Observational analysis of the double-diffusive convection in the deep Canada Basin

XIE Lingling LI Mingming LI Min

谢玲玲, 李明明, 李敏. 加拿大海盆深层双扩散对流的观测分析[J]. 海洋学报英文版, 2015, 34(11): 71-79. doi: 10.1007/s13131-015-0750-4
引用本文: 谢玲玲, 李明明, 李敏. 加拿大海盆深层双扩散对流的观测分析[J]. 海洋学报英文版, 2015, 34(11): 71-79. doi: 10.1007/s13131-015-0750-4
XIE Lingling, LI Mingming, LI Min. Observational analysis of the double-diffusive convection in the deep Canada Basin[J]. Acta Oceanologica Sinica, 2015, 34(11): 71-79. doi: 10.1007/s13131-015-0750-4
Citation: XIE Lingling, LI Mingming, LI Min. Observational analysis of the double-diffusive convection in the deep Canada Basin[J]. Acta Oceanologica Sinica, 2015, 34(11): 71-79. doi: 10.1007/s13131-015-0750-4

加拿大海盆深层双扩散对流的观测分析

doi: 10.1007/s13131-015-0750-4
基金项目: The National Natural Science Foundation of China under contract Nos 41476009, 41106012 and 41506018; the Science and Technology Program in Higher Education of Guangdong under contract No. 2013KJCX0099.

Observational analysis of the double-diffusive convection in the deep Canada Basin

  • 摘要: 加拿大海盆是北冰洋最大的亚海盆,其最深处达到3850 m. 双扩散对流过程可能是底部热通量对海盆内部孤立水体施加影响使水团性质发生变化的主要通道.本文利用2003年中国第二次北极科学考察获得的温盐深观测数据,发现在加拿大海盆中心2400 m以深存在温盐同时随深度增加的过渡层和温盐相对均匀的底部混合层,其平均厚度分别约为500 m和1000 m.在过渡层,双扩散对流引起了明显的温度阶梯结构,阶梯的均匀层厚度由下层的60 m减小到20 m,其界面厚度在10 m左右,温差在0.001-0.002 ℃.海盆深层的密度率基本小于2,双扩散强度大于上层200-400 m处的扩散对流.海盆内部最深层阶梯的热通量为0.014-0.031 W m-2,比上层双扩散对流的热通量小1-2个量级,但与地热通量的估算值相当.
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出版历程
  • 收稿日期:  2015-03-19
  • 修回日期:  2015-07-04

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