非线性波消波及波场分布研究   总被引：1，自引：1，他引：0  

王巧莎  李明海 《海洋科学》2018,42(6):30-38

本文基于雷诺平均N-S方程,并结合RNG k-e方程建立了粘性数值波浪水槽,对不同波陡、不同相对水深、不同相对波高的非线性规则波的阻尼消波问题和波场分布进行研究。文中提出了两种描述消波区内部阻尼变化的阻尼函数,分别适用于小波陡情形和高波陡情形。研究结果表明,小波陡组消波区可设为一个波长,阻尼系数取10~4～10~5即可满足消波要求,计算结果与实验结果及造波理论吻合良好;高波陡组消波区可设为两个波长,阻尼系数取10~4～10~5亦可满足消波要求,计算结果与实验结果吻合良好。此外,当波陡较小时,波场内反射情况的小幅改变即可对整个波场造成影响,特别是当水深较浅时这种影响极为明显,需谨慎考虑。当波陡较大时,水波能量较高,整个波场沿水波传播方向可观测到明显的衰减现象,在具体试验中需进行考虑。  相似文献   

唐山M 4.8地震地磁谐波振幅比变化     

贾立峰  乔子云  张国苓  寇海川 《地震地磁观测与研究》2018,39(5):39-47

针对2012年5月28日河北唐山M 4.8地震，采用地磁谐波振幅比方法，分析昌黎、静海、红山及承德地磁台2007年1月至2015年12月地磁观测数据，结果显示：各台站10 min周期的计算结果波动性明显，其他周期形态较为一致；距震中最近的昌黎地磁台Y_ZHx（NS）测向的10-40 min周期地磁谐波在下降至极低值后，开始转折时发生地震，而Y_ZHy（EW）测向未出现明显转折现象；位于河北平原地震带中部的静海地磁台对此次地震反应显著，2个测向在震前均出现下降-转折-上升的变化特征。通过对比位于不同地区的4个地磁台站地磁谐波振幅比变化，发现受大范围整体构造应力场作用的影响，计算结果具有相似的趋势性变化特征，具体到局部地区或断裂带内部，各台站之间显示出一定差异。  相似文献   

山西地区远震P波到时残差分布     

石磊  李凤  刘静  韩文英 《地震地磁观测与研究》2018,40(1):43-47

收集2008-2016年山西地震台网记录的震中距30°-90°范围内1 253个远震事件波形，拾取7 600余条高质量P波初至到时，使用IASP91模型计算相对到时残差，分析残差水平分布特征，结果显示：①以山西地区中部的山西断裂带为界，西部地震台站记录的P波初至主要表现为早到时，东部位于大同火山区的地震台站记录则主要表现为晚到时；②位于山西断裂带内部的地震台站记录的P波初至主要表现为早到时，残差水平显著低于西部地震台站；③研究区P波到时整体呈现自西向东逐渐由早到晚的分布特征。推测山西断裂带西部地区下方可能存在高速异常结构，山西断裂带内部及大同火山区下方可能存在低速异常结构。  相似文献   

Characteristics of breaking irregular wave forces on a monopile     

《Applied Ocean Research》2019

The substructures of offshore wind turbines are subjected to extreme breaking irregular wave forces. The present study is focused on investigating breaking irregular wave forces on a monopile using a computational fluid dynamics (CFD) based numerical model. The breaking irregular wave forces on a monopile mounted on a slope are investigated with a numerical wave tank. The experimental and numerical irregular free surface elevations are compared in the frequency-domain for the different locations in the vicinity of the cylinder. A numerical analysis is performed for different wave steepness cases to understand the influence of wave steepness on the breaking irregular wave loads. The wave height transformation and energy level evolution during the wave shoaling and wave breaking processes is investigated. The higher-frequency components generated during the wave breaking process are observed to play a significant role in initiating the secondary force peaks. The free surface elevation skewness and spectral bandwidth during the wave transformation process are analysed and an investigation is performed to establish a correlation of these parameters with the breaking irregular wave forces. The role of the horizontal wave-induced water particle velocity at the free surface and free surface pressure in determining the breaking wave loads is highlighted. The higher-frequency components in the velocity and pressure spectrum are observed to be significant in influencing the secondary peaks in the breaking wave force spectrum.  相似文献   

结合IR-MAD与均值漂移算法的密集城区遥感影像变化检测     

聂倩  赵艳福 《测绘通报》2020,(6):57-62

不同时相遥感影像变化检测已成为土地利用变更调查、城市扩张分析、自然灾害分析及其他环境问题必不可少的技术手段之一。本文提出了一种结合IR-MAD与均值漂移算法的密集城区遥感影像变化检测方法。该方法通过伪不变特征法完成两期影像的相对辐射校正，有效改善影像间的配准误差，并利用IR-MAD算法对校正后的影像进行迭代运算，采用均值漂移算法对迭代后的影像进行分割，同时运用形态学方法处理分割后的影像，最终提取变化图斑。试验结果表明，该方法可以有效检测出变化区域，可应用于城市地表覆盖的变化检测。  相似文献   

An extreme wave event in eastern Yucatán,Mexico: Evidence of a palaeotsunami event during the Mayan times     

Javier Lario  Chris Spencer  Teresa Bardají  Ángel Marchante  Victor H. Garduño-monroy  Jorge Macias  Sergio Ortega 《Sedimentology》2020,67(3):1481-1504

The Yucatán Peninsula, Mexico, has typically been considered a tectonically stable region with little significant seismic activity. The region though, is one that is regularly affected by hurricanes. A detailed survey of ca 100 km of the eastern Yucatán and Cozumel coast identified the presence of ridges containing individual boulders measuring >1 m in length. The boulder ridges reach 5 m in height and their origin is associated with extreme wave event activity. Previously modelled tsunami waves from known seismically active zones in the region (Muertos Thrust Belt and South Caribbean Deformed Belt) are not of sufficient scale in the area of the Yucatán Peninsula to have produced the boulder ridges recorded in this study. The occurrence of hurricanes in this region is more common, but two of the most destructive (Hurricane Gilbert 1988 and Hurricane Wilma 2005) produced coastal waves too small to have created the ridges recorded here. In this paper, a new tsunami model with a source area located on the Motagua/Swan Island Fault System has been generated that indicates a tsunami event may have caused the extreme wave events that resulted in the deposition of the boulder ridges.  相似文献   

点吸收式波浪能俘获装置结构优化方法研究     

王鑫  李大鸣  王兵振  韩林生 《海洋与湖沼》2020,51(2):293-297

根据布设海域波浪能资源特征,对点吸收式波浪能装置结构进行优化,可有效提高装置的能量俘获效率。本文以威海褚岛北部海域为装置布设目标海域,在对该海域波浪资源特征进行统计分析的基础上,计算得到装置的直径,同时利用数值软件计算出多组工况下点吸收装置吃水深度和装置固有周期的对应关系,并利用统计学方法得出装置固有周期随吃水深度的变化规律,进而分析得出装置在该海域的最佳设计吃水深度,为点吸收波浪能装置结构优化设计提供了新的思路。该方法对于其他技术类型波浪能装置的结构优化设计同样具有借鉴意义。  相似文献   

我国海洋动力灾害研究进展与展望   总被引：1，自引：0，他引：1  

侯一筠  尹宝树  管长龙  郭明克  刘桂梅  胡珀 《海洋与湖沼》2020,51(4):759-767

海洋动力灾害(包括灾害性海浪、风暴潮、海冰、海啸等)是对我国沿海地区造成破坏和损失最大的自然灾害之一。开展海洋动力灾害研究具有重要意义和迫切的国家需求。本文回顾我国建国以来在海洋动力灾害研究方向的主要进展,重点针对近年来我国在海洋动力灾害数值模拟预报以及灾害风险评估等方面的进展进行综述,并在此基础上提出未来的发展展望,希望给海洋防灾减灾科研工作者提供参考。  相似文献   

海岸波浪多次破碎波能耗散模型   总被引：1，自引：0，他引：1  

闫圣  邹志利 《海洋学报》2020,42(9):30-37

在坡度很缓(接近或小于1∶100)的海岸，波浪在向海岸传播的过程中，可能经历多次破碎，而在两次波浪破碎之间将伴随着波浪恢复(波浪恢复到不破碎状态)。在现有海岸波高计算模型中，波浪破碎是通过波能耗散来模拟的，但所采用的波能耗散模型都不能自动考虑波浪出现多次破碎的过程，特别精确模拟这一过程中出现的波浪恢复。本文提出了解决这一问题的新的波能耗散模型，模型的建立是通过在Dally模型中重新建立稳定波能、饱和波高水深比和波能耗散系数，并引入了波浪恢复的判断条件实现的。该模型的波能耗散在波浪恢复区的值很小故能描述波浪恢复区的波浪运动。与实验结果的对比表明，新模型可以适合缓坡情况波浪多次破碎的波高模拟，而且对不同坡度的平坡和沙坝海岸(1∶100～1∶10)的破碎波模拟都可以给出与实验结果符合的结果，并且可以自动识别多次波浪破碎的存在和波浪恢复的发生。  相似文献   

北极薄冰-煎饼冰区域中不同重力波驱动形成海流的敏感性分析     

张雪妍  戴海瑨  赵军  殷何卿 《海洋学报(英文版)》2020,39(3):123-129

A coupled ocean-ice-wave model is used to study ice-edge jet and eddy genesis during surface gravity wave dissipation in a frazil-pancake ice zone. With observational data from the Beaufort Sea, possible wave dissipation processes are evaluated using sensitivity experiments. As wave energy dissipated, energy was transferred into ice floe through radiation stress. Later, energy was in turn transferred into current through ocean-ice interfacial stress. Since most of the wave energy is dissipated at the ice edge, ice-edge jets, which contained strong horizontal shear, appeared both in the ice zone and the ocean. Meanwhile, the wave propagation direction determines the velocity partition in the along-ice-edge and cross-ice-edge directions, which in turn determines the strength of the along-ice-edge jet and cross-ice-edge velocity. The momentum applied in the along-ice-edge(cross-ice-edge)direction increased(decreased) with larger incident angle, which is favorable condition for producing stronger mesoscale eddies, vice versa. The dissipation rate increases(decreases) with larger(smaller) wavenumber, which enhances(reduces) the jet strength and the strength of the mesoscale eddy. The strong along-ice-edge jet may extend to a deep layer(> 200 m). If the water depth is too shallow(e.g., 80 m), the jet may be largely dampened by bottom drag, and no visible mesoscale eddies are found. The results suggest that the bathymetry and incident wavenumber(magnitude and propagation direction) are important for wave-driven current and mesoscale eddy genesis.  相似文献