Page 62 - 《高原气象》2021年第5期
P. 62
5 期 刘雅静等:NCEP CFSv2对北半球平流层极涡边界年代际变化特征模拟的评估 1023
学,6:1191-1206. 熊光明,陈权亮,朱克云,等,2012. 平流层极涡变化与我国冬季气
陆春晖,丁一汇,张莉,2014. BCC_AGCM2. 1 模式对平流层环流变 温、降水的关系[J]. 高原气象,31(4):1001-1006.
化特征的数值模拟及其模式评估[J]. 气象学报,72(1):49-61. 易明建,2009. 平流层极涡异常及其对对流层的影响研究[D]. 合
沈柏竹,廉毅,李尚锋,等,2010. 北半球对流中,上层及平流层极涡 肥:中国科学技术大学.
特征初步分析[J]. 吉林大学学报:地球科学版,(S1):140-145. 张恒德,2005. 极涡的活动特征与数值模拟及其对我国气候的影响
王嘉禾,2018. 东亚典型极端低温事件中大尺度环流系统组合性异 [D]. 南京:南京信息工程大学.
常特征研究[D]. 兰州:兰州大学. 张婧雯,李栋梁,柳艳菊,2014. 北半球极涡新特征及其对中国冬
韦志刚,朱献,董文杰,等,2019. CFSv2 系统对 2015 年 11 月中国 季气温的影响[J]. 高原气象,33(3):721-732. DOI:10. 7522/
一次寒潮过程及其欧亚冷空气活动的预报评估[J]. 高原气象, j. issn. 1000-0534. 2013. 00044.
38(4):673-684. DOI:10. 7522/j. issn. 1000-0534. 2019. 00014. 周宁芳,贾小龙,2018. NCEP CFSv2对北半球夏季中高纬阻塞高压
谢韶青,卢楚翰,2018. 近 16 a 来冬季欧亚大陆中纬度地区低温事 的预测检验[J]. 高原气象,37(2):469-480. DOI:10. 7522/j.
件频发及其成因[J]. 大气科学学报,41(3):423-432. issn. 1000-0534. 2017. 00036.
Evaluation on Simulation of the Inter-decadal Variation Characteristics
of the Stratospheric Polar Vortex Boundary in the Northern
Hemisphere by NECP CFSv2
LIU Yajing ,WEI Zhigang ,CHEN Guangyu ,LIU Yujia 1
1
2
1
(1. State Key Laboratory of Earth Surface Processes and Resource Ecology,Faculty of Geographical Science,
Beijing Normal University,Beijing 100875,China;
2. Key Laboratory of Wind Power Technology of Zhejiang Province,Zhejiang Windey
Company Limited,Hangzhou 310012,Zhejiang,China)
Abstract:By using the ERA-I,the NECP CFSR reanalysis data and the CFSv2 of NECP reforecasts and fore‐
casts data,the inter-decadal variations of the stratospheric polar vortex boundary in the northern hemisphere
since the 1980s are analyzed,the ability of the CFSv2 to simulate the polar vortex boundary is evaluated. Results
show that,from 1980 to 2017,the Arctic polar vortex retreats northward in North American and expands south‐
ward in Eurasia in winter,but the polar vortex expands in North America and retreats in Europe in autumn. The
polar vortex expands obviously from the 1980s to the 2000s and retreats in the 2010s in Asia. In winter,the re‐
traction of the polar vortex occurs mainly in the 1990s in North America,but the expansion of the polar vortex
occurs mainly in the 2000s in Europe and in the 1990s in Asia. In autumn,the southern expansion of the polar
vortex boundary in North America is mainly in the 1990s,the retraction of polar vortexes in Eurasia occurs in the
2010s,and the retraction in Western Europe is the most obvious. The overall trend of the winter polar vortex
boundary and area simulated by CFSv2 is consistent with the ERA-I data in the 1980s-2010s,especially for the
trend of expansion in North America and Asia in the 2010s. However,the boundary of the polar vortex simulated
by CFSv2 is more to the east,and more to the south in the 2010s in North America. The boundary of the polar
vortex simulated by CFSv2 is north in the 1990s and south in the 2010s in Europe. The expansions of Asia polar
vortex boundary in the 1990s and 2000s in Asia cannot be simulated. In autumn,the simulation abilities of
CFSv2 on the boundary positions and areas are poor than that in the winter,the simulations on the overall trend
of polar vortex boundary and area variation are poor. The North American polar vortex boundaries simulated by
CFSv2 are consistent with the ones of the ERA-I data in 1990s-2010s,but the range of expansion is larger in the
1990s. The retraction of the polar vortex boundary is mainly in the 2000s from CFSv2 while in the 2010s from
ERA-I in Europe. The polar vortex boundary simulated by CFSv2 is consistent in the 1990s but exists more errors
in the 2000s-2010s with the one of the ERA-I data in Asia.
Key words:Polar vortex;boundary;simulation;evaluation