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1.
基于2015年9月和12月闽北附近海域3条断面上的同步连续沉积动力学观测,结合对应时段的卫星遥感海表温度资料,研究了闽北近岸海域冬季和夏季悬浮体分布和输运通量的变化规律。结果表明,该区域的悬浮体浓度存在明显的季节性变化,冬季季风活动对水体扰动强烈,水体垂向混合较为均匀,近岸沉积物再悬浮活跃,其浓度值明显高于外海;而夏季近岸悬浮体浓度明显降低。在50m以深的外海海域,悬浮体浓度无显著的季节差异,且空间变化幅度很小。受东北季风和闽浙沿岸流的影响,冬季悬浮体总体上沿东北向西南的沿岸方向输送,输运通量由近岸向外海逐渐减小;在夏季,闽北近岸海域悬浮体输运方向与冬季一致,但输运通量显著减小;外海海域的悬浮体输运方向指向东北,输运通量明显高于冬季。在离岸断面上,中间站位(水深约50m)的悬浮体浓度低于其两侧站位的浓度,这是由于在近岸一侧主要受控于闽浙沿岸流,而外海海域主要受控于台湾暖流,50m等深线为闽浙沿岸流和台湾暖流相互作用的交汇处,受闽浙沿岸流和台湾暖流的共同影响。温度锋面与闽北附近海域内的泥质区对应关系较好,温度锋面对悬浮体向外海扩散有明显的抑制作用,温度锋面西北侧悬浮体浓度较高且沉积速率较高。 相似文献
2.
本文利用中国海洋大学极地变化重点实验室提供的2008年3月与7月白令海陆架水资料,对白令海200 m内水域温盐及水团进行了分析和对比,对白令海陆架区冬季水团形成机制做了初步的探讨。白令海冬季陆架水的温盐结构垂向均匀;夏季层化明显,存在垂直温盐跃层;白令海由夏季表层水和冬季水两种水团组成;白令海冬季残留水团在陆架区水深20 m处即出现,最低温度较大洋深处冬季水温偏低。 相似文献
3.
2006年夏季珠江冲淡水驱动的上升流 总被引：2，自引：1，他引：1
根据珠江口及其附近海域2006年夏季（7-8月）航次水文调查资料，发现调查期间，除了西南季风驱动下的冲淡水东向扩散外，粤西珠江口外冲淡水主要呈西向扩散趋势，并且西向扩散的冲淡水下存在上升流。已有的模型研究中，西南季风下珠江口外没有出现上升流，说明西南季风不是珠江口外上升流产生的主导因素。观测的温盐分布、潜标流速时间序列与走航ADCP流态表明，上升流产生的原因是:（1）口门外冲淡水南向扩展驱动了垂向重力环流；（2）密度跃层以下东北向沿岸流的底边界层Ekman效应；（3）口门外冲淡水团之间的气旋型中尺度涡旋作用。 相似文献
4.
本文利用历史水文观测数据研究了南海西南部巽他陆架水团特征,结果表明:(1)巽他陆架纳土纳群岛周围底层存在着低温高盐的冷水,该冷水沿地形爬升分为两支,一支可延伸至泰国湾,另一支伸向卡里马塔海峡;(2)巽他陆架底层冷水有明显的季节变化,该底层冷水在春季开始形成,夏季达到最强,秋季开始衰退,最后在冬季完全消失;(3)巽他陆架底层冷水来源于南海次表层水的涌升。夏季西南季风使陆架表层水向南海流动,有利于南海次表层低温高盐水沿地形向陆架爬升,此时底层冷水与表层水温差超过8°C。冬季东北季风,使南海表层水向陆架流动,海水在陆架堆积,从而阻止了南海次表层低温高盐水的爬升。 相似文献
5.
对中国第四次北极科学考察期间在白令海北部获取的海水样品进行悬浮体含量及其颗粒组分特征的分析。结果表明,白令海陆架海区悬浮体含量大体呈现出表层浓度低而底层浓度高的特点。表层海水悬浮体含量在白令海峡西侧和陆架东侧靠近阿拉斯加沿岸含量较高,而底层海水中悬浮体含量则在白令海峡西侧,以及白令海陆架西南部的圣马修岛西北侧较高。陆架流系对底床物质的再悬浮作用致使白令海悬浮颗粒物浓度的高值区多位于近底层海水中。受白令陆坡流沿陆架坡折带输运作用,研究区西南部悬浮体浓度较高。白令海陆架水以及阿纳德尔流携带悬浮颗粒向北输运,使得底层悬浮体浓度呈现出自南向北逐渐减弱的模式。圣劳仑斯岛以北靠近楚科奇半岛一侧海域,受高营养盐的阿纳德尔流的影响,悬浮颗粒物以藻类为主;东侧阿拉斯加沿岸流区悬浮颗粒则以陆源的碎屑矿物为主。 相似文献
6.
基于2020年夏季的大面航次观测数据,分析了烟台—威海北部海洋牧场及邻近海域海水溶解氧浓度垂向分布最小值（氧最小值层）的空间分布特征,并探讨了影响因素。从6月至8月,海水溶解氧浓度不断减小,垂向结构亦存在显著变化。海水溶解氧浓度垂向分布的最小值主要集中于7月的近岸海域,最小值大致从外海向近岸方向减小,其距离海底高度及与底层溶解氧浓度之差的绝对值均于双岛湾邻近海域为最大。海水溶解氧浓度垂向分布的最小值位于最强密度层结以下。但是海水溶解氧浓度垂向分布最小值的强度向北减小,而密度层结向北增大,两者的空间分布基本相反,说明密度层结抑制垂向湍流扩散可极大减少深层海水溶解氧的来源,是海水溶解氧浓度垂向分布最小值形成的必要条件,但不是主导因素。在海水溶解氧浓度垂向分布的最小值层,表观耗氧量存在垂向分布的最大值,大部分站点的pH存在垂向分布的最小值,说明局地增强、持续的生物地球化学耗氧是控制海水溶解氧浓度垂向分布最小值形成和空间分布的一个重要过程。研究结果表明氧最小值层是夏季烟台—威海北部近岸海水溶解氧垂向结构的典型特征之一。 相似文献
7.
台湾海峡西部海域温、盐度跃层初步分析 总被引：2，自引：1，他引：2
本文根据1984—1985年台湾海峡西部海域海洋综合调查的实测资料,描述和分析了本海区温、盐度跃层的强度、深度和厚度的分布特征。结果表明,温、盐跃层具有明显季节变化,其强度分布为海区南部大,北部小;夏季大,冬季小。温跃层最大强度可达1.5℃/m,盐跃层为0.8左右。在几个强跃层区内,温跃层的强度主要取决于海水上、下层水系的性质,盐跃层的强度,主要取决于江河入海流量的大小,同时与沿岸流亦关系密切。 相似文献
8.
对白令海表层海水228Ra的分析表明,白令海表层海水228Ra比活度从低于检测限变化至0.81 Bq/m3,低于西北冰洋陆架区的报道值。表层水228Ra比活度和228Ra/226Ra)A.R.的空间分布均呈现由西南部中心海盆向东北部陆架区增加的趋势。由228Ra/226Ra)A.R.和盐度的关系揭示出白令海环流、白令海陆坡流和阿拉斯加沿岸流对228Ra和228Ra/226Ra)A.R.分布有明显影响。运用一维稳态扩散模型计算出白令海由中心海盆向东北部陆架方向上水体混合的水平涡动扩散系数为1.9×108 m2/d。结合海盆-陆架界面营养盐的水平浓度梯度,估算得硝酸盐、活性磷酸盐和活性硅酸盐由白令海中心海盆向东北部陆架区的水平输送通量,该通量对白令海东北部陆架区新生产力的贡献很小,其他途径输送的营养盐更为重要。 相似文献
9.
利用调查数据及遥感数据揭示了2013年南沙群岛海域温跃层的季节变化特征,温跃层上界深度平均值春、夏、冬季基本一致,介于45~47 m之间,秋季最大,达60 m;温跃层厚度平均值夏、秋、冬季基本一致,介于85~87 m之间,春季相对较小,为78 m。温跃层强度平均值春、夏、秋、冬季几乎一致,介于0.13~0.15℃/m之间。调查海域温跃层上界深度季节变化的形成机理为:春季西深东浅的原因是西部受净热通量较小、大风速、负的风应力旋度以及中南半岛东部外海的中尺度暖涡和反气旋环流共同作用,东部近岸海域净热通量高值、风速相对较小及风应力旋度引起的Ekman抽吸效应共同控制;夏季深度分布较均匀的原因是10°N以北风致涡动混合强但受Ekman抽吸影响,10°N以南风致涡动混合弱但风应力旋度为负值;秋季深度较其他季节平均加深15 m的原因是南沙群岛海域被暖涡占据,暖涡引起的反气旋式环流使得温跃层上界深度被海水辐聚下压;冬季正的风应力旋度产生的Ekman抽吸和冷涡引起的气旋式环流共同作用,使得温跃层上界深度较秋季平均抬升15 m。 相似文献
10.
大亚湾温跃层形成及其对有关环境要素的影响 总被引：4，自引：0，他引：4
温跃层是海洋环境中的一种重要物理现象,对海洋的环境生态系统有着重要的影响。大亚湾温跃层是受粤东上升流和夏季表层海水升温双重作用而形成的。通过对大亚湾海域水温、盐度、溶解氧等众多环境要素的长期调查取样分析显示,该海域温跃层是季节性温跃层,一般发生在每年的5—10月份,6月下旬到9月中旬分层现象比较显著,盐跃层和氧跃层会相伴发生。受核电站热排水的影响,湾西侧尤其是核电站前海域的温跃层较其它区域明显和持久。数据显示在温跃层发生期内,由于海水的分层效应,温度、盐度、pH值、DO、BOD5和COD、营养盐及叶绿素等都受到不同程度的影响,形成明显的表底层差异或层次梯度。 相似文献
11.
东海沿岸海区垂直环流及其温盐结构动力过程研究Ⅱ．温盐结构 总被引：2，自引：0，他引：2
对于本研究采用的动力学模型及其垂直环流的模拟结果已在第Ⅰ部分论述。作者将对与垂直环流对应的温、盐结构进行分析。温度和盐度模拟结果表明：冬季东海沿岸海区的温、盐分布均为近岸低、外海高;近岸温、盐呈垂直均匀分布,在外海出现分层,其温度为表层高、底层低,而盐度却为表层和底层高,中层偏低,长江口以南的近表层以下形成自近岸伸向外海的弱低盐水舌;长江冲淡水区及长江口以北和其以南外海的近表层有温、盐跃层生成,深底层温、盐呈均匀分布,且保持低温高盐特征;随着海区自北往南纬度的降低,岸坡和水深的增大及沿岸下降流的增强,温度和盐度自近岸至外海的垂直均匀分布跨度逐渐变窄;外海近表层的温、盐跃层强度自北至长江口逐渐增强,而自长江口至南逐渐减弱,其位置自北往南逐渐上移;冬季沿岸下降流使长江冲淡水区的盐跃层变厚。夏季海区的温度分布为近岸和外海高,近岸稍远出现冷水涌升,垂向上呈现显著分层,盐度分布为近岸低、外海高;长江冲淡水区及杭州湾以南外海的次表层存在温、盐跃层,其跃层以上出现混合层,且保持高温低盐特征,跃层以下温、盐大致呈均匀分布,并保持低温高盐特征;随着海区自南往北纬度的增高、岸坡和水深的减小及沿岸上升流自南至长江口和自长江口至北的增强和继而减弱,长江冲淡水区的温、盐跃层强度自南至长江口逐渐增强,而自长江口至北逐渐减弱,外海次表层的温、盐跃层强度却自南至长江口逐渐减弱,自长江口至北又逐渐增强,其温、盐跃层的位置自南往北逐渐上移;夏季沿岸上升流使长江冲淡水区的盐跃层变薄。 相似文献
12.
沿岸海区冬季垂直环流及其温盐结构的数值研究──Ⅱ.温盐结构 总被引：1，自引：1，他引：0
冬季沿岸海区温度和盐度的数值计算结果表明：温度在近岸近表层大致呈垂直均匀分布,外海近表层形成较强的温跃层,近岸至外海的下层保持冷水特征。表层和底层盐度高,中层盐度低,在中层形成自近岸伸向外海且盐度逐渐由低变高的低盐水舌,河口冲淡水区形成较强的盐跃层。随着自南往北海区水深的逐渐变浅、岸界坡度的由大变小和沿岸下降流的由强变弱,近岸温度和盐度的垂直分布越来越均匀,外海近表层的温跃层强度越来越弱。盐度自南至河口区逐渐由高变低,而自河口区至北逐渐由低变高。沿岸下降流使河流冲淡水区的益跃层变厚。 相似文献
13.
A three-dimensional numerical model is developed and used to study the coastal upwelling processes and corresponding seasonal changes in the sea level along the west coast of India. The upwelling and associated sea level variations are seen as a response of coastal ocean to pure wind stress forcing. The model is designed to represent coastal ocean physics by resolving surface and bottom Ekman layers as realistically as possible. The prognostic variables are the three components of the velocity field, temperature, salinity and turbulent energy. The governing equations together with their boundary conditions are solved by finite-difference techniques. Experiments are performed to investigate sea level fluctuations associated with the thermal response and alongshore currents of the coastal waters. The model is forced with mean monthly wind stress forcing of January, May, July and September representing northeast monsoon and different phases of the southwest monsoon. It is known from the observational study that the upwelling process reaches to the surface waters by May along the coastal waters of the extreme southwest peninsular region. The process is more intense in July compared to May and September and its strength decreases from south to north. However, during the northeast monsoon season, which is represented by January wind stress forcing in the model, downwelling is simulated along the coast. The model simulations of the coastal response are compared with the observations and are found to be in good agreement. The maximum computed vertical velocity of about 2.0 ×10 -3 cm s -1 is predicted in July in the southern region off the coast. 相似文献
14.
A three-dimensional numerical model is developed and used to study the coastal upwelling processes and corresponding seasonal changes in the sea level along the west coast of India. The upwelling and associated sea level variations are seen as a response of coastal ocean to pure wind stress forcing. The model is designed to represent coastal ocean physics by resolving surface and bottom Ekman layers as realistically as possible. The prognostic variables are the three components of the velocity field, temperature, salinity and turbulent energy. The governing equations together with their boundary conditions are solved by finite-difference techniques. Experiments are performed to investigate sea level fluctuations associated with the thermal response and alongshore currents of the coastal waters. The model is forced with mean monthly wind stress forcing of January, May, July and September representing northeast monsoon and different phases of the southwest monsoon. It is known from the observational study that the upwelling process reaches to the surface waters by May along the coastal waters of the extreme southwest peninsular region. The process is more intense in July compared to May and September and its strength decreases from south to north. However, during the northeast monsoon season, which is represented by January wind stress forcing in the model, downwelling is simulated along the coast. The model simulations of the coastal response are compared with the observations and are found to be in good agreement. The maximum computed vertical velocity of about 2.0 2 10 -3 cm s -1 is predicted in July in the southern region off the coast. 相似文献
15.
中沙群岛主要由中沙大环礁和黄岩岛组成,其温盐分布对于本区渔业生产、航海保障和水下通讯等具有重要意义。尤其是春夏之交的季节转换时期,该海域水温和盐度及其相应的跃层特性存在显著的季节变化,掌握其季节变化特征具有重要现实意义。本文基于2019年5月（南海春夏季风转换期）中沙大环礁、黄岩岛和2020年6月（夏季风爆发期）中沙大环礁海域大面站调查数据分析,发现中沙大环礁海域水温和盐度分布特征在夏季风爆发前后具有显著的差异性,2个航次的温跃层分布也呈现出较大不同,2019年5月黄岩岛海域温盐中上层分布与中沙大环礁相似,但底层有所差异,跃层深度也较大。2020年6月中沙大环礁内水体升温较快,各层水温均高于2019年5月,其中以底层水体升温最为显著;2019年5月中沙大环礁内水温水平梯度较大,且随着水深加大水平梯度也越大,2020年6日水平温度梯度逐渐减小。2个航次的盐度分布与水温分布较为相似。结合调查时段的海表热通量变化和卫星高度计资料分析认为,2019年5月中沙大环礁西南部海洋吸热高于东北部,故表层水温西南高东北低;2020年6月至7月环礁西南部海洋吸热低于东北部,故表层水温西南低东北高。由于中尺度涡的作用,中沙大环礁区域局部产生低温高盐或高温低盐水,并导致2020年6月中沙大环礁大部分海域的温跃层加深。 相似文献
16.
To address the mechanisms controlling halocline variability in the Beaufort Sea, the relationship between halocline shoaling/deepening and surface wind fields on seasonal to decadal timescales was investigated in a numerical experiment. Results from a pan-Arctic coupled sea ice-ocean model demonstrate reasonable performances for interannual and decadal variations in summer sea ice extent in the entire Arctic and in freshwater content in the Canada Basin. Shelf-basin interaction associated with Pacific summer and winter transport depends on basin-scale wind patterns and can have a significant influence on halocline variability in the southern Beaufort Sea. The eastward transport of fresh Pacific summer water along the northern Alaskan coast and Ekman downwelling north of the shelf break are commonly enhanced by cyclonic wind in the Canada Basin. On the other hand, basin-wide anti-cyclonic wind induces Ekman upwelling and blocks the eastward current in the Beaufort shelf-break region. Halocline shoaling/deepening due to shelf-water transport and surface Ekman forcing consequently occur in the same direction. North of the Barrow Canyon mouth, the springtime down-canyon transport of Pacific winter water, which forms by sea ice production in the Alaskan coastal polynya, thickens the halocline layer. The model result indicates that the penetration of Pacific winter water prevents the local upwelling of underlying basin water to the surface layer, especially in basin-scale anti-cyclonic wind periods. 相似文献
17.
Tomoharu Senjyu Hidekazu Yasuda Shigehiko Sugihara Masato Kamizono 《Journal of Oceanography》2001,57(1):15-27
A hydrographic survey and a 25-hour stationary observation were carried out in the western part of Suo-Nada in the summer of 1998 to elucidate the formation mechanism of the oxygen-deficient water mass. A steep thermocline and halocline separated the upper layer water from the bottom water over the observational area except for near the Kanmon Strait. The bottom water, in comparison with the upper layer water, indicated lower temperature, higher salinity, lower dissolved oxygen, higher turbidity, and higher chlorophyll a. Turbidity in the upper layer water changed with semi-diurnal period while the bottom water turbidity showed a quarter-diurnal variation, though the M2 tidal current prevailed in both waters. From the turbidity distribution and the current variation, it is revealed that the turbidity in the upper layer water is controlled by the advection due to the M2 tidal current. On the other hand, the quarter-diurnal variation in the bottom water turbidity is caused by the resuspension of bottom sediments due to the M2 tidal current. The steep thermocline and halocline were maintained throughout the observation period in spite of the rather strong tidal currents. This implies an active intrusion of the low temperature and high salinity water from the east to the bottom of Suo-Nada. Based on the observational results, a hypothesis on the oxygen-deficient water mass formation was proposed; the periodical turbidity variation in the bottom water quickly modifies the oxygen-rich water in the east to the oxygen-deficient bottom water in Suo-Nada in a course of circulation. 相似文献
18.
Resuspension, transport, and deposition of sediments over the continental shelf and slope are complex processes and there is still a need to understand the underlying spatial and temporal dynamical scales. As a step towards this goal, a two-dimensional slice model (zero gradients in the alongshore direction) based on the primitive flow equations and a range of sediment classes has been developed. The circulation is forced from rest by upwelling or downwelling winds, which are spatially uniform. Results are presented for a range of wind speeds and sediment settling speeds. Upwelling flows carry fine sediments (low settling speeds) far offshore within the surface Ekman layer, and significant deposition eventually occurs beyond the shelf break. However, coarser sediments quickly settle out of the deeper onshore component of the circulation, which can lead to accumulation of bottom sediments within the coastal zone. Downwelling flows are more effective at transporting coarse sediments off the shelf. However, strong vertical mixing at the shelf break ensures that some material is also carried into the surface Ekman layer and returned onshore. The concentrations and settling fluxes of coarse sediments decrease offshore and increase with depth under both upwelling and downwelling conditions, consistent with trends observed in sediment trap data. However, finer sediments decrease with depth (upwelling) or reach a maximum around the depth of the shelf break (downwelling). It is shown that under uniform wind conditions, suspended sediment concentrations and settling fluxes decay offshore over a length scale of order τs/ρf|ws|, where τs is the wind stress, ρ the water density, f the Coriolis parameter, and ws is the sediment settling velocity. This scaling applies to both upwelling and downwelling conditions, provided offshore transport is dominated by wind-driven advection, rather than horizontal diffusion. 相似文献
19.
ＯｎｔｈｅｏｒｉｇｉｎｏｆｔｈｅＴｓｕｓｈｉｍａＷａｒｍＣｕｒｒｅｎｔＷａｔｅｒ￥ＴａｎｇＹｕｘｉａｎｇａｎｄＨｅｕｎｇ－ＪａｅＬｉｅ（ＦｉｒｓｔｉｎｓｔｉｔｕｔｅＯｆＯｃｅａｎｏｇｒａｐｈｙ，ＳｔａｔｅＯｃｅａｎｉｃＡｄｍｉｎｉｓｔｒａｔｉｏｎ，Ｑ... 相似文献
20.
Laboratory experiments on the dynamics of a downwelling coastal current over a sloping bottom were conducted in a tank on a rotating platform. The current was generated by a source of stable water flow of the same density (barotropic case) or of lesser density (baroclinic case) compared with the surrounding water in the tank. It was found that even in the case of the baroclinic current, a less dense water downflow in the bottom Ekman layer was formed under certain conditions. At some moment, this downflow undergoes convective instability. Taking into account the results of the experiment, the parameters of the bottom Ekman layer on the continental shelf/slope of the Black Sea were preliminarily estimated and the possible sinking depth of less dense water was calculated. 相似文献