2013
DOI: 10.1016/j.jfluidstructs.2013.03.008
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Computational study of vortex-induced vibration of a sprung rigid circular cylinder with a strongly nonlinear internal attachment

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Cited by 38 publications
(16 citation statements)
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“…The coupled system of equations (11,12) and the discretized equations governing the motion of the fluid flow, used to evaluate the lift coefficient, are solved in a staggered fashion; i.e., we have assumed that, in the solution of the fluid-structure interaction problem, there is no need for equilibrating iterations in each time step, since the structure considered here is rigid, and provided that the time-step size is chosen small enough. This assumption was shown to be satisfactory by Tumkur [33], who performed computations in which the fluid and structural responses at each time step were computed iteratively, with insignificant effects on the response of the system (compared to the solution obtained without equilibrating iterations).…”
Section: Physical Model and Governing Equationsmentioning
confidence: 99%
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“…The coupled system of equations (11,12) and the discretized equations governing the motion of the fluid flow, used to evaluate the lift coefficient, are solved in a staggered fashion; i.e., we have assumed that, in the solution of the fluid-structure interaction problem, there is no need for equilibrating iterations in each time step, since the structure considered here is rigid, and provided that the time-step size is chosen small enough. This assumption was shown to be satisfactory by Tumkur [33], who performed computations in which the fluid and structural responses at each time step were computed iteratively, with insignificant effects on the response of the system (compared to the solution obtained without equilibrating iterations).…”
Section: Physical Model and Governing Equationsmentioning
confidence: 99%
“…A prototypical VIV model consists of the flow past a circular cylinder mounted on a grounded linear spring, and constrained to move in the cross-flow direction. Recent studies have investigated the dynamics of a system in which the dimensionality of the standard VIV configuration is augmented by coupling the cylinder with an essentially nonlinear dissipative attachment (or nonlinear energy sink, NES), which is free to translate and/or rotate inside the cylinder (with no gravitational effects) [33][34][35]. The NES, because it features a dissipative element and strong inertial nonlinearity, has the capacity to absorb vibrational energy from the primary structure to which it is attached, over broad frequency and energy ranges and for various types of narrowband or broadband excitations.…”
Section: Introductionmentioning
confidence: 99%
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“…In [17], a nonlinear damping element was added in parallel with the LTVA to decrease the maximum LCO amplitude. Other nonlinear vibration absorbers, including the autoparametric vibration absorber [18,19], the nonlinear energy sink (NES) [20][21][22][23][24][25][26][27][28] and the hysteretic tuned vibration absorber [29], have also been considered to increase the effectiveness of vibration attenuation. In particular, the NES exhibited three different mechanisms to suppress LCOs, namely complete, partial and intermittent suppression.…”
Section: Introductionmentioning
confidence: 99%