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1.
东北地区汛期降水与全球大洋海温异常关系的SVD分析 总被引：3，自引：0，他引：3
利用中国160站月平均降水量资料和英国气象局整编的1950.1～1998.12全球逐月海温格点资料(格点分辨率2°×2°),采用相关分析和SVD方法研究了东北地区汛期(7～8月)降水异常与印度洋和大西洋海温异常的关系。结果表明:不同的海区对东北汛期降水异常有不同的影响。东北汛期降水与前一年6～7月西南印度洋海温有较好的负相关关系,东北西南部、东北部和西南印度洋KeyⅠ海区(23～13°S,57～77°E)为SVD耦合相关的显著区域。东北汛期降水与当年3～5月北大西洋KeyⅡ海区(21～27°N,61～75°W)有较好的正相关关系,对应了海温分布型是南北“翘翘板”型。两海区的海温异常共同对东北地区汛期降水异常有较好的预示作用。两海区海温异常对应的全国降水异常的空间分布在东北和华北地区是一致的。 相似文献
2.
影响中国东部夏季降水的前期海温关键区 总被引：5，自引：1，他引：4
使用 1 95 1～ 1 994年的全球海温和中国降水资料 ,利用反复求相关的方法 ,确定了前期 3月北太平洋海区 ( 42 .5～ 5 2 .5°N,1 70°E～ 1 70°W)为影响后期中国夏季降水的海温关键区 ,给出了前期 3月海温关键区海温通过影响前期大气环流遥相关波列影响中国夏季降水的可能途径。前期北太平洋海温关键区海温与中国夏季降水的相关性很高且比较稳定 ,不受 1 978年发生的海温年代际变化的影响。 相似文献
3.
我国东部夏季极端降水与北太平洋海温的遥相关研究 总被引：12，自引：2，他引：12
采用1951—1998年我国东部(105°E以东)59个站点夏季大雨及以上降水量资料与北太平洋海温场资料,借助于SVD分析方法,逐季分析我国东部极端降水与北太平洋海温及南方涛动指数的遥相关,进而检测影响我国东部地区极端降水空间分布的海温关键区和南方涛动及其显著季节(月份)。结果表明,我国东部夏季极端降水与同期太平洋SST的遥相关主要在太平洋130～170°E,5～25°N之间海域;Ni-no区域SST与次年夏季极端降水的相关主要表现在与华东地区的正相关;黑潮海域及加利福尼亚海流区春季SST与我国东部夏季极端降水呈明显的负相关;冬季太平洋SST与我国东部夏季极端降水的遥相关主要表现在,赤道东太平洋、黑潮海域的冬季海温与华东地区、河套地区降水的正相关;我国东部夏季极端降水与前一年秋季Nino区海温为负相关,与西太平洋海温为正相关。 相似文献
4.
热带太平洋和印度洋海温年际变化的均方差分析 总被引：5，自引：0，他引：5
运用1951～1997年热带（20°N～20°S,50°E～80°W）海温（SST）资料求出其各月的均方差,结果表明:太平洋海温变化相对印度洋海温变化要明显,特别是赤道中东太平洋附近 （165～90°W,6°N～6°S）的海温变化比较显著,其海温的变化范围在2～4°C左右,3～4月份海温年际变化小,11～12月海温年际变化大;“暖池”附近洋面海温年际变化也小。而印度洋海域的海温变化范围在1～2°C左右,在印度洋南半球洋面海温变化比北半球洋面海温变化相对较大。同时,根据上述海温变化特征确定了几个海温年际变化最大的关键区。 相似文献
5.
利用华北17站1951～2000年的逐月降水资料,与前期的100 hPa高度场(1958～1997年)求相关,找到了100 hPa高度场影响华北地区汛期降水的关键影响区为25°～35°N,85°～105°E,对应的关键影响时段为前一年3～5月.然后用SVD方法证实了前一年春季正是与华北汛期降水相关最显著的时段;而所选关键区正是处于一种范围更大的100 hPa高度场空间分布型的关键部位,而华北地区是关键区影响中国东部降水的最显著的区域之一. 相似文献
6.
研究了前期热带海温分布型对6月西北太平洋异常环流的影响。结果表明,奇异值分解(SVD)的前期夏季、秋季至冬季热带海洋第一模态呈现出印度洋全海盆一致型海温异常和东太平洋西伸显著的ENSO事件,该模态与6月西北太平洋反气旋(气旋)环流场没有明显的关联。在第二模态中,前期热带太平洋海表温度呈现为ENSO正位相向负位相转换特征,印度洋海表温度变化呈现出赤道东南印度洋（90～110 °E,10 °S～0 °）显著的准IOD事件的变化特征。而这一联合模态与6月西北太平洋异常反气旋(气旋)环流场有显著关联。关联的可能原因是前期海温为El Ni?o和正IOD时,横跨热带印度洋-太平洋的沃克环流的减弱导致在西太平洋-海洋大陆的负降水异常,在Matsuno-Gill效应下西北太平洋形成反气旋异常环流。同时由于两大洋的共同作用和局地海气相互作用使得该环流加强并维持到6月。 相似文献
7.
采用1961—2018年中国160站降水资料、NOAA海面温度资料及NCEP/NCAR再分析资料,利用回归分析等方法,对九江夏季降水的年际变化特征及其可能原因进行分析。结果表明：九江夏季降水具有明显的年际变化特征,存在准4 a的变化周期;九江夏季降水与中国105°E以东的长江中下游及以南地区夏季降水呈显著正相关关系;中国邻近海域的西北太平洋（140°—150°E,15°—25°N）为影响九江夏季降水的海面温度关键区。西北太平洋海温异常与九江夏季降水异常的对应关系为：当西北太平洋夏季海温偏高时,西北太平洋副热带高压偏强偏南、贝加尔湖阻塞高压偏活跃、东亚副热带夏季风偏弱,长江中下游及以南有异常南、北风交汇,且水汽充沛、垂直运动旺盛。这种环流配置有利于长江中下游及以南地区包括九江的夏季降水偏多;反之亦然。 相似文献
8.
北太平洋中纬海温异常对中国东部夏季降水影响的可能途径 总被引：12，自引：4，他引：8
用 8 5 0 h Pau场分解为正、斜分量的方法研究了前期北太平洋中纬 ( 42 .5～5 2 .5°N,1 70°E～ 1 70°W)海温关键区海温异常对其后期中国东部夏季降水影响的可能途径。结果表明 ,前期海温关键区海温首先对其同期 85 0 h Pau场斜压波列施加影响 ,该斜压波列又对其后期斜压波列施加影响 ,最后此斜压波列影响中国东部夏季降水异常。 相似文献
9.
10.
进一步从资料分析和大气环流模式的敏感性试验, 对西北太平洋海温异常与亚太中高纬度地区冬季海平面气压异常经向偶极模的关系及影响进行了研究。资料分析表明, 对应冬季亚太地区海平面气压的经向(ME)型偶极模, 西北太平洋中高纬度海温异常的影响存在两个重要关键区。尤其是(40°N～55°N, 150°E～160°W)海区的海温异常与冬季东亚经向型气压偶极模指数IME有明显正相关, (20°N～35°N, 125°E～170°W)海区的海温异常与指数IME有明显负相关。而上述两个关键海区的SSTA对经向型振荡模的影响, 主要是通过热通量异常的作用。敏感性模拟试验清楚表明, 西北太平洋关键区的海温异常对亚洲—太平洋地区冬季海平面气压场的经向偶极模有一定影响。区域1(42°N～62°N, 145°E～165°W)的负异常相对于其自身的正异常来说, 对亚太地区海平面气压场的负经向偶极模贡献更大, 而区域2 [(22°N～42°N, 135°E～175°E)和(26°N～42°N, 175°E～170°W)]的正异常相对区域1的负异常来说对负经向偶极模的贡献更大一些。但是, 单独区域1的负异常海温和单独区域2的正异常海温影响下的海平面气压场响应的负经向偶极模都会有不同程度的位置偏移。当存在区域1的负异常海温和区域2的正异常海温相互匹配的情况下, 亚洲—太平洋地区冬季海平面气压场的负经向偶极模特征更为显著。 相似文献
11.
The development and application of a regional ocean data assimilation system are among the aims of the Global Ocean Data Assimilation Experiment. The ocean data assimilation system in the regions including the Indian and West Pacific oceans is an endeavor motivated by this goal. In this study, we describe the system in detail. Moreover, the reanalysis in the joint area of Asia, the Indian Ocean, and the western Pacific Ocean(hereafter AIPOcean) constructed using multi-year model integration with data assimilation is used to test the performance of this system. The ocean model is an eddy-resolving,hybrid coordinate ocean model. Various types of observations including in-situ temperature and salinity profiles(mechanical bathythermograph, expendable bathythermograph, Array for Real-time Geostrophic Oceanography, Tropical Atmosphere Ocean Array, conductivity–temperature–depth, station data), remotely-sensed sea surface temperature, and altimetry sea level anomalies, are assimilated into the reanalysis via the ensemble optimal interpolation method. An ensemble of model states sampled from a long-term integration is allowed to change with season, rather than remaining stationary. The estimated background error covariance matrix may reasonably reflect the seasonality and anisotropy. We evaluate the performance of AIPOcean during the period 1993–2006 by comparisons with independent observations, and some reanalysis products. We show that AIPOcean reduces the errors of subsurface temperature and salinity, and reproduces mesoscale eddies. In contrast to ECCO and SODA products, AIPOcean captures the interannual variability and linear trend of sea level anomalies very well. AIPOcean also shows a good consistency with tide gauges. 相似文献
12.
Under external heating forcing in the Southern Ocean, climate models project anomalous northward atmosphere heat transport (AHT) across the equator, accompanied by a southward shift of the intertropical convergence zone (ITCZ). Comparison between a fully coupled and a slab ocean model shows that the inclusion of active ocean dynamics tends to partition the cross-equatorial energy transport and significantly reduce the ITCZ shift response by a factor of 10, a finding which supports previous studies. To understand how ocean dynamics damps the ITCZ's response to an imposed thermal heating in the Southern Ocean, we examine the ocean heat transport (OHT) and ocean circulation responses in a set of fully coupled experiments. Results show that both the Indo-Pacific and the Atlantic contribute to transport energy across the equator mainly through its Eulerian-mean component. However, different from previous studies that linked the changes in OHT to the changes in the wind-driven subtropical cells or the Atlantic meridional overturning circulation (AMOC), our results show that the cross-equatorial OHT anomaly is due to a broad clockwise overturning circulation anomaly below the subtropical cells (approximately bounded by the 5℃ to 20℃ isotherms and 50°S to 10°N). Further elimination of the wind-driven component, conducted by prescribing the climatological wind stress in the Southern Ocean heat perturbation experiments, leads to little change in OHT, suggesting that the OHT response is predominantly thermohaline-driven by air-sea thermal interactions. 相似文献
13.
Intraseasonal Oscillation in the Tropical Indian Ocean 总被引：1，自引：1，他引：1
1. Introduction The intraseasonal oscillation (ISO or Madden- Julian Oscillation, MJO) in the tropical atmosphere has been studied extensively, including its existence, structure, evolution and propagation (Madden and Ju- lian, 1971; Murakami, et al., 198… 相似文献
14.
利用GFDL CM2p1模式, 本文探讨了初始海温误差对印度洋偶极子(IOD)事件可预报性的影响. 当热带印度洋存在初始海温误差时, IOD预报发生了冬季预报障碍(WPB)现象和夏季预报障碍(SPB)现象. WPB发生与否与正IOD事件发展位相冬季的厄尔尼诺-南方涛动(ENSO)有关. 即当冬季存在ENSO时, IOD预测不发生WPB现象, 反之亦然. 相比之下, SPB发生与否和ENSO没有必然联系. 此外, 进一步探讨了最容易导致SPB现象的初始海温误差的主要模态, 指出该模态在热带印度洋上表现为东-西偶极子型, 这和前人研究中最容易导致WPB现象的初始海温误差模态相似. 当在热带印度洋上叠加这些初始海温误差后, 热带太平洋上出现了海表温度异常和风场异常, 进而通过大气桥和印尼贯穿流的作用影响热带印度洋, 使之在夏季出现了东-西偶极子型的海表温度异常, 该异常在Bjerknes作用下快速发展, 加强, 最终导致SPB现象的发生. 相似文献
15.
10月份热带印度洋海气耦合的统计动力诊断 总被引：2，自引：2，他引：0
本文将热带印度洋10月份的大气风场和海洋上层流场看作一个整体, 对其作了动力统计诊断, 即作了复EOF分析, 考察了其年际和年代际变化, 并揭示其与印度洋偶极子 (IOD) 和ENSO的关系。结果表明: 在同一模态中, 海洋模态表现出很强的赤道俘获现象, 而大气则无此现象; 第一模态为印度洋偶极子模态; 第二模态为ENSO前期在印度洋的延伸模态。前2个模态的风场都揭示了Walker环流异常的结构; 印度洋海温的年际变化主要取决于印度洋地区的海气耦合状态, 但太平洋的ENSO循环对其也有一定影响。 相似文献
16.
E.K. Bigg 《Atmospheric Research》1990,25(6)
In a first attempt to assess a proposed climatic change feedback process involving cloud condensation nuclei (CCN) and cloud albedo, CCN concentrations N as a function of supersaturation S were measured on a voyage from latitude 43 to 65°S in October–November 1988. The usual relationship N=CSk, with k=0.5 and C a constant was a fair apprraximation for S in the range 0.3–0.7% implying that CCN concentrations should largely determine cloud drop concentrations and hence albedo for clouds with S in that range. South of latitude 50°S and at smaller S,k was 1 or larger on average, which would lead to reduced dependence of albedo on CCN for the relevant clouds. N varied very widely for separations of the order of 100 km or 6 hours in time, particularly when the sea was partly ice-covered, suggesting strong local influences. During a large increase in N 60°S, unaccompanied by an increase in condensation nuclei (CN), cloud drops grew more rapidly than usual. In a subsidiary experiment particles were collected and examined by transmission electron microscopy. For particles less than 0.2 μm diameter, 80–90% appeared to consist of ammonium sulfate, the remainder being sea salt or an unknown substance which was more liquid and heat-resistant. Dialysis showed that the sulfate particles contained a few percent of insoluble material. Particles which formed cloud drops in vapours other water, were also studied. Comparison of these and water CCN and the rates of droplet suggested that the water insoluble portion of the particles was ethanol-soluble and surface-active. CN concentrations decreased by a factor of about 2 between 43 and 65°S, a change closely paralleled by ethanol CCN concentrations. 相似文献
17.
An ocean reanalysis system for the joining area of Asia and Indian-Pacific Ocean (AIPO) has been developed and is currently delivering reanalysis data sets for study on the air-sea interaction over AIPO and its climate variation over China in the inter-annual time scale.This system consists of a nested ocean model forced by atmospheric reanalysis,an ensemble-based multivariate ocean data assimilation system and various ocean observations.The following report describes the main components of the data assimilation system in detail.The system adopts an ensemble optimal interpolation scheme that uses a seasonal update from a free running model to estimate the background error covariance matrix.In view of the systematic biases in some observation systems,some treatments were performed on the observations before the assimilation.A coarse resolution reanalysis dataset from the system is preliminarily evaluated to demonstrate the performance of the system for the period 1992 to 2006 by comparing this dataset with other observations or reanalysis data. 相似文献
18.
把建好的海洋碳模式应用于印度洋区域,模拟得到了印度洋中与碳有关各化学量的表层分布、垂直分布和沿子午线面的等值线分布。与实测的ＧＥＯＳＥＣＳ（ＧｅｏｃｈｅｍｉｃａｌＯｃｅａｎ—Ｓｅｃｔｉｎｎ Ｓｔｕｄｙ）数据作对比,模式较好地再现了印度洋上营养盐浓度、总碳浓度、总碱度和溶解氧的二维分布。通过模拟还发现,在稳定状态下,大气和海洋中总碳含量的分布依赖于发生在海洋中的各种物理化学过程及边界条件,水平扩散系数Ｋｈ和光合作用常数率Ｋｇ对各化学量的分布有较大影响（以前有学者认为不太重要,如 Ｂａｅｓ［１］）;南印度洋中纬地区 １０°Ｓ至 ３０°Ｓ是１４Ｃ的重要向下渗透区域,人为排放的ＣＯ２可通过这片渗透区从海洋的表层输入海洋的深层。 相似文献
19.
Hydrogen peroxide (H2O2) and organic hydroperoxides (ROOH) were measured on board of theRV Polarstern during its cruise across the Atlantic Ocean from 20 October to 12 November 1990 (54° N to 51° S latitude) by the enzyme fluorometric method. The H2O2 mixing ratio varied from below the detection limit of about 0.12 ppbv up to 3.89 ppbv, showing a latitudinal dependence with generally higher values around the equator and decreasing values poleward. The shape of the latitudinal H2O2 distribution agrees well with an analytical steady state expression for H2O2 using the measured H2O and O3 distribution and a wind dependent H2O2 deposition rate. The ROOH mixing ratio varied from below the detection limit of about 0.08 ppbv up to 1.25 ppbv with qualitatively the same latitudinal dependence as H2O2. The observed ratio ROOH/(ROOH + H2O2) varied between 0.17 and 0.98 showing higher values at the lowest H2O2 mixing ratios at high latitudes. The measured H2O2 mixing ratio shows a significant diurnal variation with a maximum around 14:00 local time, explicable by a superposition of the photochemical H2O2 production with a constant H2O2 deposition rate. Four independent estimations of the average effective H2O2 deposition rate inferred from the H2O2 decrease in the night, from the midday H2O2 production deficit (as derived from comparison with a photochemical model and from the daily ozone loss), and from the offset in the latitudinal H2O2 distribution, were consistent. An episode of maximum H2O2 concentration suggests the possibility of its formation in clouds. 相似文献
20.
把建好的海洋碳模式应用于印度洋区域，模拟得到了印度洋中与碳有关各化学量的表层分布、垂直分布和沿子午线面的等值线分布。与实测的GEOSECS(Geochemical Ocean－Section Study)数据作对比，模式较好地再现了印度洋上营养盐浓度、总碳浓度、总碱度和溶解氧的二维分布。通过模拟还发现，在稳定状态下，大气和海洋中总碳含量的分布依赖于发生在海洋中的各种物理化学过程及边界条件，水平扩散系数Kh和光合作用常数率Kg对各化学量的分布有较大影响(以前有学者认为不太重要，如Baes[1])；南印度洋中纬地区10°S至30°S是14C的重要向下渗透区域，人为排放的CO2可通过这片渗透区从海洋的表层输入海洋的深层。 相似文献