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海冰快速减退背景下大气动量输入对波弗特流涡长期变化的影响

陶树豪 杜凌

陶树豪,杜凌. 海冰快速减退背景下大气动量输入对波弗特流涡长期变化的影响[J]. 海洋学报,2021,43(7):100–113 doi: 10.12284/hyxb2021123
引用本文: 陶树豪,杜凌. 海冰快速减退背景下大气动量输入对波弗特流涡长期变化的影响[J]. 海洋学报,2021,43(7):100–113 doi: 10.12284/hyxb2021123
Tao Shuhao,Du Ling. Influence of atmospheric momentum input on Beaufort Gyre long term changes under the Arctic sea ice retreat[J]. Haiyang Xuebao,2021, 43(7):100–113 doi: 10.12284/hyxb2021123
Citation: Tao Shuhao,Du Ling. Influence of atmospheric momentum input on Beaufort Gyre long term changes under the Arctic sea ice retreat[J]. Haiyang Xuebao,2021, 43(7):100–113 doi: 10.12284/hyxb2021123

海冰快速减退背景下大气动量输入对波弗特流涡长期变化的影响

doi: 10.12284/hyxb2021123
基金项目: 全球变化研究国家重大科学研究计划(2015CB953902);国家自然科学基金(41576020)
详细信息
    作者简介:

    陶树豪(1996-),男,安徽省合肥市人,主要从事气候变化研究。E-mail:taoshuhao@stu.ouc.edu.cn

    通讯作者:

    杜凌,副教授,主要从事气候变化与极地海洋学研究。E-mail:duling@ouc.edu.cn

  • 中图分类号: P731.2; P732.7

Influence of atmospheric momentum input on Beaufort Gyre long term changes under the Arctic sea ice retreat

  • 摘要: 随着北冰洋海冰快速减退,气–冰–海系统发生显著变化,波弗特流涡也发生显著变化。本文使用实测资料和海洋大气再分析数据,探讨北冰洋波弗特流涡的长期变化和大气动量输入对波弗特流涡变化的影响。波弗特流涡的长期变化可以分为3个典型时期(1980–1995年,1996–2007年,2008–2018年)。最近时期(2008–2018年),波弗特流涡平均流涡强度达到4.39×10–7,相较于第1个时期(1980–1995年),流涡强度增加近2倍,达到稳定的状态。波弗特流涡范围扩大,主体向西北移动;上层海洋斜压性增强。与此同时,上层海洋环流主模态已发生显著转变:1980–1995年,环流主模态为影响整个加拿大海盆的加拿大海盆模态;2008–2018年的主模态则转变为影响整个研究海域的太平洋扇区模态。最近时期,表征气–海之间动量输入的气–海应力显著增加,尤其是夏末秋初的8–10月,与冰–海应力几乎相当。增加的大气动量输入带来平均动能增加,埃克曼泵压效应增强,下盐跃层深度加深,增加的大气动量输入进而导致近年来波弗特流涡的显著增强。加拿大海盆南部是大气动量输入的关键区。
  • 图  1  波弗特流涡强度的长期变化(a)及其滑动t检验(b,滑动窗口长度5年)

    Fig.  1  Long term changes (a) and the moving 5-a t-test (b) of Beaufort Gyre strength

    图  2  波弗特流涡内BGEP锚定点流速、WOD盐度和SODA再分析数据的垂直结构

    a−c 中细绿(红)线表示锚定点 1996−2007年(2008−2018 年)的年平均流速。a−c(d−f )中粗蓝、绿和红线表示 1980−1995 年、1996−2007年和2008−2018 年的平均流速(盐度)

    Fig.  2  The velocity vertical structure of BGEP moorings data and SODA reanalysis datasets as well as the salinity vertical structure of WOD data and SODA reanalysis datasets in the Beaufort Gyre

    a−c indicate the annual mean current velocity of three moorings during 1996−2007 (2008−2018) by the thin green (red) lines. a−c (d−f) indicate the mean velocity (salinity) during 1980−1995, 1996−2007 and 2008−2018 by the thick blue, green and red lines

    图  3  1980−1995 年、2008−2018 年 SODA 海面高度异常EOF 分析的前两个空间模态及其对应的时间系数

    a, b(c, d)为1980−1995年(2008−2018年)海面高度异常EOF分解的前两个空间模态,灰色实线为500 m等深线。e,f图是空间模态对应的时间系数,其中粗实线为经过12个月低通滤波的时间系数

    Fig.  3  First two spatial patterns and the corresponding time series of EOF analysis of SODA sea surface height anomalies during 1980−1995 and 2008−2018

    a, b (c, d) show the spatial patterns of EOF of the first two sea level height anomalies during 1980−1995 (2008−2018), and the gray solid line indicates the 500 m isobath. e,f show the time series corresponding to the spatial patterns, and the thick solid line indicate the 12 months low-pass filtering results of the first two modes

    图  4  波弗特流涡范围(a)、断面流速垂直结构(b, c)和断面流量(d)的长期变化

    a中阴影代表2003−2014年的平均海洋动力地形,粗实线分别为1984年、1997年和2012年SODA数据刻画的年平均波弗特流涡范围,灰色实线为选取断面。b, c为1980−1995年和2008−2018年断面流速,负值表示海流向南

    Fig.  4  Beaufort Gyre area (a) as well as the velocity vertical structure (b, c) and the volume transport long term changes (d) of the selected section

    a shows the mean ocean dynamic topography during 2003−2014, by the thick blue, green and red lines indicate annual mean Beaufort gyre area in 1984, 1997 and 2012 derived by SODA datasets, respectively, the gray solid line indicates the selected section. b and c show the section velocity during 1980−1995 and 2008−2018, negative values indicate southward current vector

    图  5  1980−1995年、2008−2018年的盐跃层深度和淡水库深度的空间分布

    Fig.  5  Spatial characteristics of halocline depth and freshwater reservoir depth during 1980−1995 and 2008−2018

    图  6  1980−1995年、2008−2018年的10 m风场、表层流场和海冰漂流场

    Fig.  6  Wind speed at 10 m, sea surface current and sea ice motion during 1980−1995 and 2008−2018

    图  7  上层海洋应力的长期变化、气−海应力和冰−海应力的小波分析

    Fig.  7  Long term changes of upper ocean stress as well as air-ocean stress and ice-ocean stress wavelet analysis

    图  8  气−海应力、冰−海应力的季节变化和夏末秋初(8−10月)上层海洋应力的长期变化

    Fig.  8  Seasonal variations of air-ocean stress and ice-ocean stress as well as long term changes of upper ocean stress in late summer and early autumn (August, September, October)

    图  9  应力旋度和由实测数据计算得到盐跃层深度的长期变化

    b−d给出了实测 CTD 站点的位置(红色点)和波弗特流涡平均范围(黑色实线)。 e−j 中蓝色误差棒为年平均值加减1倍标准差,红色实线为不同时期的变化趋势(第1个时期由于数据样本个数少,未求其趋势)

    Fig.  9  Long term changes of stress curl and halocline depth derived from observed data

    b−d indicate the locations of CTD stations by red dots and the mean Beaufort Gyre area by black solid line. e−j indicate annual mean plus or minus one standard deviation by the blue bar and the trend of different periods by the red solid line (the trend of the first period was not calculated due to lacked of data samples)

    图  10  上层海洋的大气动量输入和流涡强度长期变化

    Fig.  10  Long term changes of Beaufort Gyre strength and upper ocean atmospheric momentum input

    图  11  1980−1995年、2008−2018年的气象要素和上层海洋动能的空间分布和差异

    图中异常指的是各物理量2008−2018年和1980−1995年气候态平均的差异。a中蓝线为加拿大海盆模态,b中绿线为太平洋扇区模态,c中灰色方框为关键区位置

    Fig.  11  Spatial characteristics and difference of meteorological factors as well as upper ocean kinetic energy during 1980−1995 and 2008−2018

    The discrepancy in the figures refers to the physical characteristics difference between the mean state during 2008−2018 and 1980−1995. a. Blue line is the Canada basin mode, b. green line is Pacific sector mode, c. gray box is on behalf of the location of the key area

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出版历程
  • 收稿日期:  2020-12-30
  • 修回日期:  2021-04-30
  • 网络出版日期:  2021-06-21
  • 刊出日期:  2021-07-25

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