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王凯, 朱彬, 徐永福, 巴琦, 李阳春. 全球海洋环流模式中氚分布的模拟[J]. 气候与环境研究, 2013, 18(4): 491-506. DOI: 10.3878/j.issn.1006-9585.2012.11198
引用本文: 王凯, 朱彬, 徐永福, 巴琦, 李阳春. 全球海洋环流模式中氚分布的模拟[J]. 气候与环境研究, 2013, 18(4): 491-506. DOI: 10.3878/j.issn.1006-9585.2012.11198
WANG Kai, ZHU Bin, XU Yongfu, BA Qi, LI Yangchun. Simulation of Distribution of Tritium in the Global Ocean General Circulation Model[J]. Climatic and Environmental Research, 2013, 18(4): 491-506. DOI: 10.3878/j.issn.1006-9585.2012.11198
Citation: WANG Kai, ZHU Bin, XU Yongfu, BA Qi, LI Yangchun. Simulation of Distribution of Tritium in the Global Ocean General Circulation Model[J]. Climatic and Environmental Research, 2013, 18(4): 491-506. DOI: 10.3878/j.issn.1006-9585.2012.11198

全球海洋环流模式中氚分布的模拟

Simulation of Distribution of Tritium in the Global Ocean General Circulation Model

  • 摘要: 氚(3H)作为一种重要的被动示踪物,经常被用于研究海洋中的物理过程及评估海洋环流模式的模拟性能.使用一个全球海洋环流模式(LICOM)来研究氚在海洋中的分布、存储和输送.模拟的全球氚通量表明,1975年之前氚主要由海气交换输入海洋,特别是在1963年,氚的气体交换输入约为降水输入的2.5倍,1975年之后两种方式的氚输入通量都大幅减少.比对GEOSECS(Geochemical Ocean Sections Study,1972~1978年)和WOCE(World Ocean Circulation Experiment,1989~1995年)大洋观测计划期间的观测资料发现,我们的模式很好地模拟出了氚的海表分布、水柱总量、经向分布以及次表层的高值信号,主要缺点在于模拟的氚向深层的穿透不足,特别是在全球的两个副热带地区,表现尤为明显,氚输入函数的不确定性和模式物理场描述的不足可能是造成误差的主要原因.模式给出的海洋中氚储存总量的结果与基于观测得到的结果比较吻合,如北太平洋海区:1973~1974年模拟结果约为20.4 kg,相同期间观测估计值为21.1±4.7 kg,1989~1995年模拟结果为20.7 kg,相同期间观测估计值为23.4±2.0 kg.氚在等密度面上高低纬的侧向通风明显,模式成功模拟出氚从中高纬的海表进入,沿等密度面向低纬的次表层输送,又经大洋环流和扩散分别向南半球和高纬输送的过程.

     

    Abstract: Tritium (3H) is often used as an important passive tracer to study physical processes in the ocean and to assess the performance of the ocean general circulation model (OGCM). A global OGCM (LICOM) is employed to study the distribution, storage, and transport of tritium in the ocean. Simulated results for the global tritium flux show that before 1975, tritium entered the ocean mainly from the atmosphere via vapor exchange, especially in 1963, when the tritium input by vapor exchange was 2.5 times larger than that by precipitation. However, after 1975 these two types of inputs decreased quickly and became quite close to each other. Compared to the observations obtained during GEOSECS (Geochemical Ocean Sections Study, 1972-1978) and WOCE (World Ocean Circulation Experiment, 1989-1995), our model reproduces well the observed features of the sea surface distribution, water column inventory, meridional gradient, and local maximum values of tritium. The main weakness of our model is that the simulated penetration depth of tritium is too small, especially in the two subtropical regions. Uncertainties are believed to exist in the development of the tritium input function, and the description of the physical processes, which probably influences the simulated results, needs to be improved in the OGCM. The total tritium inventory estimated by our model is close to the data-based estimate. For example, our model estimates that the North Pacific contained 20.4 kg and 20.7 kg of tritium during 1973-1974 and 1989-1995, respectively, which is in good agreement with the data-based estimates of 21.1±4.7 kg and 23.4±2.0 kg. The lateral ventilation of tritium from the subarctic to tropical regions is obvious along isopycnal surfaces. Our model successfully simulates the entry of tritium into the ocean from the high-latitude sea surface and its transport along isopycnals to the subsurface layer in the low-latitude region and then to the Southern Hemisphere and high-latitude regions by circulation and diffusion.

     

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