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Vertical distributions of the strong organic ligand in the twilight zone of Southern Hemisphere Ocean particulate matter

机译:南半球海洋颗粒物暮光区强有机配体的垂直分布

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摘要

Vertical distributions of the strong organic ligand (SOL) in oceanic particulate matter (PM), as determined from the amount of thorium adsorption onto PM in 0.1 M HC1, were measured for the twilight zone (100-to 1000-m depth) of the Southern Hemisphere Ocean (Pacific, Atlantic and Indian) mid-latitude regions. The SOL concentrations in South Pacific PM collected at a depth of 100 m, ranging from 0.56 to 5.4 nM, showed a longitudinal variation with low concentrations occurring from 180° to 150°W in the South Pacific subtropical gyre and high in the Tasman Sea and the eastern South Pacific. The SOL concentrations in 100-m-depth South Atlantic PM, ranging from 1.19 to 2.5 nM, showed a longitudinal gradient with low in the west and high in the east. The SOL concentrations in 100-m-depth Indian Ocean PM, ranging from 1.16 to 5.25 nM, showed a longitudinal variation with a maximum near 69°E and low in the eastern Indian Ocean. The SOL concentrations in PM of the South Pacific and Atlantic twilight zones decreased with increasing depth, whereas the high SOL concentrations in 1000 m depth PM occurred in the central Indian Ocean. Each depth-decreasing vertical profile of the SOL concentration in PM except the central Indian Ocean was expressed by the empirical equation C_(SOl) = C_(Sol,100) (z/l00)~(-b). The dimensionless scaling factor b in the South Pacific, South Atlantic and Indian Ocean varied from 0.83 to 2.5, from 0.54 to 0.86 and from 0.24 to 0.91, respectively, and was positively correlated with the SOL concentration in PM at 100 m in each sea area. This is a first global measurement of the particulate SOL in the twilight zone. The paniculate SOL is a useful tool for better understanding of particle dynamics in the twilight zone, if we have more detail knowledge on spatial and temporal variability of the paniculate SOL.
机译:根据在0.1 M HC1中PM在PM上的吸附量确定了海洋微粒物质(PM)中强有机配体(SOL)的垂直分布,该垂直分布是通过对海洋中微弱区域(深度为100-1000 m)进行的。南半球海洋(太平洋,大西洋和印度)为中纬度地区。在100 m深度处收集的南太平洋PM中的SOL浓度范围为0.56至5.4 nM,表现出纵向变化,南太平洋亚热带回旋中的低浓度出现在180°至150°W,而塔斯曼海和塔斯曼海中则较高。南太平洋东部。在南大西洋100米深度PM中的SOL浓度范围为1.19至2.5 nM,显示出一个纵向梯度,其西部较低,东部较高。在印度洋深达100 m的PM中,SOL浓度范围为1.16至5.25 nM,表现出纵向变化,最大变化接近69°E,在印度洋东部低。随着深度的增加,南太平洋和大西洋暮光区的PM中的SOL浓度降低,而印度中部中部1000 m深度PM中的SOL浓度较高。除中印度洋以外,PM中SOL浓度的每个深度递减垂直剖面都由经验方程C_(SO1)= C_(Sol,100)(z / 100)〜(-b)表示。南太平洋,南大西洋和印度洋的无量纲缩放因子b分别从0.83到2.5、0.54到0.86和0.24到0.91,并且与每个海域100 m PM中的SOL浓度呈正相关。这是暮光区中颗粒SOL的首次全局测量。如果我们对颗粒状SOL的时空变异性有更详细的了解,则颗粒状SOL是一个有用的工具,可用于更好地了解暮光区中的粒子动力学。

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  • 来源
    《Progress in Oceanography》 |2011年第4期|p.108-119|共12页
  • 作者单位

    Geochetnical Department, Meteorological Research Institute, Nagamine 7-1, Tsukuba, lbaraki 305-0052, Japan;

    Radiation Safety and Hygiene Division, Osaka University, Yamada-oka 1-1, Suita, Osaka 565-0871, Japan;

    Korea Research Institute of Standards and Science, Daejeon, South Korea;

    Marine Environment Laboratories, International Atomic Energy Agency, MC-98000, Monaco;

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