Page 55 - Mechanical Engineer's Data Handbook
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44                                                  MECHANICAL ENGINEER’S DATA HANDBOOK

             Annulus bonded to sleeve:                   1.6.6   Critical speed of whirling of shatits
                 ~RLG
                                                         When a shaft rotates there is a certain speed at which, if
                                                         there is an initial deflection due to imperfections, the
                                                         centripetal force is equal to the elastic restoring force.
                                                         At this point the deflection increases to a large value
                                                         and the shaft is said to ‘whirl’. Above this speed, which
                                                         depends on the shaft dimensions, the material and the
                                                         loads carried by the shaft, the shaft whirling decreases.
                                                         Shafts must be run well below or well above this speed.
                                                         It can be shown that numerically the critical speed is
                                                         the  same as the  frequency  of  transverse  vibrations.
                                                         Formulae are given for several common cases.
                                                         Critical speed for all cases:
             Annulus bonded to disks:
                                                             1
                ZG                                       Nc=j+ii
                  (r:
             s == -rf)
                                                         where:  g=acceleration  due  to  gravity,  y= ‘static’
                                                         deflection at mass.


                                                         Cantilevered  shaft with disc at end

                                                         Mass of  shaft neglected.
                                                         N, = 1/2x,/m



             Hyperbolic contour:





                                                         Central disc, ‘short’ bearings

                                                         N,=  1 / 2 R J w ~












                                                         Non-central disc, short  bearings

                                                         N, = 1 / 2 R , / m
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