{"title":"Three anticyclonic slope water oceanic eDDIES (SWODDIES) in the Southern Bay of Biscay in 1990","authors":"R.D Pingree , B Le Cann","doi":"10.1016/0198-0149(92)90062-X","DOIUrl":null,"url":null,"abstract":"<div><p>Jet-like extensions of the slope current off northern Spain and France in the southern Bay of Biscay in the winter develop into anticyclonic eddies with an upper core of slope water. Three eddies were observed to develop in the winter of 1989/1990, subsequently named F90a, F90b and O90. F90a was an anticclonic eddy of radius 50–60 km, with a central core of mixed water of slope origin (from the slopes in the vicinity of Cap Ferret Canyon) and of volume ∼400 k<sup>3</sup>. In the eddt centre, the mixed core extended from ∼70 to ∼280 m. Measurements at sea showed minimal changes in the core characteristics of F90a (potential temperature, 12.95°C, salinity, 35.74 psu) with time, and remote sensing studies demonstrated that these slope water core eddies can maintain their identities for about a year. Rotation rates in the central core of F90a were about 3 days and values of normalized relative vorticity were about −0.5. Maximummean azimuthal velocities were about 30 cm s<sup>−1</sup> at a radius of 30 km. Hydrographic data showed that the presence of the core was felt to a depth of ∼1500m, resulting in an azimuthal transport of about 8 Sv. Both F90a and O90 moved westward across the deep (4800 m) Bay of Biscay, and the westward migration speed (2 cm s<sup>−1</sup>) seems in excess of simple theoretical estimates for the β-induced westward propagation speed (0.4 cm s<sup>−1</sup>) of anticyclonic eddies. If the latter figure is used for self-advection and the effects of topography and mutual influence are neglected, the observed westward movement suggests a clockwise mean circulation −2 cm s<sup>−1</sup>) for the oceanic water in the Bay of Biscay. By contrast, F90b remained nearly stationary near 4°W. Remote sensing studies indicate that the occurence of a 4°W eddy in the summer of any year miight be attributed to warm slope water inflow along the northern Spanish slope in the previous winter.</p></div>","PeriodicalId":81079,"journal":{"name":"Deep-sea research. Part A, Oceanographic research papers","volume":"39 7","pages":"Pages 1147-1175"},"PeriodicalIF":0.0000,"publicationDate":"1992-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0198-0149(92)90062-X","citationCount":"287","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Deep-sea research. Part A, Oceanographic research papers","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/019801499290062X","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 287
Abstract
Jet-like extensions of the slope current off northern Spain and France in the southern Bay of Biscay in the winter develop into anticyclonic eddies with an upper core of slope water. Three eddies were observed to develop in the winter of 1989/1990, subsequently named F90a, F90b and O90. F90a was an anticclonic eddy of radius 50–60 km, with a central core of mixed water of slope origin (from the slopes in the vicinity of Cap Ferret Canyon) and of volume ∼400 k3. In the eddt centre, the mixed core extended from ∼70 to ∼280 m. Measurements at sea showed minimal changes in the core characteristics of F90a (potential temperature, 12.95°C, salinity, 35.74 psu) with time, and remote sensing studies demonstrated that these slope water core eddies can maintain their identities for about a year. Rotation rates in the central core of F90a were about 3 days and values of normalized relative vorticity were about −0.5. Maximummean azimuthal velocities were about 30 cm s−1 at a radius of 30 km. Hydrographic data showed that the presence of the core was felt to a depth of ∼1500m, resulting in an azimuthal transport of about 8 Sv. Both F90a and O90 moved westward across the deep (4800 m) Bay of Biscay, and the westward migration speed (2 cm s−1) seems in excess of simple theoretical estimates for the β-induced westward propagation speed (0.4 cm s−1) of anticyclonic eddies. If the latter figure is used for self-advection and the effects of topography and mutual influence are neglected, the observed westward movement suggests a clockwise mean circulation −2 cm s−1) for the oceanic water in the Bay of Biscay. By contrast, F90b remained nearly stationary near 4°W. Remote sensing studies indicate that the occurence of a 4°W eddy in the summer of any year miight be attributed to warm slope water inflow along the northern Spanish slope in the previous winter.
冬季,西班牙北部和法国南部比斯开湾的斜坡流的射流状延伸发展成反气旋涡流,上部核心为斜坡水。1989/1990年冬季观测到形成了三个涡旋,随后命名为F90a、F90b和O90。F90a是一个半径为50-60 km的反涡旋,其中心核心是斜坡来源的混合水(来自雪雷帽峡谷附近的斜坡),体积约为400 k3。在eddt中心,混合岩心从~ 70米延伸到~ 280米。海上测量显示,F90a的核心特征(位势温度12.95°C,盐度35.74 psu)随时间变化很小,遥感研究表明,这些斜坡水核心漩涡可以保持大约一年的特征。F90a中心涡旋速率约为3 d,标准化相对涡度值约为- 0.5。在半径30公里处,最大平均方位角速度约为30 cm s - 1。水文数据显示,在约1500米的深度可以感觉到岩心的存在,导致了大约8 Sv的方位传输。F90a和O90都在比斯开湾深处(4800 m)向西移动,向西移动的速度(2 cm s−1)似乎超过了β诱导的反气旋涡旋向西传播速度(0.4 cm s−1)的简单理论估计。如果后一个图用于自平流,并且忽略地形和相互影响的影响,则观测到的向西运动表明比斯开湾海水的平均顺时针环流为- 2 cm s - 1)。相比之下,F90b在4°W附近几乎保持静止。遥感研究表明,每年夏季出现的4°W涡旋可能是由于前一个冬季沿西班牙北部斜坡流入的暖坡水。