Arctic Dipole as primary driver of summer LKF variability in a high-resolution ice-ocean model
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摘要: 观测手段的局限性长期以来制约着对北极线性运动学特征(LKF)的深入研究。本研究基于一套为期28 a、水平分辨率约为2 km的全北极冰海耦合模式数据,并结合冬季RGPS观测资料(1996–2008年)进行验证,系统分析了北极LKF的长期变化及其气候驱动因子。结果表明,尽管北极海冰持续减薄可能促进冰内断裂,但全北极范围的LKF数量和密度并未呈现显著趋势,仅表现出极其微弱的增长(0.003 a−1)。模型模拟的冬季LKF密度与RGPS观测具有较好的一致性(r = 0.57),证实了模型在刻画LKF空间分布与季节变化方面的可靠性。此外,夏季LKF密度与北极偶极子(AD指数)存在强烈的负相关关系(r = −0.66),其影响力明显超过北极涛动(AO)。在空间分布上,AO与AD指数均与中央北极区夏季LKF密度呈负相关,而在喀拉海和巴伦支海,LKF密度与AO指数呈正相关,与AD指数呈负相关。这种区域响应的非均匀性,最终导致全北极尺度上夏季LKF密度与AD指数的负相关关系更为突出。
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关键词:
- 北极线性运动特征 /
- 北极偶极子 /
- 海冰形变 /
- 高分辨率冰海耦合模式
Abstract: Observational limitations constrain long-term studies of Arctic linear kinematic features (LKFs). This study systematically analyzes the long-term changes of Arctic LKFs and their climate drivers using a 28-year, ~2 km resolution pan-Arctic sea ice-ocean simulation, validated against winter RGPS data (1996–2008). We find no pronounced trend in pan-Arctic LKF number or density, though a very weak increase (0.003 a−1) aligns with thinning-enhanced fracturing. Modeled winter LKF density correlates well with RGPS observations (r = 0.57), confirming the model’s reliability in capturing the spatial distribution and seasonal variations of LKFs. Summer LKF density shows a strong negative correlation with the Arctic Dipole (AD) (r = −0.66), exceeding the Arctic Oscillation (AO) influence. While both AO and AD correlate negatively with LKF density in the central Arctic, LKF density correlates positively with AO but negatively with AD in the Kara Sea and Barents Sea, resulting in an overall stronger negative correlation with AD. -
图 1 海冰形变场与LKF的时空分布
a−d. 分别展示了根据模型输出得出的1995年3月1日、6月1日、9月1日和12月1日的海冰形变场;e−h. 为使用检测与追踪算法识别出的相应LKF,并使用形态学细化算法缩减为单像素宽度。形变率超过 0.5 d−1 的值以深红色显示,以突出强烈形变区域;i−an. 为2000、2005、2010和2015年对应的形变场与检测到的LKF。LKF时空分布图中,红色虚线与绿色实线分别表示海冰密集度为0.15与0.7
Fig. 1 Spatio-temporal distribution of sea ice deformation fields and LKFs
a−d. Sea ice deformation fields derived from model outputs on March 1, June 1, September 1, and December 1, 1995; e−h. corresponding LKFs identified using a detection and tracking algorithm and subsequently reduced to single-pixel width via a morphological thinning algorithm. Deformation rates exceeding 0.5 d−1 are highlighted in dark red to denote regions of intense deformation; i−an. deformation fields and detected LKFs for the years 2000, 2005, 2010 and 2015. In LKFs’ spatio-temporal distribution figures, the red dashed line and the green solid line represent sea ice concentrations of 0.15 and 0.7, respectively
图 2 LKF数量(a)与LKF密度(b)的时间序列与长期趋势
灰色实线表示模拟的LKF数量/密度时间序列,蓝色圆点代表RGPS观测数据。两条时间序列均经过其众数值归一化。黑色与红色虚线分别表示模拟数据与观测数据的线性趋势,绿色虚线则对应RGPS观测期内模拟数据的趋势
Fig. 2 Time series and long-term trends of LKF number (a) and LKF density (b)
Solid gray lines represent simulated LKF number/density time series, and blue dots represent RGPS observations. Both time series are normalized by their respective modal values. Black and red dashed lines indicate the linear trends of the simulated and observed data, respectively. Green dashed line indicates the trend of the simulated data over the RGPS observational period
图 3 LKF数量(a)与LKF密度(b)的季节变化
蓝色与红色实线分别代表模拟结果与 RGPS 观测的平均季节变化,其周围阴影带表示基于两周移动窗口计算的标准差。时间序列数据均经其众数值归一化处理。阴影反映了所有可用年份(模拟数据:1992–2019 年,RGPS 数据:1996–2008 年)内的年际变异性
Fig. 3 Seasonal variations in LKF number (a) and LKF density (b)
Solid blue and red lines denote the mean seasonal cycles from the simulation and RGPS observations, respectively, with surrounding shaded bands representing the standard deviation calculated with a two-week moving window. All time series are normalized by their respective modal values. Shadings reflect interannual variability across all available years (simulation: 1992–2019, RGPS: 1996–2008)
图 4 对SLP进行EOF分解所选取的区域(红色区域)(a)和不同海区的划分(b)
a. 该区域排除了在1992–2019年研究期间未被海冰持续覆盖的陆地和开阔海域;b. 依据美国国家冰雪数据中心(NSDIC)定义的区域划分方案绘制
Fig. 4 Region (the red area) selected for EOF decomposition of SLP (a) , and division of different sea regions (b)
a. The region excludes land and open ocean areas which were not continuously covered by sea ice during the study period 1992–2019; b. mapped according to the regional division scheme defined by the National Snow and Ice Data Center (NSIDC)
图 5 模拟 LKF密度与AO、AD指数在冬季(11月至次年5月)(a) 和夏季(6–10月)(b)期间的归一化时间序列;冬季 AO+(c)、冬季 AD+(d)、夏季 AO+(e)、夏季 AD+(f) 的空间分布;LKF 发生概率的空间分布:年平均值(1992–2019年)(g) ,夏季(6–10月)(h),冬季(11月至次年5月)(i)
a, b.相关系数在图例中标注为 cor。灰色与蓝色实线分别代表 AO指数(PC1) 和 AD 指数(PC2),红色与绿色实线分别表示模拟的与观测的(RGPS)LKF 密度。LKF 密度与 AO、AD 指数均经过方差标准化处理;c–f. 各图中标注了其解释方差(Var);g–i. 由于 LKF 宽度在检测中被简化表示,图中LKF出现概率值低于实际值
Fig. 5 Simulated LKF density and normalized time series of AO and AD indices during winter (November–May) (a) and summer (June–October) (b); spatial patterns of winter AO+ (c), winter AD+ (d), summer AO+ (e), and summer AD+ (f); spatial distribution of LKF occurrence probability: annual mean (1992–2019) (g) , summer (June–October) (h) , winter (November–May) (i)
a, b. Correlation coefficients denoted as “cor” in the legend. Solid gray and blue lines represent the AO (PC1) and AD (PC2) indices respectively, while solid red and green lines represent the simulated and observed (RGPS) LKF densities respectively. Both LKF densities and the AO and AD indices are normalized by their variances; c–f. explained variance (Var) is indicated in each panel; g–i. the LKF occurrence probability values shown in the panel are lower than the actual values due to the simplified representation of LKF width in the detection process
图 6 夏季北极8个海区LKF密度与大气环流的关系
每个海区展示3个散点图:LKF密度与AO指数的关系(a, d, g, j, m, p, s, v)、LKF密度与AD指数的关系(b, e, h, k, n, q, t, w)和LKF密度与SLP指数的关系(c, f, i, l, o, r, u, x)。LKF密度数据已进行去均值及标准差归一化处理。黑色圆点表示月平均数据,蓝色线条表示线性回归拟合线。各子图右上方显示统计信息,包括回归斜率(α)、标准误差(SE)和p值(若p > 0.05则标为红色)。通过学生t检验(p < 0.05)的回归系数以黑色显示,未通过以红色显示
Fig. 6 Relationships between LKF density and atmospheric circulation in eight Arctic sea regions during summer
There are three scatter plots for each region: LKF density versus AO indices (a, d, g, j, m, p, s, v), LKF density versus AD indices (b, e, h, k, n, q, t, w) and LKF density versus SLP indices (c, f, i, l, o, r, u, x). LKF density data have been normalized by standard deviation. Black dots represent monthly mean data, and blue lines indicate linear regression fits. Statistical information is shown in the upper right corner of each subplot, including regression slope (α), standard error (SE), and p-value (p > 0.05 shown in red). Regression coefficients that pass the Student’s t-test (p < 0.05) are shown in black, while those do not are shown in red
图 7 夏季AO正位相与AD正位相期间各物理量异常场的合成分析
a–h. AO+位相期间的异常场:海平面气压梯度(a),10 m风速(b),海冰漂移速度(c),海冰密集度(d),海冰厚度(e),海冰形变率(f),海冰覆盖天数(g)和归一化LKF 密度(h);i–p. AD+位相期间对应的异常场,排列顺序同(a–h)
Fig. 7 Composite analysis of anomalous fields of physical variables during summer AO positive phase and AD positive phase
a–h. Anomalous fields during the AO+ phase: sea level pressure gradient (a), 10 m wind speed (b), sea ice drift velocity (c), sea ice concentration (d), sea ice thickness (e), sea ice deformation rate (f), sea ice cover days (g), and normalized LKF density (h); i–p. corresponding anomalous fields during the AD+ phase, arranged in the same order as (a–h)
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[1] Shokr M, Sinha N K. Sea Ice: Physics and Remote Sensing[M]. Hoboken, United States: John Wiley & Sons, 2015. [2] Leppäranta M. The Drift of Sea Ice[M]. 2nd ed. Berlin, Heidelberg: Springer, 2011. [3] Kwok R. Deformation of the Arctic Ocean sea ice cover between November 1996 and April 1997: a qualitative survey[M]//Dempsey J P, Shen H H. IUTAM Symposium on Scaling Laws in Ice Mechanics and Ice Dynamics. Dordrecht: Springer, 2001: 315−322. [4] Maykut G A. Large-scale heat exchange and ice production in the Central Arctic[J]. Journal of Geophysical Research: Oceans, 1982, 87(C10): 7971−7984. doi: 10.1029/JC087iC10p07971 [5] Alam A, Curry J A. Evolution of new ice and turbulent fluxes over freezing winter leads[J]. Journal of Geophysical Research: Oceans, 1998, 103(C8): 15783−15802. doi: 10.1029/98JC01188 [6] Lüpkes C, Vihma T, Birnbaum G, et al. Influence of leads in sea ice on the temperature of the atmospheric boundary layer during polar night[J]. Geophysical Research Letters, 2008, 35(3): L03805. doi: 10.1029/2007GL032461 [7] Rampal P, Weiss J, Marsan D. Positive trend in the mean speed and deformation rate of Arctic sea ice, 1979−2007[J]. Journal of Geophysical Research: Oceans, 2009, 114(C5): C05013. doi: 10.1029/2008JC005066 [8] Bates N R, Mathis J T. The Arctic Ocean marine carbon cycle: evaluation of air-sea CO2 exchanges, ocean acidification impacts and potential feedbacks[J]. Biogeosciences, 2009, 6(11): 2433−2459. doi: 10.5194/bg-6-2433-2009 [9] Kupiszewski P, Leck C, Tjernström M, et al. Vertical profiling of aerosol particles and trace gases over the central Arctic Ocean during summer[J]. Atmospheric Chemistry and Physics, 2013, 13(24): 12405−12431. doi: 10.5194/acp-13-12405-2013 [10] Castellani G, Lüpkes C, Hendricks S, et al. Variability of Arctic sea-ice topography and its impact on the atmospheric surface drag[J]. Journal of Geophysical Research: Oceans, 2014, 119(10): 6743−6762. doi: 10.1002/2013JC009712 [11] Landy J C, Ehn J K, Barber D G. Albedo feedback enhanced by smoother Arctic sea ice[J]. Geophysical Research Letters, 2015, 42(24): 10714−10720. doi: 10.1002/2015GL066712 [12] Salganik E, Lange B A, Itkin P, et al. Different mechanisms of Arctic first-year sea-ice ridge consolidation observed during the MOSAiC expedition[J]. Elementa: Science of the Anthropocene, 2023, 11(1): 00008. doi: 10.1525/elementa.2023.00008 [13] Hunkins K. The oceanic boundary layer and stress beneath a drifting ice floe[J]. Journal of Geophysical Research, 1975, 80(24): 3425−3433. doi: 10.1029/JC080i024p03425 [14] Lindsay R W, Rothrock D A. Arctic sea ice leads from advanced very high resolution radiometer images[J]. Journal of Geophysical Research: Oceans, 1995, 100(C3): 4533−4544. doi: 10.1029/94JC02393 [15] Willmes S, Heinemann G. Daily pan-Arctic sea-ice lead maps for 2003−2015, with links to maps in NetCDF format[DS/OL]. Bremerhaven: PANGAEA, 2015. Doi: 10.1594/PANGAEA.854411. [16] Hoffman J P, Ackerman S A, Liu Yinghui, et al. Application of a convolutional neural network for the detection of sea ice leads[J]. Remote Sensing, 2021, 13(22): 4571. doi: 10.3390/rs13224571 [17] Murashkin D, Spreen G, Huntemann M, et al. Method for detection of leads from Sentinel-1 SAR images[J]. Annals of Glaciology, 2018, 59(76pt2): 124−136. doi: 10.1017/aog.2018.6 [18] Murashkin D, Spreen G. Sea ice leads detected from Sentinel-1 SAR images[C]//Proceedings of 2019 IEEE International Geoscience and Remote Sensing Symposium (IGARSS 2019). Yokohama, Japan: IEEE, 2019: 174−177. [19] Bouchat A, Hutter N, Chanut J, et al. Sea Ice Rheology Experiment (SIREx): 1. Scaling and statistical properties of sea-ice deformation fields[J]. Journal of Geophysical Research: Oceans, 2022, 127(4): e2021JC017667. doi: 10.1029/2021JC017667 [20] Hutter N, Losch M, Menemenlis D. Scaling properties of Arctic sea ice deformation in a high-resolution viscous-plastic sea ice model and in satellite observations[J]. Journal of Geophysical Research: Oceans, 2018, 123(1): 672−687. doi: 10.1002/2017JC013119 [21] Wang Q, Danilov S, Jung T, et al. Sea ice leads in the Arctic Ocean: model assessment, interannual variability and trends[J]. Geophysical Research Letters, 2016, 43(13): 7019−7027. doi: 10.1002/2016GL068696 [22] Hutter N, Zampieri L, Losch M. Leads and ridges in Arctic sea ice from RGPS data and a new tracking algorithm[J]. The Cryosphere, 2019, 13(2): 627−645. doi: 10.5194/tc-13-627-2019 [23] Deser C, Walsh J E, Timlin M S. Arctic sea ice variability in the context of recent atmospheric circulation trends[J]. Journal of Climate, 2000, 13(3): 617−633. doi: 10.1175/1520-0442(2000)013<0617:ASIVIT>2.0.CO;2 [24] Maslanik J A, Fowler C, Stroeve J, et al. A younger, thinner Arctic ice cover: increased potential for rapid, extensive sea-ice loss[J]. Geophysical Research Letters, 2007, 34(24): L24501. doi: 10.1029/2007GL032043 [25] Bi Haibo, Wang Yunhe, Liang Yu, et al. Influences of summertime Arctic dipole atmospheric circulation on sea ice concentration variations in the pacific sector of the Arctic during different pacific decadal oscillation phases[J]. Journal of Climate, 2021, 34(8): 3003−3019. doi: 10.1175/JCLI-D-19-0843.1 [26] Marshall J, Adcroft A, Hill C, et al. A finite-volume, incompressible Navier Stokes model for studies of the Ocean on parallel computers[J]. Journal of Geophysical Research: Oceans, 1997, 102(C3): 5753−5766. doi: 10.1029/96JC02775 [27] Schaffer J, Timmermann R, Arndt J E, et al. A global, high-resolution data set of ice sheet topography, cavity geometry, and ocean bathymetry[J]. Earth System Science Data, 2016, 8(2): 543−557. doi: 10.5194/essd-8-543-2016 [28] Kobayashi S, Ota Y, Harada Y, et al. The JRA-55 reanalysis: general specifications and basic characteristics[J]. Journal of the Meteorological Society of Japan. Ser. II, 2015, 93(1): 5−48. doi: 10.2151/jmsj.2015-001 [29] Griffies S M, Danabasoglu G, Durack P J, et al. OMIP contribution to CMIP6: experimental and diagnostic protocol for the physical component of the Ocean Model Intercomparison Project[J]. Geoscientific Model Development, 2016, 9(9): 3231−3296. doi: 10.5194/gmd-9-3231-2016 [30] Zhang Jinlun, Thomas D R, Rothrock D A, et al. Assimilation of ice motion observations and comparisons with submarine ice thickness data[J]. Journal of Geophysical Research: Oceans, 2003, 108(C6): 3170. doi: 10.1029/2001JC001041 [31] Large W G, McWilliams J C, Doney S C. Oceanic vertical mixing: a review and a model with a nonlocal boundary layer parameterization[J]. Reviews of Geophysics, 1994, 32(4): 363−403. doi: 10.1029/94RG01872 [32] Leith C E. Stochastic models of chaotic systems[J]. Physica D: Nonlinear Phenomena, 1996, 98(2/4): 481−491. doi: 10.1016/0167-2789(96)00107-8 [33] Hibler III W D. A dynamic thermodynamic sea ice model[J]. Journal of Physical Oceanography, 1979, 9(4): 815−846. doi: 10.1175/1520-0485(1979)009<0815:ADTSIM>2.0.CO;2 [34] Zhang Jinlun, Hibler III W D. On an efficient numerical method for modeling sea ice dynamics[J]. Journal of Geophysical Research: Oceans, 1997, 102(C4): 8691−8702. doi: 10.1029/96JC03744 [35] Hutter N, Losch M. Feature-based comparison of sea ice deformation in lead-permitting sea ice simulations[J]. The Cryosphere, 2020, 14(1): 93−113. doi: 10.5194/tc-14-93-2020 [36] Hutter N, Bouchat A, Dupont F, et al. Sea ice rheology experiment (SIREx): 2. Evaluating linear kinematic features in high-resolution sea ice simulations[J]. Journal of Geophysical Research: Oceans, 2022, 127(4): e2021JC017666. doi: 10.1029/2021JC017666 [37] Hutter N, Zampieri L, Losch M. Linear kinematic features (leads & pressure ridges) detected and tracked in RADARSAT Geophysical Processor System (RGPS) sea-ice deformation data from 1997 to 2008[DS/OL]. Bremerhaven: PANGAEA, 2019. Doi: 10.1594/PANGAEA.898114. [38] Kwok R. The RADARSAT geophysical processor system[M]//Tsatsoulis C, Kwok R. Analysis of SAR Data of the Polar Oceans. Berlin, Heidelberg: Springer, 1998: 235−257. [39] Hersbach H, Bell B, Berrisford P, et al. ERA5 monthly averaged data on single levels from 1940 to present[DS/OL]. Brussels: Copernicus Climate Change Service (C3S) Climate Data Store (CDS), 2023. Doi: 10.24381/cds.f17050d7. [40] Linow S, Dierking W. Object-based detection of linear kinematic features in sea ice[J]. Remote Sensing, 2017, 9(5): 493. doi: 10.3390/rs9050493 [41] Diebold F X, Rudebusch G D, Göbel M, et al. When will Arctic sea ice disappear? Projections of area, extent, thickness, and volume[J]. Journal of Econometrics, 2023, 236(2): 105479. doi: 10.1016/j.jeconom.2023.105479 [42] Thompson D W J, Wallace J M. The Arctic Oscillation signature in the wintertime geopotential height and temperature fields[J]. Geophysical Research Letters, 1998, 25(9): 1297−1300. doi: 10.1029/98GL00950 [43] Wu Bingyi, Wang Jia, Walsh J E. Dipole anomaly in the winter Arctic atmosphere and its association with sea ice motion[J]. Journal of Climate, 2006, 19(2): 210−225. doi: 10.1175/JCLI3619.1 [44] Weiss J. Sea ice deformation[M]//Weiss J. Drift, deformation, and fracture of sea ice. Dordrecht: Springer, 2013: 31−51. -
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