Page 65 - Mechanical Engineers' Handbook (Volume 4)
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54   Fluid Mechanics

                             The equations of streamlines are described by stream functions  , from which the ve-
                          locity components in two-dimensional flow are u     / y and v     / x. Streamlines
                          are lines of constant stream function. In polar coordinates
                                                     1
                                                v            and    v
                                                 r
                                                      r  
                 r
                             Some streamline patterns are shown in Figs. 11, 12, and 13. The lines at right angles
                          to the streamlines are potential lines.


           4.3  Deformation of a Fluid Element
                          Four types of deformation or movement may occur as a result of spatial variations of velocity:
                          translation, linear deformation, angular deformation, and rotation. These may occur singly
                          or in combination. Motion of the face (in the x-y plane) of an elemental cube of sides  x,
                           y, and  z in a time dt is shown in Fig. 14. Both translation and rotation involve motion or
                          deformation without a change in shape of the fluid element. Linear and angular deformations,
                          however, do involve a change in shape of the fluid element. Only through these linear and
                          angular deformations are heat generated and mechanical energy dissipated as a result of
                          viscous action in a fluid.
                             For linear deformation the relative change in volume is at a rate of
                                                             u   v    w
                                                       —
                                             ( — V dt     — V )/ V            div V
                                                     0
                                                        0
                                                             x   y    z
                          which is zero for an incompressible fluid, and thus is an expression for the continuity equa-
                          tion. Rotation of the face of the cube shown in Fig. 14d is the average of the rotations of
                          the bottom and left edges, which is
                                                                  dt
                                                       1   v    u
                                                       2   x    y
                          The rate of rotation is the angular velocity and is
                                                 v       about the z axis in the x-y plane
                                             1
                                                     u
                                          z
                                                     y
                                             2
                                                 x
                                             1
                                                 w
                                                      v
                                          x
                                             2   y    z   about the x axis in the y-z plane









                           Figure 11 Flow around a corner in a duct.  Figure 12 Flow around a corner into a duct.
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