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孤立波与淹没平板相互作用的三维波面和水动力实验研究 被引量:8
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作者 王千 刘桦 +1 位作者 房詠柳 邵奇 《力学学报》 EI CSCD 北大核心 2019年第6期1605-1613,共9页
在波浪水池中进行了孤立波作用下有限长度和有限宽度淹没平板的三维模型水池实验.首次应用多目视觉立体重构技术测量局部三维自由表面变形,该系统的有效测量水平范围为1.7 m×1.6 m.用4个三分力测力传感器组成水下测力系统,在不影... 在波浪水池中进行了孤立波作用下有限长度和有限宽度淹没平板的三维模型水池实验.首次应用多目视觉立体重构技术测量局部三维自由表面变形,该系统的有效测量水平范围为1.7 m×1.6 m.用4个三分力测力传感器组成水下测力系统,在不影响波面的情况下测量孤立波对平板的作用力和力矩.针对波浪不破碎的情况,选择0.4 m水深和0.16 m波高的来波条件,平板淹没深度为0.1 m.实验结果表明,孤立波经过淹没平板时自由面有明显的三维变形,导致孤立波波幅的时空变化.波幅在平板尾缘中心线处达到最大值,并沿展向逐渐减小.利用多目视觉立体重构系统得到的波面变化过程与浪高仪给出定点波面时间序列相互印证,表明建立的三维波面测量方法是有效的.孤立波对淹没平板作用的水动力载荷变化分为6个典型阶段,并与利用波面三维重构得到的波面测量结果一并讨论.基于多目视觉立体重构技术得到了垂向力和俯仰力矩极值点出现时的三维波面形态.建立的多目视觉立体重构系统将为海洋工程结构物的水池物理模型实验提供新的波面测量手段. 展开更多
关键词 物理实验 孤立波 淹没平板 波面重构 波浪载荷
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孤立波对淹没平板作用力的经验预报模型
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作者 杨凯恩 王千 刘桦 《水动力学研究与进展(A辑)》 CSCD 北大核心 2021年第2期288-294,共7页
该文通过物理模型实验和理论推导,研究了孤立波对淹没结构的载荷经验预报问题。基于狭道流动假设,推导了孤立波中临界淹没平板的Froude-Krylov力,得到了表征水平波浪力、垂向波浪力和倾覆力矩等水动力载荷系数有关的无量纲复合因子。考... 该文通过物理模型实验和理论推导,研究了孤立波对淹没结构的载荷经验预报问题。基于狭道流动假设,推导了孤立波中临界淹没平板的Froude-Krylov力,得到了表征水平波浪力、垂向波浪力和倾覆力矩等水动力载荷系数有关的无量纲复合因子。考虑波高和淹没深度对水动力载荷系数的影响,采用基于六分力天平组测量得到的孤立波经过平板时受到的水动力载荷,分别拟合了用复合因子和简单因子表征的经验公式,结果表明,基于复合因子给出的拟合公式较为简洁。基于无量纲复合因子,进一步考虑平板淹没深度的影响,在实验给定平板厚度和长宽比的条件下,建立了平板所受波浪载荷系数随孤立波相对波高、相对板长和相对淹没深度变化的经验公式。结果表明,在临界淹没状态下,随着相对波高增大,水平波浪力和垂向波浪力的首个极值系数均变大,其第二个极值系数均变小;俯仰力矩系数的前两个极值系数变大,而第三个极值系数变小;随着相对淹没深度增大,水平波浪力和垂向波浪力的极值系数均变小,俯仰力矩的第二个极值系数也变小。 展开更多
关键词 孤立波 淹没平板 水动力载荷 Froude-Krylov力 经验公式
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Hydroelastic Analysis of a Very Large Floating Structure Edged with a Pair of Submerged Horizontal Plates 被引量:2
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作者 MA Zhe CHENG Yong +1 位作者 ZHAI Gangjun OU Jinping 《Journal of Ocean University of China》 SCIE CAS 2015年第2期228-236,共9页
This paper is concerned with the hydroelastic problem of a very large pontoon-type floating structure(VLFS) edged with a pair of submerged horizontal plates, which is a combination of perforated and non-perforated pla... This paper is concerned with the hydroelastic problem of a very large pontoon-type floating structure(VLFS) edged with a pair of submerged horizontal plates, which is a combination of perforated and non-perforated plates attached to the for-end and back-end of the VLFS. For the hydroelastic analysis, the fluid is assumed to be ideal and its motion is irrotational so that a velocity potential exists. The VLFS is modeled as an elastic plate according to the classical thin plate theory. The fluid-structure interaction problem is separated into conventional hydrodynamics and structure dynamics by using modal expansion method in the frequency-domain. It involves, firstly, the deflection of the VLFS, which is expressed by a superposition of modal functions and corresponding modal amplitudes. Then the boundary element method is used to solve the integral equations of diffraction and radiation on the body surface for the velocity potential, whereas the vibration equation is solved by the Galerkin's method for modal amplitudes, and then the deflection is obtained by the sum of multiplying modal functions with modal amplitudes. This study examines the effects of the width and location of the non-perforated horizontal plates on the hydroelastic response of the VLFS, then the performance of perforated plates is investigated to reduce the motion near the fore-end of the VLFS. Considering the advantages and disadvantages of submerged plates without and with cylindrical holes, we propose a simple anti-motion device, which is a combination of a pair of perforated and non-perforated plates attached to the for-end and back-end of the VLFS. The effectiveness of this device in reducing the deformation and bending moment of the VLFS has been confirmed, and is compared with the results in cases without and with the submerged horizontal plates by the analysis in this paper. 展开更多
关键词 VLFS anti-motion device hydroelastic problems perforate horizontal plate submerged horizontal plate
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