Turbulent mixing in the upper ocean of the northwestern Weddell Sea, Antarctica

GUO Guijun SHI Jiuxin JIAO Yutian

郭桂军, 史久新, 矫玉田. 南极西北威德尔海上层海洋湍流混合研究[J]. 海洋学报英文版, 2016, 35(3): 1-9. doi: 10.1007/s13131-016-0816-y
引用本文: 郭桂军, 史久新, 矫玉田. 南极西北威德尔海上层海洋湍流混合研究[J]. 海洋学报英文版, 2016, 35(3): 1-9. doi: 10.1007/s13131-016-0816-y
GUO Guijun, SHI Jiuxin, JIAO Yutian. Turbulent mixing in the upper ocean of the northwestern Weddell Sea, Antarctica[J]. Acta Oceanologica Sinica, 2016, 35(3): 1-9. doi: 10.1007/s13131-016-0816-y
Citation: GUO Guijun, SHI Jiuxin, JIAO Yutian. Turbulent mixing in the upper ocean of the northwestern Weddell Sea, Antarctica[J]. Acta Oceanologica Sinica, 2016, 35(3): 1-9. doi: 10.1007/s13131-016-0816-y

南极西北威德尔海上层海洋湍流混合研究

doi: 10.1007/s13131-016-0816-y

Turbulent mixing in the upper ocean of the northwestern Weddell Sea, Antarctica

  • 摘要: 利用中国第30次南极考察期间于2014年2月在西北威德尔海获得的温度、盐度剖面数据和湍流数据,本文对该海域上层海洋(30-200 m)混合过程进行了研究。受地形特征和海冰分布影响,观测海域垂向热盐结构存在着明显的不同,使得湍动能耗散率(ε)和湍扩散率(K)在垂向和空间上都存在着显著的差异。在南极半岛北侧陆架和菲利普海岭处,上层200 m温度和盐度剖面垂向上相对均匀,εK在此显著高于其他区域,分别达到O(10-7)-O(10-6) W·kg-1O(10-3)-O(10-2) m2·s-1量级,比开阔大洋要高两到三个量级。在鲍威尔海盆和南奥克尼海台,受上层海洋强层化遏制,该区域上层海洋混合水平与开阔大洋水平相当。在此,ε随着深度加深从O(10-8)降到O(10-9) W·kg-1,而K受密度跃层内强层化制约呈现出与ε相反的垂向变化趋势,随深度从O(10-6)增长到O(10-5) m2·s-1。在海冰外缘区,虽然耗散水平在50-100 m出现了较高水平,但是密度跃层内层化的加强弱于无冰区威德尔海海域,因此K在垂向上保持相对稳定,维持在10-4 m2·s-1量级。目前的研究将风和潮汐作为近岸海域海洋混合的主要能量来源,但我们的结果显示湍扩散率K与风应力和潮汐动能关系并不显著。混合强烈的海域一般都伴有海底粗糙度高值的出现,表明风和潮汐产生的内波只有在撞击到陡峭地形时才能耗散到湍流尺度激发混合的发生。另外威德尔海水通过菲利普通道西侧的缺口流出威德尔海,这也是造成此处产生强混合的一个能量来源。
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  • 收稿日期:  2015-09-10
  • 修回日期:  2015-11-09

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