Elsevier

Applied Ocean Research

Volume 2, Issue 1, January 1980, Pages 3-12
Applied Ocean Research

Fluid-induced inertia and damping in vibrating offshore structures

https://doi.org/10.1016/0141-1187(80)90042-5Get rights and content

Abstract

The problem addressed in this paper is that of the fluid-structure interaction in offshore structures for which effects due to fluid viscosity are negligible. A method for evaluating the dynamic response of structures is described in which the generalized coordinates for the analysis are associated with the ‘dry’ modes of the structure. All hydrodynamic actions, including those induced by motions of the structure, are retained on the right-hand side of the equations of motion. This formulation requires the determination of generalized added mass and damping matrices associated with motions of the structure in its first few ‘dry’ modes. By these means, free surface and three dimensional fluid flow effects are retained in the analysis. Examples of the resulting frequency dependent matrices, computed using the boundary integral method, are presented for some common structural forms, and the validity of this approach is demonstrated through some experiments on a deforming column structure. Finally, results for the wave-excited dynamic response of a typical offshore structure obtained using (i) conventional strip theory ‘wet’ modes, and (ii) ‘dry’ modes, are compared.

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  • Simplified methods for efficient seismic design and analysis of water-surrounded composite axisymmetric structures

    2015, Ocean Engineering
    Citation Excerpt :

    When subjected to earthquake loads, the interaction between an axisymmetric structure and the surrounding water induces hydrodynamic loads while affecting the structural dynamic properties such as natural periods. Earlier literature devoted to the analysis of the vibration characteristics and dynamic response of immersed axisymmetric structures can be roughly classified into three categories depending on the type of modeling adopted for hydrodynamic loads: (i) added-mass formulations where the effect of surrounding water is approximated by added masses distributed along the height of the structure (Lamb, 1932; Nagaya and Hai, 1985; Chang and Liu, 1989; Barltrop and Adams, 1991; Spyrakos and Xu, 1997; Uowska and Koodziej, 1998; Öz, 2003; Wu and Chen, 2005), (ii) continuum-based solutions where hydrodynamic loads are obtained as analytical solutions of the wave equation governing hydrodynamic pressure (Liaw and Chopra, 1974; Eatock Taylor and Duncan, 1980; Williams, 1986; Tanaka and Hudspeth, 1988; Goyal and Chopra, 1989; Xing and Price, 1997; Wei et al., 2012), and (iii) finite element, boundary element or scaled boundary finite element approaches based on the discretization of the surrounding water (Everstine, 1981; Olson and Bathe, 1985; Chen, 2000; Czygan and von Estorff, 2002; Sigrist and Garreau, 2007; Millán et al., 2009; Lu and Jeng, 2010; Tao et al., 2007; Meng and Zou, 2012; Li et al., 2013a,b; Liu and Lin, 2013). Although the dynamic response of axisymmetric structures surrounded by water can now be solved using coupled fluid–structure finite or boundary elements, most of these techniques have not yet been fully implemented in day-to-day engineering practice, especially at the early stages of seismic design, as they require specialized software or advanced programming, and may result in extensive modeling and computational efforts, combined with high-level expertise.

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