Page 82 - Singiresu S. Rao-Mechanical Vibrations in SI Units, Global Edition-Pearson (2017)
P. 82

1.9  dampinG elements    79
                                    From the definition of the rotational damping constant of the bearing 1c t 2:
                                                                         T
                                                                     c t =                              (E.5)
                                                                         v
                                    we obtain the desired expression for the rotational damping constant as
                                                                           3
                                                                       2pmR l
                                                                   c t =                                (E.6)
                                                                         d
                                    Note: Equation (E.4) is called Petroff’s law and was published originally in 1883. This equation is
                                    widely used in the design of journal bearings [1.43].

                                                                                                           ■

                                    piston-Cylinder dashpot
                 example 1.16
                                    Develop an expression for the damping constant of the dashpot shown in Fig. 1.44(a).
                                    Solution:  The damping constant of the dashpot can be determined using the shear-stress equation
                                    for viscous fluid flow and the rate-of-fluid-flow equation. As shown in Fig. 1.44(a), the dashpot
                                    consists of a piston of diameter D and length l, moving with velocity v 0  in a cylinder filled with a
                                    liquid of viscosity m [1.24, 1.32]. Let the clearance between the piston and the cylinder wall be d. At
                                    a distance y from the moving surface, let the velocity and shear stress be v and t, and at a distance
                                    1y + dy2, let the velocity and shear stress be 1v - dv2 and 1t + dt2, respectively (see Fig. 1.44(b)).
                                    The negative sign for dv shows that the velocity decreases as we move toward the cylinder wall. The
                                    viscous force on this annular ring is equal to
                                                                             dt
                                                              F = pDl dt = pDl    dy                    (E.1)
                                                                              dy


                                                P                                 P






                                                             Cylinder                          Cylinder
                                                                               y      y
                                                                      dy                     dy


                                    l           v 0          Piston   l           v 0          Piston
                                         d      D      d                   d      D      d
                                                             Viscous                           Viscous
                                                               fluid                            fluid
                                                (a)                               (b)

                                    FiGure 1.44  A dashpot.
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