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PIPES CONVEYING FLUID: NONLINEAR  AND CHAOTIC DYNAMICS         349

              show that the interpretation of  the dynamics is very sensitive, in a way  that nonchaotic
              dynamics can never be, particularly when judging  the success or otherwise of  analytical
              modelling. This  will become evident  in the course of  the presentation,  and is discussed
              in the two paragraphs preceding the last two of  this section.
                The  system,  first  studied  experimentally  (Paidoussis  &  Moon  1988),  is  shown  in
              Figure 5.30. It consists of an elastomer vertical pipe conveying fluid. As already discussed
              in Chapter 3 and Section 5.7, at sufficiently high flow velocity, a Hopf bifurcation leads
              to a stable limit cycle. As the amplitude of motion increases with flow, for appropriately
              positioned  motion  constraints  (typically  metal  bars),  the  pipe  bangs  on  one constraint,
              rebounds  from  it,  and  then  generally  on  the  other,  back  and  forth,  without  making
              permanent  contact.  Thus, at  location  Xb,  a  very  large  restraining  force  is  operative  on
              impact, while during  ‘free flight’ between restraints there is none. It should be remarked
              that,  even  when  the  constraints  are rigid,  the  impact  involves local  deformation  of  the
              pipe, and hence the constraint may be modelled by a strongly nonlinear spring, involving
              a spring constant which varies discontinuously with displacement (see Figure 5.33).
                Experiments  were conducted  with several pipes, e.g. those listed in Table 5.3, mostly
              conveying water, but in a few cases conveying air. For these pipes the limit-cycle motions
              are planar - in a plane defined by minute imperfections in the pipe. At impact, however,
              the motion tends to deteriorate into a three-dimensional one. In order to keep the dynamics
              as simple as possible  for analytical  modelling, the oscillation was restricted to a plane,














                                         Motion sensor
                                         light beam











                                                         Embedded
                                                         steel strip
                                                        Constraining
                                                              bars

              Figure 5.30  (a)  Schematic  of  the  experimental  system  of  a  loosely  constrained  vertical
              cahevered pipe;  (b) scheme  of  achieving  planar  motions  by  guide-bars;-(c) refined  scheme  for
                planar motions, with steel strip embedded in the pipe, also showing motion-constraining bars.
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