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Advection and diffusion of Indonesian throughflow water within the Indian Ocean South Equatorial Current.

机译:印度尼西亚通流水在印度洋南赤道洋流内的平流和扩散。

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摘要

Using WOCE WHP CTD and ADCP sections in Indian Ocean from 1995 and ARLINDO 1994 CTD data within the Timor Sea, the throughflow component of the SEC transport is investigated. Throughflow water is well represented by its nearly homogenous low salinity feature within the SEC thermocline, extending from 60 m to about 300–400 m (or 10°C isotherm). Over 80% of its initial T/S signature is still present half way across the Indian Ocean, with over 60% reaching well into the western Indian Ocean. While the transport of thermocline water within the SEC from 5°S to 20°S varies from 10 to 35 Sv (Sv = 1 × 106 m3 s−1), the throughflow portion varies from 3 to 12 Sv, probably in response to variations of the throughflow transport, which changing with the phase of the monsoon and ENSO, and of the Indian Ocean Equatorial recirculation cell between the Equatorial Counter Current (5°S) and the SEC in the Indian Ocean. The throughflow water low salinity signal within the SEC thermocline diminishes enroute across the Indian Ocean. Assuming this is accomplished by isopycnal mixing with adjacent thermocline water, an isopycnal mixing coefficient of the order of 10 4 m2 s−1, with average value of (1.1 ± 0.8) × 104 m2 s−1 , is determined, which is reduced to 103 m2 s−1 if there is no zonal equatorial recirculation.; Estimates of the eddy fluxes across I-2 are made using a filtering procedure which filters out the fields of mesoscale eddy components using an ideal pass filter. The total eddy heat flux across 12 section from about 57° to 90.5°E, over the 60–300 m depth range is towards the south, of approximately 0 (hull ADCP), 2.2 (LADCP), 6.1 (geostrophic reference to hull ADCP meridional velocity at 200 m) and 2.8 × 1012 W (geostrophic reference to LADCP meridional velocity at 1000 m), about 2 orders of magnitude less than the total heat flux. The eddy flux of salt is southward at 3.7, 1.7, 3.2 and 1.0 × 105 kg s−1. The geostrophic velocity field reference the ADCP at 200 m provides the best estimate of eddy heat and salt transports. These correspond to the diffusivity Ky of the order of 2.0–4.5 and 3.6–8.6 × 103 m2 s−1 for temperature and salinity, respectively, which is one order of magnitude smaller than the lateral mixing coefficient calculated by the method of stationary lateral mixing of the Indonesian Throughflow, but is consistent with the situation of no equatorial recirculation. (Abstract shortened by UMI.)
机译:利用1995年印度洋的WOCE WHP CTD和ADCP断面以及帝汶海内的ARLINDO 1994 CTD数据,研究了SEC输运的通流成分。 SEC恒温槽内的几乎均匀的低盐度特征很好地代表了通流水,从60 m延伸到大约300-400 m(或等温线10°C)。最初的T / S签名中有80%以上仍然存在于整个印度洋的一半,其中60%以上进入印度洋西部。 SEC中的温跃层水从5°S到20°S的传输范围从10到35 Sv(Sv = 1×10 6 m 3 s -1 ),通流部分在3到12 Sv之间变化,这可能是由于通流输运的变化而引起的,该变化随季风和ENSO的相位以及赤道之间的印度洋赤道回流单元的变化而变化。逆流(5°S)和印度洋的SEC。 SEC温跃层中的通水低盐度信号减弱了穿越印度洋的航路。假设这是通过与相邻的温跃线水进行等温混合实现的,等温混合系数为10 4 m 2 s -1 ,确定(1.1±0.8)×10 4 m 2 s −1 的平均值,将其减少到10 3 m 2 s −1 (如果没有纬向赤道再循环)。使用滤波程序对I-2上的涡通量进行估算,该滤波程序使用理想的通过滤波器滤出中尺度涡流分量的场。在60-300 m深度范围内,从大约57°到90.5°E的12个部分的总涡流通量都朝南,大约为0(船体ADCP),2.2(LADCP),6.1(对船体ADCP的地转参考) 200 m时的子午速度)和2.8×10 12 W(以1000 m时的LADCP子午速度为地转参考),比总热通量小大约2个数量级。盐的涡流向南分别为3.7、1.7、3.2和1.0×10 5 kg s −1 。在200 m处以ADCP为参考的地转速度场提供了涡流热量和盐分传输的最佳估计。这些对应于温度和盐度的扩散系数Ky约为2.0–4.5和3.6–8.6×10 3 m 2 s -1 分别比通过印尼通流的静态横向混合方法计算的横向混合系数小一个数量级,但与没有赤道再循环的情况是一致的。 (摘要由UMI缩短。)

著录项

  • 作者

    Ma, Shubin.;

  • 作者单位

    Columbia University.;

  • 授予单位 Columbia University.;
  • 学科 Physical Oceanography.
  • 学位 Ph.D.
  • 年度 2002
  • 页码 122 p.
  • 总页数 122
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 海洋物理学;
  • 关键词

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