds = -dy.  It therefore follows that Eqn (2.84) is equivalent to







            2.8  The Navier-Stokes  equations

         2.8.1  Relationship between rates of strain
                 and viscous stresses
          In solid mechanics the fundamental  theoretical model linking the  stress and strain
          fields is Hooke’s law that states that

                                       Stress 0; Strain                     (2.85)
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