Page 82 - Industrial Ventilation Design Guidebook
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4,1 FLUID FLOW                                                             47














                  FIGURE 4.1  Viscosity



                     Surface Tension
                     Surface tension is the property of a fluid that produces capillary action, the
                  rise and fall in a tube.
                     Water in a tube wets the glass, and the liquid rises, producing a cup. In
                  the case of mercury, the glass is not wetted and the liquid falls, producing an
                  inverted cup.

                     Viscosity
                     Viscosity is the shear resistance between adjacent fluid layers. Con-
                  sider in Fig. 4.1 the shearing action between two parallel planes, each of
                  area A, separated by a distance Y. The tangential force F for a given area
                  required to slide one plate over the other at a velocity (v) parallel to each
                  other is




                  The proportionality factor /u, is the dynamic viscosity of the fluid, its units be-
                                     2
                                                              2
                  ing force x time/length  and is expressed as N s m~  or Pa s.
                     Examination of the thermodynamic properties of fluid tables shows how
                  the viscosity varies with temperature. In order to obtain a general impression
                  of this, consider the data in the thermal properties of fluid tables and the vari-
                  ous values at different temperatures.
                     Another viscosity unit is the kinematic viscosity v. This is the ratio of vis-
                                                                          2
                                                                             1
                  cosity to density. Common units used for this are the stoke (1 cm  s"" ) and the
                                   1
                                 2
                  centistoke (1 mm  s" ).
                     Because the velocity change in the y direction is linear, Eq. (4.8) can be
                  written as


                  When the shearing stress T — F/A,




                  With most fluids the shearing stress r is linearly proportional to the change of
                 velocity; hence viscosity /u, is not a function of dv/dy, A fluid having these
                 characteristics is called a Newtonian fluid.
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