Influences of Floater Motion on Gap Resonance Triggered by Focused Wave Groups

The current study investigates the hydrodynamic characteristics of gap resonance within a narrow gap formed by two adjacent boxes subjected to incident focused transient wave groups. A two-dimensional (2D) numerical wave tank based on the OpenFOAM package is utilized for this purpose. The weather-si...

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Bibliographic Details
Published inChina ocean engineering Vol. 37; no. 4; pp. 685 - 697
Main Authors Gao, Jun-liang, Lyu, Jing, Zhang, Jian, Zang, Jun
Format Journal Article
LanguageEnglish
Published Berlin/Heidelberg Springer Berlin Heidelberg 01.08.2023
Springer Nature B.V
Key Laboratory of Water Security Guarantee in Guangdong-Hong Kong-Marco Greater Bay Area of Ministry of Water Resources,Guangzhou 510611,China%School of Naval Architecture and Ocean Engineering,Jiangsu University of Science and Technology,Zhenjiang 212100,China%Centre for Infrastructure,Geotechnical and Water Engineering(IGWE),Department of Architecture and Civil Engineering,University of Bath,BA2 7AY,UK
Key Laboratory of Port,Waterway and Sedimentation Engineering of MOT,Nanjing Hydraulic Research Institute,Nanjing 210029,China
School of Naval Architecture and Ocean Engineering,Jiangsu University of Science and Technology,Zhenjiang 212100,China
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ISSN0890-5487
2191-8945
DOI10.1007/s13344-023-0057-8

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Summary:The current study investigates the hydrodynamic characteristics of gap resonance within a narrow gap formed by two adjacent boxes subjected to incident focused transient wave groups. A two-dimensional (2D) numerical wave tank based on the OpenFOAM package is utilized for this purpose. The weather-side box is fixed while the lee-side box is allowed to heave freely under wave actions. The effects of the focused wave amplitude and spectral peak period on the wave amplification within the gap, motion of the lee-side box, and wave forces (including horizontal and vertical wave forces) acting on each box are systematically examined. For comparison, another structural layout consisting of two fixed boxes is also considered. The results reveal that the release of the heave degree of freedom (DoF) of the leeside box results in remarkably distinct resonance features. In the heave-box system, both its fluid resonant period and the period corresponding to the maximum heave displacement of the lee-side box are significantly larger (i.e., 1.6–1.7 times) than the fluid resonant period of the fixed-box system. However, the wave amplification factor inside the gap in the heave-box system is significantly lower than that in the fixed-box one. Both the variations of the maximum horizontal and vertical wave forces with the spectral peak period and their magnitudes are also significantly different between the two structural systems.
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ISSN:0890-5487
2191-8945
DOI:10.1007/s13344-023-0057-8