Page 102 - Thomson, William Tyrrell-Theory of Vibration with Applications-Taylor _ Francis (2010)
P. 102

Chap. 3   Problems                                              89


                                 instrument  on  a  rubber  pad  with  the  following  properties:  k  =  2802  N /cm   and
                                 f  ==  0.10.  W hat  acceleration  is  transmitted  to  the  instrument?
                             3-30  If the  instrument of Prob.  3-29 can  only tolerate  an  acceleration  of 2.03 cm /s^,  suggest
                                 a  solution  assuming  that  the  same  rubber  pad  is  the  only  isolator  available.  Give
                                 numerical  values  to  substantiate  your  solution.
                             3-31  For  the  system  shown  in  Fig.  P3-31,  verify  that  the  transmissibility  TR  =  \x /y  \  is  the
                                 same  as  that  for  force.  Plot  the  transmissibility  in  decibels,  201og|TO|  versus  (o/a>^
                                 between  co/co^  =  1.50  to  10 with  ^  =  0.02, 0 .0 4 ,..., 0.10.




                                                          X         Figure  P3-31.





                             3-32  Show  that  the  energy  dissipated  per  cycle  for  viscous  friction  can  be  expressed  by
                                                iV,,

                                                         1 -   ((0/i0„y]  +  [2é{(ü/(0„)Ÿ
                             3-33  Show  that  for viscous  damping,  the  loss  factor  rj  is  independent  of the  amplitude  and
                                 proportional  to  the  frequency.
                             3-34  Express the  equation  for the  free vibration  of a  single-DOF system  in  terms of the  loss
                                 factor  7]  at  resonance.
                             3-35  Show  that  t„ / tj  plotted  against   is  a  quarter  circle  where  tj  is  the  damped  natural
                                 period,  and   is  the  undamped  natural  period.
                             3-36  For  small  damping,  the  energy  dissipated  per  cycle  divided  by  the  peak  potential
                                 energy  is  equal  to  28  and  also  to  1 /Q .  [See  Eq.  (3.7-6).]  For  viscous  damping,  show
                                 that
                                                               TTCO, ,
                                                                  i
                                                            5  =  —r ^
                             3-37  In  general,  the  energy  loss  per  cycle  is  a  function  of  both  amplitude  and  frequency.
                                 State  under  what  condition  the  logarithmic  decrement  8  is  independent  of  the
                                 amplitude.
                             3-38  Coulomb damping between dry surfaces is  a constant  D  always opposed to the  motion.
                                 Determine  the  equivalent  viscous  damping.
                             3-39  Using  the  result  of  Prob.  3-38,  determine  the  amplitude  of  motion  of  a  spring-mass
                                 system  with  Coulomb  damping  when  excited  by  a  harmonic  force   sin (ot.  U nder
                                 what  condition  can  this  motion  be  maintained?
                             3-40  Plot  the  results  of Prob.  3-39  in  the  permissible  range.
                             3-41  The  shaft  of  a  torsiograph,  shown  in  Fig.  P3-41,  undergoes  harmonic  torsional
                                 oscillation   sin cot.  Determ ine  the  expression  for  the  relative  amplitude  of the  outer
                                 wheel  with  respect  to  (a)  the  shaft  and  (b)  a  fixed  reference.
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