冬季东中国海环流中的中尺度涡旋数值模拟   总被引：5，自引：0，他引：5       下载免费PDF全文

陈敏  侯一筠  赵保仁 《海洋科学》2003,27(1):53-60

采用高精度的POM模式 ,考虑了海底地形、外来流、长江径流、海面风应力、海面热通量等多方面因素的影响 ,模拟了冬季东中国海环流结构。模拟结果显示 :在黄海东部很可能存在两个涡 ,中心分别在124°37′E ,37°N ,124°E ,35°30′N ;东海北部存在一个大型的气旋式涡旋 ,其中心位置在125.1°E ,30.5°N附近 ,该涡旋是由东北向的台湾暖流、西北向的黄海暖流及南下的沿岸流组成的封闭结构 ;日本九州以西黑潮入侵分支形成一涡旋 ,黑潮分支是形成此涡旋的直接动力因素 ,另外地形和冬季盛行的偏北风也对该涡旋的形成有一定正面影响。  相似文献   

Stochastic Response Analysis of Piled Offshore Platform Excited by Stationary Filtered White Noise     

Luo Chuanxin Wu Zhiping Professor 《中国海洋工程》1997,(1)

In this paper,the analysis method of stochastic response of piled offshore platform excited bystationary filtered white noise is presented.With this method,the strong ground motion is considered asthree direction stationary filtered white noise process,the theoretic solutions of three special integrationequations are derived with the residue theorem,and the expression of response nodal displacements andmember forces of offshore platform excited by the stationary filtered white noise is put forward.Thestochastic response of a piled offshore platform excited by the stationary filtered white noise,which is lo-cated 114.3m in water depth,is computed.The results are compared with those obtained with the re-sponse spectrum analysis method and the stationary white noise model analysis method,and the corre-sponding conclusion is drawn.  相似文献   

McCreary和Fickian湍扩散形式差异的分析     

吴德星  李国璋  李宝辉  陈峰 《中国海洋大学学报(自然科学版)》1993,(Z2)

用矩阵方法,求解McCreary和Fickian铅垂向湍扩散形式下,无界海洋条件时在风应力和深层浮力作用下的线性解。得出不同的湍扩散系数A情况下McCreary与Fickian湍扩散形式的流场结构。指出随湍扩散系数的增加,McCreary和Fickian湍扩散形式下u分量结构及其量值差异增大。在Fickian湍扩散形式下,能量穿越密度跃层的传递能力较强。当A=0.1cm~2s~(-3)时,在风应力和深层浮力作用下两种湍扩散形式造成流场的差异很小。提出在小湍扩散系数下,用McCreary湍扩散形式研究热带海洋环流,其结果和Fickian形式应相当一致。  相似文献   

The influence of island generated eddies on the carbon dioxide system, south of the Canary Islands     

Melchor Gonzlez-Dvila  J. Magdalena Santana-Casiano  Demetrio de Armas  Jos Escnez  Miguel Suarez-Tangil 《Marine Chemistry》2006,99(1-4):177

Measurements of surface partial pressure of CO₂ and water column alkalinity, pH_T, nutrients, oxygen, fluorescence and hydrography were carried out, south of the Canary Islands during September 1998. Cyclonic and anticyclonic eddies were alternatively observed from the northwestern area to the central area of the Canary Islands. Nutrient pumping and vertical uplifting of the deep chlorophyll maximum by cyclonic eddies were also ascertained by upward displacement of dissolved inorganic carbon. A model was applied to determine the net inorganic carbon balance in the cyclonic eddy. The fluxes were determined considering both the diffusive and convective contributions from the upward pumping and the corresponding horizontal transport of water outside the area. An increase in the total inorganic carbon concentration in the upper layers inside the eddy field of 133 mmol C m^− 2 d^− 1 was determined. The upward flux of inorganic carbon decreased the effect of the increased primary production on the carbon dioxide chemistry. The reduced fCO₂ inside the cyclonic eddy, 15 μatm lower than that observed in non-affected surface water, was explained by thermodynamic aspects, biological activity, eddy upward pumping and diffusion and air–sea water exchange effects.  相似文献   

Large eddy simulation of hydrocyclone—prediction of air-core diameter and shape     

M. Narasimha  Mathew Brennan  P.N. Holtham 《International Journal of Mineral Processing》2006

Hydrocyclones are widely used in the mining and chemical industries. An attempt has been made in this study, to develop a CFD (computational fluid dynamics) model, which is capable of predicting the flow patterns inside the hydrocyclone, including accurate prediction of flow split as well as the size of the air-core. The flow velocities and air-core diameters are predicted by DRSM (differential Reynolds stress model) and LES (large eddy simulations) models were compared to experimental results. The predicted water splits and air-core diameter with LES and RSM turbulence models along with VOF (volume of fluid) model for the air phase, through the outlets for various inlet pressures were also analyzed. The LES turbulence model led to an improved turbulence field prediction and thereby to more accurate prediction of pressure and velocity fields. This improvement was distinctive for the axial profile of pressure, indicating that air-core development is principally a transport effect rather than a pressure effect.  相似文献   

近百年中国东部夏季降水的时空变率   总被引：4，自引：0，他引：4  

Li Xiaodong  Zhu Yafen  Qian Weihong 《大气科学进展》2002,19(6):1055-1068

利用中国东部25°N以北28个站1880-1999年夏季季降水序列,用旋转复经验正交函数（RCEOF）方法,研究了中国东部地区百年干湿的时空演变规律。结果表明,夏季降水空间变率大值区依次为:长江中下游地区、淮河流域、江南、华北、西南及东北。除西南外的5个关键区大体上反映了从6月到8月夏季雨带自南向北椎进所滞留的地区。旋转空间位相分布揭示了长江中下游地区、江南、东北的旱涝异常主要表现为驻波振动特征;而淮河流域、华北、西南地区显示出降水异常信号具有部分的行波特征。尤其第4空间模显示出旱涝异常信号从东北南部可沿着黄淮下游传到长江下游地区。对于近百年中国东部地区夏季于湿变化,长江中下游地区、淮河流域、华北及东北四个地区都存在20-25年时间尺度的周期振荡;长江中下游地区及华北地区都存在准60年时间尺度的振荡周期;东北地区主要表现出36年时间尺度的振荡周期;淮河流域存在明显的70-80年时间尺度的振荡周期;华北地区存在的11年时间尺度的振荡周期恰好与太阳黑子活动的11年周期相一致。在年代际时间尺度（包括次年代际时间尺度）上,长江中下游、淮河流域及华北地区的夏季降水的变化与太阳活动有显著的正相关。  相似文献   

湍流混合动力学机理研究   总被引：7，自引：0，他引：7       下载免费PDF全文

武道吉  张永吉  李圭白  谭风训 《水科学进展》2003,14(6):706-709

在分析传统混合动力学机理基础上,通过宏观混合与微观混合时间量级的对比,提出了湍流条件下,涡流扩散主导宏观混合,分子扩散主导微观混合,而混合过程由宏观混合主导,欧拉数Eu可作为混合效果的控制指标,并通过3种不同容积反应器的混合搅拌试验,进一步证实了该指标的实用性。  相似文献   

Monitoring volcanic hazard using eddy covariance at Solfatara volcano, Naples, Italy     

C Werner  G Chiodini  D Voigt  S Caliro  R Avino  M Russo  T Brombach  J Wyngaard  S Brantley 《Earth and Planetary Science Letters》2003,210(3-4):561-577

An eddy covariance (EC) station was deployed at Solfatara crater, Italy, June 8–25, 2001 to assess if EC could reliably monitor CO₂ fluxes continuously at this site. Deployment at six different locations within the crater allowed areas of focused gas venting to be variably included in the measured flux. Turbulent (EC) fluxes calculated in 30-min averages varied between 950 and 4460 g CO₂ m⁻² d⁻¹; the highest measurements were made downwind of degassing pools. Comparing turbulent fluxes with chamber measurements of surface fluxes using footprint models in diffuse degassing regions yielded an average difference of 0% (±4%), indicating that EC measurements are representative of surface fluxes at this volcanic site. Similar comparisons made downwind of degassing pools yielded emission rates from 12 to 27 t CO₂ d⁻¹ for these features. Reliable EC measurements (i.e. measurements with sufficient and stationary turbulence) were obtained primarily during daytime hours (08:00 and 20:00 local time) when the wind speed exceeded 2 m s⁻¹. Daily average EC fluxes varied by ±50% and variations were likely correlated to changes in atmospheric pressure. Variations in CO₂ emissions due to volcanic processes at depth would have to be on the same order of magnitude as the measured diurnal variability in order to be useful in predicting volcanic hazard. First-order models of magma emplacement suggest that emissions could exceed this rate for reasonable assumptions of magma movement. EC therefore provides a useful method of monitoring volcanic hazard at Solfatara. Further, EC can monitor significantly larger areas than can be monitored by previous methods.  相似文献   

South　China　Sea　Warm　Pool　in　Boreal　Spring   总被引：36，自引：1，他引：36  

Peter C. Chu  C.-P. Chang 《大气科学进展》1997,14(2):195-206

During the boreal spring of 1966, a warm-core eddy is identified in the upper South China Sea (SCS) west of the Philippines through an analysis of the U.S. Navy’s Master Oceanographic Observation Data Set. This eddy occurred before the development of the northern summer monsoon and disappeared afterward. We propose that this eddy is a result of the radiative warming during spring and the downwelling due to the anticyclonic forcing at the surface. Our hypothesis suggests an air-sea feedback scenario that may explain the development and withdrawal of the summer monsoon over the SCS. The development phase of the warm-core eddy in this hypothesis is tested by using the Princeton Ocean model  相似文献   

对流边界层中泡状结构的大涡模拟研究   总被引：7，自引：3，他引：7       下载免费PDF全文

蔡旭晖  陈家宜 《大气科学》1997,21(2):223-230

本文提出“连续垂直运动区”的概念，对边界层中的对流泡状运动进行了重新定义。由此将对流边界层划分为上升泡区、下沉泡区和环境气流区，并利用大涡模拟提供的对流边界层数值模拟结果研究这种泡状运动的结构。研究结果较好地解释了一些有关泡状运动结构方面的似乎相互矛盾的观测事实，并揭示了对流泡状运动的一些新的特征。  相似文献