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A global analysis of subtropical underwater (STUW) using drifter and tracer methods.

机译:使用漂流和示踪方法对亚热带水下(STUW)进行全局分析。

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摘要

The STUW, a component of the Central Waters, is an upper thermocline water mass present in the subtropics and tropics. It is distinguished as a vertical salinity maximum below the mixed layer. The STUW is formed by subduction within the subtropical gyres, where Ekman convergence, and the ambient evaporation-precipitation (E-P) are large. As part of the shallow subtropical cell, it has potentially important implications for climate, due to feedback on the atmosphere of upwelled water property anomalies near the equator, and poleward heat and salt fluxes in the Western Boundary Currents. The STUW is not symmetric about the equator in any of the oceans, but seems to be symmetric about the ITCZ.; An analysis of the fate of STUW shows that in the Pacific and Atlantic oceans, the southern STUW dominates the equatorial region. This is not the case in the Indian Ocean. The STUW in the South Indian Ocean does not seem to reach the equator, possibly due to the influence of the Indonesian Throughflow. The strong mixing in the pathway of the fresher Pacific water carried by the Throughflow, destroys the salinity maximum and seems to confine the STUW in the South Indian Ocean. In the North Atlantic, about 2/3 of the STUW circulates in the Gulf Stream recirculation, increasing salinity in the formation region of Subtropical Mode Water (STMW). Most of the STUW in the North Atlantic that flows north in the Gulf Stream is convected into STMW as suggested by Talley et al. (1996).; The first calculations of subduction and formation rates for STUW are presented using: (1) drifter data (1988–1998) and (2) CFC-12 data (1987–1995). The two methods are independent except for the calculation of the outcrop area. The use of two independent methods allows us to put bounds on the subduction rate. The subduction rate in the North Atlantic is 36–44 m/yr, in the South Pacific it is 32–33 m/yr, in the South Indian it is 22–25 m/yr and in the North Pacific it is 17–26 m/yr. The formation rates correlate with outcrop area: South Pacific 7 Sv, North Pacific 5 Sv, North Atlantic 2 Sv, and South Indian Ocean 1 Sv. The tracer and drifter methods agree remarkably well (within the estimated uncertainties), with the exception of the North Pacific.; To estimate the effect of mixing on the subduction (not included in the drifter calculation), diapycnal salt fluxes are calculated.; Effects of interannual variability on the STUW subduction rates are examined in the Pacific, and North Atlantic. (Abstract shortened by UMI.)
机译:STUW是中央水域的组成部分,是亚热带和热带地区的较高的跃层水团。它以混合层以下的垂直盐度最大值为特征。 STUW是由亚热带回旋中的俯冲作用形成的,在该副热带中,埃克曼会聚,并且环境蒸发-降水(E-P)很大。作为浅亚热带单元的一部分,由于对赤道附近上升的水属性异常的大气的反馈以及西边界流中的极热和盐通量的反馈,它对气候具有潜在的重要意义。 STUW在任何海洋中都不与赤道对称,但似乎与ITCZ对称。对STUW命运的分析表明,在太平洋和大西洋中,南部STUW主导着赤道地区。在印度洋,情况并非如此。南印度洋的STUW似乎没有到达赤道,这可能是由于印度尼西亚流量的影响。通流携带的太平洋淡水路径中的强烈混合破坏了盐度最大值,并且似乎将南印度洋的STUW限制在范围之内。在北大西洋,大约2/3的STUW在墨西哥湾流的再循环中循环,从而增加了亚热带模式水(STMW)形成区的盐度。 Talley et al 建议,北大西洋沿海湾流向北的大部分STUW被对流成STMW。 (1996)。 STUW的俯冲和形成速率的首次计算是使用:(1)离心机数据(1988-1998)和(2)CFC-12数据(1987-1995)。除计算露头面积外,这两种方法是独立的。两种独立方法的使用允许我们对俯冲率进行界定。北大西洋的俯冲速率为36–44 m / yr,南太平洋的俯冲速率为32–33 m / yr,南印度的俯冲速率为22–25 m / yr,北太平洋的俯冲速率为17–26每年形成速率与露头面积相关:南太平洋7 Sv,北太平洋5 Sv,北大西洋2 Sv和南印度洋<1 Sv。除北太平洋地区外,示踪剂法和漂移法方法非常吻合(在估计的不确定性范围内)。为了估计混合对俯冲作用的影响(不包括在浮子计算中),计算出了二向盐通量。在太平洋和北大西洋,研究了年际变化对STUW俯冲率的影响。 (摘要由UMI缩短。)

著录项

  • 作者单位

    University of Miami.;

  • 授予单位 University of Miami.;
  • 学科 Biology Oceanography.
  • 学位 Ph.D.
  • 年度 2001
  • 页码 161 p.
  • 总页数 161
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 海洋生物;
  • 关键词

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