Wave-Induced Turbulence, Linking Metocean and Large Scales

A. Babanin
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At the atmospheric side of the interface, the air-sea coupling is usually described by means of the drag coefficient Cd, which is parameterised in terms of the wind speed, but the scatter of experimental data with respect to such dependences is very significant and has not improved noticeably over some 40 years. It is argued that the scatter is due to multiple mechanisms which contribute into the sea drag, many of them are due to surface waves and cannot be accounted for unless the waves are explicitly known.\n The Cd concept invokes the assumption of constant-flux layer, which is also employed for vertical profiling of the wind measured at some elevation near the ocean surface. The surface waves, however, modify the balance of turbulent stresses very near the surface, and therefore such extrapolations can introduce significant biases. This is particularly essential for buoy measurements in extreme conditions, when the anemometer mast is within the Wave Boundary Layer (WBL) or even below the wave crests. In this presentation, field data and a WBL model are used to investigate such biases. It is shown that near the surface the turbulent fluxes are less than those obtained by extrapolation using the logarithmic-layer assumption, and the mean wind speeds very near the surface, based on Lake George field observations, are up to 5% larger. The dynamics is then simulated by means of a WBL model coupled with nonlinear waves, which revealed further details of complex behaviours at wind-wave boundary layer.\n Furthermore, we analyse the structure of WBL for strong winds (U10 > 20 m/s) based on field observations. We used vertical distribution of wind speed and momentum flux measured in Topical Cyclone Olwyn (April 2015) in the North-West shelf of Australia. A well-established layer of constant stress is observed. The values obtained for u⁎ from the logarithmic profile law against u⁎ from turbulence measurements (eddy correlation method) differ significantly as wind speed increases.\n Among wave-induced influences at the ocean side, the ocean mixing is most important. Until recently, turbulence produced by the orbital motion of surface waves was not accounted for, and this fact limits performance of the models for the upper-ocean circulation and ultimately large-scale air-sea interactions.\n While the role of breaking waves in producing turbulence is well appreciated, such turbulence is only injected under the interface at the vertical scale of wave height. The wave-orbital turbulence is depth-distributed at the scale of wavelength (∼10 times the wave height) and thus can mix through the ocean thermocline in the spring-summer seasons. Such mixing then produces feedback to the large-scale processes, from weather to climate. In order to account for the wave-turbulence effects, large-scale air-sea interaction models need to be coupled with wave models.\n Theory and practical applications for the wave-induced turbulence will be reviewed in the presentation. These include viscous and instability theories of wave turbulence, direct numerical simulations and laboratory experiments, field and remote sensing observations and validations, and finally implementations in ocean, Tropical Cyclone, ocean and ice models.\n As a specific example of a wave-coupled environment, the wave climate in the Arctic as observed by altimeters will be presented. This is an important topic for the Arctic Seas, which are opening from ice in summer time. Challenges, however, are many as their Metocean environment is more complicated and, in addition to winds and waves, requires knowledge and understanding of ice material properties and its trends. On one hand, no traditional statistical approach is possible since in the past for most of the Arctic Ocean there was limited wave activity. Extrapolations of the current trends into the future are not feasible, because ice cover and wind patterns in the Arctic are changing. On the other hand, information on the mean and extreme wave properties is of great importance for oceanographic, meteorological, climate, naval and maritime applications in the Arctic Seas.","PeriodicalId":297013,"journal":{"name":"Volume 2A: Structures, Safety, and Reliability","volume":"10 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2020-08-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Volume 2A: Structures, Safety, and Reliability","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1115/omae2020-18373","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

Until recently, large-scale models did not explicitly take account of ocean surface waves which are a process of much smaller scales. However, it is rapidly becoming clear that many large-scale geophysical processes are essentially coupled with the surface waves, and those include ocean circulation, weather, Tropical Cyclones and polar sea ice in both Hemispheres, climate and other phenomena in the atmosphere, at air/sea, sea/ice and sea/land interface, and many issues of the upper-ocean mixing below the surface. Besides, the wind-wave climate itself experiences large-scale trends and fluctuations, and can serve as an indicator for changes in the weather climate. In the presentation, we will discuss wave influences at scales from turbulence to climate, on the atmospheric and oceanic sides. At the atmospheric side of the interface, the air-sea coupling is usually described by means of the drag coefficient Cd, which is parameterised in terms of the wind speed, but the scatter of experimental data with respect to such dependences is very significant and has not improved noticeably over some 40 years. It is argued that the scatter is due to multiple mechanisms which contribute into the sea drag, many of them are due to surface waves and cannot be accounted for unless the waves are explicitly known. The Cd concept invokes the assumption of constant-flux layer, which is also employed for vertical profiling of the wind measured at some elevation near the ocean surface. The surface waves, however, modify the balance of turbulent stresses very near the surface, and therefore such extrapolations can introduce significant biases. This is particularly essential for buoy measurements in extreme conditions, when the anemometer mast is within the Wave Boundary Layer (WBL) or even below the wave crests. In this presentation, field data and a WBL model are used to investigate such biases. It is shown that near the surface the turbulent fluxes are less than those obtained by extrapolation using the logarithmic-layer assumption, and the mean wind speeds very near the surface, based on Lake George field observations, are up to 5% larger. The dynamics is then simulated by means of a WBL model coupled with nonlinear waves, which revealed further details of complex behaviours at wind-wave boundary layer. Furthermore, we analyse the structure of WBL for strong winds (U10 > 20 m/s) based on field observations. We used vertical distribution of wind speed and momentum flux measured in Topical Cyclone Olwyn (April 2015) in the North-West shelf of Australia. A well-established layer of constant stress is observed. The values obtained for u⁎ from the logarithmic profile law against u⁎ from turbulence measurements (eddy correlation method) differ significantly as wind speed increases. Among wave-induced influences at the ocean side, the ocean mixing is most important. Until recently, turbulence produced by the orbital motion of surface waves was not accounted for, and this fact limits performance of the models for the upper-ocean circulation and ultimately large-scale air-sea interactions. While the role of breaking waves in producing turbulence is well appreciated, such turbulence is only injected under the interface at the vertical scale of wave height. The wave-orbital turbulence is depth-distributed at the scale of wavelength (∼10 times the wave height) and thus can mix through the ocean thermocline in the spring-summer seasons. Such mixing then produces feedback to the large-scale processes, from weather to climate. In order to account for the wave-turbulence effects, large-scale air-sea interaction models need to be coupled with wave models. Theory and practical applications for the wave-induced turbulence will be reviewed in the presentation. These include viscous and instability theories of wave turbulence, direct numerical simulations and laboratory experiments, field and remote sensing observations and validations, and finally implementations in ocean, Tropical Cyclone, ocean and ice models. As a specific example of a wave-coupled environment, the wave climate in the Arctic as observed by altimeters will be presented. This is an important topic for the Arctic Seas, which are opening from ice in summer time. Challenges, however, are many as their Metocean environment is more complicated and, in addition to winds and waves, requires knowledge and understanding of ice material properties and its trends. On one hand, no traditional statistical approach is possible since in the past for most of the Arctic Ocean there was limited wave activity. Extrapolations of the current trends into the future are not feasible, because ice cover and wind patterns in the Arctic are changing. On the other hand, information on the mean and extreme wave properties is of great importance for oceanographic, meteorological, climate, naval and maritime applications in the Arctic Seas.
波浪引起的湍流,连接海洋和大尺度
直到最近,大尺度模式还没有明确地考虑到海洋表面波,这是一个小得多的尺度过程。然而,人们很快就清楚地认识到,许多大规模的地球物理过程本质上是与表面波相结合的,这些过程包括海洋环流、天气、热带气旋和两个半球的极地海冰、大气、气/海、海/冰和海/陆界面的气候和其他现象,以及表面以下的上层海洋混合的许多问题。此外,风浪气候本身具有较大的趋势和波动,可以作为天气气候变化的指标。在报告中,我们将讨论波浪在尺度上的影响,从湍流到气候,在大气和海洋方面。在界面的大气侧,海气耦合通常用阻力系数Cd来描述,该系数以风速为参数化,但是关于这种依赖性的实验数据的分散是非常显著的,并且在大约40年中没有明显改善。有人认为,散射是由多种机制造成的,这些机制导致了海洋阻力,其中许多是由表面波引起的,除非对表面波有明确的了解,否则无法解释。Cd概念引用了恒定通量层的假设,这也被用于在海洋表面附近的某个高度测量的风的垂直剖面。然而,表面波改变了非常接近表面的湍流应力的平衡,因此这种外推可能会引入明显的偏差。这对于极端条件下的浮标测量尤其重要,当风速计桅杆位于波浪边界层(WBL)内甚至低于波峰时。在本报告中,使用现场数据和WBL模型来研究这种偏差。结果表明,地表附近的湍流通量比采用对数层假设外推得到的湍流通量要小,而根据乔治湖野外观测得到的非常接近地表的平均风速要大5%。在此基础上,利用WBL模型与非线性波浪耦合进行了动力学模拟,进一步揭示了风浪边界层复杂行为的细节。此外,在野外观测的基础上,分析了强风(U10 > 20 m/s)的WBL结构。我们使用了澳大利亚西北大陆架局部气旋Olwyn(2015年4月)测量的风速和动量通量的垂直分布。观察到一个成熟的恒应力层。从湍流测量(涡相关法)的对数剖面律得到的u值随着风速的增加而显著不同。在海洋侧的波浪影响中,海洋混合是最重要的。直到最近,由表面波的轨道运动产生的湍流还没有被考虑在内,这一事实限制了上层海洋环流和最终大规模海气相互作用模型的性能。虽然破碎波在产生湍流中的作用已得到充分认识,但这种湍流仅在波高的垂直尺度上注入界面下。波轨湍流在波长尺度(~ 10倍波高)上深度分布,因此可以在春夏季节通过海洋温跃层混合。这样的混合会对从天气到气候的大规模过程产生反馈。为了解释波浪湍流效应,需要将大尺度的海气相互作用模型与波浪模型相结合。本报告将回顾波致湍流的理论与实际应用。这些包括波浪湍流的粘性和不稳定性理论、直接数值模拟和实验室实验、现场和遥感观测和验证,以及最终在海洋、热带气旋、海洋和冰模型中的实现。作为波耦合环境的一个具体例子,将介绍高度计观测到的北极的波气候。这对北冰洋来说是一个重要的话题,因为北冰洋在夏季结冰。然而,挑战也很多,因为他们的海洋环境更加复杂,除了风和海浪,还需要了解和理解冰的材料特性及其趋势。一方面,传统的统计方法是不可能的,因为过去北冰洋的大部分地区波浪活动有限。将目前的趋势外推到未来是不可行的,因为北极的冰盖和风的模式正在发生变化。另一方面,关于平均波和极端波特性的信息对于北冰洋的海洋学、气象、气候、海军和海事应用具有重要意义。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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