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PIPES CONVEYING FLUID: NONLINEAR AND CHAOTIC DYNAMICS          3 15

              state  by  integrating  numerically  the  time-independent  version  of  the  full  equations  of
              motion.
                Experiments  have  also  been  conducted  by  Yoshizawa  et al. (1985,  1986), utilizing
               vertical  silicone  rubber  pipes  (Do = 5 mm,  Di = 3 mm,  L = 600mm) conveying  water.
              Two stainless steel wires were attached to the pipe in one plane, to ensure that motions
              occur normal to that plane. The pinned, axially-sliding lower end was achieved by a short
              bar perpendicular to the pipe axis, in contact with the pipe.
                Typical results  are shown  in Figure 5.10(a) for the variation of  the first-mode eigen-
               frequency up to divergence, when theoretically w1  = 0. The experimental frequencies are
               in excellent  agreement with theory. Nevertheless, for obvious reasons, the experimental
              frequencies could not be measured all the way to divergence, the precise onset of  which
               was difficult to pin-point.





















               Figure 5.10  (a) Variation of  the first-mode eigenfrequency with  u2 for a clamped-pinned  pipe
               with an axially sliding downstream end (B = 0.273, y = 34.4, a!  = 4.68): -,   theory;  0, exper-
               iments. (b) The post-divergence maximum static pipe deflection, qmax versus u2  (a! = 5.56): - - -,
                  approximate analytical; -,   numerical; 0, experimental (Yoshizawa et al. 1985, 1986).


                 The variation of  the maximum,  steady post-divergence  amplitude with  u2 is given in
               Figure 5.10(b). It is seen that  (i) the approximate analytical and the numerical solutions
               agree for qmax i 0.1 approximately, and (ii) agreement with experimental values is very
               good overall, particularly for the more accurate numerical results.


               5.5.4  Impulsively excited 3-D motions

               An interesting, application-related study, examines the dynamics of inhibited flow/porous
               tubes  (INPORTs) used  to  protect  the  inner  wall  of  inertial  confinement  fusion  (ICF)
               reactors? from X-rays, neutron bombardment and dCbris (Engelstad & Love11 1985, 1995;
               Engelstad  1988). The porous,  braided  silicon-carbide-fibre tubes  convey  Li-Pb  (molten
               lithium-lead),  the  fluid acting both  as a coolant  and a breeder;  the tubes  are porous,  to
               ooze  out  a  liquid  film for protection  from the  same hazards.  These  very  slender  tubes

                 +The ICF is a precursor concept to the LIBRA fusion reaction chamber.
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