共查询到20条相似文献，搜索用时 62 毫秒
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臭氧和平流层动力学的相互作用 总被引：1，自引：0，他引：1
讨论了给定的南极春季臭氧洞(取自1979—1985年臭氧减少的观测结果)对二维平流层—对流层模式中温度和环流的影响。11月份,南极上空约17km处,温度最多可降低6℃。这种温度变化引起的平均经向环流对臭氧洞起填塞作用,不过,这种影响很小,每年仅产生14DU的变化。观测事实表明,近年来10月份,南半球波活动减弱。为此,我们作了南半球波作用全年都减少一半,并考虑了臭氧洞的数值试验。结果表明,臭氧柱在11月份76°S减少了44DU,在赤道却增加了12DU。 相似文献
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从ＮＡＳＡ卫星地球探测卫星（ＴＯＭＳ－ＥＰ）装载的臭氧总量绘图光谱仪（ＴＯＭＳ）获得的资料表明，１９９９年南极上空臭氧低值区小于去年。ＮＯＡＡ设在南极的气球探测所得资料也表明南极的臭氧洞尽管还是很大，但比去年有所减小。尽管南极臭氧洞的微小年际变化是预料中的，但与１９９８年比１９９９年臭氧洞不再加深加大是个好征兆。美国科罗拉多州博尔德气候监测与诊断实验室的ＤａｖｉｄＨｏｆｍａｎｎ说∶“该测量事实说明平流层中的氯不再增加，这是臭氧层恢复的第一步。现在我们要做的是，密切监视大气中的臭氧洞和破坏臭氧的物… 相似文献
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南极对流层—平流层下部气候变化特征及其原因 总被引：9，自引：4，他引：9
利用南极１６站３０余年地面至３０ｈＰａ１０层月平均气温距平序列资料，采用最大熵功率谱方法，研究了南极对流层至平流层下部气候变化的长期趋势和周期性特征，并讨论了平流层（对流层）气候变化与南极臭氧总量（南半球５００ｈＰａ环流）变化之间的联系。指出：南极气温具有明显的长期趋势和周期性变化；平流层下部显著变冷，对流层增暖，变化最大层高度在１００，７００ｈＰａ，最大降冷速率远大于增暖速率，气层稳定度趋于减弱 相似文献
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青藏高原东北侧臭氧垂直分布与平流层-对流层物质交换 总被引：3，自引：0，他引：3
利用臭氧和温度探空廓线,结合NCEP/NCAR资料、TOMS臭氧总量卫星观测资料和NOAAHYSPLIT后向轨迹模式资料,通过个例分析探讨了影响青藏高原(下称高原)附近臭氧垂直分布的因子和过程。结果表明,动力过程是影响高原上空臭氧垂直分布的主要因子,特别是中高纬度高臭氧浓度的空气向南入侵会导致高原上空臭氧浓度的升高,影响高原上空臭氧低谷的范围大小和形态;尽管大气化学过程对高原上空的平流层下层臭氧垂直分布的影响并不显著,但是高原上空的平流层臭氧变化与温度变化具有较好的一致性。同时还发现,对流层上层的强反气旋系统,特别是中高纬度阻塞高压的边缘有明显的平流层空气向对流层入侵,从而导致对流层内臭氧浓度的增加。 相似文献
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利用1957～1992年南极地区大气臭氧总量地面观测站资料，对南极地区臭氧的时空变化特征进行了研究。结果表明，虽然近35年来南极地区的大气臭氧有较明显的减小趋势，但在不同地区、时段和季节，其变化趋势也不同。近年来南极地区大气臭氧的显著亏损，主要是由南极臭氧洞的形成和发展所造成的。南极地区的大气臭氧存在明显的年振荡、准20个月和准30个月的振荡周期。臭氧变化与天文日照、平流层温度场、平流层冰晶云及人类活动排放到大气中的氟氯烃和溴化烃等污染物质有关。 相似文献
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利用中高层大气模式（MUAM）研究20世纪末12月平流层气候态的十年际变化,基于一组敏感性试验评估下边界条件、二氧化碳及臭氧浓度变化对平流层温度变化的分别影响,着重探讨了南北极局部增暖的机制差异。结果表明,相较于20世纪80年代,90年代12月北极中上平流层西风减速,中低层增温,这主要与下边界条件变化导致行星1波的上传显著增强（2波削弱）有关。同一时期,南极平流层低层西风加速温度降低,中上层东风减速温度升高,这主要与南极低平流层显著的臭氧损耗有关;下边界条件变化和中层局地的臭氧增加也有一定的贡献,但低层臭氧损耗所诱导的极涡加速使得波传播环境或条件有利于1～2波上传增强（1波主导）至更高高度可能是最终导致中上层增暖的主要原因。 相似文献
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利用南极16站30余年地面至30hPa10层月平均气温距平序列资料,采用最大熵功率谱方法,研究了南极对流层至平流层下部气候变化的长期趋势和周期性特征,并讨论了平流层(对流层)气候变化与南极臭氧总量(南半球500hPa环流)变化之间的联系。指出:南极气温具有明显的长期趋势和周期性变化;平流层下部显着变冷、对流层增暖,变化最大层高度在100、700hPa,最大降冷速率远大于增暖速率,气层稳定度趋于减弱;30、50hPa气温具有准两年周期,100hPa上下具有显着的年周期,对流层是以3.5年甚低频周期为主;对流层顶气温无显着趋势变化和周期性变化;南极最大臭氧层高度显着变冷与近15年来臭氧层损耗有关。南半球对流层中部极涡及绕极气流减弱是南极对流层气候变暖的直接原因。 相似文献
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平流层对对流层的作用是准确评估、预测对流层气候变化的一个重要方面。其中平流层成分尤其是臭氧的变化,可以改变平流层乃至对流层的辐射平衡,从而影响平流层、对流层的热动力过程。本文从辐射、动力2个角度介绍了平流层臭氧影响对流层气候变化的若干研究进展。平流层臭氧可以通过长短波辐射的方式对对流层大气造成辐射强迫,利用大气化学气候模式可以定量计算平流层臭氧变化引起的辐射强迫,但是辐射强迫的估算受模式中辐射传输模块本身缺陷的影响存在不确定性。动力方面,平流层臭氧变化产生的辐射效应可以改变温度的垂直和经向梯度,造成波折射指数的变化,进而影响平流层甚至对流层内波的折射与反射,通过上对流层下平流层区域内的波—流相互作用,对对流层气候产生影响。另外,南极臭氧损耗可通过大气环状模影响冬春季中高纬度对流层的天气气候,但是其影响的强度大小以及物理机制仍需进一步的确认。值得注意的是,北极平流层臭氧的变化与北半球中高纬度气候变化之间的关系相比南半球要更加复杂,需要更为深入的研究。 相似文献
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Recent studies demonstrate that the Antarctic Ozone Hole has important influences on Antarctic sea ice.While most of these works have focused on effects associated with atmospheric and oceanic dynamic processes caused by stratospheric ozone changes,here we show that stratospheric ozone-induced cloud radiative effects also play important roles in causing changes in Antarctic sea ice.Our simulations demonstrate that the recovery of the Antarctic Ozone Hole causes decreases in clouds over Southern Hemisphere(SH)high latitudes and increases in clouds over the SH extratropics.The decrease in clouds leads to a reduction in downward infrared radiation,especially in austral autumn.This results in cooling of the Southern Ocean surface and increasing Antarctic sea ice.Surface cooling also involves ice-albedo feedback.Increasing sea ice reflects solar radiation and causes further cooling and more increases in Antarctic sea ice. 相似文献
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S. P. Smyshlyaev P. A. Blakitnaya M. A. Motsakov 《Russian Meteorology and Hydrology》2020,45(3):153-160
The variability of Antarctic total column ozone
in 1980–2018 is considered. The study analyzes trends in Antarctic total
column ozone during the study period as well as the physical and
chemical processes affecting the seasonal variability of total column
ozone. The main attention is paid to the influence of dynamical
processes on the stability of the Antarctic polar vortex, to the
formation of polar stratospheric clouds, and to the influence of
gas-phase and heterogeneous processes on the surface of polar
stratospheric clouds and sulfate aerosol. The method of research is the
analysis of the results of ground and satellite observations and
numerical modeling of physical and chemical processes over the Antarctic
using a global chemistry transport model with the dynamical parameters
specified from reanalysis data. 相似文献
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With the gradual yet unequivocal phasing out of ozone depleting substances(ODSs), the environmental crisis caused by the discovery of an ozone hole over the Antarctic has lessened in severity and a promising recovery of the ozone layer is predicted in this century. However, strong volcanic activity can also cause ozone depletion that might be severe enough to threaten the existence of life on Earth. In this study, a transport model and a coupled chemistry–climate model were used to simulate the impacts of super volcanoes on ozone depletion. The volcanic eruptions in the experiments were the 1991 Mount Pinatubo eruption and a 100 × Pinatubo size eruption. The results show that the percentage of global mean total column ozone depletion in the 2050 RCP8.5 100 × Pinatubo scenario is approximately 6% compared to two years before the eruption and 6.4% in tropics. An identical simulation, 100 × Pinatubo eruption only with natural source ODSs, produces an ozone depletion of 2.5% compared to two years before the eruption, and with 4.4% loss in the tropics. Based on the model results,the reduced ODSs and stratospheric cooling lighten the ozone depletion after super volcanic eruption. 相似文献
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随着大气探测技术以及计算机性能的不断提高,近年来平流层探测数据日渐丰富,中层大气模式也得到了快速发展,平流层中一些重要的物理、化学以及动力过程得以深入研究,对平流层大气环流的认识也进一步加深。本文分析了平流层准2 a振荡（Quasi-Biennial Oscillation,QBO）、平流层残余（Brewer-Dobson,BD）环流和平流层极地环流等主要的平流层大气环流系统和信号的气候态特征、形成机制、年际变率以及长期趋势等,阐述了它们的主要影响因子和过程,讨论并展望了与平流层环流有关的一些主要科学问题。 相似文献
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Kequan ZHANG Jiakang DUAN Siyi ZHAO Jiankai ZHANG James KEEBLE Hongwen LIU 《大气科学进展》2022,39(7):1167-1183
Total column ozone (TCO) over the Tibetan Plateau (TP) is lower than that over other regions at the same latitude, particularly in summer. This feature is known as the “TP ozone valley”. This study evaluates long-term changes in TCO and the ozone valley over the TP from 1984 to 2100 using Coupled Model Intercomparison Project Phase 6 (CMIP6). The TP ozone valley consists of two low centers, one is located in the upper troposphere and lower stratosphere (UTLS), and the other is in the middle and upper stratosphere. Overall, the CMIP6 models simulate the low ozone center in the UTLS well and capture the spatial characteristics and seasonal cycle of the TP ozone valley, with spatial correlation coefficients between the modeled TCO and the Multi Sensor Reanalysis version 2 (MSR2) TCO observations greater than 0.8 for all CMIP6 models. Further analysis reveals that models which use fully coupled and online stratospheric chemistry schemes simulate the anticorrelation between the 150 hPa geopotential height and zonal anomaly of TCO over the TP better than models without interactive chemistry schemes. This suggests that coupled chemical-radiative-dynamical processes play a key role in the simulation of the TP ozone valley. Most CMIP6 models underestimate the low center in the middle and upper stratosphere when compared with the Microwave Limb Sounder (MLS) observations. However, the bias in the middle and upper stratospheric ozone simulations has a marginal effect on the simulation of the TP ozone valley. Most CMIP6 models predict the TP ozone valley in summer will deepen in the future. 相似文献
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利用第5代欧洲中心—汉堡大气环流模式ECHAM5全球大气环流谱模式和中国气象局自主研发的GRAPES全球同化与预报模式分别对2010年1月1—6日全球平流层温度进行了模拟分析,结合相应时段的全球最终分析资料FNL,对比评估了两个模式对平流层温度的模拟效果,并对较为显著的误差现象进行了分析与探讨。结果表明:对于50 h Pa高度上的温度,ECHAM5模式模拟的温度与FNL资料的结果在研究时段内随时间的变化很小,而GRAPES模式模拟的结果在南半球随时间变化显著偏暖。进一步将ECHAM5和GRAPES模式所用的温度初始场进行对比研究表明,两者的分布形态非常形似,尤其是在南半球地区,大部分差值接近于零。将ECHAM5采用的全球臭氧廓线应用于GRAPES模式中,对比发现南半球平流层异常增温的现象仍然存在。因此,温度初始场和臭氧廓线的选取不是造成GRAPES模式模拟出现南半球平流层异常增温的主要原因,需要对GRAPES模式中其他动力及物理过程或参数选取做进一步的深入分析,以弄清其在平流层温度模拟中出现较大偏差的原因。 相似文献
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Scientists have long debated the relative importance of tropospheric photochemical production versus stratospheric influx as causes of the springtime tropospheric ozone maximum over northern mid-latitudes. This paper investigates whether or not stratospheric intrusion and photochemistry play a significant role in the springtime ozone maximum over Northeast Asia,where ozone measurements are sparse.We examine how tropospheric ozone seasonalities over Naha(26°N,128°E),Kagoshima(31°N,131°E),and Pohang(36°N,129°E),which are located on the same meridional line,are related to the timing and location of the jet stream.The ozone seasonality shows a gradual increase from January to the maximum ozone month,which corresponds to April at Naha,May at Kagoshima,and June at Pohang.In order to examine the occurrence of stratospheric intrusion,we analyze a correlation between jet stream activity and tropospheric ozone seasonality.From these analyses,we did not find any favorable evidence supporting the hypothesis that the springtime enhancement may result from stratospheric intrusion.According to trajectory analysis for vertical and horizontal origins of the airmass,a gradual increasing tendency in ozone amounts from January until the onset of monsoon was similar to the increasing ozone formation tendency from winter to spring over mainland China,which has been observed during the build-up of tropospheric ozone over Central Europe in the winter-spring transition period due to photochemistry.Overall,the analyses suggest that photochemistry is the most important contributor to observed ozone seasonality over Northeast Asia. 相似文献
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We investigate the Madden–Julian Oscillation(MJO) signal in wintertime stratospheric ozone over the Tibetan Plateau and East Asia using the harmonized dataset of satellite ozone profiles. Two different MJO indices — the all-season Real-Time multivariate MJO index(RMM) and outgoing longwave radiation-based MJO index(OMI) — are used to compare the MJOrelated ozone anomalies. The results show that there are pronounced eastward-propagating MJO-related stratospheric ozone anomalies(mainly within 20–200 h Pa) over the subtropics. The negative stratospheric ozone anomalies are over the Tibetan Plateau and East Asia in MJO phases 4–7, when MJO-related tropical deep convective anomalies move from the equatorial Indian Ocean towards the western Pacific Ocean. Compared with the results based on RMM, the MJO-related stratospheric column ozone anomalies based on OMI are stronger and one phase ahead. Further analysis suggests that different sampling errors, observation principles and retrieval algorithms may be responsible for the discrepancies among different satellite measurements. The MJO-related stratospheric ozone anomalies can be attributed to the MJO-related circulation anomalies,i.e., the uplifted tropopause and the northward shifted westerly jet in the upper troposphere. Compared to the result based on RMM, the upper tropospheric westerly jet may play a less important role in generating the stratospheric column ozone anomalies based on OMI. Our study indicates that the circulation-based MJO index(RMM) can better characterize the MJOrelated anomalies in tropopause pressure and thus the MJO influence on atmospheric trace gases in the upper troposphere and lower stratosphere, especially over subtropical East Asia. 相似文献
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利用ECMWF资料分析了平流层爆发性增温 (SSW) 过程中臭氧体积混合比的垂直分布的变化, 结果表明: 平流层爆发性增温过程中臭氧体积混合比增大, 而其极大值大多数形成在增温盛期。同时臭氧体积混合比的高值区在爆发性增温过程中随高度发生一定的变化, 据此对其变化分为两类: (1) 下传型: 在增温初期臭氧体积混合的高值区随高度下传至一定高度, 在增温盛期形成极大值然后随高度抬升到大致增温前的高度。 (2) 增厚型: 在增温过程中臭氧体积混合比的高值区厚度增加, 同时附近区域的臭氧体积混合比也增大, 而且在增温前臭氧体积混合比高值区在高度上没有多大变化, 增温开始后有所抬升。平流层爆发性增温过程中臭氧高值区随高度变化的这两种类型, 是由于平流层爆发性增温期间剩余环流对臭氧输送的结果。臭氧变化的下传型是由于在爆发性增温前剩余环流存在着中纬度向极地的明显输送, 并且伴随着极地强烈的下沉运动, 这就使得中纬度输送来的臭氧向下输送, 因此出现了臭氧高值区的下传; 而臭氧变化的增厚型是由于在爆发性增温期间剩余环流不但有中纬度向极地的输送, 而且在极地附近5 hPa高度处出现了上下两支输送气流, 向上的输送气流使中纬度输送来的臭氧向上输送, 而向下的输送气流使中纬度输送来的臭氧向下输送, 进而使增温期间极地附近的臭氧的高值区增厚。同时分析还表明: 平流层爆发性增温过程中中纬度臭氧体积混合比减少。 相似文献