共查询到19条相似文献，搜索用时 125 毫秒
1.
以描述中尺度涡旋对示踪物的输送作用为目的的湍流混合方案GM90经证明对海洋模式的模拟能力较以前的湍流混合方案有较大的提高.该方案涉及到两个主要参数:等密度面扩散系数(AI)和等密度面厚度扩散系数(Aith).该文的目的就是利用中国科学院大气物理研究所(IAP)全球海洋环流模式L30T63研究以上两个系数取值大小对主动示踪物(温盐)以及被动示踪物(CFC-11)海洋分布的影响.实验结果表明这两个系数的取值可明显改变大洋温盐垂直分布以及海洋对CFC-11的吸收,且两个系数在其中起到的作用有很大的差异.从几个剖面的分析结果可知,总的来说,AI的增加使得CFC-11主要储存区的模拟结果更接近观测资料,而Aith的增大使得模拟结果变差. 相似文献
2.
风生近惯性内波破碎引起的跨等密度面混合在海洋内部混合中起重要作用。然而其参数化对海洋模式的模拟影响仍有待进一步认识。本文给出的是在模块化海洋模式（MOM）中海洋表面边界层以下引入一个考虑风驱动近惯性内波破碎引起的跨等密度面混合参数化方案的研究工作。模拟结果显示，该方案有效改善MOM4模拟的上层1 000 m以上的温盐偏差，特别是在北太平洋和北大西洋的通风地区。数值试验表明，风生近惯性内波破碎有可能是维持海洋通风过程的重要机制之一，它使得海洋通风区的位温变冷，盐度变淡，整层等位密面加深。维持的通风过程使得北太平洋副极地大涡的影响延伸到副热带大涡。从而模拟的北太平洋中层水源头及其副热带大涡东侧的温盐更接近观测实际。同时，模拟的北大西洋经圈翻转环流强度也更为合理。 相似文献
3.
Langmuir环流影响着海洋上层的能量输入,对海洋上混合层的形成和加深起着重要作用,对于海洋上混合层具有重要意义。近年来许多学者采用大涡模拟(LES)方法对Langmuir环流进行机制研究,并通过在雷诺平均模型中参数化Langmuir环流效应,将Langmuir环流过程引入到三维海洋环流或海洋耦合模式中,提出了一系列混合参数化方案。本文回顾了Langmuir环流在雷诺平均模式参数化中的研究进展,主要可分为以下几种方案:一种方法是用Langmuir数在KPP垂直混合参数化方案中引入湍流特征速度增强因子,并不断发展Langmuir数的定义;一种是在Mellor-Yamada2.5湍流闭合模型中增加斯托克斯漂流剪切效应项,此外还有通过修改模式中混合长方程来加入Langmuir效应等。通过在雷诺平均模式中应用的结果来看,现有的参数化方案在一定程度上改善了混合层深度和SST的模拟,肯定了Langmuir环流在加深混合等方面的作用,但仍存在一些问题需要在今后的研究中进一步改进。 相似文献
4.
台风条件下朗缪尔环流对上层海洋混合的影响研究进展 总被引：1，自引：1，他引：0
回顾了近10年来台风条件下朗缪尔环流影响上层海洋混合的研究进展，朗缪尔致湍流对海洋上混合层的形成和加深的重要作用已形成了基本共识，但对于朗缪尔致湍流对海洋上混合层的混合作用机制和程度仍然存在诸多不确定性。观测表明台风条件下台风眼附近的混合层平均湍流动能受到了较强的抑制，可能与台风不同位置朗缪尔致湍流的特征变异有关；台风条件下，现有的朗缪尔致湍流参数化方案在上层混合过程模拟中还有显著误差。在今后研究中，通过改进斯托克斯漂流剖面的计算方法，优化表征台风条件下海面状况的朗缪尔致湍流参数化计算方案，是进一步揭示台风条件下朗缪尔环流对海洋上层混合的影响机理的必要途径。 相似文献
5.
利用1个等密度面坐标大洋环流模式,研究了热带太平洋地区局地混合率变化对局地海表面温度的影响.研究表明,局地混合率的变化对热带中-东部地区以及海盆东边界处的海表面温度影响较强,而对海盆西部的海表面温度影响较弱,这些影响主要与局地温跃层的深度有关,此外海洋表层与温跃层的温度差等也会对局地海表面温度产生影响. 相似文献
6.
近惯性内波广泛存在于全球海洋,是维持深层海洋跨等密度面湍流混合及海洋层结的重要能量来源。基于黑潮-亲潮混合区的多年深海潜标数据,分析了:(1)该海域近惯性内波及其能量的季节变化特征与影响因素,(2)上层和深层近惯性运动的频率、波数谱及垂向分布等特征。结果表明,该海域存在丰富的近惯性动能,无论海洋上层还是深层均呈现显著的冬季强、夏季弱的季节变化特征,冬季(12～2月)上层的近惯性能量可占全年能量的41%,深层近惯性信号同样显著,同潮汐信号相当。平板模型分析表明,该区域近惯性动能的季节循环特征主要受风场的季节变化所主导,同时受到黑潮延伸体流轴的摆动调制。 相似文献
7.
完善莱州湾三维环流结构,对进一步认识莱州湾海域的物质输运和生态环境保护具有重要科学意义,但前人对于莱州湾环流三维结构的研究相对较少。本文基于一套高分辨率的海洋数值模式,从三维角度研究了莱州湾夏季8月份环流的气候态特征及其影响机制。数值研究表明,莱州湾夏季环流垂向结构呈现双层环流特征,其中在跨等深线方向,环流的双层结构环流特征比较显著且存在显著的密度锋面结构。动量诊断的结果进一步表明,这种双层结构环流的形成与底层密度锋面所导致的斜压梯度力密切相关。此外,通过量化温盐场对于密度锋面的贡献,本文证实了温度梯度是莱州湾顶的密度锋面的主要影响因素,其对斜压梯度力的贡献占比达到99%,而盐度梯度对于莱州湾中部区域的密度锋面十分重要,对斜压梯度力的贡献占比达到58%,这与夏季黄河所带来的淡水通量密切相关。 相似文献
8.
基于全球多年来积累的大量温盐观测剖面计划资料,利用精细尺度参数化方案估算了太平洋上层600米区域内的跨等密度面混合系数。结果表明,在不同季节跨等密度面混合系数的整体分布类似,但是细节上存在很大的不同。跨等密度面混合系数的加强与底部摩擦、海表面近惯性能量输入、赤道效应等因素密切相关。由于粗糙的地形,混合在东北太平洋门多西诺断裂带附近存在明显加强。同时,在南大洋西风带区域,由于大风引起的近惯性能量输入也导致了混合的强化。 与前人的研究结果相比,本文的估算具有更好的空间覆盖率以及更高的分辨率,更重要的是我们的结果体现了季节性变化。由于我们给出的是网格化产品,非常适合在数值模式中的应用。 相似文献
9.
低层大气季节变化及与黄海雾季的关系 总被引：5，自引：1，他引：4
根据2005～2006年青岛气象台逐日L波段探空雷达资料和地面观测资料,计算、分析了低层大气湍流混合高度、湍流混合强度和温度层结的季节变化,并分析了其与黄海海雾季节变化的关系.结果表明:温度层结、湍流强度和高度均有明显的季节变化,这些变化与海雾的季节变化密切关联.春、夏季节湍流强度较强,湍流混合高度相对较低,有利于近海面的凝结水汽在低空聚集而形成雾.雾季典型的层结结构是"上稳下湍",即:近地(海)面至150 m左右为条件性不稳定,其上方为大约400 m厚的稳定层.盛雾期稳定层的稳定性减弱,湍流强度加强.另外,黄海雾季由7月最盛到8月突然结束,与东海雾季逐渐结束明显不同.8月黄海终雾期迅速的原因与风向的突然转变有关.偏东风为整个黄海带来较冷的空气,使条件性不稳定发展,雾季终止.风向的突然转变与区域性海陆热性质差异和大尺度背景环流的调整有关. 相似文献
10.
海洋湍流模型研究自二十世纪 70年代中发展至今 ,在海洋动力学研究中 ,特别是关于混合 /层化研究中广泛应用 ,近年来由于认识到湍流对海洋生物过程的重要影响 ,对海洋湍流的客观描述更加关注。文中详细介绍了几个主要海洋动力学模型中的湍流封闭模式 ,如 HAMSOM中的Prandtl混合长模型、Johns模式中的 k-方程模型、POM中的 k- kl模型、水动力学中常用的 k-ε模型等等 ,介绍了海洋湍流模型的应用。对于湍流模型的使用提出针对具体问题选择的原则 ,复杂的并非最优的。 相似文献
11.
The variation of turbulent diapycnal mixing at 18°N in the South China Sea stirred by wind stress 总被引：1，自引：0，他引：1
The spatial and temporal variations of turbulent diapycnal mixing along 18°N in the South China Sea(SCS) are estimated by a fine-scale parameterization method based on strain, which is obtained from CTD measurements in yearly September from 2004 to 2010. The section mean diffusivity can reach ~10~(–4)m~2/s, which is an order of magnitude larger than the value in the open ocean. Both internal tides and wind-generated near-inertial internal waves play an important role in furnishing the diapycnal mixing here. The former dominates the diapycnal mixing in the deep ocean and makes nonnegligible contribution in the upper ocean, leading to enhanced diapycnal mixing throughout the water column over rough topography. In contrast, the influence of the wind-induced nearinertial internal wave is mainly confined to the upper ocean. Over both flat and rough bathymetries, the diapycnal diffusivity has a growth trend from 2005 to 2010 in the upper 700 m, which results from the increase of wind work on the near-inertial motions. 相似文献
12.
The pattern and magnitude of the global ocean overturning circulation is believed to be strongly controlled by the distribution
of diapycnal diffusivity below 1000 m depth. Although wind stress fluctuation is a candidate for the major energy sources
of diapycnal mixing processes, the global distribution of wind-induced diapycnal diffusivity is still uncertain. It has been
believed that internal waves generated by wind stress fluctuations at middle and high latitudes propagate equatorward until
their frequency is twice the local inertial frequency and break down via parametric subharmonic instabilities, causing diapycnal
mixing. In order to check the proposed scenario, we use a vertically two-dimensional primitive equation model to examine the
spatial distribution of “mixing hotspots” caused by wind stress fluctuations. It is shown that most of the wind-induced energy
fed into the ocean interior is dissipated within the top 1000 m depth in the wind-forced area and the energy dissipation rate
at low latitudes is very small. Consequently, the energy supplied to diapycnal mixing processes below 1000 m depth falls short
of the level required to sustain the global ocean overturning circulation. 相似文献
13.
The near-inertial waves (NIWs) are important for energy cascade in the ocean. They are usually significantly reinforced by strong winds, such as typhoon. Due to relatively coarse resolutions in contemporary climate models, NIWs and associated ocean mixing need to be parameterized. In this study, a parameterization for NIWs proposed by Jochum in 2013 (J13 scheme), which has been widely used, is compared with the observations in the South China Sea, and the observations are treated as model outputs. Under normal conditions, the J13 scheme performs well. However, there are noticeable discrepancies between the J13 scheme and observations during typhoon. During Typhoon Kalmaegi in 2014, the inferred value of the boundary layer is deeper in the J13 scheme due to the weak near-inertial velocity shear in the vertical. After typhoon, the spreading of NIWs beneath the upper boundary layer is much faster than the theoretical prediction of inertial gravity waves, and this fast process is not rendered well by the J13 scheme. In addition, below the boundary layer, NIWs and associated diapycnal mixing last longer than the direct impacts of typhoon on the sea surface. Since the energy dissipation and diapycnal mixing below the boundary layer are bounded to the surface winds in the J13 scheme, the prolonged influences of typhoon via NIWs in the ocean interior are missing in this scheme. Based on current examination, modifications to the J13 scheme are proposed, and the modified version can reduce the discrepancies in the temporal and vertical structures of diapycnal mixing. 相似文献
14.
南海是存在强湍流混合的边缘海之一, 但前人对南海湍流混合的研究更多关注的是中上层, 对底层则鲜有关注。本文基于高分辨率温度传感器于2019年5月在南海东北部22个站位海底上方0.5m处持续观测4.4d的温度数据, 分析了2216~3200m深度范围内底层海水温度的时间变化特征, 并探讨了地形粗糙度和内潮对底层湍流混合的影响。分析结果表明, 南海东北部各站位底层海水的温度变化量级约为10-4~10-3℃; 温度变化趋势与正压潮变化趋势不同, 温度能谱显示多数站位在全日和半日频带区间出现谱峰, 温度变化更多地受斜压潮影响, 全日、半日内潮起主要调制作用。陆坡-深海盆过渡区及深海盆底层的湍动能耗散率量级为10-10~10-9m2∙s-3, 涡扩散系数量级为10-4~10-3m2∙s-1。观测数据未能显示底层湍流混合与地形粗糙度存在明显的相关性。底层湍流混合的空间分布与过去观测到的南海北部深海盆内潮的南北不对称性分布一致。 相似文献
15.
Oceanic vertical mixing of the lower halocline water (LHW) in the Chukchi Borderland and Mendeleyev Ridge was studied based on in situ hydrographic and turbulent observations. The depth-averaged turbulent dissipation rate of LHW demonstrates a clear topographic dependence, with a mean value of 1.2×10–9 W/kg in the southwest of Canada Basin, 1.5×10–9 W/kg in the Mendeleyev Abyssal Plain, 2.4×10–9 W/kg on the Mendeleyev Ridge, and 2.7×10–9 W/kg on the Chukchi Cap. Correspondingly, the mean depth-averaged vertical heat flux of the LHW is 0.21 W/m2 in the southwest Canada Basin, 0.30 W/m2 in the Mendeleyev Abyssal Plain, 0.39 W/m2 on the Mendeleyev Ridge, and 0.46 W/m2 on the Chukchi Cap. However, in the presence of Pacific Winter Water, the upward heat released from Atlantic Water through the lower halocline can hardly contribute to the surface ocean. Further, the underlying mechanisms of diapycnal mixing in LHW—double diffusion and shear instability—was investigated. The mixing in LHW where double diffusion were observed is always relatively weaker, with corresponding dissipation rate ranging from 1.01×10–9 W/kg to 1.57×10–9 W/kg. The results also show a strong correlation between the depth-average dissipation rate and strain variance in the LHW, which indicates a close physical linkage between the turbulent mixing and internal wave activities. In addition, both surface wind forcing and semidiurnal tides significantly contribute to the turbulent mixing in the LHW. 相似文献
16.
Estimates of Energy Dissipation Rates in the Three-Dimensional Deep Ocean Internal Wave Field 总被引：2，自引：0，他引：2
Using the “Eikonal Approach” (Henyey et al., 1986), we estimate energy dissipation rates in the three-dimensional Garrett-Munk internal wave field. The total energy dissipation rate within the undisturbed GM internal wave field is found to be 4.34 × 10−9 W kg−1. This corresponds to a diapycnal diffusivity of about 0.3 × 10−4 m2s−1, which is less than the value 10−4 m2s−1 required to sustain the global ocean overturning circulation. Only when the high vertical wavenumber, near-inertial current shear is enhanced can diapycnal diffusivity reach ∼10−4 m2s−1. It follows that the energy supplied at low vertical wavenumbers and low frequencies is efficiently transferred to high vertical wavenumbers and near-inertial frequencies in the mixing hotspots in the real ocean. 相似文献
17.
Estimates of mixing on the South China Sea shelf 总被引：3，自引：3，他引：0
1 Introduction The outer shelf of the South China Sea is a di- verse environment characterized by sharp changes in bottom topography (Wang et al., 2002). Internal wave and diapycnal mixing may be a vital mechanism con- trolling the distribution of physical water properties, nutrient fluxes, and concentrations of particulate mat- ter. Therefore, the research on diapycnal mixing on the outer shelf in the South China Sea is of great impor- tance to explore the level and variability of the abov… 相似文献
18.
Under strong surface wind forcing during winter, direct current observations in the northern Sea of Japan show the existence of strong near-inertial currents in the deep water that is characterized by the extremely homogeneous vertical structures of temperature and salinity. However, the mechanism generating internal waves in the deep water of the northern Sea of Japan has not been well understood. In this study, to clarify the dynamical link between the surface wind forcing and near-inertial currents in the deep water of the northern Sea of Japan, we drive a general circulation model taking into account realistic wind stress, ocean bottom and land topography. In the northern Sea of Japan, the numerical results show that vertically coherent horizontal currents with a speed of ~ 0.05 m s?1 are excited throughout the homogeneous deep water. A two-layer model successfully reproduces the pattern of the horizontal current velocities shown by the general circulation model, indicating that internal waves emanate westward from the northwestern coast of Japan through coastal adjustment to the strong wind forcing event and, while propagating into the ocean interior, they excite evanescent near-inertial response throughout the lower layer below the interface. 相似文献
19.
B. A. Kagan E. V. Sofina A. A. Timofeev 《Izvestiya Atmospheric and Oceanic Physics》2010,46(2):224-231
In order to reproduce the diapycnal mixing induced by internal tidal waves (ITWs) in the Arctic Ocean, we use a modified version
of the three-dimensional finite-element hydrothermodynamic model QUODDY-4. We found that the average (over the tidal cycle)
and integral (by depth) baroclinic tidal energy dissipation rate in individual areas of the Siberian continental shelf and
in the straits between the Canadian Arctic archipelago are much higher than in the open ocean and its values on ridges and
troughs are qualitatively similar to one another. Moreover, in the area of open-ocean ridges, the baroclinic tidal energy
dissipation rate increases as it approaches the bottom, but only in the bottom boundary layer; on the Mid-Atlantic and Hawaii
ridges, such an increase is observed within a few hundreds of meters away from the bottom. The average (in area and depth
of the open ocean) coefficient of diapycnal mixing defined by the baroclinic tidal energy dissipation rate is higher than
the coefficient of molecular kinematic viscosity and only a few times lower than the canonical value of the coefficient of
vertical turbulent viscosity, which is used in models of global oceanic circulation. Coupled with the reasoning on the localization
of baroclinic tidal energy dissipation, this fact leads to the conclusion that disregarding the contribution that ITW-induced
diapycnal mixing makes to the ocean-climate formation is hardly justified. 相似文献