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1.
冬春季节北极海冰的年际和年代际变化 总被引：6，自引：0，他引：6
利用1953～1990年海冰密集度资料,研究了冬、春季节北极海冰的时空变化特征.结果表明:冬,春季节海冰变率大的海区主要有巴伦支海、格陵兰海、巴芬湾、戴维斯海峡以及白令海;在巴芬湾、戴维斯海峡和白令海海区,冬季海冰变率比春季的大;冬、春季节喀拉海、巴伦支海海冰面积均与春季白令海海冰面积呈反向变化关系,与巴芬湾、戴维斯海峡海冰面积也存在相反的变化趋势.分析还表明:北极海冰面积还表现出年代际时间尺度变化,尤其在冬季.春季格陵兰海海冰明显存在12年变化周期,而在冬、春季节,喀拉海、巴伦支海海冰存在l0年变化周期. 相似文献
2.
利用北极1°×1°海冰面积指数、海平面气压、500hPa高度场和中国160站气温等资料,运用统计分析方法讨论了戴维斯海峡海冰的长期变化趋势、年代际变化及其与大气环流的关系。结果发现,冬季戴维斯海峡海冰面积呈明显增多趋势,且具有较显著的年代际变化,其长期变化趋势、年代际变化与500hPa高度场的WA型、EU型遥相关、西伯利亚高压及中国北部气温等存在密切的关系。冬季戴维斯海峡海冰在1981年发生突变,突变前后相应高度场、海平面气压场和流场等大气环流场均有显著差异。 相似文献
3.
利用1979~2011年中国东北地区119站气温观测数据,对东北春季寒潮的年代际变化特征进行了分析,并在此基础上通过分析大气环流及北极海冰的变化,对寒潮年代际变化的可能原因进行了探讨。结果表明,东北地区春季寒潮的频次及强度在20世纪80年代末和21世纪初均有明显年代际转折,即20世纪90年代寒潮频次减少而强度增加,21世纪初寒潮频次有所回升但强度减弱。北极新地岛地区海冰的变化可能是造成我国东北地区寒潮活动年代际变化的原因之一。20世纪90年代新地岛附近海冰迅速减少,地表温度明显升高,而高纬海平面气压偏低,此处冷空气不易南下,同时东亚大槽偏强,冷空气强度增加。21世纪初该区海冰减少趋势减缓,冷空气频次有所回升,强度减弱。 相似文献
4.
北极海冰年际变化对东亚中纬度夏季陆面热力异常的指示作用及其可能原因 总被引：1，自引：0，他引：1
本文分析了夏季东亚中纬度近地面温度和春、夏北极海冰时空变化特征,探讨了格陵兰海、巴伦支海海冰异常变化与夏季东亚中纬度陆面热力异常在年际上的可能联系。结果表明:(1)1950—2014年,东亚中纬度夏季近地面温度明显增暖,并伴有明显的年际变化,年际变率最大值的区域主要位于40°N以北至贝加尔湖地区;春、夏格陵兰海和巴伦支海的海冰也呈现明显的减少趋势,同时表现出较强的年际变化特征。(2)春、夏格陵兰海、巴伦支海海冰异常对东亚中纬度夏季陆面热力异常具有一定的指示作用:春、夏格陵兰海、巴伦支海海冰异常偏多,通常对应夏季东亚中纬度近地面的东亚中纬度夏季增暖现象;反之亦然。(3)春、季格陵兰海、巴伦支海北极海冰指数(Arctic Sea Ice Index,ASII)高值年(海冰异常偏多年份),贝加尔湖及西南的蒙古高原地区通常为大范围的异常高压控制,有利于近地面温度升高;同时由于乌拉尔山阻塞高压减弱,极地南下的冷空气减弱,有利于东亚中纬度区域的温度升高。而ASII低值年的情形则相反,贝加尔湖以南地区受异常低压控制,乌拉尔山阻塞高压增强,冷空气易向南侵袭,不利于东亚中纬度近地面升温。 相似文献
5.
6.
北极海冰的气候变化与20世纪90年代的突变 总被引：5，自引：0，他引：5
应用英国Had ley气候研究中心1968~2000年的1°×1°的北半球逐月海冰密集度资料,使用EOF分解等统计方法,探讨北极海冰的气候变化趋势、海冰的突变、海冰的季节持续性和各季的特色。结果表明:(1)自1968年以来,北极海冰的减小是北半球海冰变化的总趋势;海冰的趋势变化在海冰的年际总变化中占有相当重要的地位,可达50%左右。冬春季主要减少区域在格陵兰海、巴伦支海和白令海;夏秋季海冰减少是唯一趋势,中心在北冰洋边缘的喀拉海、拉普捷夫海、东西伯利亚海、楚科奇海、波弗特海。(2)20世纪80年代中后期北极海冰已出现减小趋势,在20世纪90年代,海冰又出现范围和面积的突然减少,中心在格陵兰海和巴伦支海;即海冰减少是加速的,其变化程度已远远超过一般的自然变化。(3)海冰有很好的季节持续性,有很强的隔季相关,也有较好的隔年相关;各季节海冰分布型之间有很好的联系,表现为海冰分布型的总体变化趋势是一致的,在海冰的减少中也体现了分布型的特征。 相似文献
7.
中国地面气温年际和年代际变化及其与北冰洋涛动指数的关系 总被引：8，自引：1，他引：8
利用中国气象局气候中心数据库1958-1994年中国160个测站的月平均温度资料,分析了中国37年气温的年际和年代际变化及其与北冰洋涛动指数的关系.结果表明(1)1958-1994年以来,东北地区全年、秋季和冬季温度上升都很明显,其中冬季最明显;新疆冬季温度升高也很明显;华南夏季温度明显升高.(2)通过对各区温度的年代际变化检验可知,东北全年、秋季和冬季1983年以后温度有非常显著的升高;新疆冬季1976年以后温度也有显著升高;华南夏季1976年以后温度有明显升高.(3)从全国来看,北方各区气候变暖要比南方显著一些,特别是冬季.(4)北冰洋涛动与我国东北温度有十分密切的联系,当AO指数偏小时,冬季冰岛附近海平面气压偏低,西伯利亚高压范围缩小,东亚冬季风比较弱,我国东北冬半年的温度出现明显上升. 相似文献
8.
利用Hadley海冰密集度资料和NCEP/NCAR再分析资料,分析了北极海冰融冰量及其与大气变量年际关系的年代际变化。结果表明,北极海冰存在显著的年代际变化,且有较强的区域性。东西伯利亚海和波弗特海海冰融冰量的平均值变大且方差增大,格陵兰岛以东洋面海冰融冰量的量值和变率均在减弱。对3个不同气候时段内北极海冰融冰量进行EOF分解,前两个模态均在3个气候时段发生显著的年代际变化,东西伯利亚海海冰融冰量的增加与EOF第一模态年代际变化相关,而EOF第二模态则明显造成了波弗特海海冰的年代际消融。并且,与之相应的大气环流也出现了明显的年代际变化,它们与AO/NAO的年际关系也存在年代际转折,融冰量第二模态与AO的年际关系更为紧密,1960—1990年第二模态与AO的相关系数仅为0.186,而1980—2010年相关系数已升高至0.367。整个北冰洋的海冰融冰量与AO的年际关系也出现了年代际增强,尤其是东西伯利亚地区海冰融冰量与AO的年际关系发生了年代际增强,1980—2010年两者相关达到了0.4以上。而波弗特海融冰量与AO相关系数变化较大,1960—1990年其的相关系数高达-0.488,1980年后却减少至0.161。然而AO却未发生明显的年代际变化。造成北极海冰融冰量及其与大气变量年际关系发生年代际变化的主要因子之一是波弗特高压,其年代际减弱使得极区向东西伯利亚海和波弗特海的海冰输送减弱,导致这两个区域海冰减少,使得AO与北极海冰的年际关系发生了年代际转折。 相似文献
9.
基于一个全球气-海-冰耦合模式数值模拟结果,对北半球高纬度地区年际尺度的气-海-冰相互作用进行了分析。在所使用的全球气-海-冰耦合模式中,大气环流模式和陆面过程模式来自国家气候中心,海洋环流模式和海冰模式来自中国科学院大气物理研究所大气科学和地球流体力学数值模拟国家重点实验室。采用一种逐日通量距平耦合方案实现次网格尺度海冰非均匀条件下大气环流模式和海洋环流模式在高纬地区的耦合。只对50 a模拟结果中的后30 a结果进行了分析。在分析中,首先对滤波后的北半球高纬度地区海平面气压、表面大气温度、海表面温度、海冰密集度及海表面感热通量的标准化距平做联合复经验正交函数分解,取第一模进行重建,然后讨论了在一个循环周期(约4 a)中北半球高纬度地区气-海-冰的作用关系。结果表明:(1)当北大西洋涛动处于正位相时,格陵兰海出现南风异常,使表面大气温度升高,海洋失去感热通量减少,海洋表面温度升高,海冰密集度减小;当北大西洋涛动处于负位相时,格陵兰海出现北风异常,使表面大气温度降低,海洋失去感热通量增多,海洋表面温度降低,海冰密集度增加。巴伦支海变化特点与格陵兰海相似,但在时间上并不完全一致。(2)多年平均而言,北冰洋内部靠近极点区域为冷中心。当北冰洋内部为低压异常时,因异常中心偏向太平洋一侧,使北冰洋内部靠近太平洋部分为暖平流异常,靠近大西洋一侧为冷平流异常。伴随着暖、冷平流异常,这两侧分别出现暖异常和冷异常,海表面给大气的感热通量分别偏少和偏多,上述海区海表面温度分别偏高和偏低,海冰密集度分别偏小和偏大。当北冰洋内部为高压异常时特点正好与上述相反。由上述分析结果可知,在海洋、大气年际循环中,大尺度大气环流变率起主导作用,海洋表面温度和海冰密集度变化主要是对大气环流变化的响应。 相似文献
10.
南、北极海冰的时空演变特征 总被引：7，自引：4，他引：3
利用海水面积指数,分析了南、北极海冰年际时间尺度的时空演变特征。结果表明：南极海冰具有明显的年际振荡。南极夏季海水年际异常具有一定的整体性,秋、冬、春季海冰年际异常则表现出较强的区域性。北极海冰也具有显著的年际振荡。北极冬、春季海冰年际异常主要发生在格陵兰海、巴伦支海和喀拉海,夏、秋季海冰年际异常主要发生在东西伯利亚和海和波旨特海。 相似文献
11.
北极海冰与ENSO事件在准四年时间尺度上的可能联系 总被引：4，自引：0，他引：4
分析了北极海冰的变化规律及其与ENSO循环在准四年时间尺度上的可能联系.结果表明(59.5～179.5°E,60.5～89.5.N)的高纬海域范围内(包括喀拉海、拉普捷夫海及东西伯利亚海,简称为A区)的北极海冰变化以9月份变率最大并具有准四年周期,在这个周期段上A区极冰与Nino 3区的海温变化有明显的位相差.当Nino 3区SST滞后海冰约16个月时,两者达到最大负相关.A区的9月海冰面积指数和SST的时滞相关系数分布表明,次年4月开始在赤道东太平洋区域出现一显著负相关区,次两年的2月负相关达到最大,之后减弱消失.这表明9月A区海冰面积偏小,则次年春季以后出现E1 Nin0现象.海冰与环流相关分析表明,其相互影响机制可能是由于少冰年的弱冷源效应,使得该地区上空气旋环流发展,并通过中高纬相互作用促进北太平洋西北部及东亚沿岸距平气旋式环流的发展,有利于赤道异常西风形成从而触发和维持El Nino事件的产生和发展. 相似文献
12.
Using monthly mean sea ice velocity data obtained from the International Arctic Buoy Programme (IABP) for the period of 1979–1998 and the monthly mean NCEP/NCAR re-analysis dataset (1960–2002), we investigated the spatiotemporal evolution of the leading sea ice motion mode (based on a complex correlation matrix constructed of normalized sea ice motion velocity) and their association with sea level pressure (SLP) and the predominant modes of surface wind field variability. The results indicate that the leadi... 相似文献
13.
R. L. Raddatz R. J. Galley B. G. Else T. N. Papakyriakou M. G. Asplin L. M. Candlish 《大气与海洋》2014,52(2):125-141
The data-collection campaign for the 2008 International Polar Year–Circumpolar Flaw Lead System Study saw the Canadian Coast Guard Ship (CCGS) Amundsen, a research icebreaker, overwinter in high-concentration unconsolidated sea ice in Amundsen Gulf. Environmental monitoring continued into the open-water season. During this period, the Amundsen registered five relatively deep mean sea-level pressure minima (less than 100?kPa). Three were selected for further analysis based on season and the nature of the underlying ocean or sea-ice surface: (1) a winter pressure minimum over unconsolidated sea ice, (2) a spring pressure minimum which likely contributed to the break-up of the sea-ice cover on Amundsen Gulf, and (3) a summer pressure minimum over open water. The characteristics of these pressure minima and the impact of their passage on the atmospheric boundary layer and on the sea-ice cover as they crossed Amundsen Gulf were examined. Several features were revealed by the analysis. (1) The winter and summer pressure minima were migratory cyclones accompanied by Arctic frontal waves with characteristics very similar to the polar frontal waves associated with the migratory cyclones found at more southerly latitudes, whereas the spring pressure minimum was attributed to an Arctic frontal trough of low pressure with the cyclonic centre remaining south of the Gulf. (2) The passage of the frontal-wave cyclone in winter and the frontal trough of low pressure in spring disrupted the equilibrium that had been established during more settled periods between the atmospheric boundary layer and the mosaic surface (leads, polynyas, and sea ice); however, equilibrium was quickly re-established. (3) In summer, the thermal structure of the lower atmospheric boundary layer persisted through the passage of the frontal-wave cyclone over the open-water surface. (4) The passage of the frontal-wave cyclone in winter and the frontal trough of low pressure in spring modified the mesoscale sea-icescape. 相似文献
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15.
Synoptic-scale atmospheric circulation patterns drive wind forcing of dynamic and thermodynamic processes in Arctic sea ice. Synoptic typing and compositing are common techniques used to identify a limited number of prevailing weather classifications that govern a region's climate. This work investigates atmospheric circulation patterns (surface to 250?hPa) for the southern Beaufort Sea and corresponding surface wind regimes within each synoptic type. Significant changes (p?<?0.05) in relative frequencies of a number of synoptic types were attributed to declining summer sea ice. Corresponding upper-level circulation anomalies show increasingly meridional atmospheric circulation. Synoptic Types 9 and 11 were identified as key October-November-December circulation features that represent deepening of the Aleutian low with concomitant strengthening of pressure gradients over the southern Beaufort Sea. Classification of coastal-based wind observations shows a shift towards increased easterly wind forcing. A case study of surface wind data from the CCGS Amundsen (2009–2011) provided a direct example of the surface wind regime within the marginal ice zone within each synoptic type during a period of reduced Arctic sea-ice cover. 相似文献
16.
冬季北极海冰运动主模态的构成及其与海平面气压变化的关系 总被引：2，自引：0，他引：2
利用国际北极浮冰运动观测资料（IABP）（1979-1998）以及NCEP／NCAR月平均海平面气压再分析资料（1960-2002）,通过求解海冰运动异常的复斜方差矩阵,研究了冬季北极海冰运动主模态构成及其与海平面气压变化的关系。冬季海冰运动主模态是由两个海冰运动优势模态的一个线性组合构成,与这两个运动优势模态有直接关系的海平面气压变化主要发生在北极海盆及其边缘海区。尽管北极涛动（北大西洋涛动）通过影响海平面气压进而影响北极海冰运动,但是,北极涛动（北大西洋涛动）并不是决定海冰运动主模态的关键性因素。 相似文献
17.
北极楚克奇海上空臭氧垂直变化的探测与分析 总被引：2，自引：0，他引：2
1999年夏季,中国首次组织北极地区科学考察.分析此次考察中楚克奇海海域上空获得的大气结构和臭氧探空资料,结合臭氧总量观测光谱仪(TOMS)臭氧总量和NCEP大气环流资料,指出:考察期间楚克奇海海域上空臭氧总量与13 km以下臭氧含量关系密切,而在20 km附近最大臭氧浓度处的臭氧变化与大气臭氧总量关系较差,表明整层臭氧总量的变化主要受低层大气臭氧变化的影响.大气臭氧总量呈高-低-高变化,对流层顶高度呈低-高-低变化,分析500hPa高度场表明:考察期间的天气系统可能是造成局地臭氧变化的主要原因. 相似文献
18.
Associations between the autumn Arctic sea ice concentrations (SICs) and North American winter precipitation were examined using singular value decomposition. The results show that a reduced SIC in the majority of the Arctic is accompanied by dry conditions over the Great Plains, the southern United States, Mexico, eastern Alaska, and southeastern Greenland, and by wet conditions over the majority of Canada, the northeastern United States, and the majority of Greenland. Atmospheric circulation anomalies associated with the SIC variability show a wave train structure that is persistent from autumn to winter and is responsible for the covariability between the autumn Arctic SICs and North American winter precipitation. This relationship suggests a potential long-term outlook for the North American winter precipitation. 相似文献
19.
WANG Xuezhong SUN Zhaobo HU Banghui TAN Yanke ZENG Gang 《Acta Meteorologica Sinica》2012,26(2):189-204
Based on the simulated ice thickness data from 1949 to 1999, monthly mean temperature data from 160
stations, and monthly mean 1°×1° precipitation data reconstructed from 749 stations in China from 1951 to
2000, the relationship between the Arctic sea ice thickness distribution and the climate of China is analyzed
by using the singular value decomposition method. Climate patterns of temperature and precipitation are
obtained through the rotated empirical orthogonal function analysis. The results are as follows. (1) Sea ice
in Arctic Ocean has a decreasing trend as a whole, and varies with two major periods of 12-14 and 16-20
yr, respectively. (2) When sea ice is thicker in central Arctic Ocean and Beaufort-Chukchi Seas, thinner in
Barents-Kara Seas and Baffin Bay-Labrador Sea, precipitation is less in southern China, Tibetan Plateau,
and the north part of northeastern China than normal, and vice versa. (3) When sea ice is thinner in the
whole Arctic seas, precipitation is less over the middle and lower reaches of Yellow River and north part of
northeastern China, more in Tibetan Plateau and south part of northeastern China than normal, and the
reverse is also true. (4) When sea ice is thinner in central Arctic Ocean, East Siberian Sea, Beaufort-Chukchi
Seas, and Greenland Sea; and thicker in Baffin Bay-Labrador Sea, air temperature is higher in northeastern
China, southern Tibetan Plateau, and Hainan Island than normal. (5) When sea ice is thicker in East
Siberian Sea 5 months earlier, thinner in Baffin Bay-Labrador Sea 7-15 months earlier, air temperature is
lower over the north of Tibetan Plateau and higher in the north part of northwestern China than normal,
and a reverse correlation also exists. 相似文献
20.
This paper evaluates the simulation of Arctic sea ice states using an ocean-ice coupled model that employs LASG/IAP(the State Key Laboratory of Numerical Modeling for Atmospheric Sciences and Geophysical Fluid Dynamics/the Institute of Atmospheric Physics) Climate Ocean Model(LICOM) and the sea-ice model from the Bergen Climate Model(BCM).It is shown that the coupled model can reasonably reproduce the major characteristics of the mean state,annual cycle,and interannual variability of the Arctic sea ice concentration.The coupled model also shows biases that were generally presented in other models,such as the underestimation of summer sea ice concentration and thickness as well as the unsatisfactory sea ice velocity.Sensitivity experiments indicate that the insufficient performance of the ocean model at high latitudes may be the main reason for the biases in the coupled model.The smoother and the fake "island",which had to be used due to the model’s grid in the North Pole region,likely caused the ocean model’s weak performance.Sea ice model thermodynamics are also responsible for the sea ice simulation biases.Therefore,both the thermodynamic module of the sea ice component and the model grid of the ocean component need to be further improved. 相似文献