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1.
利用加拿大环极冰间水道系统研究项目,作者对2007年11月24日至2008年1月26日北极群岛阿蒙森湾海域秋冬季节一年冰的物理和光学性质进行了观测研究。结果显示,观测期间的海冰厚度整体在27~108 cm范围内变化,积雪厚度仅为0~6 cm。海冰温度、盐度和密度在冰内的分布特征为:海冰表层最低温度为–22.4℃,底层最高温度为–2.2℃,冰内温度随深度单调增大;盐度变化范围为3.30~11.70,冰内盐度剖面呈现“C”形,即表层和底层盐度较大,而中间层盐度较小;海冰的平均密度略大,为(0.91±0.03)g/cm3。通过观测人造光源在海冰中的透射辐射谱分布,发现一年冰的光谱透射辐射在490 nm和589 nm处呈明显的双峰结构,但随着海冰厚度的增加,双峰结构逐渐减弱,体现了海冰对于不同谱段辐射能衰减作用的差异。在可见光范围内,裸冰和雪覆冰的吸收率最小值出现在490 nm,在443~490 nm范围内二者的吸收率随波长增大而降低,在490~683 nm范围内二者的吸收率随波长增大而升高,但雪覆冰的吸收率在可见光范围内基本保持不变,体现了雪覆冰吸收率的光谱独立性。一年冰的谱衰减系数随波长呈“U”字形分布,紫光和红光谱段的衰减系数较大,中间谱段的衰减系数较小,589 nm波长的衰减系数最小,为1.7 m–1。将谱衰减系数在可见光范围内积分,得到一年冰的积分漫射衰减系数约为2.3 m–1,略高于多年浮冰的漫射衰减系数1.5 m–1。阿蒙森湾一年冰与加拿大海盆北部多年浮冰辐射光学性质的差异,主要源于陆源物质输入引起的海冰内含物组分的改变,而不同组分对光谱的吸收和散射性质不同,进一步导致了光学性质的整体变化。  相似文献   

2.
本文利用2010年6-7月的实测温盐、水位、海流等资料,结合风场数据,讨论了在台风影响较小的情况下,粤东及闽南近岸上升流对局地风场变化的响应特征,主要结论如下:(1)谱分析结果显示,沿岸风、水位、海流、近底层水温均具有3.5~4.0 d、5.0~5.5 d、8.3~9.0 d的波动周期,沿岸风的变化引起上升流强度在3~9 d周期上的波动;(2)上升流对局地风场变化的响应过程如下:利于上升流产生的局地风场发生变化时,沿岸风作用下产生的Ekman输运促使的上升流区水位的下降幅度发生改变,随即向岸方向的压强梯度力也发生变化,进而导致沿岸流及近底层向岸流的增强或减弱,而近底层向岸流强度的改变又会引起近底层水温的变化;(3)相关分析及交叉谱分析的结果表明,沿岸风的变化将在3 d以内影响上升流区近底层水温。以34 m向岸流代表近底层向岸流,则“沿岸风-水位-近底层向岸流-近底层水温”这一过程的响应时间依次为24 h、7 h、27 h左右。  相似文献   

3.
In order to study the mechanism of flow-sediment movement, it is essential to obtain measured data of water hydrodynamic and sediment concentration process with high spatial and temporal resolution in the bottom boundary layer (BBL). Field observations were carried out in the northwest Caofeidian sea area in the Bohai Bay. Near 2 m isobath (under the lowest tidal level), a tripod system was installed with AWAC (Acoustic Wave And Current), ADCP (Acoustic Doppler Current Profilers), OBS-3A (Optical Backscatter Point Sensor), ADV (Acoustic Doppler Velocimeters), etc. The accurate measurement of the bottom boundary layer during a single tidal period was carried out, together with a long-term sediment concentration measurement under different hydrological conditions. All the measured data were used to analyze the characteristics of wave-current-sediment movement and the BBL. Analysis was performed on flow structure, shear stress, roughness, eddy viscosity and other parameters of the BBL. Two major findings were made. Firstly, from the measured data, the three-layer distribution model of the velocity profiles and eddy viscosities in the wave-current BBL are proposed in the observed sea area; secondly, the sediment movement is related closely to wind-waves in the muddy coast area where sediment is clayey silt: 1) The observed suspended sediment concentration under light wind conditions is very low, with the peak value generally smaller than 0.1 kg/m3 and the average value being 0.03 kg/m3; 2) The sediment concentration increases continuously under the gales over 6-7 in Beaufort scale, under a sustained wind action. The measured peak sediment concentration at 0.4 m above the seabed is 0.15-0.32 kg/m3, and the average sediment concentration during wind-wave action is 0.08-0.18 kg/m3, which is about 3-6 times the value under light wind conditions. The critical wave height signaling remarkable changes of sediment concentration is 0.5 m. The results show that the suspended load sediment concentration is mainly influenced by wave-induced sediment suspension.  相似文献   

4.
We discuss the current state of the problem of experimental investigation of the bottom boundary layer of the Black Sea and present the data on a new measuring complex (designed and constructed at the Marine Hydrophysical Institute and called the OLT-D profilometer of the bottom layer) together with some results of its application. On the basis of the analysis of the data on the distributions of geothermal fluxes and parameters of the bottom boundary layer in the deep-water part of the sea, we deduce and justify the relations for the evaluation of the critical thickness of the bottom boundary layer as a function of the intensities of geothermal fluxes. It is shown that the numerical results are in good agreement with the data of direct measurements of the thickness of the bottom boundary layer. Translated by Peter V. Malyshev and Dmitry V. Malyshev  相似文献   

5.
2008年夏季中国第3次北极科学考察期间,利用锚碇潜标对北冰洋楚科奇陆架海域进行了为期33 d的海流剖面、近底层温度与盐度连续观测。观测数据显示楚科奇陆架海域近底层海水温度出现了两次较大幅度的快速升降现象。结合此次科学考察R断面温盐深仪(CTD)观测资料、以及卫星遥感海表温度(SST)和海表风场等资料,综合分析表明:观测到的这种快速升、降温现象不仅发生在近底层;这种快速升、降温现象应该是由海水温度锋面在夏季整体缓慢北移的同时存在短暂南北摆动所导致;温度锋面的季节性北移属于北极气候特征,而温度锋面短暂的南北摆动则与短期天气过程有关。  相似文献   

6.
根据2017年8月北极斯瓦尔巴德地区王湾海域微小型浮游动物调查资料,研究了该区域微小型浮游动物的种类组成及群落特征。结果表明:王湾海域在水深10~50 m内存在一个明显温跃层,该温跃层内水温高于其他水层;不同水层盐度变化表现为从表层到底层逐渐增高的趋势,70 m以深海域的盐度基本保持稳定;微小型浮游动物包括无壳纤毛虫(Aloricate Ciliates)、砂壳纤毛虫(Tintinnida Ciliates)和甲壳类无节幼体(Crustacea Nauplii)3个类别,其中砂壳纤毛虫10种。甲壳类无节幼体和无壳纤毛虫均为微小型浮游动物的优势类群,砂壳纤毛虫中的钝笛杯虫(Ptychocylis obtusa)、挪威棘口虫(Acanthostomella norvegica)、网纹虫(Favella sp.)、百乐拟铃虫(Tintinnopsis beroidea)和白领细壳虫(Stenosemella nivalis)均为优势种类;微小型浮游动物主要集中分布在水体的中上层水域10~30 m,该海域温跃层内微小型浮游动物种类和丰度最为丰富,30 m以浅海域微小型浮游动物丰度约占整个水体微小型浮游动物丰度的54.8%,而100 m以浅海域这一比例高达93%以上,其中10 m层为最多(均值为343.3 ind./L),底层为最少(均值为50.9 ind./L);整个调查区域微小型浮游动物的多样性指数均大于2.5,丰富度指数均大于1.2,均匀度均大于0.7,不同站位多样性指数、均匀度指数和丰富度指数波动范围不大,站位间差异不大。  相似文献   

7.
In order to study the mechanism of flow-sediment movement, it is essential to obtain measured data of water hydrodynamic and sediment concentration process with high spatial and temporal resolution in the bottom boundary layer (BBL). Field observations were carried out in the northwest Caofeidian sea area in the Bohai Bay. Near 2 m isobath (under the lowest tidal level), a tripod system was installed with AWAC (Acoustic Wave And Current), ADCP (Acoustic Doppler Current Profilers), OBS-3A (Optical Backscatter Point Sensor), ADV (Acoustic Doppler Velocimeters), etc. The accurate measurement of the bottom boundary layer during a single tidal period was carried out, together with a long-term sediment concentration measurement under different hydrological conditions. All the measured data were used to analyze the characteristics of wave-current-sediment movement and the BBL. Analysis was performed on flow structure, shear stress, roughness, eddy viscosity and other parameters of the BBL. Two major findings were made. Firstly, from the measured data, the three-layer distribution model of the velocity profiles and eddy viscosities in the wave-current BBL are proposed in the observed sea area; secondly, the sediment movement is related closely to wind-waves in the muddy coast area where sediment is clayey silt: 1) The observed suspended sediment concentration under light wind conditions is very low, with the peak value generally smaller than 0.1 kg/m^3 and the average value being 0.03 kg/m^3; 2) The sediment concentration increases continuously under the gales over 6-7 in Beaufort scale, under a sustained wind action. The measured peak sediment concentration at 0.4 m above the seabed is 0.15-0.32 kg/m^3, and the average sediment concentration during wind-wave action is 0.08-0.18 kg/m^3, which is about 3-6 times the value under light wind conditions. The critical wave height signaling remarkable changes of sediment concentration is 0.5 m. The results show that the suspended load sediment concentration is mainly influenced by wave-induced sediment suspension.  相似文献   

8.
严律  朱首贤 《海洋通报》2021,40(2):133-141
利用2018年夏季在西南黄海的现场调查资料,分析了海温、盐度和溶解氧(dissoloved oxygen,DO)分布特征.海区西侧的江苏沿海有明显的冷水带,冷水带对应表层较高的DO浓度.在海区南侧的长江口附近,盐度由南向北升高,上部海水DO浓度高,下部海水DO浓度低.综合现场观测数据、CCMP (Cross Calib...  相似文献   

9.
胶州湾水域有机农药六六六的污染源及分布   总被引:1,自引:0,他引:1  
根据1982年的胶州湾水域调查资料,分析了有机农药HGH在胶州湾水域的分布、污染源和季节变化。结果表明,胶州湾水域在4月、6月、7月和10月,HCH的污染较轻。在胶州湾水域,4月、6月和7月,HCH的含量变化由近岸向湾中心有梯度形成:从大到小呈下降趋势,10月HCH的梯度变化刚好相反。表层HCH的水平分布状况与底层HCH的水平分布状况一致。HCH含量变化展示HCH通过河流输入近岸水域要比通过地表径流直接输入近岸水域的质量浓度要高。因此,胶州湾水域HCH含量变化证明了HCH的陆地迁移过程。这表明在夏季,输入的胶州湾水域HCH的含量与春季相比,相对较高;HCH表、底层含量变化在时间尺度和空间尺度上证明了HCH的水域迁移过程。这揭示了HCH的表层含量高,通过沉降,HCH的底层含量就高。根据表、底层的HCH含量变化,提出了HCH的水体效应、稀释效应和累积效应,并用模型框图,表明了HCH穿过水体的含量变化,定量描述水体对HCH的作用。  相似文献   

10.
海冰表面和底层形态的特征相关性分析对海冰分类、气候研究以及海冰厚度估计等方面具有重要作用.目前,海冰底层形态的研究较少,且缺乏海冰表面和底层形态的相关性研究.针对这一问题,本文利用加拿大渔业和海洋局提供的积雪表面粗糙度高度(定义为海冰或积雪表面相对于周围平整表面的高度)、海冰底层轮廓、积雪深度以及海冰厚度数据,采用均方...  相似文献   

11.
The relationship between the vertical profile of current on the bottom slope southeast of Okinawa Island and the offshore meso-scale eddy propagated from the east was examined by combined use of the data obtained by a moored upward-looking ADCP (Acoustic Doppler Current Profiler), PIES (Inverted Echo Sounder with Pressure gauge), hydrographic surveys and satellite altimetry during a period from November 2000 to August 2001. The variability of current component parallel to the isobath in the layer over 600 m is found to be markedly different from that in the layer below 600 m. The current variability in the upper and the lower layer can be well explained by the first and second modes of the EOF (Empirical Orthogonal Function) decomposition. The PIES and the sea surface height anomaly data suggest that the first mode represents the surface-trapped current associated with the approach of the offshore meso-scale eddy from the east, whereas the second mode has a bottom-intensified structure. The second mode velocity tends to delay to the first mode. The hydrographic data derived from CTD (Conductivity-Temperature-Depth meter) and PIES data along the line across the isobath suggest that the second mode component is generated by the interaction between the meso-scale eddy and the bottom topography.  相似文献   

12.
基于长期观测的辽东湾口东部海域水动力特征研究   总被引:1,自引:0,他引:1  
辽东湾口东部海域是辽东湾与渤海中部进行物质和能量交换的主要通道之一。本文利用坐底式海床基平台获取的近8个月的水动力连续观测资料,通过谱分析和调和分析方法对该海域的潮汐、潮流特征进行分析,并讨论了余流及底层温度的季节变化规律。研究结果表明:该海域潮汐属于不规则半日潮,平均潮差为0.95 m,最大可能潮差为2.27 m。潮流属于不规则半日潮流,M2分潮流为其优势分潮流。主要分潮流运动形式为往复流,最大流速方向为西南-东北向。余流的季节性特征较为明显:秋季,余流流速在中层达到最大,流向以西南向为主;冬季,余流流速垂向变化较小,并呈西南偏西向流动;春季,流速随深度增加而减小,流向从表层至底层呈现逆时针旋转的特征。受底层潮流、水平温度梯度及海面温度日变化的影响,底层温度表现出短期的高频变化特征:秋季,短期振荡以半日周期信号为主;冬季,全日周期信号较为显著;春季,短期振荡的现象较弱。  相似文献   

13.
The physical structures of snow and sea ice in the Arctic section of 150°-180°W were observed on the basis of snow-pit, ice-core, and drill-hole measurements from late July to late August 2010. Almost all the investigated floes were first-year ice, except for one located north of Alaska, which was probably multi-year ice transported from north of the Canadian Arctic Archipelago during early summer. The snow covers over all the investigated floes were in the melting phase, with temperatures approaching 0℃ and densities of 295-398 kg/m3 . The snow covers can be divided into two to five layers of different textures, with most cases having a top layer of fresh snow, a round-grain layer in the middle, and slush and/or thin icing layers at the bottom. The first-year sea ice contained about 7%-17% granular ice at the top. There was no granular ice in the lower layers. The interior melting and desalination of sea ice introduced strong stratifications of temperature, salinity, density, and gas and brine volume fractions. The sea ice temperature exhibited linear cooling with depth, while the salinity and the density increased linearly with normalized depth from 0.2 to 0.9 and from 0 to 0.65, respectively. The top layer, especially the freeboard layer, had the lowest salinity and density, and consequently the largest gas content and the smallest brine content. Both the salinity and density in the ice basal layer were highly scattered due to large differences in ice porosity among the samples. The bulk average sea ice temperature, salinity, density, and gas and brine volume fractions were-0.8℃, 1.8, 837 kg/m3 , 9.3% and 10.4%, respectively. The snow cover, sea ice bottom, and sea ice interior show evidences of melting during mid-August in the investigated floe located at about 87°N, 175°W.  相似文献   

14.
基于西北太平洋Argo数据资料,利用参数化方法,从Argo温盐剖面数据中提取出一系列特征动力参数,定量分析黑潮延伸体海域水体的三维热结构的时-空变化特征、季节变化特征及其与地形和环流的关系.结果表明:黑潮延伸体海域水体的海表面温度存在着明显的冬春弱,夏秋强的季节变化特征,冬季平均海表面温度为15℃,夏季则达到了27℃;...  相似文献   

15.
We present a semiempirical model of the bottom turbulent boundary layer aimed at the application as one of the components of the procedure of evaluation of the vertical distribution of the concentration of suspensions in the coastal region of the sea. The model is based on data of laboratory experiments and is suitable for the sand bottom in a broad range of amplitudes of the bottom velocities of the wave origin.  相似文献   

16.
林龙  赵进平 《海洋学报》2018,40(11):23-32
雪热传导系数是海冰质量平衡过程中的重要物理参数,决定了穿透海冰的热传导通量。北冰洋海冰质量平衡浮标观测获得多年冰上冬季温度链剖面可以明显地区分冰雪界面。本文考虑到冰雪界面处温度随时间变化,再根据冰雪界面热传导通量连续假定,提出了新的雪热传导系数计算方法。受不同环境因素影响,多年冰上各个浮标的雪热传导系数在0.23~0.41 W/(m·K)之间,均值为(0.32±0.08) W/(m·K)。北冰洋多年冰上冬季穿过海冰的热传导通量最大发生在11月至翌年3月,约14~16 W/m2。结冰季节,来自海冰自身降温的热量对穿过海冰向大气传输的热量贡献逐月减少,从9月100%减小到12月的35%,翌年的1月至3月稳定在10%左右。夏季,短波辐射通能量通过热传导自上而下加热海冰,海冰上层温度高于下层,热量传播方向与冬季反向,往海冰内部传递。直到9月短波辐射完全消失,气温下降,热量再次转变为自下往上传递。从冰底热传导来看,夏季出现海冰向冰水界面传递热量现象。由于雪较好的绝热性,冰上覆雪极大地削弱了海冰上层热传导通量,从而减缓了秋冬季节的结冰速度。尽管受雪厚影响,多年冰上层热传导通量与气温依旧具有很好的线性关系,气温每降低1℃,热传导通量增加约0.59 W/m2。  相似文献   

17.
We performed a search for local coastal submarine springs of fresh water in the region from Cape Feolent to Cape Sarych (down to an isobath of 40m). Stable submarine springs of brackish water with the minimum salinity of 5.5‰ and the minimum total output of 30,000 m3/day were discovered only near the west wall of Cape Aiya. It is shown that brackish waters discharging from these springs spread over the sea surface in the form of a thin layer (up to 1 m in thickness) characterized by lower salinity, higher transparency, and an elevated content of silicic acid. We make a conjecture that the appearance of 2–3-m-thick layers of water with higher transparency and lower salinity at depths of 5–8 m is explained by the discharge of unknown bottom springs of underground fresh water. Translated by Peter V. Malyshev and Dmitry V. Malyshev  相似文献   

18.
In this work, the vertical structure and variability along the western boundary of the Philippines are investigated using direct observations from acoustic Doppler current profiler (ADCP), Doppler volume sampler (DVS) and Aanderaa Seaguard instruments, which are mounted on a subsurface mooring deployed at 8°N, 127°3′E. In climatology, the southward Mindanao Current (MC) and northward Mindanao Undercurrent (MUC) play a dominant role in the upper layer. The mean currents at 1200 and 3500 m flow northward, whereas those at 2500 and 5600 m flow equatorward. The power spectral density (PSD) shows that an intraseasonal signal of 60–80 days is common from the sea surface to the bottom. The semiannual signals are strongest in the MUC layer, and the amplitude then decreases with depth to 3500 m. The seasonal variability at 2500 and 5600 m is similar between the two depths, suggesting a southward current in winter and northward flow in autumn. The current at 3500 m exhibits a northward direction in spring and southward flow in winter. In addition, the linear correlations between mooring data and altimetry products indicate that the variations in surface meridional currents along the western boundary of the Pacific Ocean can reach the bottom via low-frequency processes. The vertical-mode decomposition for observations indicates that the first four modes can effectively capture the original data. The relative contributions of different modes exhibit seasonal variability. The first baroclinic mode plays a dominant role in spring and autumn. In winter and summer, its contribution decreases and becomes comparable to that of the other modes.  相似文献   

19.
南海北部陆架陆坡区海流观测研究   总被引:3,自引:0,他引:3  
针对2006-2009年期间,南海北部陆架陆坡区3个站ADCP海流连续观测资料,采用功率谱分析、潮流调和分析方法,重点分析了陆架陆坡区100 m,200 m和1 200 m水深海域海流的垂向结构,探讨了环流的季节变化和空间分布特征,特别讨论了南海暖流和北陆坡流的时空变化特征。结果表明,陆架陆坡区潮流类型属于不规则日潮,深水站点中层表现为正规全日潮类型,垂向为"三层结构",甚至更加复杂。O1,K1,M2,S2等分潮总体上为顺时针旋转,在深水站点,基本表现为西北-东南走向的往复流形态。从能量角度看,表层和底层海流中,潮流所占份额较大,分别占30%~40%和40%~50%,中层较小,约为20%。对东沙群岛西南陆架陆坡区环流,观测计算结果证实了西向强流的存在,且垂向结构具有显著的季节变化,在200 m水深处没有明显的南海暖流,只是10~30 m以上层次存在逆风海流。海南岛以东海域连续15个月表层环流的结果表明,冬季明显受到南海暖流的影响,存在东北向的逆风海流,夏秋季的环流表现为西南向,流速较强,夏季也存在逆风情况,造成上述情形的原因可能是该地南海暖流的流轴具有季节性变化——冬季偏南,夏季偏北。  相似文献   

20.
Current meter data from various depths near the sea bottom collected for 31 days at time intervals of 10 minutes using a subsurface buoy system at a depth at 38 m on the continental shelf off Akita, Japan have been analyzed. The results show the existence of a stationary Ekman layer. The typical range of the characteristic parameters are estimated as follows; friction velocity: 0.38 cm s–1; Ekman layer thickness: 16 m; logarithmic layer thickness: 4 m–6 m; constant flux layer thickness: 0.4–0.6 m; Ekman veering: 28.7°; drag coefficient: 0.24×10–2–0.53×10–2. Veering was also observed in the logarithmic layer.  相似文献   

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