Page 64 - Thomson, William Tyrrell-Theory of Vibration with Applications-Taylor _ Francis (2010)
P. 64

Harmonically

                                              Excited Vibration












                              When  a  system  is  subjected  to  harmonic  excitation,  it  is  forced  to  vibrate  at  the
                              same frequency as that of the  excitation.  Common  sources of harmonic excitation
                              are  unbalance  in  rotating  machines,  forces  produced  by  reciprocating  machines,
                              and  the  motion  of  the  machine  itself.  These  excitations  may  be  undesirable  for
                              equipment whose  operation  may be  disturbed  or  for the  safety of the  structure  if
                              large vibration  amplitudes develop.  Resonance is to be avoided in most cases, and
                              to  prevent  large  amplitudes  from  developing,  dampers  and  absorbers  are  often
                              used. Discussion of their behavior is of importance for their intelligent use. Finally,
                              the  theory of vibration-measuring  instruments  is  presented  as  a  tool  for vibration
                              analysis.


                       3.1  FORCED HARMONIC VIBRATION

                              Harmonic  excitation  is  often  encountered  in  engineering systems.  It  is  commonly
                             produced by the unbalance in rotating machinery. Although pure harmonic excita­
                              tion is less likely to occur than periodic or other types of excitation, understanding
                              the  behavior  of  a  system  undergoing  harmonic  excitation  is  essential  in  order  to
                              comprehend  how  the  system  will  respond  to  more  general  types  of  excitation.
                              Harmonic excitation may be  in the form of a force or displacement of some point
                              in the system.
                                  We will first consider a single-DOF system with viscous damping, excited by a
                              harmonic force   sin cot, as shown in Fig. 3.1-1. Its differential equation of motion
                              is found from the free-body diagram to be
                                                    mx   cx  -\-  kx  = Ff. sin cot       (3.1-1)

                                  The  solution  to  this  equation  consists  of  two  parts,  the  complementary
                             function,  which  is  the  solution  of  the  homogeneous  equation,  and  the  particular

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