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1.
东北季风期台湾海峡的逆温现象   总被引:3,自引:1,他引:2  
利用2006-2008年3个航次水文资料,结合日本海洋数据中心(JODC)的历史温度数据分析了东北季风期台湾海峡的逆温现象。结果显示,除台湾浅滩及海峡西岸浅水区外,几乎整个台湾海峡皆有逆温现象。逆温幅度和发生频率在海峡西部较高,海峡东部及粤东近海较低。逆温层上界深度春季较秋、冬季深,逆温频发区(发生频率大于60%)随着季节南北向移动,秋季频发区的最南端位于厦门近海,冬季扩展至台湾浅滩北部,春季回退至平潭近海。分析表明,浙闽沿岸水随季节南北向伸缩导致了逆温频发区的同步移动。除了季节变化外,逆温现象在2006年和2007年冬季有显著差异,2006年逆温仅出现在海峡西部近岸海域,2007年扩展至海峡东部且向南伸至粤东近岸,浙闽沿岸水的横向伸缩是造成此差异的主因。  相似文献   

2.
基于阿拉斯加湾(Gulf of Alaska, GOA)2002—2020年的Argo浮标数据,本研究分析了该海湾逆温现象的时空变化特征,并探讨其年际变化与水体垂向位温异常的联系。结果显示,阿拉斯加湾逆温现象存在明显的时空变化。空间上,逆温幅度(ΔT)在湾北部最大,湾东南部次之,湾西南部最弱。逆温厚度(ΔD)在湾西南部最厚,湾北部和东南部依次变薄。在季节尺度上,湾北部逆温现象的季节变化最明显,冬季ΔT最大和ΔD最厚,随季节性的加热和混合作用,ΔT持续减弱,ΔD不断变薄。在湾东南部,ΔT分别在3月和9月具有0.46、0.40 ℃的峰值;ΔD在整个海湾中最薄,冬季最大为44 m,而秋季最小仅为23 m。在湾西南部,ΔT介于0.24~0.33 ℃之间,分别于4月和10月具有0.31、0.33 ℃的峰值;ΔD冬季最大超过100 m,秋季最薄约为57 m。年际变化上,ΔT在2002、2007—2009、2012、2017年表现为正异常,但在2003—2005、2010、2013—2016、2018—2020年表现为负异常;ΔD在2002、2007—2008、2012、2017—2020年主要偏厚,在2003—2006、2015—2016年偏薄。湾北部和东南部ΔT和ΔD的年际变化较为一致,但两者在西南部并没有明显的联系。ΔT和ΔD年际变化与水体垂向位温异常有密切联系。当水体位温具有冷(暖)异常时,整个海湾ΔT往往具有正(负)异常,湾北部和东南部ΔD趋于偏厚(薄),但湾西南部ΔD趋于偏薄(厚)。  相似文献   

3.
引用《渤海、黄海、东海海洋图集——水文》分册中有关逆温跃层分布变化图幅以及海流和温、盐度历史资料 ,指出山东半岛北及东沿岸区域冬季出现的逆温跃层现象与这里冬季潜伏于深底层暖流水有密切关系 ,并进一步认为围绕山东半岛北及东沿岸海域冬季的海水交换可能呈 2层模式 :在上层 ,低温、低盐的沿岸水自西向东南下 ;在深底层 ,相对高温、高盐的逆流水北上自东向西有直逼渤海海峡南部的势头。  相似文献   

4.
东海西部沿岸海域冬季的逆温跃层现象及其与环流的关系   总被引:1,自引:0,他引:1  
本文引用《渤海、黄海、东海海洋图集──水文》分册(1992)中有关逆温跃层分布变化的图幅以及温盐历史资料,指出东海西部沿岸(22~32°N)冬季出现逆温跃层的区域北起长江口,南到南澳岛以南几乎相联成片的现象,论述了这一分布与中国东南近海冬季潜伏于深底层的暖流水的区域相吻合,从而从水文结构上证实了冬季在深底层粤东沿岸的南海暖流北上通过台湾海峡西部与闽浙沿岸的台湾暖流相接这一环流特征。  相似文献   

5.
引用《渤海、黄海、东海海洋图集-水文》分册中有关逆温跃层分布变化图幅以及海流和温、盐度历史资料,指出山东半岛北及东沿岸区域冬季出现的逆温跃层现象与这里冬季潜伏于深底层暖流水有密切关系,半进一步认为围绕山东半岛北及东沿岸海域冬季的海水交换可能呈2层模式,在上层,低温,低盐的沿岸水自西向东南下;在深底层,相对高温、高盐的逆流水北上自东向西有直逼渤海海峡南部的势头。  相似文献   

6.
根据珠江口2015年7月6日至17日航次的CTD(conductivity, temperature, and depth)观测结果,分析得到:珠江口附近海域存在海水的垂向逆温现象,逆温差平均值为0.42 oC,上界深度在1 m-6 m间,下界深度在3 m-10 m间,逆温层平均厚度约为4 m。根据时空分布差异的不同,逆温现象可区分为以下三种情况:(1)在狮子洋、太平水道和蕉门水道的出口汇集处,存在温、盐差异的不同水体的交互过程中,由于潮汐和径流的作用所形成的水平流场差异导致了垂向温度的逆转现象。(2)在珠江口西侧的盐度锋面区域附近,第一航段观测期间锋面内侧低盐水团的温度低于锋面外侧高盐水团约2 oC,此时可观测到逆温现象;但在同一区域的第二航段观测期间由于河口内表层水温的上升,导致了逆温现象消失。该区域盐度锋面附近的两个水团在锋面位置附近发生叠置,冲淡水覆盖于海水之上,两个水团的温、盐差异是温度逆转现象的主因。(3)香港西南侧的上升流区域与盐度锋面的相互作用导致了该区域逆温现象的产生。  相似文献   

7.
初春南黄海水文特征及环流状况的分析   总被引:10,自引:4,他引:6  
根据1996年初春中韩黄海水循环动力学合作调查所获资料,分析了南黄海水文特征及其环流状况,并获得了以下几点主要认识:(1)初春南黄海的温、盐分布特征及环流基本形态,与以往所揭示的冬季状况基本相似.然而,本次调查发现,在30m以浅,黄海中部暖水舌轴线比冬季的明显偏东;且出现一范围较小的孤立的相对高温高盐区.在垂向,一种中层冷水和表层逆温跃层现象出现在黄海局部区域.(2)直接测流的结果,不仅部分地印证了由温、盐场所显示的环流基本形态,而且较好地揭示了流场中发生的一些新现象,其中尤其是绕济州岛的流动.(3)黄海暖流水是对马暖流水和陆架水混合而成.而且,它主要是在济州岛西侧水域,从锋带中衍生出来的.  相似文献   

8.
青岛逆温层特征及其对空气质量的影响分析   总被引:1,自引:0,他引:1  
郭丽娜  黄容  马艳 《海岸工程》2014,33(4):14-25
利用2006-2012年青岛站逐日08时和20时(北京时)的探空资料,研究了青岛市大气逆温层特征和变化规律以及大气逆温层和城市空气质量之间的关系.结果表明,青岛的逆温在春季最多,夏季最少,以接地逆温为主.接地逆温层平均厚度为290.6 m,最大厚度可达1443m;平均强度为0.56℃·(100m)-1,最大强度为10.00℃·(100 m)-1.空气污染前和污染时出现的逆温中,接地逆温占73.2%.空气污染前24 h内的20时和污染时08时的逆温强度与污染日API呈正相关关系,逆温层厚度与空气质量关系不明显.中度以上污染时,08时接地逆温强度与污染日API相关系数达0.99,通过0.001的置信度检验.  相似文献   

9.
本文利用多普勒声雷达所获取的在时间、空间(垂直方向)较为密集的实时资料,分别对两次性质不同的(平流和辐射)大雾的边界层温度场、风场结构特征进行了对比分析.得出在华北地形槽下的平流雾得以稳定维持的根本原因是与位于各逆温层之上的、和平均极大风速达10.72m/s的偏北大风相联系的下沉逆温密切相关.下沉逆温随着与之相伴的偏北大风的减弱、消失而逐渐趋于消失.其边界层逆温较大辐度地减弱是动力(动量下传)、热力(对流)共同作用的结果.而发生在雨(雪)之后的变性冷高压之下的辐射雾,其温度场结构为主付层式的逆温结构.自始至终,逆温处在弱的均一风场之中,没有湍流的发生发展,其逆温的减弱消散仅和热力作用有关.  相似文献   

10.
1205号台风“泰利”影响下台湾海峡风浪特征分析   总被引:1,自引:0,他引:1  
利用相对密集的海上浮标和岸基台站观测资料,分析、总结了1205号台风"泰利"影响期间台湾海峡及周边海域的风浪特征,得到如下结论:(1)台湾海峡东南海域海浪始终相对较大,过程极值出现在该区域的七股浮标;(2)台风中心位于台湾海峡中部和南部时,海峡中线浪高自台风中心向外递减,台风中心位于台湾海峡北部时,海峡中线浪高自台风中心向外递增;(3)台湾海峡西南侧1号浮标风速曲线两次出现漏斗型向下波动;(4)在13个主要浮标站点中有8个浮标的风浪经验相关系数未达到高度相关。本文从台风机构、风浪成长要素、相关天气系统、台湾海峡特殊地形、边界层风场环流等方面分析了台湾海峡的台风浪分布特征及形成机理,研究成果可为该类型台风浪预报提供参考。  相似文献   

11.
In the northern Bay of Bengal, the existence of intense temperature inversion during winter is a widely accepted phenomenon. However, occurrences of temperature inversion during other seasons and the spatial distribution within and adjacent to the Bay of Bengal are not well understood. In this study, a higher resolution spatiotemporal variation of temperature inversion and its mechanisms are examined with mixed layer heat and salt budget analysis utilizing long-term Argo(2004 to 2020) and RAMA(2...  相似文献   

12.
东海北部陆架区温、盐度逆转现象的分析   总被引:1,自引:0,他引:1  
东海陆架区的温、盐度逆转现象,有关研究已作了一些论述(苏育嵩等,1989;蓝淑芳等,1984; Nakao,1977),指出东海陆架区存在两个温、盐度逆转结构出现频率高的海区:一个位于江苏、浙江近海的狭长海区内;另一个位于东海北部济州岛西南海区,即东海北部底层冷水及其附近海域(蓝淑芳等,1993)。翁学传(1984)、曹欣中等(1982)利用常规调查资料,曾分别对第一高频区的中层冷水和温度逆转现象作了初步分析;丁宗信(1994,1995)利用常规调査资料和CTD资料,对黄海、东海春、夏、秋、冬四季温、盐度垂直分布类型及逆转现象的成因进行了研究。本文根据中国科学院海洋研究所1984年和1985年6月在东海北部陆架区进行的大面水文调査资料(该资料由“科学一号”调査船使用Mark-Ⅲ CTD 探测仪获取),以及国家海洋局1975-1980年在东海取得的标准断面BT观测资料,对东海北部陆架区,特别是上述第二高频区的温、盐度逆转现象和成因作进一步研究。 由于该海区的温、盐度逆转现象与水团的配置及交汇密切相关,所以首先讨论该海区的水团。  相似文献   

13.
Seasonal and interannual variations of the mixed layer properties in the Antarctic Zone (AZ) south of Tasmania are described using 7 WOCE/SR3 CTD sections and 8 years of summertime SURVOSTRAL XBT and thermosalinograph measurements between Tasmania and Antarctica. The AZ, which extends from the Polar Front (PF) to the Southern Antarctic Circumpolar Current Front (SACCF), is characterized by a 150 m deep layer of cold Winter Water (WW) overlayed in summer by warmer, fresher water mass known as Antarctic Surface Water (AASW). South of Tasmania, two branches of the PF divide the AZ into northern and southern zones with distinct water properties and variability. In the northern AZ (between the northern and southern branches of the PF), the mixed layer depth (MLD) is fairly constant in latitude, being 150 m deep in winter and around 40–60 m in summer. In the southern AZ, the winter MLD decreases from 150 m at the S-PF to 80 m at the SACCF and from 60 to 35 m in summer. Shallower mixed layers in the AZ-S are due to the decrease in the wind speed and stronger upwelling near the Antarctic Divergence. The WW MLD oscillates by ±15 m around its mean value and modest interannual changes are driven by winter wind stress anomalies.The mixed layer is on annual average 1.7 °C warmer, 0.06 fresher and 0.2 kg m−3 lighter in the northern AZ than in the southern AZ. The Levitus (1998) climatology is in agreement with the observed mean summer mixed layer temperature and salinity along the SURVOSTRAL line but underestimates the MLD by 10–20 m. The winter MLD in the climatology is also closed to that observed, but is 0.15 saltier than the observations along the AZ-N of the SR3 line. MLD, temperature and density show a strong seasonal cycle through the AZ while the mixed layer salinity is nearly constant throughout the year. During winter, the AZ MLD is associated with a halocline while during summer it coincides with a thermocline.Interannual variability of the AZ summer mixed layer is partly influenced by large scale processes such as the circumpolar wave which produces a warm anomaly during the summer 1996–1997, and partly by local mechanisms such as the retroflection of the S-PF which introduces cold water across the AZ-N.  相似文献   

14.
利用2014年3–4月北象海豹携带的自动温盐深仪(CTD-SRDL)在阿拉斯加湾东部陆坡海域上采集到的温盐剖面数据,分析了该海域逆温现象的空间分布和演变过程。结果显示,研究海域存在明显的逆温现象,逆温幅度和逆温厚度范围分别介于0.2~1.6?C和20~280 m之间,前者沿陆坡向北幅度逐渐增大,后者在50?~58?N间往北逐渐变厚,在58?N以北海域平均厚度较薄。3月25日至4月22日,逆温层处于衰退阶段。逆温层下界温度不断下降,逆温幅度呈变弱趋势,逆温厚度呈变薄趋势。一维扩散模型模拟结果表明,湍扩散作用下,观测期间海表受热导致混合层上部位温升高,但底部仍保持低温,因此逆温层上界温度变化并不明显。次表层由于具有强的位温梯度,湍扩散导致逆温层下界温度显著降低,是观测期间逆温衰退的主要原因。湍扩散作用导致次表层水体温盐属性趋于均匀,这一过程对于阿拉斯加湾逆温现象的形成及演变研究具有重要意义。  相似文献   

15.
The mean seasonal cycle of mixed layer depth (MLD) in the extratropical oceans has the potential to influence temperature, salinity and mixed layer depth anomalies from one winter to the next. Temperature and salinity anomalies that form at the surface and spread throughout the deep winter mixed layer are sequestered beneath the mixed layer when it shoals in spring, and are then re-entrained into the surface layer in the subsequent fall and winter. Here we document this ‘re-emergence mechanism’ in the North Pacific Ocean using observed SSTs, subsurface temperature fields from a data assimilation system, and coupled atmosphere–ocean model simulations. Observations indicate that the dominant large-scale SST anomaly pattern that forms in the North Pacific during winter recurs in the following winter. The model simulation with mixed layer ocean physics reproduced the winter-to-winter recurrence, while model simulations with observed SSTs specified in the tropical Pacific and a 50 m slab in the North Pacific did not. This difference between the model results indicates that the winter-to-winter SST correlations are the result of the re-emergence mechanism, and not of similar atmospheric forcing of the ocean in consecutive winters. The model experiments also indicate that SST anomalies in the tropical Pacific associated with El Niño are not essential for re-emergence to occur.The recurrence of observed SST and simulated SST and SSS anomalies are found in several regions in the central North Pacific, and are quite strong in the northern (>50°N) part of the basin. The winter-to-winter autocorrelation of SSS anomalies exceed those of SST, since only the latter are strongly damped by surface fluxes. The re-emergence mechanism also has a modest influence on MLD through changes in the vertical stratification in the seasonal thermocline.  相似文献   

16.
Intercomparison of three South China Sea circulation models   总被引:2,自引:1,他引:1  
1IntroductionTheSouthChinaSeaisthelargesttropicalmarginaldeepsealocatingbetweenthewesternPacificOceanandtheeasternIndianOcean.AsapartofAsia-Australiamaritimecontinent,monsoonisaprimaryfactorforcingtheSouthChinaSeaCurrent(SCSC)variation.Drivenbynortheasterlymonsooninwinterandsouth-westerlymonsooninsummer,respectively,theSCSCbehavesacyclonicgyreandananticy-clonicgyre,correspondingly(Wyrtki,1961;Xuetal.,1982).Owingtotheshortageandexpen-sivenessofdirectobservationsintheSCS,fur-therunder…  相似文献   

17.
1 Introduction Ocean upper mixed layer, with nearly uniform temperature, salinity and density, is formed by sea sur- face forces such as wind stress, buoyancy flux and sur- face waves, etc. Under the mixed layer, thermocline and halocline often exist. Usually the depth of them is almost equal. But in the tropical ocean, the halocline is often shallower than the thermocline. Then between the layer of uniform salinity and the thermocline, there is a layer which has a rather strong density gradi…  相似文献   

18.
In this paper, effort is made to demonstrate the quality of high-resolution regional ocean circulation model in realistically simulating the circulation and variability properties of the northern Indian Ocean(10°S–25°N,45°–100°E) covering the Arabian Sea(AS) and Bay of Bengal(BoB). The model run using the open boundary conditions is carried out at 10 km horizontal resolution and highest vertical resolution of 2 m in the upper ocean.The surface and sub-surface structure of hydrographic variables(temperature and salinity) and currents is compared against the observations during 1998–2014(17 years). In particular, the seasonal variability of the sea surface temperature, sea surface salinity, and surface currents over the model domain is studied. The highresolution model's ability in correct estimation of the spatio-temporal mixed layer depth(MLD) variability of the AS and BoB is also shown. The lowest MLD values are observed during spring(March-April-May) and highest during winter(December-January-February) seasons. The maximum MLD in the AS(BoB) during December to February reaches 150 m (67 m). On the other hand, the minimum MLD in these regions during March-April-May becomes as low as 11–12 m. The influence of wind stress, net heat flux and freshwater flux on the seasonal variability of the MLD is discussed. The physical processes controlling the seasonal cycle of sea surface temperature are investigated by carrying out mixed layer heat budget analysis. It is found that air-sea fluxes play a dominant role in the seasonal evolution of sea surface temperature of the northern Indian Ocean and the contribution of horizontal advection, vertical entrainment and diffusion processes is small. The upper ocean zonal and meridional volume transport across different sections in the AS and BoB is also computed. The seasonal variability of the transports is studied in the context of monsoonal currents.  相似文献   

19.
Temperature, salinity and density structures were observed on Sept. 23 and 24, 1986 at one vertical section across the East China Sea shelf edge by an advanced type of towed vehicle with CTD sensors which was developed by the Japan Marine Science and Technology Center. The vehicle was towed at a speed of 2.5 m s−1 down to 150 m depth and at intervals of 170–500 m width. The observed profile was 50 km long on Sept. 23 and 70 km long on Sept. 24 along the cross-shelf section. An on-ship acoustic Doppler current profiler was simultaneously used to measure current velocities at depths of 20, 50 and 100 m.Interesting features were noticed. Firstly, there was a vertical displacement of pycnoclines at the lower edge of the surface mixed layer accompanied by vertical inversion of the salinity and temperature in the vicinity of the shelf edge. Pycnoclines were displaced upward by 12 m toward the outer edge on Sept. 23 and by 20 m on Sept. 24. On Sept. 23, the salinity inversion took place in a layer 20 m thick and 8 km wide, whereas the temperature inversion took place in a layer 8 m thick and 1.5 km wide. These vertical inversions were probably generated by vertical shear of tidal currents which was observed by the Doppler current profiler. These results throw light on understanding the vertical mixing process of stratified water on the continental shelf edge. Secondly, an intrusion of the shelf water into the Kuroshio water was observed along pycnoclines below the surface mixed layer 60 to 70 m deep in the Kuroshio region outer break. The measurement was successful in showing a horizontal mixing process of the shelf water and the Kuroshio water which could not be found out by standard CTD observations.  相似文献   

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