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61.
棉兰老岛以东反气旋涡的Argo观测研究 总被引：1，自引：0，他引：1
报道了2003年1月至10月期间,由布放于西北太平洋中的Argo剖面浮标捕获的位于棉兰老岛以东海域的反气旋涡。该涡中心位于8.7°N、127.6°E附近,距大陆坡不远,沿等深线走向呈椭圆形分布。其长轴(NW-SE)约200km,短轴(NE-SW)长约120km。Argo浮标的漂移轨迹及其在表层及1 500db层的漂移速度场表明,该反气旋涡位于温跃层以下,中层海洋特征。在1 500db层上,涡的外围平均切向速度为11.9—14.0cm.s-1,旋转周期约为40d。温、盐度断面分布表明,该反气旋涡内的温盐结构非常复杂,可能与源自南、北半球的中层水团在涡旋内交汇并发生变性有关。 相似文献
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Argo浮标是靠浮标体底部一个可改变体积的盛油皮囊,使其获得不同的净浮力来实现下潜、上升和深度控制.盛油皮囊的膨胀和收缩又是通过液压柱塞泵向盛油皮囊内注入或抽出液压油来实现的,以液压柱塞泵为主的浮标注油系统的运转状况关系到整个Argo浮标的性能.因此,为了提高Argo浮标的工作可靠性,在Argo浮标的生产制作及其检测过... 相似文献
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Simon Pels 《Australian Journal of Earth Sciences》2013,60(1):27-40
Studies of the Murray River have revealed that its ancestral river system is the result of three separate phases of river activity, each consisting of a degradational and aggradational sub‐phase. To illustrate the relations, certain sections of the rivers were mapped in detail revealing characteristic terrace levels for the various phases. The regional pattern shows that immediately upstream from the Cadell Fault, and for a distance of 100 miles (160 km.) downstream, tectonically induced topographical changes have separated the individual ancestral rivers representative of each phase. Elsewhere, the three rivers are superimposed and follow the same general course. This pattern of separation by diversion also applies to the present rivers so that, in the diverted sector of the river system, old floodplains occur which were deserted by the present river. Initial water logging and salting problems were restricted to these deserted floodplains where they occur in the Irrigation Districts. A relative chronology of Quaternary events has been drawn up. 相似文献
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西北太平洋副热带模态水形成区声传播特性分析 总被引：4，自引：1，他引：3
利用Argo剖面数据和水声学数值模型,分析了西北太平洋副热带模态水(STMW)形成区因季节性环境差异所引起的水声传播变化特征。声场计算结果表明,STMW形成区域的声传播为近表层波导与会聚区的复合形式,其中会聚区终年存在,表面波导在秋、冬两季混合层加深的环境条件下出现,次表层波导在夏季STMW潜沉的环境条件下出现。上层海洋中两类不同形式的波导使表层和次表层的声能分布呈反相变化,波导内与波导外的声能差异可达10~15dB(声波频率为1 000Hz)。STMW的季节性变化还会引起会聚区的位置差异,具体情况与声源深度有关。声源在20m时,夏季会聚区距离最远,秋季、春季次之,冬季最近,夏季和冬季相差6.6km;声源在150m时,夏季会聚区距离缩短了3.1km,其他季节变化不大。 相似文献
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The Argo data are used to calculate eddy(turbulence)heat transport(EHT)in the global ocean and analyze its horizontal distribution and vertical structure.We calculate the EHT by averaging all the v′,T′profiles within each 2×2 bin.The velocity and temperature anomalies are obtained by removing their climatological values from the Argo"instantaneous"values respectively.Through the Student’s t-test and an error evaluation,we obtained a total of 87%Argo bins with significant depth-integrated EHTs(D-EHTs).The results reveal a positive-and-negative alternating D-EHT pattern along the western boundary currents(WBC)and Antarctic Circumpolar Current(ACC).The zonally-integrated D-EHT(ZI-EHT)of the global ocean reaches 0.12 PW in the northern WBC band and–0.38 PW in the ACC band respectively.The strong ZI-EHT across the ACC in the global ocean is mainly caused by the southern Indian Ocean.The ZI-EHT in the above two bands accounts for a large portion of the total oceanic heat transport,which may play an important role in regulating the climate.The analysis of vertical structures of the EHT along the 35 N and45 S section reveals that the oscillating EHT pattern can reach deep in the northern WBC regions and the Agulhas Return Current(ARC)region.It also shows that the strong EHT could reach 600 m in the WBC regions and 1 000 m in the ARC region,with the maximum mainly located between 100 and 400 m depth.The results would provide useful information for improving the parameterization scheme in models. 相似文献
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Effects of interannual salinity variability on the barrier layer in the western-central equatorial Pacific: A diagnostic analysis from Argo 总被引：4，自引：0，他引：4
ABSTRACT In this paper, interannual variations in the barrier layer thickness （BLT） are analyzed using Argo three-dimensional temperature and salinity data, with a locus on the effects of interannually varying salinity on the evolution of the El Nifio Southern Oscillation （ENSO）. The interannually varying BLT exhibits a zonal seesaw pattern across the equatorial Pacific during ENSO cycles. This phenomenon has been attributed to two different physical processes. During E1 Nifio （La Nifia）, the barrier layer （BL） is anomalously thin （thick） west of about 160°E, and thick （thin） to the east. In the western equatorial Pacific （the western part： 130°-160°E）, interannual variations of the BLT indicate a lead of one year relative to those of the ENSO onset. The interannual variations of the BLT can be largely attributed to the interannual temperature variability, through its dominant effect on the isothermal layer depth （ILD）. However, in the central equatorial Pacific （the eastern part： 160~E- 170~W）, interannual variations of the BL almost synchronously vary with ENSO, with a lead of about two months relative to those of the local SST. In this region, the interannual variations of the BL are significantly affected by the interannually varying salinity, mainly through its modulation effect on the mixed layer depth （MLD）. As evaluated by a onedimensional boundary layer ocean model, the BL around the dateline induced by interannual salinity anomalies can significantly affect the temperature fields in the upper ocean, indicating a positive feedback that acts to enhance ENSO. 相似文献
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利用小波分析方法,对2003-2008年周平均的Argo(地转海洋学实时观测阵)海温资料进行了分析,给出了全球上层海温年周期和半年周期振荡的空间分布特征.结果表明,南北半球中高纬地区以表层海温的年周期变化为主,在低纬度地区,表层海温以半年周期为主,而温跃层附近海温既有年周期也有半年周期(赤道太平洋、东南印度洋和赤道西大西洋以年周期为主;赤道东、西印度洋以半年周期为主).南北半球中高纬的年周期海温和北半球中纬度的半年周期海温在表层范围最大,显著性最高,强度最强,位相最前.随深度的增加,范围减小,显著性降低,强度减弱,位相滞后.信号主要集中在水深50 m以上,影响深度在150m以浅;赤道附近的太平洋和热带东南印度洋的年周期海温以及赤道东、西印度洋的半年周期海温在水深100m范围最大,显著性最高,强度最强,位相最前,信号主要集中在温跃层附近,影响深度均可达500m. 相似文献
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海洋渔业预报使用的遥感数据一般只能获得海洋表面的环境信息,而Argo数据可以为渔业预报提供较深处的温盐数据,为了在渔业预报中按其时间周期进行使用,需要计算它的周期以提高预报质量。通过功率谱估计计算出2001-2008年的数据存在的较长的周期为62．7天和117．5天,较短的周期为4．9天和9．8天,同时还有一个约为7天的不明显周期,观测剖面数据总量在年际与年内都存在较大变化。 相似文献