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1.
海洋内波具有振幅大、流速强和周期短等特点,可对海上施工和水下作业安全造成严重威胁。南海北部陆坡海域是内孤立波和中尺度涡频发的海域之一,研究中尺度涡对内孤立波传播的影响对深入了解南海北部内孤立波在反气旋涡过境时的传播特征、提高该海域内波预报准确性具有重要意义。基于此,本文利用布放于南海北部东沙群岛西侧陆坡海域的潜标观测数据,针对2017年3月一个反气旋中尺度涡经过潜标站位的过程,探讨了中尺度涡对内孤立波传播的影响。结果表明：①受反气旋涡影响,内孤立波的平均振幅减小28.6%,其主要原因是中尺度涡导致等温线下压,进而对内孤立波的振幅产生抑制作用,其影响过程可用趋浅温跃层理论描述。②反气旋涡影响期间,内孤立波的平均波速由1.26 m/s增大到1.47 m/s,增幅约16.7%,反映了反气旋涡对内孤立波波速的强化作用,这种强化作用主要是由中尺度涡边缘流场引起背景流场变化所致,而中尺度涡引起的温盐场变化对内孤立波波速的影响相对较小。 相似文献
2.
基于卫星高度计观测的全球中尺度涡的分布和传播特征 总被引：7，自引：0，他引：7
利用将近12 a的融合高度计资料获得了全球海洋中尺度涡的空间分布和传播特征。结果表明,中尺度涡在副热带海域呈明显的带状分布,反气旋涡和气旋涡的数目相当,但在某些海域它们的数目有很大不同;在40°S-60°N间,大多数涡的运动方向向西,然而在40°-60°S间约有70%的涡向东传播;对于西向传播的涡而言,纬向平均速度随纬度有明显的变化,在赤道附近的西向传播速度为13 cm/s,而在高纬度递减到不足1 cm/s,中尺度涡的传播表现出类似于Rossby波的传播特征。 相似文献
3.
基于1993-2017年卫星高度计数据得到的中尺度涡追踪产品，分析了1000 m以深南海海盆中尺度涡移动速度C的时空分布特征。结果表明，南海海盆气候态平均的中尺度涡纬向移动速度cx均为西向，经向移动速度cy在海盆西北侧为南向，东南侧为北向。cy随经度的变化与背景经向流的变化一致，相关系数达0.96，而cx的变化与背景纬向流和β效应有关。cx和C存在明显季节变化，夏季最慢，冬季最快。年际变化上，cx和cy的大值多发生在太平洋年代际涛动（PDO）负位相期的La Nina年。中尺度涡在其生命周期的开始和结束阶段（即生成和耗散阶段）移速较快，而在稳定的“中期”阶段移动缓慢。该趋势与涡旋转速呈反相关，相关系数为-0.93。以移速小于1.5 cm/s和大于15.4 cm/s定义的极慢和极快涡旋，分别占总涡旋数量的1.5%和1.9%。移速极慢的涡多出现在海盆的中部，且主要发生在夏季；移速极快的涡多出现在海盆的边缘，且主要发生在冬季。机制分析显示，南海海盆中尺度涡移动速度的时空分布受到大尺度背景流场调制。 相似文献
4.
海洋中尺度涡作为物质循环、能量串级和信息传递的关键尺度和重要环节，具有丰富的热动力学内涵。文章基于中国近海及毗邻海域的涡动能分区，重点综述中尺度涡的运动属性、动力学本质和局地特征，从尺度局限与尺度关联的角度阐示中尺度涡旋的扰动生成、传播、能量级联和耗散，及其在海洋多尺度动力过程、热盐配置、生源要素调控和中尺度海气相互作用中的影响，并就相关科学问题和进展提出研究建议。研究结果表明：研究中尺度涡的演变规律对理解海洋物质能量传递的多维度层次、尺度规模和过程形式具有重要意义，需整体加深海洋中尺度涡自适应观测和可预报性研究，增强海洋中尺度涡的尺度演绎分析和特异性分析，建立从天气尺度到气候环境变化、生物生态影响以及致害致灾风险的能量信息通道，构建中观海洋生态系统动力学理论与模型，探索海洋中尺度涡精细化灾害风险预评估区划和安全保障新途径。 相似文献
5.
6.
海洋内孤立波和中尺度涡是南海北部常见的中尺度动力过程。本文利用2010?2015年的Terra/Aqua-MODIS、ENVISAT ASAR和多源卫星高度计资料开展了南海海洋内孤立波和中尺度涡遥感探测研究,分析了中尺度涡对内孤立波传播方向的影响。结果表明,中尺度涡和内孤立波主要在南海东北部海域共存,当二者共存时,气旋（冷涡）促使内孤立波偏离原来的传播方向,向西偏南方向传播;反气旋（暖涡）促使内孤立波向西偏北方向传播,气旋与反气旋改变的内孤立波传播方向刚好相反。内孤立波和中尺度涡共存时间主要集中在3?9月,其中,3月受气旋和反气旋的共同作用,内孤立波传播方向几乎无变化;4月和5月,主要受气旋影响,内孤立波偏离原来传播方向向南传播;6?9月,主要受反气旋影响,内孤立波偏离原来的传播方向向北传播。本文利用遥感手段探索了海洋中尺度涡对内孤立波传播方向的影响,结果与现场观测结果一致。 相似文献
7.
采用AVISO提供的中尺度涡最新数据集,分析了孟加拉湾1993—2016年中尺度涡的总体特征和季节变化。结果表明:研究期间在孟加拉湾共有822个气旋涡,731个反气旋涡,主要分布在湾北部(15°N以北海域)和安达曼海。涡旋生命周期以28～59 d为主,平均振幅为7. 5 cm,平均半径为119. 6 km。在纬度变化上,涡旋振幅随纬度的增加有两个峰值,分别位于6°～9°N和15°～20°N之间,而涡旋半径随纬度增加而减少。涡旋的振幅、半径在随生命周期演变过程中生长过程较慢,消散过程较快。气旋涡和反气旋涡主要是向西移动,且均以向赤道方向偏移为主。在季节变化上,孟加拉湾较长生命周期(60 d以上)的中尺度涡具有明显的季节变化,春季生成的涡旋数量最多,冬季次之,夏季最少。通过合成分析得出风应力旋度是孟加拉湾中尺度涡季节变化的主要原因,而沿岸Kelvin波激发的西传Rossby波对涡旋的产生也有一定影响。涡动能分析表明,涡动能的高值区主要位于海盆的西边界和斯里兰卡东部海域,同时,在冬季、春季海盆的西边界和夏季、秋季海盆的北部涡旋活动较多的区域对应着较大的涡动能。 相似文献
8.
基于自动探测方法的南海北部涡致海表温度锋面的特征研究 总被引：1，自引：0，他引：1
南海北部具有丰富的温度锋面和中尺度涡，它们调节着局地的热量和能量平衡。本文利用卫星海洋高度异常和海表温度数据，并基于自动探测方法，探究了2007年至2017年南海北部中尺度涡边缘的海表温度锋面（涡致锋面）特征。反气旋/气旋边缘出现锋面的概率可达20%。气旋涡在各个方向上出现锋面的概率比较均匀，反气旋涡的东北部和西南部出现锋面的概率大于西北部和东南部。中尺度涡致锋面的数量有明显的季节变化，而涡动能未表现出明显的季节变化。中尺度涡致锋区的总涡动能是中尺度涡内动能的3倍，并且反气旋涡致锋面的总涡动能明显强于气旋涡致锋面的总涡动能。中尺度涡致锋面的数量和涡动能的年际变化与厄尔尼诺南方涛动指数没有明显的相关性。本研究也讨论了中尺度涡致锋面的可能机制，但是中尺度涡对海表温度锋的贡献需要进一步定量研究。 相似文献
9.
根据Kjeldsen对畸形波的定义：波高大于有效波高的2倍（H/H1/3＞2），基于实测波浪资料，统计分析了江苏射阳海域和广东南澳海域的畸形波个数和波浪要素。江苏射阳海域畸形波发生概率为0.005 7%，广东南澳海域畸形波发生概率为0.007%。用Rayleigh分布、双参数Weibull 分布和MER分布对实测数据得到的特征波高进行了拟合，研究了海域内畸形波发生的概率分布。拟合结果表明：MER分布更适合描述两个海域畸形波的发生概率，两个海域畸形波的发生概率均高于Rayleigh分布和Weibull分布。在测量数据期间，台风在海域过境可能增加畸形波的发生概率；同时两个海域的双峰谱占比为22.7%和5.8%，可能也是导致畸形波发生概率增加的原因之一。 相似文献
10.
南海深层环流作为印太海域热盐环流的重要组成部分,研究其时间变异特征对于深入认识印太海域大洋环流具有重要意义。中尺度涡作为南海极为活跃的动力过程,有观测显示其影响深度可超过2000m。结合海表面高度计资料与潜标观测资料,识别南海区域中尺度涡,并分析了中尺度涡对深层流场以及温度场的影响。针对三个中尺度涡的潜标实测结果表明:在涡旋经过时,海洋深层流动有明显的变异,表现在速度、温度方面,速度增加量能达到5.5cm/s,温度变异可达到0.02℃。涡旋经过时,海洋上层、深层流向呈相反态势,第一斜压模动能显著增强。 相似文献
11.
Alternating zonal flows in an idealized wind-driven double-gyre ocean circulation have been investigated using a two-layer
shallow-water eddy-permitting numerical model. While the alternating zonal flows are found almost everywhere in the time-mean
zonal velocity field, their meridional scales differ from region to region. In the subpolar western boundary region, where
the energetic eddy activity induces quasi two-dimensional turbulence, the alternating zonal flows are generated by the inverse
energy cascade and its arrest by Rossby waves, and the meridional scale of the flows corresponds well to the Rhines scale.
In the eastern part of the basin, where barotropic basin modes are dominant, the zonal structure is formed through the nonlinear
effect of the basin modes and is wider than the Rhines scale. Both effects are likely to form zonal structure between the
two regions. These results show that Rossby basin modes become an important factor in the formation of alternating zonal flows
in a closed basin in addition to the arrest of the inverse energy cascade by Rossby waves. The wind-driven general circulation
associated with eddy activities plays an essential role in determining which mechanism of the alternating zonal flows is possible
in each region. 相似文献
12.
基于卫星高度计和浮标漂流轨迹的海洋涡旋特征信息对比分析 总被引：1，自引：0，他引：1
本文基于Chelton提供的涡旋数据集和浮标漂流轨迹提取的涡旋结果,对1993—2015年的全球涡旋进行特征信息对比分析。结果表明,在全球范围内高度计涡旋数据集中的欧拉涡旋和浮标漂流轨迹提取的拉格朗日涡旋的配对成功率在空间分布上并不均衡,在中纬度(20°—60°S,20°—60°N)配对成功率最高可达25%,而在20°S—20°N区域内配对成功率不到10%。由于低纬度地转效应并不显著,卫星高度计无法有效观测到涡旋,但通过浮标漂流轨迹识别出的拉格朗日涡旋却大量存在,这说明在低纬度区域内,采用漂流浮标手段对涡旋进行观测,能够有效地弥补卫星高度计识别涡旋的区域限制。进一步分析表明,总体而言,提取的欧拉涡旋半径要大于拉格朗日涡旋闭合回路半径。两种识别方法获得的涡旋(闭合回路)在20°—50°S, 20°—50°N的副热带和中纬度海区半径大致相当; 20°S—20°N度以内(特别是近赤道区域)、高纬度区域以及西边界流区域,欧拉涡旋半径是同期拉格朗日涡旋闭合回路半径的3倍或更多。此外,对配对涡旋的Rossby数分析结果显示,拉格朗日涡旋较小的闭合回路对应较大的平均相对涡度,这表明浮标在被中尺度涡俘获后,更容易在相对涡度较大的地方(如中尺度涡中心、中尺度涡边缘等)形成闭合回路。 相似文献
13.
This study produced a statistical analysis of multicore eddy structures based on 23 years' altimetry data in global oceans. Multicore structures were identified using a threshold-free closed-contour algorithm of sea surface height, which was improved for this study in respect of certain technical details. Meanwhile a more accurate definition of eddy boundary was used to estimate eddy scale. Generally, multicore structures, which have two or more closed eddies of the same polarity within their boundaries, represent an important transitional stage in their lives during which the component eddies might experience splitting or merging. In comparison with global eddies, the lifetimes and propagation distances of multicore eddies were found to be much smaller because of their inherent structural instability. However, at the same latitude, the spatial scale of multicore eddies was found larger than that of single-core eddies, i.e., the eddy area could be at least twice as large. Multicore eddies were found to exhibit some features similar to global eddies. For example, multicore eddies tend to occur in the Antarctic Circumpolar Current, some western boundary currents, and mid-latitude regions around 25°N/S, the majority(70%) of eddies propagate westward while only 30% propagate eastward, and large-amplitude eddies are restricted mainly to reasonably confined regions of highly unstable currents. 相似文献
14.
Chunjian Sun Xidong Wang Anmin Zhang Lianxin Zhang Caixia Shao Guosong Wang 《海洋学报(英文版)》2022,41(5):27-40
The statistical characteristics and mechanisms of mesoscale eddies in the North Indian Ocean are investigated by adopting multi-sensor satellite data from 1993 to 2019. In the Arabian Sea(AS), seasonal variation of eddy characteristics is remarkable, while the intraseasonal variability caused by planetary waves is crucial in the Bay of Bengal(BOB). Seasonal variation of the eddy kinetic energy(EKE) is distinct along the west boundary of AS,especially in the Somali Current region. In the BOB, lar... 相似文献
15.
次中尺度过程的水平空间尺度约为0.1~10km, 时间尺度约为1天, 里查森数和罗斯贝数为0(1), 能有效地从中尺度环流中汲取能量向小尺度湍流串级, 并对上层海洋物质的垂向交换有着重要影响。本文基于水平分辨率为~500m的高分辨率ROMS(regional ocean modeling system)数值模拟结果, 采用方差椭圆方法, 评估了黑潮延伸体海域上层海洋次中尺度涡旋的各向异性特征, 并探讨了涡旋各向异性值的大小与次中尺度过程特征参数的相关性。研究结果表明, 黑潮延伸体主轴强流区域的次中尺度涡旋各向异性值明显小于两侧海域, 主轴区域的次中尺度涡旋特征明显强于流轴两侧海域, 各向异性值与次中尺度过程的强弱有着较为显著的负相关关系, 表明次中尺度过程具有较小的各向异性特征(更趋各向同性)。方差椭圆表征了涡与平均流相互作用过程中的能量反馈机制, 较大的各向同性特征意味着动能更趋正向串级。 相似文献
16.
Global observations of nonlinear mesoscale eddies 总被引：51，自引：0，他引：51
Sixteen years of sea-surface height (SSH) fields constructed by merging the measurements from two simultaneously operating altimeters are analyzed to investigate mesoscale variability in the global ocean. The prevalence of coherent mesoscale features (referred to here as “eddies”) with radius scales of O(100 km) is readily apparent in these high-resolution SSH fields. An automated procedure for identifying and tracking mesoscale features based on their SSH signatures yields 35,891 eddies with lifetimes ?16 weeks. These long-lived eddies, comprising approximately 1.15 million individual eddy observations, have an average lifetime of 32 weeks and an average propagation distance of 550 km. Their mean amplitude and a speed-based radius scale as defined by the automated procedure are 8 cm and 90 km, respectively.The tracked eddies are found to originate nearly everywhere in the World Ocean, consistent with previous conclusions that virtually all of the World Ocean is baroclinically unstable. Overall, there is a slight preference for cyclonic eddies. However, there is a preference for the eddies with long lifetimes and large propagation distances to be anticyclonic. In the southern hemisphere, the distributions of the amplitudes and rotational speeds of eddies are more skewed toward large values for cyclonic eddies than for anticyclonic eddies. As a result, eddies with amplitudes >10 cm and rotational speeds >20 cm s−1 are preferentially cyclonic in the southern hemisphere. By contrast, there is a slight preference for anticyclonic eddies for nearly all amplitudes and rotational speeds in the northern hemisphere.On average, there is no evidence of anisotropy of these eddies. Their average shape is well represented as Gaussian within the central 2/3 of the eddy, but the implied radius of maximum rotational speed is 64% smaller than the observed radius of maximum speed. In part because of this mismatch between the radii of maximum axial speed in the observations and the Gaussian approximation, a case is made that a quadratic function that is a very close approximation of the mode profile of the eddy (i.e., the most frequently occurring value at each radius) is a better representation of the composite shape of the eddies. This would imply that the relative vorticity is nearly constant within the interiors of most eddies, i.e., the fluid motion consists approximately of solid-body rotation.Perhaps the most significant conclusion of this study is that essentially all of the observed mesoscale features outside of the tropical band 20°S-20°N are nonlinear by the metric U/c, where U is the maximum circum-average geostrophic speed within the eddy interior and c is the translation speed of the eddy. A value of U/c > 1 implies that there is trapped fluid within the eddy interior. Many of the extratropical eddies are highly nonlinear, with 48% having U/c > 5 and 21% having U/c > 10. Even in the tropics, approximately 90% of the observed mesoscale features are nonlinear by this measure.Two other nondimensional parameters also indicate strong degrees of nonlinearity in the tracked eddies. The distributions of all three measures of nonlinearity are more skewed toward large values for cyclonic eddies than for anticyclonic eddies in the southern hemisphere extratropics but the opposite is found in the northern hemisphere extratropics. There is thus a preference for highly nonlinear extratropical eddies to be cyclonic in the southern hemisphere but anticyclonic in the northern hemisphere.Further evidence in support of the interpretation of the observed features as nonlinear eddies is the fact that they propagate nearly due west with small opposing meridional deflections of cyclones and anticyclones (poleward and equatorward, respectively) and with propagation speeds that are nearly equal to the long baroclinic Rossby wave phase speed. These characteristics are consistent with theoretical expectations for large, nonlinear eddies. While there is no apparent dependence of propagation speed on eddy polarity, the eddy speeds relative to the local long Rossby wave phase speeds are found to be about 20% faster in the southern hemisphere than in the northern hemisphere. The distributions of the propagation directions of cyclones and anticyclones are essentially the same, except mirrored about a central azimuth angle of about 1.5° equatorward. This small, but we believe statistically significant, equatorward rotation of the central azimuth may be evidence of the effects of ambient currents (meridional advection or the effects of vertical shear on the potential vorticity gradient vector) on the propagation directions of the eddies.While the results presented here are persuasive evidence that most of the observed westward-propagating SSH variability consists of isolated nonlinear mesoscale eddies, it is shown that the eddy propagation speeds are about 25% slower than the westward propagation speeds of features in the SSH field that have scales larger than those of the tracked eddies. This scale dependence of the propagation speed may be evidence for the existence of dispersion and the presence of features that obey linear Rossby wave dynamics and have larger scales and faster propagation speeds than the nonlinear eddies. The amplitudes of these larger-scale signals are evidently smaller than those of the mesoscale eddy field since they are not easily isolated from the energetic nonlinear eddies. 相似文献
17.
孟加拉湾内和湾口附近有丰富的中尺度现象,本文利用2.0版可分辨低纬地区中尺度涡的Chelton数据集,通过溯源的方法得到中尺度涡的源地分布。苏门答腊岛西北海域(以5°N,94°E为核心的区域)是中尺度涡重要源区之一。通过拉格朗日方法的涡旋追踪表明,1993—2017年该海域(3°N—6°N、92°E—95°E),分别有57个气旋式和40个反气旋式中尺度涡。频谱分析显示海表面高度异常存在180 d和360 d两个显著周期。地形和风场的共同作用是该海域产生中尺度涡的动力机制：沿5°N西传的罗斯贝波在海岭地形的作用下触发了中尺度涡的生成;赤道风场是源区重要的能量来源,局地风场能诱发中尺度涡的极性。本研究也揭示了以往文献虽刻画了苏门答腊岛西北部海域为高涡动能区,却没有识别出较多中尺度涡的原因。 相似文献
18.
Mesoscale eddies play vital roles in ocean processes. Although previous studies focused on eddy surface features and individual three-dimensional (3D) eddy cases in the northwestern Pacific Ocean, the analysis of unique eddy 3D regional characteristics is still lacking. A 3D eddy detection scheme is applied to 9 years (2000–2008) of eddy-resolving Regional Ocean Modeling System (ROMS) output to obtain a 3D eddy dataset from the surface to a depth of 1 000 m in the northwestern Pacific Ocean (15°–35°N, 120°–145°E). The 3D characteristics of mesoscale eddies are analyzed in two regions, namely, Box1 (Subtropical Countercurrent, 15°–25°N, 120°–145°E) and Box2 (Southern Kuroshio Extension, 25°–35°N, 120°–145°E). In Box1, the current is characterized by strong vertical shear and weak horizontal shear. In Box2, the current is characterized by the strong Kuroshio, topographic effect, and the westward propagation of Rossby waves. The results indicate the importance of baroclinic instability in Box1, whereas in Box2, both the barotropic and baroclinic instability are important. Moreover, the mesoscale eddies’ properties in Box1 and Box2 are distinct. The eddies in Box1 have larger number and radius but a shorter lifetime. By contrast, Box2 has fewer eddies, which have smaller radius but longer lifetime. Vertically, more eddies are detected at the subsurface than at the surface in both regions; the depth of 650 m is the turning point in Box1. Above this depth, the number of cyclonic eddies (CEs) is larger than that of anticyclonic eddies (AEs). In Box2, the number of CEs is dominant vertically. Eddy kinetic energy (EKE) and mean normalized relative vorticity in Box2 are significantly higher than those in Box1. With increasing depth, the attenuation trend of EKE and relative vorticity of Box1 become greater than those of Box2. Furthermore, the upper ocean (about 300 m in depth) contains 68.6% of the eddies (instantaneous eddy). Only 16.6% of the eddies extend to 1 000 m. In addition, about 87% of the eddies are bowl-shaped eddies in the two regions. Only about 3% are cone-shaped eddies. With increasing depth of the eddies, the proportion of bowl-shaped eddies gradually decreases. Conversely, the cone- and lens-shaped eddies are equal in number at 700–1 000 m, accounting for about 30% each. Studying the 3D characteristics of eddies in two different regions of the northwestern Pacific Ocean is an important stepping stone for discussing the different eddy generation mechanisms. 相似文献
19.
吕宋海峡黑潮脱落涡旋的特征分析 总被引：2，自引：0，他引：2
涡旋脱落在西太平洋和南海的海水属性交换中起到重要作用。为研究吕宋海峡附近海域由黑潮脱落并进入南海的涡旋特征,本文采用1993—2014年法国空间局(AVISO)多卫星融合海面高度距平(SLA)和绝对动力地形(ADT)全球网格化延时数据,美国国家海洋数据中心(NODC)的WOA13年平均温盐剖面气候数据,以及1993—2010年SODA2.2.4月平均海洋同化数据集,并分析了黑潮脱落涡旋与大尺度环流的关系。结果表明:(1)暖涡脱落数量远多于冷涡数量,且脱落的冷涡绝大部分在黑潮西侧边缘生成,而脱落的暖涡则大部分在黑潮控制区生成。(2)冷涡、暖涡脱落时的平均半径、平均振幅相近,但是冷涡的平均生命、平均迁移距离约为暖涡的一半。(3)冷涡不是每年都有脱落,主要在冬季脱落;暖涡则每年均有脱落,主要发生在秋季。(4)脱落涡旋数量与脱落时的黑潮路径类型相关。(5)脱落涡旋的平均西行速度为5.8cm/s,与斜压第一模态长Rossby波波速及大尺度环流的西向平流流速之和相近。 相似文献
20.
上混合中剪切湍流和朗缪尔环流动力特征差异 总被引：1，自引：0，他引：1
LI Guojing WANG Dongxiao CHEN Ju YAO Jinglong ZENG Lili SHU Yeqiang SUI Dandan 《海洋学报(英文版)》2015,34(5):1-11
Large eddy simulation(LES) is used to investigate contrasting dynamic characteristics of shear turbulence(ST)and Langmuir circulation(LC) in the surface mixed layer(SML). ST is usually induced by wind forcing in SML. LC can be driven by wave-current interaction that includes the roles of wind, wave and vortex forcing. The LES results show that LC suppresses the horizontal velocity and greatly modifies the downwind velocity profile, but increases the vertical velocity. The strong downwelling jets of LC accelerate and increase the downward transport of energy as compared to ST. The vertical eddy viscosity Km of LC is much larger than that of ST. Strong mixing induced by LC has two locations. They are located in the 2ds–3ds(Stokes depth scale) and the lower layer of the SML,respectively. Its value and position change periodically with time. In contrast, maximum Km induced by ST is located in the middle depth of the SML. The turbulent kinetic energy(TKE) generated by LC is larger than that by ST. The differences in vertical distributions of TKE and Km are evident. Therefore, the parameterization of LC cannot be solely based on TKE. For deep SML, the convection of large-scale eddies in LC plays a main role in downward transport of energy and LC can induce stronger velocity shear(S2) near the SML base. In addition, the large-scale eddies and S2 induced by LC is changing all the time, which needs to be fully considered in the parameterization of LC. 相似文献