陈浩民,倪云林. 非淹没双直立圆柱系统波浪爬升的数值模拟[J]. 水利水运工程学报,2020(6):42-47. doi: 10.12170/20191018004
引用本文: 陈浩民,倪云林. 非淹没双直立圆柱系统波浪爬升的数值模拟[J]. 水利水运工程学报,2020(6):42-47. doi: 10.12170/20191018004
(CHEN Haomin, NI Yunlin. Numerical analysis of wave run-up characteristics on dual non-submerged vertical cylinders system[J]. Hydro-Science and Engineering, 2020(6): 42-47. (in Chinese)). doi: 10.12170/20191018004
Citation: (CHEN Haomin, NI Yunlin. Numerical analysis of wave run-up characteristics on dual non-submerged vertical cylinders system[J]. Hydro-Science and Engineering, 2020(6): 42-47. (in Chinese)). doi: 10.12170/20191018004

非淹没双直立圆柱系统波浪爬升的数值模拟

Numerical analysis of wave run-up characteristics on dual non-submerged vertical cylinders system

  • 摘要: 波浪爬升是近海构筑物和海洋平台结构设计中的重要参数。全面掌握波浪的爬升特性有利于结构的安全保证和优化。采用有限元方法建立了求解Berkhoff缓坡方程的数值模型,并计算了非淹没单个直立圆柱周围的波高分布,计算结果与解析解吻合很好。以非淹没双直立圆柱为研究对象,探讨了圆柱间距对波浪爬升的影响。结果表明:上游圆柱周围的波高分布曲线波动较大,但最大相对波高和最小相对波高的发生位置基本与单个圆柱的情况相同;当圆柱间距为1/4波长的奇数倍时,最小相对波高明显减小,圆柱肩部出现第二峰值;而当圆柱间距为1/4波长的偶数倍时,最小相对波高则明显增加,圆柱肩部出现第二谷值。下游圆柱周围的波高分布曲线与单个圆柱的情况相似,但波高相对较小。

     

    Abstract: Wave run-up is an important parameter in offshore structures and ocean platforms design. A comprehensive understanding of its characteristics benefits the structural safety and design optimization. In this study, a numerical model is set up to solve the mild slope equation proposed by Berkhoff using the finite element method. The computational results of wave height distribution around the single non-submerged vertical cylinder match with the analytical solutions very well, verifying the validity of the numerical model. Subsequently, the effect of the spacing between two cylinders on wave run-up is investigated by observing the dual non-submerged vertical cylinders system. The numerical results show that the curve of wave height distribution around the upstream cylinder has a big fluctuation. However, the positions of maximum and minimum wave heights are the same as those in the single cylinder case. When the spacings are odd times of 1/4 incident wavelength, the minimum wave height decreases obviously and the secondary peak appears on the shoulder of the cylinder; when the spacings are even times of 1/4 incident wavelength, the minimum wave height obviously increases and the secondary trough appears on the shoulder of the cylinder. The curve of wave height distribution around the downstream cylinder is similar but smaller than that in the single cylinder case.

     

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