Page 309 - Thomson, William Tyrrell-Theory of Vibration with Applications-Taylor _ Francis (2010)
P. 309

296                             Vibration of Continuous Systems   Chap. 9
                              9-14  Show  that  c  =  y¡G/p  is  the velocity of propagation of torsional  strain  along the  rod.
                                  What  is the  numerical value of c  for steel?
                              9-15  Determine  the  expression  for  the  natural  frequencies  of  torsional  oscillations  of  a
                                  uniform  rod  of length  /  clamped at  the  middle  and free  at the  two ends.
                              9-16  Determine  the  natural  frequencies of a  torsional  system  consisting of a  uniform  shaft
                                  of mass moment of inertia   with a disk of inertia  / q attached to each end. Check the

                                  fundamental  frequency  by  reducing  the  uniform  shaft  to  a  torsional  spring  with  end
                                  masses.
                              9-17  A uniform bar  has  these  specifications:  length  /,  mass  density per  unit volume  p,  and
                                  torsional  stiffness  IpG,  where  Ip  is  the  polar  moment  of inertia  of the  cross  section
                                  and  G  the  shear modulus. The  end  jc  =  0 is fastened  to a  torsional  spring of stiffness
                                  K  lb  •  in./rad,  and  the  end  /  is  fixed,  as  shown  in  Fig.  P9-17.  Determine  the
                                  transcendental equation from which natural  frequencies can be established. Verify the
                                  correctness of this equation  by considering special cases for   =  0 and  K = oc.






                                                                     Figure P9-17.


                              9-18  Name  some  of the  factors  not  accounted  for  in  the  method  presented  in  Sec.  9.4  for
                                  the calculation of the natural  frequencies of suspension bridges.
                              9-19  The  new  Tacoma  Narrows  Bridge,  reopened  on  October  14,  1950,  has  the  following
                                  data:
                                   / =  2800 ft (between  towers)
                                    =  60 ft (width between cables)
                                   k =  280 ft (maximum  sag of cables)
                                  w,  =  8570 Ib/lineal  ft
                                  /() =  ~P   (rotational  mass moment of inertia)

                                  Calculate  the  new  cable  tension,  the  cable  torsional  stiffness,  the  new  vertical  and
                                  torsional vibration  frequencies,  and  compare with  previous values.  (Assume  a reason­
                                  able  value  for  the  radius  of gyration  p  in  determining  the  torsional  mass  moment  of
                                  inertia.)
                              9-20  The following data on the Golden Gate Bridge was obtained from reports provided by
                                  the  district engineer for the bridge:
                                   /  =  4200 ft
                                  h  =  470 ft
                                  6  =  90 ft
                                   f
                                  (O =  28,720 Ib/ft (total weight per lineal  foot,  including cables)
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