共查询到19条相似文献，搜索用时 328 毫秒
1.
《中国海洋大学学报(自然科学版)》2016,(10)
通过对北太平洋中层水模拟和分析的3种结果的比较:在稀疏网格的LICOM全球大洋环流模式中使用Canuto等的湍流混合方案(简称T方案)并添加范植松等提出的惯性内波破碎混合方案(简称F方案),在LICOM模式中使用T方案,以及WOA09资料的分析结果,证明在添加F方案的情况下,北太平洋中层水的模拟有较明显的改进。惯性内波破碎混合可能是维持通风过程的重要机制之一,惯性频率风场的强迫作用可能是海洋内部混合的外部作用源。在WOA09资料的分析结果与数值模拟结果中均显示出北太平洋中层水的明显的季节变化,这意味着除表层水和模态水之外,北太平洋中层水在气候变化中扮演了重要的角色。模拟结果分析表明,为获得北太平洋中层水模拟的进一步改进,高分辨率的海洋模式和锋面与羽流的参数化方案是必要的。 相似文献
2.
基于2011年4月至2012年3月南海北部陆坡区潜标观测的高分辨率流速数据,本文研究了海洋上层细尺度流速剪切的时间变化特征及其演变规律。流速剪切的功率谱分析结果显示,南海北部上层的细尺度流速剪切主要受亚惯性运动、近惯性内波、全日内潮和半日内潮四种过程控制。其中,风生近惯性内波和中尺度涡旋所对应的亚惯性运动是造成上层流速剪切时间变化的主要原因,以往研究强调的全日和半日內潮的贡献则相对较弱。进一步分析发现,冬季中尺度暖涡能够极大地增强海洋上层的亚惯性剪切;夏、秋季南海活跃的台风所激发的近惯性内波能够造成近惯性剪切增强。另外,研究还发现,背景涡度对近惯性剪切具有重要的调制作用,即负涡度相较于正涡度更有利于近惯性剪切增强。该研究所揭示的流速剪切的时间变化规律及调控机制对改进海洋混合的参数化方案具有重要的参考价值。 相似文献
3.
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
4.
继第部分之后研究了惯性内波和近惯性内波由f～的作用所致的剪切不稳定引起的破碎机制。物理上,该机制很象存在由风应力所致薄表面涡旋漂流层时表面波的破碎与饱和过程。惯性内波和近惯性内波的破碎产物与小尺度湍流一起形成了混合块,它与Gregg等人(1986)的持久混合观测结果一致。依据Thorpe(1973)实验的结果作者提出了一个估计湍流动能耗散率和消衰时间的方法。结果表明,在剪切不稳定中近惯性内波在湍动耗散中起了关键作用,而惯性内波引起非常弱的湍动耗散。使用内波能量谱的标准总能量密度估计出的近惯性内波的耗散率和消衰时间与PATCHEX测量结果非常一致。文中还讨论了几个与此破碎机制有关的问题。 相似文献
5.
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
6.
利用基于谱方法和MPI并行运算的数值模式SpectralModel,直接数值模拟了三维小振幅海洋内波的演变、破碎和所致湍流混合,指出导致其不稳定而破碎的为PSI(parametric subharmonic instability)机制;对于内波破碎所致的湍流混合过程,分析了跨等密度面扩散系数kρ、混合效率γ、浮力通量谱、动能谱以及势能谱等统计性质:内波破碎前,kρ和γ保持低值水平,浮力通量谱值为负,且集中在低波数段;内波破碎后,kρ和γ迅速增大,最大值分别约为0.9×103m2/s和0.18,浮力通量谱值在低波数段为负值,在高波数段为正值,这是因为层化湍流中势能向小尺度运动传递和动能向小尺度运动传递相比更为有效。在内波破碎、强湍流混合阶段,势能谱存在一谱段满足kz3律,P(kz)=0.2N2kz3。此外,与二维模拟结果相比较,导致内波不稳定而破碎的均为PSI机制,kρ、浮力通量谱、势能谱变化趋势大体一致;但三维数值实验中,内波破碎时间提前,湍流衰减加快;KE谱在高波数部分下降速度相对减小,更接近于kz3。 相似文献
7.
北太平洋原子弹14C分布的模拟 总被引：3，自引：1，他引：3
利用一个开边界的北太平洋海盆尺度环流模式模拟了北太平洋原子弹14C的分布和吸收。为了考察开边界与闭边界模式的不同以及开边界模式中不同等密度面扩散系数对模拟结果的影响,相应地做了一个闭边界实验和开边界的两组不同等密度面扩散系数的实验。结果表明,打开南边界改善了赤道以南海区的模拟结果,增大等密度面扩散系数使得模拟的北太平洋中层水强度增大,相应地在165°E等断面模拟的含高浓度原子弹14C的海水向南、向下输送的强度和影响范围都有比较明显的加强,改善了模式的模拟结果,证明大的等密度面扩散系数可以改善模式的模拟结果,能较好地再现在副热带海区原子弹14C水柱总量的梯度由西向东的观测特征。 相似文献
8.
基于细尺度参数化方法,利用2000—2007年的历史水文剖面资料,分析了西北太平洋海区(135°—180°E,25°—45°N)跨等密度面湍流混合的时空分布特征。结果表明,垂直平均的耗散率与地形粗糙度的空间分布基本一致,且随经度自西向东减弱。在地形粗糙的地方,耗散率达O(10–8m2/s3),而在地形平坦的地方,耗散率仅O(10–11m2/s3)。另外,上层海洋混合存在明显的季节变化,在日本近岸的海区,耗散率冬季最强而夏季最弱,与风生近惯性能量之间存在显著的正相关;在大洋内区,耗散率冬季最强而秋季最弱,与风生近惯性能量的相关关系较弱。进一步地,本文分析了风应力在不同海区对混合的影响深度,结果显示在伊豆-小笠原海脊以西,风应力的影响深度最浅为620m,而在该海脊以东最深可达1740m。 相似文献
9.
近惯性波广泛存在于全球海洋,对海洋中的能量级联非常重要。风输入海洋的近惯性能量在海洋中是如何传播和耗散的,能量在海洋中如何划分,一直是受到高度关注的话题。本文简要综述了风生近惯性波在海洋中的传播和耗散过程,包括影响近惯性波传播的因素,比如β效应、中尺度涡度、台风尾流和近惯性波自身的波数特征等;近惯性波在风暴等强天气过程下的传播方式;近惯性波在混合层中衰减时间尺度的模拟;近惯性能量在海洋中的分配以及现有研究中还未解决的问题。本文拟为今后的近惯性波研究提供一些思路,进一步促进近惯性波机制和模拟等方面研究的深入开展。 相似文献
10.
在位于澳大利亚的东海岸29°S附近的“Tasman”海洋锋面延伸区，从WOCE的PR11断面的观测中发现南太平洋副热带模态水的存在。在深度1500～2500Pa，南太平洋副热带模态水的温度范围为16．5℃～19．5℃，且温度梯度〈1．6℃／100m；密度范围为25．4～26．0kg·m^3，且位势涡度的梯度〈2×10^10^-1·s^-1。和北太平洋及北大西洋中的副热带模态水的形成过程一样，南太平洋副热带模态水由于南半球冬天失热引起的强烈的深混合而形成，与此同时，如浮标资料所示，深层的冷水会卷加进入混合层中。冬天南太平洋副热带模态水的形成过程中，局地的海洋涡旋起到了重要的作用。并且影响南太平洋副热带模态水第二年的分布型。在南太平洋模态水形成区，冬天深（浅）的混合层伴随着下降（上升）的温跃层与局地的反气旋（气旋）式得海洋涡旋有直接的关系。在反气旋存在的海域往往可以发现生成的副热带模态水的厚度〉50m且主温跃层的深度也要超过4500Pa。 相似文献
11.
在大洋环流模型中对应于惯性内波破碎的垂直混合的一个参数化方案 总被引：1，自引：0，他引：1
Based on the theoretical spectral model of inertial internal wave breaking(fine structure) proposed previously, in which the effects of the horizontal Coriolis frequency component f-tilde on a potential isopycnal are taken into account, a parameterization scheme of vertical mixing in the stably stratified interior below the surface mixed layer in the ocean general circulation model(OGCM) is put forward preliminarily in this paper. Besides turbulence, the impact of sub-mesoscale oceanic processes(including inertial internal wave breaking product) on oceanic interior mixing is emphasized. We suggest that adding the inertial internal wave breaking mixing scheme(F-scheme for short) put forward in this paper to the turbulence mixing scheme of Canuto et al.( T-scheme for short) in the OGCM, except the region from 15°S to 15°N. The numerical results of F-scheme by using WOA09 data and an OGCM(LICOM, LASG/IAP climate system ocean model) over the global ocean are given. A notable improvement in the simulation of salinity and temperature over the global ocean is attained by using T-scheme adding F-scheme, especially in the mid- and high-latitude regions in the simulation of the intermediate water and deep water. We conjecture that the inertial internal wave breaking mixing and inertial forcing of wind might be one of important mechanisms maintaining the ventilation process. The modeling strength of the Atlantic meridional overturning circulation(AMOC) by using T-scheme adding F-scheme may be more reasonable than that by using T-scheme alone, though the physical processes need to be further studied, and the overflow parameterization needs to be incorporated. A shortcoming in F-scheme is that in this paper the error of simulated salinity and temperature by using T-scheme adding F-scheme is larger than that by using T-scheme alone in the subsurface layer. 相似文献
12.
《Ocean Modelling》2002,4(2):89-120
We compared the 13 models participating in the Ocean Carbon Model Intercomparison Project (OCMIP) with regards to their skill in matching observed distributions of CFC-11. This analysis characterizes the abilities of these models to ventilate the ocean on timescales relevant for anthropogenic CO2 uptake. We found a large range in the modeled global inventory (±30%), mainly due to differences in ventilation from the high latitudes. In the Southern Ocean, models differ particularly in the longitudinal distribution of the CFC uptake in the intermediate water, whereas the latitudinal distribution is mainly controlled by the subgrid-scale parameterization. Models with isopycnal diffusion and eddy-induced velocity parameterization produce more realistic intermediate water ventilation. Deep and bottom water ventilation also varies substantially between the models. Models coupled to a sea-ice model systematically provide more realistic AABW formation source region; however these same models also largely overestimate AABW ventilation if no specific parameterization of brine rejection during sea-ice formation is included. In the North Pacific Ocean, all models exhibit a systematic large underestimation of the CFC uptake in the thermocline of the subtropical gyre, while no systematic difference toward the observations is found in the subpolar gyre. In the North Atlantic Ocean, the CFC uptake is globally underestimated in subsurface. In the deep ocean, all but the adjoint model, failed to produce the two recently ventilated branches observed in the North Atlantic Deep Water (NADW). Furthermore, simulated transport in the Deep Western Boundary Current (DWBC) is too sluggish in all but the isopycnal model, where it is too rapid. 相似文献
13.
The satellite altimeter data reveal that intraseasonal long Rossby wave is amplified in the western part of subtropical ocean. Based on a two and half layer ocean model we infer that the intraseasonal long Rossby wave may be amplified by the baroclinic instability. According to the baroclinic instability criterion derived from the two and half layer model, we calculate the baroclinic instability area of the Subtropical North Pacific Ocean based on Levitus98 data. The baroclinic instability area is well in accord with the amplification area of the intraseasonal long Rossby wave, and this also proves that the baroclinic instability is the main amplification mechanism of the intraseasonal long Rossby wave in the subtropical ocean. The consistency between the baroclinic instability area and potential vorticity (PV) pool is further proved in this paper, therefore, we have confidence that the intraseasonal long Rossby wave is amplified in the PV pool. Due to the relatively large ocean basin and weak ventilation, the PV pool is much larger in the North Pacific Ocean than in the North Atlantic Ocean, and this is the reason for the difference of wave amplification areas of these two Oceans. 相似文献
14.
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
15.
海浪搅拌混合对北太平洋海表面温度模拟的影响 总被引：1，自引：1，他引：0
利用NCEP再分析风场驱动WAVEWATCH III海浪模式对北太平洋海域的海浪过程进行模拟,利用浮标观测资料对模拟出的海浪要素有效波高进行验证,发现他们之间具有很好的一致性。基于模式输出的有效波高等波浪要素,利用特征波参数化理论,在海洋环流模式中引入海浪搅拌混合作用,分析其对北太平洋海表面温度模拟的影响,初步数值模拟结果表明,sbPOM模式在考虑海浪搅拌混合作用以后,模拟精度进一步提升,这对提供一个准确的大气模式下边界条件具有重要作用。 相似文献
16.
采用POMgcs(Princeton Ocean Model with generalized coordinate system)和MITgcm(MIT General Circulation Model)两个海洋数值模式,研究了M-Y2.0、基于固壁近似假定的M-Y2.5、基于波浪破碎作用的M-Y2.5和KPP 4种垂向混合参数化方案对模拟黄海夏季上层温度结构的影响。结果表明,M-Y2.0和基于固壁近似假定的M-Y2.5方案低估了黄海上层的湍动能,模拟的黄海夏季温度上混合层的效果与实测相比均偏浅,不能够很好地重构黄海夏季温度的垂直结构。而基于波浪破碎作用的M-Y2.5和KPP方案均可以增加海洋上层湍动能的输入量,模拟的黄海夏季温度上混合层的效果与实测较为一致。故推测黄海夏季的上层结构是受波浪混合和流场剪切等物理机制共同调节的,若通过合理的垂向混合参数化方案将这些物理机制的作用加以体现,将会较真实地模拟和重构出黄海夏季海温上层结构。 相似文献
17.
Various statistical methods (empirical orthogonal function (EOF), rotated EOF, singular value decomposition (SVD), principal
oscillation pattern (POP), complex EOF (CEOF) and joint CEOF) were applied to low-pass filtered (>7 years) sea surface temperature
(SST), subsurface temperature and 500 hPa geopotential height in order to reveal standing and propagating features of decadal
variations in the North Pacific. Four decadal ocean-atmosphere covariant modes were found in this study. The first mode is
the well-known ENSO-like mode associated with the “Pacific-North American” atmospheric pattern, showing SST variations reversed
between the tropics and the extratropics. In the western tropical Pacific, subsurface temperature variations were found to
be out of phase with the SST variations. The other three modes are related to the oceanic general circulation composed of
the subtropical gyre, the Alaskan gyre and the subpolar gyre, respectively. The 1988/89 event in the northern North Pacific
was found to be closely associated with the subtropical gyre mode, and the atmospheric pattern associated with this mode is
the Arctic Oscillation. An upper ocean heat budget analysis suggests that the surface net heat flux and mean gyre advection
are important to the Alaskan gyre mode. For the subpolar gyre mode, the mean gyre advection, local Ekman pumping and surface
net heat flux play important roles. Possible air-sea interactions in the North Pacific are also discussed. The oceanic signals
for these decadal modes occupy a thick layer in the North Pacific, so that accumulated heat content may in turn support long-term
climate variations.
This revised version was published online in July 2006 with corrections to the Cover Date. 相似文献
18.
Akio Ishida Kisaburo Nakata Shigeaki Aoki Hiroshi Kutsukake Michio J. Kishi Masahisa Kubota 《Journal of Oceanography》2001,57(4):433-450
Distributions and characteristics of water mass and chlorofluorocarbons (CFCs) in the North Pacific are investigated by using
a General Circulation Model (GCM). The anthropogenic CO2 uptake by the ocean is estimated with velocity fields derived from the GCM experiments. The sensitivity of the uptake to
different diffusion parameterizations and different surface forcing used in the GCM is investigated by conducting the three
GCM experiments; the diffusive processes are parameterized by horizontal and vertical eddy diffusion which is used in many
previous models (RUN1), parameterized by isopycnal diffusion (RUN2), and isopycnal diffusion and perpetual winter forcing
for surface temperature and salinity (RUN3). Realistic features for water masses and CFCs can be simulated by the isopycnal
diffusion models. The horizontal and vertical diffusion model fails to simulate the salinity minimum and realistic penetration
of CFCs into the ocean. The depth of the salinity minimum layer is better simulated under the winter forcing. The results
suggest that both isopycnal parameterization and winter forcing are crucial for the model water masses and CFCs simulations.
The oceanic uptake of anthropogenic CO2 in RUN3 is about 19.8 GtC in 1990, which is larger by about 10% than that in RUN1 with horizontal and vertical diffusive
parameterization. RUN3 well simulates the realistic water mass structure of the intermediate layer considered as a candidate
of oceanic sink for anthropogenic CO2. The results suggest that the previous models with horizontal and vertical diffusive parameterization may give the oceanic
uptake of anthropogenic CO2 underestimated.
This revised version was published online in August 2006 with corrections to the Cover Date. 相似文献
19.
基于海浪模式WAVEWATCH Ⅲ模拟北太平洋海浪要素,结合NDBC浮标资料进行验证,发现模拟出的有效波高与浮标测量值具有很好的一致性。基于改进型白冠覆盖率耗散模型,利用海浪模式模拟出的有效波高、有效波周期和摩擦速度等海浪要素计算出单位面积水柱内因海浪破碎产生的湍动能通量。通过改变环流模式sbPOM湍动能方程的上边界条件,引入海浪破碎产生的湍动能通量,并探究海浪破碎对北太平洋海表面温度模拟的影响。研究表明,由于海浪破碎的引入,环流模式sbPOM对北太平洋海表面温度模拟的准确程度得到提升,这为大气模式提供一个准确的北太平洋下边界条件具有重要意义。 相似文献