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1.
浙南近岸海流季节变化特征   总被引:7,自引:1,他引:6  
为了揭示浙南海流特征及其季节和垂向变化规律,于2006—2007年在浙南岸外一固定点(平均水深约32m)利用ADP潜标进行了春、夏、秋、冬季4次多个潮周期分层海流流速流向观测。结果表明:(1)测点最大流速为148.9cm/s,相应流向为75°,出现在春季表层大潮落潮阶段;垂向平均最大流速为106.2cm/s,平均流向为81°,出现在夏季大潮落潮落急阶段。(2)剖面各层流速垂向差异明显,表层流速(28m层以上)受海况影响明显,秋季平均流速最大(65.4cm/s),冬季最小(42.8cm/s),20~28m层冬季最强,春季最弱,20m层以下夏季最强,秋季最弱(仅小潮);垂线平均流速夏季最强(46.5cm/s),春季最小(33.7cm/s)。(3)夏季海流基本上为(偏)北向流;秋、冬则基本上为(偏)南向流;春季具往复流特点,但以北向流为主。(4)垂向上夏季和春季流向较一致,冬季和秋季流向分异明显(20m和10m层)。(5)垂线平均余流为12.8~29.8cm/s,夏季最强春季最弱;夏季和春季各层余流均为东北向,冬季为西南向,而秋季11m层(包括11m层)以下为E-NEE向,11m层以上为西南向。结论:测点海流受到潮汐、季风和台湾暖流的共同制约。季风的影响夏、冬两季大于春、秋两季;季风的影响自表层向底层减弱(主要限于表层以下10m)。  相似文献   

2.
基于2012年9月—2013年12月中南半岛外海累计16个月的长时间序列潜标观测数据,结合AVISO海表面高度异常(sea level anomaly,SLA)数据,首次详细分析了中南半岛外海典型中尺度涡的运动规律和垂向特征及其对环境水文特征的影响,揭示了该海域深层海流的时间变化特征。在观测期间共捕捉到3次中尺度涡过程,中尺度涡对站位所在海域主温跃层深度变化的最大影响振幅可达50 m。研究发现:1)观测站位所在海域各深度的温度异常时间变化与站位SLA时间变化的相关性随深度增加逐渐减弱。2)上层和中层的海水流动受中尺度涡影响显著。1 500 m和2 000 m的深层环流主要表现为季节变化;在强中尺度涡暖涡经过期间,中尺度涡能影响到1 500 m的环流场,同时出现30 d周期震荡。2 000 m流场则不受中尺度涡影响。3)中南半岛以东南海1 500 m处深层海流月平均流速夏季大于冬季,月平均可达3.5 cm·s~(-1);2 000 m处深层海流最大流速出现在冬季,月平均可达2.6 cm·s~(-1)。深层海流受潮汐影响显著,潮汐作用主要影响深层海流东西向流速的变化。  相似文献   

3.
2002年春季吕宋海峡海流观测及其谱分析   总被引:1,自引:0,他引:1  
基于2002年春季航次在吕宋海峡海域锚碇测流站(20°49'57"N,120°48'12"E)200,500与800m锚碇测流水层观测流,进行的海流特征分析与最大熵方法谱分析,得到以下主要结果.(1)在200m处,观测期间海流平均速度为(47.4cm/s,346°),最大观测海流速度Vmax和最大日平均海流速度Vd,max分别为(103.8cm/s,10°)和(71.6cm/s,339°);在500m处,观测期间平均流速为(20.3cm/s,350°),最大观测海流速度Vmax和最大日平均海流速度Vd,max分别为(74.1cm/s,17°)和(39.1cm/s,317°).这些都表明黑潮在吕宋海峡锚碇测流站200和500m处向西北方向入侵南海.(2)在800m处,观测期间平均流速为(1.2cm/s,35°),最大观测海流速度Vmax和最大日平均海流速度Vd,max分别为(10.8cm/s,76°)和(4.7cm/s,46°).这些都表明,它们的流向皆为东北向.比较在每层实测流的结果,表明在800m层海流状况与200和500m层海流状况是不相同的,流速随深度变深明显减弱,流向向右偏转.(3)在观测期间200,500和800m处,日平均流速在4月皆比3月时要强.(4)在200~800m潮流随深度变深有所变化,除了在500m处f<0情况全日潮峰值高于半日潮峰值以及对于半日潮以逆时针方向为主以外,其余情况在200~800m水层半日潮峰值都要高于全日潮的峰值,并且皆以顺时针方向旋转为主.(5)在200~800m水层都存在15d以上或14d左右的周期振动,例如在逆时针方向分量谱(f>0)在200,500m处存在19d左右的周期振动;在800m处存在14d左右的周期振动(f<0).(6)在200~800m处都存在4~6d周期天气过程的振动和2~3d周期振动.还都存在34.5h左右惯性振动周期,它的振动方向为顺时针方向.(7)通过交叉谱的计算,揭示:1)200与500m层两组流速时间序列对于半日潮周期、全日潮周期、15d以上的周期振动、2~3d的周期振动等都有很好的相关性,且对15d以上的长周期振动几乎是同步的;2)500与800m层两组流速时间序列对于4~6d天气过程的周期振动与2~3d的周期振动等都有很好的相关性,但它们之间有相位差,有滞后或提前现象.  相似文献   

4.
宫古海峡通道海流的高分辨率数值模拟   总被引:1,自引:0,他引:1  
运用美国麻省理工大学MITgcm模式、模式嵌套技术和高分辨率网格(水平方向为1°/48×1°/48,垂向为22层),模拟了宫古海峡通道中的海流流动状况。流场不同分辨率的模拟结果表明,海底地形对宫古海峡通道中的海流流动影响显著;宫古海峡通道中的海流流动结构具有如下特征:垂向流动可分为3层,每层均存在流速核心;400 m以浅的上层海流从太平洋流入到东海,平均流速约为10 cm/s,流速核心位于160 m附近;400~1 000 m的中层海流从东海流出到太平洋,平均流速约为2 cm/s,流速核心位于650 m附近;1 000 m以下的深层海流从太平洋流入到东海,平均流速约为1 cm/s,流速核心位于1 200 m附近。宫古海峡通道中的海流流动具有较强的季节变化特征,秋末冬初流动较强,夏季流动较弱。  相似文献   

5.
本文使用吕宋海峡以东的潜标观测的长达1年的海流数据,重点对该海域海流的高频波动(潮流)的垂向分布及其时间变化特征进行了分析,结果表明:该海域次表层(100~160 m)的潮动能比中层(1 550 m)和深层(2 560 m)大1~2个数量级,近底层(4 040 m)的潮动能略大于中、深层;次表层为不正规半日潮流,中、深层为不正规全日潮流;各层次潮动能均在夏季(6?9月)和冬季(2?3月)增强,与M2分潮和K1分潮在夏季和冬季的增强相对应;各层次海流的高频波动以顺时针旋转为主,次表层海流近惯性周期接近当地理论惯性周期,中、深层略小于当地理论惯性周期。  相似文献   

6.
为了揭示长江口外海域海流的特征及其季节和垂向变化规律,于2006年8月1日-2007年7月31日在长江口外海域(平均水深约46.0m)利用大型浮标进行了1年的分层海流流速流向观测。结果表明:(1)该海域海流为顺时针方向的旋转流,在垂向上流向较一致,季节变化不显著。(2)长江口外海域水平流速总体较大,夏季表层最大流速为128.5cm/s,冬季最大表层流速为105.5cm/s;垂线平均流速相近(差异<8.0 cm/s),夏季流速最大为47.0cm/s,冬季为40.8cm/s。小潮的平均流速为26.5cm/s,大潮平均流速为小潮的2倍。(3)剖面各层流速垂向差异明显,最大流速出现在表层(春季和冬季)或次表层(夏季和秋季),最小流速均出现在底层;各层的最大平均流速为57.9cm/s,出现在夏季的18m层。(4)垂线平均余流为7.5~11.3 cm/s,春季最强冬季最弱;春季和冬季各层余流均为东向,夏季和秋季基本为东北向或北向。(5)观测海域海流受长江冲淡水、台湾暖流、季风、潮汐等动力作用的共同制约。  相似文献   

7.
本文利用高频地波雷达获得的江苏如东海域大范围长期海流观测资料对苏北辐射沙洲南部烂沙洋海域夏季表层海流特征进行了分析。分析结果表明:研究海域表层海流靠近近岸一侧为往复流,流向总体上呈西北-东南向,靠近外海一侧为旋转流;海域潮流动力较为强劲,夏季表层海流实测最大流速达1.47 m/s,涨潮平均流速介于0.44~0.55 m/s,落潮平均流速介于0.38~0.52 m/s,海域西北部区域涨落潮平均流速明显大于其他区域;表层潮流为正规半日潮流,M2分潮为最主要分潮,其潮流椭圆长轴范围为0.57~0.71 m/s,远大于其他分潮,其次为S2分潮;该海域夏季表层余流呈现近岸大离岸小的分布趋势,余流流向基本指向近岸方向,从离岸到近岸余流流向呈现逆时针偏转。  相似文献   

8.
洋浦港附近夏季潮余流特征分析   总被引:1,自引:1,他引:0  
通过设置在洋浦外面12m等深线处锚定浮标,在2006年7月进行1个月的表、中、底层海流连续观测,通过资料分析得出如下结论:受北部潮流无流点影响,涨落潮方向基本指向北-东北方向,实测流速最大也只有37cm/s;表、中、底层的余流流向基本一致,在18~22°之间变化;表层余流流速在3~17cm/s范围内变化,变化幅度较大,中层次之,底层最小;余流流速有2个近似半个月的变化周期,流速起伏与潮位高低有很好对应关系;潮汐余流是这个海域余流形成的主要机制,风对余流流速流向也有一定影响.  相似文献   

9.
基于高频地波雷达长周期适用性比测试验数据,主要从以下3个方面系统分析国产阵列式高频地波雷达矢量流控测效果:(1)时间有效采样率和覆盖率的空间分布;(2)与反演的流速匹配的现场观测深度;(3)不同区域的探测精度.长周期的海流验证表明,雷达海流可以有效地反映有效探测区内表层海流及其时空变化,高精度区流速流向的均方根误差(RMS)分别为7.5~19.3cm/s和15.5°~33.7°,尤其是高精度区核心区域的RMS仅为7.5~10.1 cm/s和15.5°~28.5°.边缘区流速流向的RMS为16.1~25.8 cm/s和39.5°~40.7°,与国内外达到业务化运行要求的同类产品实际观测精度相当.  相似文献   

10.
通过对2010/2011年夏季南极长城湾叶绿素a浓度和海流等环境参数的传感器连续观测;研究其时空变化特征及海流对浮游植物生物量的影响。结果表明;12.9 m水层叶绿素a浓度从12月中旬开始增长;直至2月上旬开始维持相对稳定;期间出现两个高值点(2.74 μg/L和3.76 μg/L)。叶绿素a浓度表现出了24 h周期变化特征;每日叶绿素a浓度最高值出现在正午前后时段的概率要高于其他时段。表层海水受西北风影响;流速较大;约为60~100 cm/s;中层和底层水体流速较小;约为10 cm/s。表层的风海流使海水在长城湾发生辐散;下层海水向上涌升;驱动了水体的垂直交换。长城湾与麦克斯韦尔湾存在水体交换;水体主要从中层进入湾内;从表层输出。长城湾的叶绿素a浓度与流速呈显著负相关;表明低流速环境有利于长城湾浮游植物的生长。  相似文献   

11.
In this paper, the intra-seasonal variability of the abyssal currents in the China Ocean Mineral Resources Association (COMRA) polymetallic nodule contact area, located in the western part of the Clarion and Clipperton Fraction Zone in the tropical East Pacific, is investigated using direct observations from subsurface mooring instruments as well as sea-surface height data and reanalysis products. Mooring observations were conducted from September 13, 2017 to August 15, 2018 in the COMRA contact area (10°N, 154°W). The results were as follows: (1) At depths below 200 m, the kinetic energy of intra-seasonal variability (20?100 d) accounts for more than 40% of the overall low-frequency variability, while the ratio reaches more than 50% below 2 000 m. (2) At depths below 200 m, currents show a synchronous oscillation with a characteristic time scale of 30 d, lasting from October to the following January; the energy of the 30-d oscillation increases with depth until the layer of approximately 4 616 m, and the maximum velocity is approximately 10 cm/s. (3) The 30-d oscillation of deep currents is correlated with the tropical instability waves in the upper ocean.  相似文献   

12.
本文利用在西太平洋牛郎海山布放的两套锚系潜标获取的长时间海流观测数据,分析了深海的海洋动力环境特征,着重阐释了该海域海流的全水深垂向结构及其低频变化特征。结果表明:(1)年平均海流及其变化幅度均在上层最大、中层和深层次之、中深层最小;(2)年平均上,150 m以浅的海流为东向的副热带逆流,150 m以深和中层为西向流;山顶处的近底层海流为较稳定的弱南向流,山底处的近底层海流为西南向流;(3)在山顶和山底,各深度层次的海流在全年均表现出100 d左右的振荡周期;在2 000 m以浅,各深度层次的海流振荡的位相基本一致,振荡幅度在表层最强、随深度的增加而减小;在2 000 m以深,海流变化的位相与2 000 m以浅相反,振荡幅度在4 000 m最强。  相似文献   

13.
Deep flows on the slope inshore of the Kuril-Kamchatka Trench southeast off Cape Erimo, Hokkaido were observed for about five years from June 1989 to March 1995, using a mooring system with two current meters. In 1991 and 1993 directionally stable southwestward flows were observed at the upper layer (1000 m). These appear to be typical of the Oyashio because the characteristics of the flows were high mean kinetic energy, low eddy energy and high stability. However, the magnitudes of other mean flows at the upper layer, except for 1991 and 1993, were less than their standard deviations. This suggests that the Oyashio was observed for only a limited period of time. On the other hand, at the lower layer (3000 m) the magnitudes of the mean flows for 10–11 months were 1–3 cm s-1 and ellipses of their eddy kinetic energy were extremely flattened in the direction of the local isobath. The directions of the mean flows in 1990, 1991 and 1993 were southwestward along the local isobath. The relationships between the upper and the lower flows are discussed in terms of monthly change of kinetic energy, since the low-frequency fluctuations longer than 30-day are predominant from the eddy kinetic energy spectra. The results show that there are cases when the kinetic energy of the monthly mean flows at the lower layers are larger than those at the upper layers. This suggests the possibility that the lower flows are in part a southward deep western boundary current.  相似文献   

14.
On the basis of the current measurements at 200,500 and 800 m from moored current meters with the time series data from March 17 to April 15 at the mooring station (20°49′57″N, 120°48′ 12″E) and the hydrographic data obtained in the Luzon Strait during the spring of 2002 cruise, the circulation in the investigated  相似文献   

15.
The seasonal climatic circulation of the sea reconstructed on the basis of assimilation of new arrays of many-year average hydrological data in a model is analyzed. Five layers are discovered in the structure of climatic currents in the sea in depth: the surface Ekman layer (∼ 10 m), a layer with small vertical gradients of the kinetic energy (∼ 10–60 m), a layer with relatively high vertical gradients of the kinetic energy (∼ 60–150 m), a layer with gradual decrease in the kinetic energy and intensification (from 250–350 m) of the east cyclonic gyre and Batumi anticyclonic eddy (∼ 150–1000 m), and an abyssal layer characterized by an almost barotropic velocity (∼ 1000–2000 m). The specific features of the seasonal evolution of currents at these depths are investigated. It is shown that the key role in the formation of deep-water circulation of the sea is played by the south east flow, east cyclonic gyre, and Batumi anticyclonic eddy. __________ Translated from Morskoi Gidrofizicheskii Zhurnal, No. 6, pp. 28–45, November–December, 2005.  相似文献   

16.
2015年9月台风“灿鸿”经过黄海海域的QF111浮标,该浮标观测到黄海海洋的温度和流速响应。受台风影响,黄海海表温度有明显的下降,降温幅度在2~4°C,且在台风路径右侧形成了海表面温度低于20°C的低温斑块。流速的响应主要表现为台风过境期间流速增强,达1.2~1.5 m/s,呈现出全水深强化的特征。风一直对海洋有能量输入,且在台风过境期间风输入海洋的能量最大,旋转功率谱的分析结果表明台风输入海洋的能量向海洋内部传播。黄海海域由台风激发出的近惯性振荡衰减较快,近惯性振荡e折时间尺度约为2 d。  相似文献   

17.
The comprehensive three-dimensional structures of an anti-cyclonic mesoscale eddy(AE) in the subtropical northwestern Pacific Ocean were investigated by combining the Argo floats profiles with enhanced vertical and temporal sampling and satellite altimetry data. The AE originated near the Kuroshio Extension and then propagated westward with mean velocity of 8.9 cm/s. Significant changes and evolutions during the AE's growing stage(T1) and further growing stage(T2) were revealed through composite analysis. In the composite eddy core,maximum temperature(T) and salinity(S) anomalies were of 1.7(1.9)°C and 0.04(0.07) psu in T1(T2) period,respectively. The composite T anomalies showed positive in almost whole depth, but the S anomalies exhibited a sandwich-like pattern. The eddy's intensification and its influence on the intermediate ocean became more significant during its growth. The trapping depth increased from 400×10~4 Pa to 580×10~4 Pa while it was growing up, which means more water volume, heat and salt content in deeper layers can be transported. The AE was strongly nonlinear in upper oceans and can yield a typical mean volume transport of 0.17×10~6 m~3/s and a mean heat and salt transport anomaly of 3.6×10~(11) W and –2.1×10~3 kg/s during the observation period. The Energy analysis showed that eddy potential and kinetic energy increased notably as it propagated westward and the baroclinic instability is the major energy source of the eddy growth. The variation of the remained Argo float trapped within the eddy indicated significant water advection during the eddy's propagation.  相似文献   

18.
Mesoscale eddies play an important role in modulating the ocean circulation. Many previous studies on the threedimensional structure of mesoscale eddies were mainly based on composite analysis, and there are few targeted observations for individual eddies. A cyclonic eddy surveyed during an oceanographic cruise in the Northwest Pacific Ocean is investigated in this study. The three-dimensional structure of this cyclonic eddy is revealed by observations and simulated by the four-dimensional variational data assimilation(4 DVAR) system combined with the Regional Ocean Modeling System. The observation and assimilation results together present the characteristics of the cyclonic eddy. The cold eddy has an obvious dual-core structure of temperature anomaly.One core is at 50–150 m and another is at 300–550 m, which both have the average temperature anomaly of approximately-3.5°C. The salinity anomaly core is between 250 m and 500 m, which is approximately-0.3. The horizontal velocity structure is axis-asymmetric and it is enhanced on the eastern side of the cold eddy. In the assimilation experiment, sea level anomaly, sea surface temperature, and in situ measurements are assimilated into the system, and the results of assimilation are close to the observations. Based on the high-resolution assimilation output results, the study also diagnoses the vertical velocity in the mesoscale eddy, which reaches the maximum of approximately 10 m/d. The larger vertical velocity is found to be distributed in the range of 0.5 to 1 time of the normalized radius of the eddy. The validation of the simulation result shows that the 4 DVAR method is effective to reconstruct the three-dimensional structure of mesoscale eddy and the research is an application to study the mesoscale eddy in the Northwest Pacific by combining observation and assimilation methods.  相似文献   

19.
1 Introduction Hurricane is an extremely high wind event, which injects momentum into the oceanic mixed layer along its passage for a very short duration. If our interest is not at the surface, but in a depth away from the imme-diate surface wave influenc…  相似文献   

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