Page 117 - Thomson, William Tyrrell-Theory of Vibration with Applications-Taylor _ Francis (2010)
P. 117

104                                       Transient Vibration   Chap. 4

                                  Engineers  have  found  the  concept  of  the  shock  response  spectrum  to  be
                              useful in design. The shock response spectrum (SRS) is a plot of the maximum peak
                              response  of the  single-DOF  oscillator  as  a  function  of the  natural  period  of the
                              oscillator.  The  maximum  of the  peaks,  often  labeled  maximax,  represents  only  a
                              single  point  on  the  time  response  curve.  It  does  not  uniquely  define  the  shock
                              input  because  it  is  possible  for  two  different  shock  pulses  to  have  the  same
                              maximum  peak  response.  In  spite  of this  limitation,  the  SRS  is  a  useful  concept
                              that is extensively used,  especially for preliminary design.
                                  In  Eq.  (4.2-1),  the  response  of  a  system  to  arbitrary  excitation  fit)  was
                              expressed  in  terms  of the  impulse  response  hit).  For  the  undamped  single-DOF
                              oscillator, we  have
                                                      h(t)    ^  sm  (x)J
                                                             mo)„
                              so that the peak response  to be used in the response spectrum plot is given by the
                              equation
                                                       1
                                            •«(O m ax  =  moj -   i ' f i O  sin «„(i  -  (4.5-1)
                                                        n •'()
                              In the case where the shock is due to the sudden motion of the support point, fit)
                              is replaced by  —yit),  the  acceleration  of the support point,  as  in  Eq.  (4.2-5).
                                                      - 1
                                             ^ ( 0  max   i y(^) sin (o^it  -   O         (4.5-2)
                                                         •'n
                              With T as the natural period of the oscillator, the maximum value of xit) or zit) is
                              plotted as a function of  t^/r, where  r  is the natural period of the oscillator and  t^
                              is the pulse duration time.






















                                    Figure  4.5-1.  Response  for  t^/r  =  1/8,  which  gives ixk/Ffi^.^,^  =  0.80
                                    at  t^  =  0 . 3 2 t .
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