Page 432 - Thomson, William Tyrrell-Theory of Vibration with Applications-Taylor _ Francis (2010)
P. 432

13







                                           Random Vibrations













                             The  types  of  functions  we  have  considered  up  to  now  can  be  classified  as
                             deterministic,  i.e.,  mathematical  expressions  can  be  written  that  will  determine
                             their instantaneous values at any time  t. There are,  however, a number of physical
                             phenomena  that  results  in  nondeterministic  data  for  which  future  instantaneous
                             values cannot be predicted  in  a deterministic sense.  As examples, we can mention
                             the  noise  of  a jet  engine,  the  heights  of waves  in  a  choppy  sea,  ground  motion
                             during  an  earthquake,  and  pressure  gusts  encountered  by  an  airplane  in  flight.
                             These  phenomena  all  have  one  thing  in  common:  the  unpredictability  of  their
                             instantaneous  value  at  any  future  time.  Nondeterministic  data  of  this  type  are
                             referred to  as  random  time functions.


                      13.1  RANDOM PHENOMENA

                             A sample of a typical random time function is shown in Fig.  13.1-1.  In spite of the
                             irregular character of the function, many random phenomena exhibit some degree
                             of  statistical  regularity,  and  certain  averaging  procedures  can  be  applied  to
                             establish  gross characteristics useful in engineering design.
                                 In  any  statistical  method,  a  large  amount  of  data  is  necessary  to  establish
                             reliability. For example, to establish the statistics of the pressure fluctuation due to
                             air turbulence over a certain air route, an airplane may collect hundreds of records
                             of the type shown  in  Fig.  13.1-2.
                                 Each  record  is  called  a  sample,  and  the  total  collection  of samples  is  called
                             the ensemble. We can compute the ensemble average of the instantaneous pressure
                             at  time  t^.  We  can  also  multiply  the  instantaneous  pressures  in  each  sample  at
                             times   and   +  r,  atid  average  these  results  for  the  ensemble.  If such  averages
                             do  not  differ  as  we  choose  different  values  of  t^,  then  the  random  process
                             described by this ensemble  is said to be  stationary.


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