2002
DOI: 10.1006/jfls.2002.0445
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Linear and Nonlinear Dynamics of Cantilevered Cylinders in Axial Flow. Part 3: Nonlinear Dynamics

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Cited by 69 publications
(41 citation statements)
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“…with a well streamlined end, yields distinct results depending on the length ℓ, figure 3(b). For short cylinders, ℓ ≪ 1, the divergence and flutter limits decrease with ℓ in a manner similar to that of the previous case, as could be predicted from the results of Semler et al (2002) (v =1.79/ℓ for divergence, v =4.72/ℓ for flutter). However, for long cylinders, divergence and flutter persist, in contrast to the previous case with f =0.5.…”
Section: 2supporting
confidence: 83%
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“…with a well streamlined end, yields distinct results depending on the length ℓ, figure 3(b). For short cylinders, ℓ ≪ 1, the divergence and flutter limits decrease with ℓ in a manner similar to that of the previous case, as could be predicted from the results of Semler et al (2002) (v =1.79/ℓ for divergence, v =4.72/ℓ for flutter). However, for long cylinders, divergence and flutter persist, in contrast to the previous case with f =0.5.…”
Section: 2supporting
confidence: 83%
“…The cylinder is modelled as a beam (with flexural rigidity set to zero in some cases), coupled with the fluid dynamics via inviscid terms (Lighthill 1960), friction and specific models of the flow-induced forces at the trailing end. Prediction of divergence and flutter using this model were found to be in good agreement with experiments in Semler et al (2002). Further refinements, including accounting for nonlinear effects, showed that the linear approach was robust, at least for the first instabilities encountered: divergence occurs in a supercritical form and is followed by flutter.…”
Section: Introductionsupporting
confidence: 53%
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