Intercomparisons of temperature,density and wind measurements from in situ and satellite techniques

Intercomparisons between satellite retrieved temperatures (TIROS N series) and those derived from radiosonde and rocketsonde profiles have been made covering the years 1980–1984. Differences in the measurement parameters between 100 and 0.4 mbar (～16–55 km) are described; generally radiosonde/satellite differences are less than 1°K, while rocketsonde/satellite differences reach 7–8°K in the upper stratosphere. Comparisons between the various $\text{in situ}$ devices indicate that radiosonde/rocketsonde differrences are less than 1°K while precision studies of the rocketsonde instrument find that the rocketsonde measurements are internally consistent to less than 1°K up to 50 km and to less than 3°K to 60 km. Density data obtained with the small rocketsondes ($\text{in situ}$ thermistors and inflatable spheres) and with the large sounding rocket systems show that density measurements usually agree to within 15 percent up to 85 km. Comparisons of the various atmospheric parameters obtained from different instruments are important, however the usefulness of intermixing the measurements is obvious and increased emphasis should be placed on procedures for intermingling such data. Suggestions are made on how this might be accomplished.     

Temperature comparison between CHAMP radio occultation and TIMED/SABER measurements in the lower stratosphere

Global Positioning System (GPS) receiver on the CHAllenging Mini-satellite Payload (CHAMP) and the Sounding of the Atmosphere using Broadband Emission Radiometry (SABER) instrument, one of four on board the TIMED satellite, provide middle atmosphere temperature profiles by Radio Occultation (RO) and limb viewing infrared emission measurements, respectively. These temperature profiles retrieved by two different techniques in the stratosphere are compared with each other using more than 1300 correlative profiles in March, September and December 2005. The over-all mean differences averaged over 15 and 35 km are approximately −2 K and standard deviation is less than 3 K. Below 20 km of altitude, relatively small mean temperature differences ∼1 K are observed in wide latitudinal range except for June (during the SABER nighttime observation). In the middle to low latitudes, between 30°S and 30°N, the temperature difference increases with height from ∼0–1 K at 15 km, to ∼−4 K at 35 km of altitude. Large temperature differences about −4 to −6 K are observed between 60°S and 30°N and 31–35 km of altitude for all months and between 0° and 30°N below 16 km during June (nighttime).     

平流层臭氧和辐射场的季节分布特征

利用美国NCAR化学气候耦合模式WACCM3对平流层温度场、风场、臭氧及辐射场进行了模拟.结果表明,在适宜飞艇长期驻留的准零风层高度20～22km(对应大气压强范围为50～30hPa,以下均采用气压值表征对应大气高度),7-8月风速小于5m·s-1的风带可长期稳定在40°N以北.臭氧空间分布显示,在30hPa气压高度处中国地区臭氧浓度出现了带状分布,30hPa高度以下低纬度地区臭氧浓度低于中纬度地区.平流层太阳加热率的时空变化表明,在平流层上层,太阳加热率可达100×10-6K·s-1,而在平流层下层,只有10×10-6K·s-1.6-8月中国区域的太阳加热率大于9月;在100～30hPa高度内,中纬度地区太阳加热率高于低纬度地区,在30hPa高度以上,低纬度地区太阳加热率高于中纬度地区;8-9月30～40hPa高度处,太阳加热率的空间变化较小.在30hPa高度上,太阳加热率在40°N昼夜变化最大;50hPa高度处,太阳加热率的昼夜变化小于30hPa高度处,而且白天太阳加热率出现极大值的纬度明显靠北.平流层低纬度地区的长波加热率小于中纬度地区.青藏高原由于地形特殊,其6-7月的臭氧浓度、太阳加热率和长波加热率均小于同纬度其他地区.      

Detection of long-term trends in global stratospheric temperature from NMC analyses derived from NOAA satellite data

Since 24 September 1978 global daily fields of temperature and geopotential height at 8 stratospheric pressure levels 70 to 0.4 mb (18–55 km) have been produced at the U.S. National Meteorological Center. Temperature profiles derived from NOAA operational satellites constitute the sole data source for the upper stratospheric levels 5, 2, 1, and 0.4 mb (35, 42, 48 and 55 km). Significant changes in upper stratosphere reported temperatures have accompanied each of the eight changes in either operational satellite or method of data processing. Comparisons with rocketsonde data from 1978 to 1986 show bias changes of 1 to 5 Celsius degrees at various levels. For detecting long term trends of ambient stratospheric temperature, adjustments based on rocket comparisons must be applied to the NMC fields. Lack of data at north polar latitudes and in the southern hemisphere limits comprehensive characterization of temperature uncertainty. We discuss in detail our ability to characterize temperature uncertainty of the NMC stratospheric analyses. We specifically discuss our ability to detect a trend in the middle stratosphere temperature of about 1.5 celsius degrees per decade, the amount of change indicated likely by current theoretical models.     

Air depression over south pole during Antarctic spring and its possible influence on ozone content in this region

Air depression during Antarctic spring, its long-term behaviour and connection with ozone content has been investigated on base of rocket data for polar regions and total ozone data sets for South pole (TOMS data) for 1979–1990. It was shown, that air pressure depression near South polar region in September in the lower stratosphere has a visible (about 5% per decade) negative trend similar to the tendency which total ozone records reveal. Rather high correlation (+0.82) between air pressure in the stratosphere and total ozone content for spring in Antarctica was found.     

Strategy for early detection of climatic change

A general strategy for detection of climatic changes of stratospheric temperatures is discussed in the light of expected short-term and long-term natural and spurious (instrumentally-induced) variability. The effects of the brevity of both the radiosonde record and the satellite sounding record are stressed, and the need is emphasised for homogeneous time-series from satellites as well as from sondes.The general principles are illustrated by means of an attempt to detect climatic changes in the extratropical upper troposphere and lower stratosphere using radiosonde data for approximately the past 25 years. It is shown that, even in the absence of instrumental shortcomings, a further 35 years of radiosonde data, or 20–25 years of satellite sounding data, are needed for detection of temperature trends of the size indicated by global circulation models for the present rate of increase of concentration of atmospheric carbon dioxide.     

Middle atmosphere summer duration as an indicator of long-term circulation changes

Summer duration (SD) is defined here as the time interval between spring and autumn turn around of zonal winds in the stratosphere. SD long-term trends are obtained from analysis of middle stratosphere NCEP and ECMWF data. They are found to be dependent on latitude and altitude. Wind data are available since 1948. The corresponding analysis suggests a breakpoint in the trend at around 1980: SD increases before 1980, and decreases afterwards. Corresponding changes of stratospheric wave activity are analyzed and found to be a major contribution to the SD trends. Long-term computer runs of the Whole Atmosphere Community Climate Model (WACCM 1b) are consistent with these results. Vegetation data on the ground indicate similar trends with a break.     

2009年冬季平流层爆发性增温期间行星波活动特征

利用2008年12月至2009年4月的MERRA再分析数据资料,对2009年1月下旬北半球高纬平流层发生的强增温事件以及与之相关的行星波活动进行了研究.谱分析发现,SSW发生前后极区平流层内准16天行星波活动显著.利用二维谐波拟合法分别拟合温度场准16天波4个波模（W1,W2,E1,E2）的振幅和相位,结果表明:背景西风减弱时四个波模的振幅均有不同程度的增大,且都在50°-80°N范围内的平流层中上层达到最大值;准16天W2波的增幅最大且辐合最强烈,其引起的背景流最大西风减速超过4m·-1·d-1,说明准16天W2波在该次增温事件中占主导地位;行星波传播与零风线移动关系密切,准16天W2波在中高纬地区垂直向上传播并近似呈现经向驻波结构,然后分别向极点和赤道两个方向传播,这表明中高纬地区可能是行星波的一个源区.      

Measurements of upper atmosphere wind and temperature from meteorological rocket experiments during winter 1979

This institute conducted a series of meteorological rocket experiments for the upper-atmospheric sounding in the winter of 1979. Within the overlap altitude range with balloon flights, a comparison of the results with the standard radiosonde data indicated that the rocket-borne system was reliable. The measurements from foru rocket flights for the region between 20 and 30 km showed a degree of compatibility to each other while those for above 30 km differed considerably from one another. At low latitude, the temperature profiles in the winter stratosphere in general showed a reasonably good agreement with the U.S. Standard Atmospheric Supplements, 1966 (USSAS 66). A temperature of 2–24°C lower than the USSAS 66, however, was recorded in the lower mesosphere. Above 30 km the maximum diurnal variation in temperature was 9°C or so. In the winter, the wind profile showed the westerlies and the maximum wind velocity of 92.1 Msec^?1 was obtained from these experiments at the height of 60 km.     

人为活动对高平流层,中间层大气的影响

利用一维光化、辐射耦合模式研究了人为活动所排放出的废弃物ＣＨ４、Ｎ２Ｏ和ＣＯ２含量增加对高平流层，中间层大气的影响。结果指出，对流层中这些气体增加一倍将导致上中层大气水汽、Ｏ３和温度的明显变化。ＣＯ２含量增加将使上中层温度降低约１０Ｋ；而ＣＨ４含量的加倍不仅使中层顶附近水汽含量增加５０％以上，也使其温度有更明显的下降，这将更有利于於光云的形成。     

Periodic and aperiodic ozone variations in the middle and upper stratosphere

Umkehr, ozonesonde and satellite observations were used to determine the height/latitude distribution of the amplitude and phase of the periodic components of the variation of the ozone mixing ratio in the middle and upper stratosphere. The amplitude of the first (annual) harmonic is small in the subtropics and increases to a maximum at polar latitudes. It also increases with height in the mid and upper stratosphere to an apparent maximum just below the stratopause. The second (semi-annual) harmonic has an amplitude that is largest in tropical regions and in subpolar regions at a level of about 40 km. There seems to be very little ozone variation above 30 km with dominant periods close to the quasi-biennial period of total ozone observed in the tropics. The percent of the total variance of the ozone mixing ratio accounted for by the first harmonic is larger than 60 percent at all heights from 20° – 60° latitude in both hemispheres (except near 40 km in the Northern Hemisphere). The percent of the total variance accounted for by the second harmonic is maximum at a height of about 40 km in the tropics and at subpolar latitudes where, as mentioned, its amplitude is also largest.The phase of the first harmonic shows a marked transition from a winter/spring maximum below 30 km to a summer maximum at 30 km, changing rapidly to a maximum in winter in both hemispheres. The regions of minimum amplitude of the annual variation and the marked phase shifts with height both indicate the separation by levels of the dominant physical control mechanisms on the periodic changes of the ozone mixing ratio in the middle and upper stratosphere. Changes below 30 km respond primarily to dynamic influences in the lower stratosphere while above 30 km the periodic variations result mainly from photochemical processes. Above 40 km these variations are strongly temperature dependent.     

青岛上空中层大气密度和温度的激光雷达探测

介绍了中国电波传播研究所瑞利散射激光雷达系统的结构和性能, 阐述了激光雷达探测中层大气密度和温度的工作原理, 给出了青岛地区中层大气密度和温度的初步探测结果. 通过与卫星、探空气球和大气模式数据的结果对比, 验证了激光雷达探测大气温度的可靠性. 基于2008-2009两年的观测, 获得了青岛地区上空中层大气温度的季节变化和平均分布. 激光雷达观测结果表明, 青岛地区平流层温度比CIRA86模式结果高, 且二者偏差呈夏秋季小、冬春季大的特点, 中间层温度则正好相反.      

Spring-ozone change in Antarctica and the role of the polar vortex

Observations since the late 1970's have shown that from late September until the end of November (austral spring) the total ozone over the southern polar region has declined by up to 30% when compared with the ozone average of the 1957–1978 period. The decline is not uniform in time and space; from January through August, the ozone changes are very small, well within the year-to-year fluctuation limits. Satellite observations confirm that the significant ozone decline is centered over and does not expand outside of the Antarctic continent, e.g. it coincides with the location of the Antarctic stratospheric winter vortex; moreover, the decline increases poleward. Analysis of the stratospheric temperatures and geopotential heights confirms that the spring-to-spring ozone changes closely follow the changes of the thermobaric field, and that the rapid increase of ozone (and stratospheric temperature) in the spring is dependent on the time of the polar vortex breakdown, when favorable conditions for continuous meridional exchange of ozone-rich air from the middle latitudes are re-established. The stratospheric heating rates and the weak gradient in the vortex central region during early spring provide favorable conditions for weak upward motions, responsible for a substantial part of the ozone loss between the date of the solar penetration of the stratosphere, and the date of the vortex breakdown. Since the late 1970's, the breakdown of the Antarctic vortex has occured about mid-November, a month later than in years of early breakdown. It is suggested that an early breakdwon of the Antarctic vortex would interrupt the trend of declining spring ozone established over the past few years.     

平流层冬季增温及大气中的行星波

本文利用NIMBUS-7SAMS资料分析了东经100度子午线上的两个站点(67.5°N和42.5°N)在10mb和0.0827mb高度上从1978年底至1982年间的大气温度,获得几年的平流层冬季增温结果.在1978/1979年和1981年初的冬季,高纬站点几天内出现的平流层增温最大幅度可达65K.对平流层增温的谱分析结果指出,在高纬冬季平流层有很强的16天、32夭、21天周期的行星波。中纬冬季平流层增温幅度较小,约为20K.中纬的中间层高度上整年存在有5天、8天和16天的行星波。分析研究、南、北半球不同纬度的温度随经度的分布,得出高纬冬季平流层、中间层大气温度随经度有明显的变化。波数1和波数2的波有大的幅度(主要是波数1),从高纬到低纬,波幅逐渐减小在冬季的平流层和中间层大气中,波数1和波数2的行星波在短期内可强烈增强,引起平流层冬季增温。      

北京上空高分辨率气球探空观测的温度垂直波数谱

使用分辨率为10 m的温度剖面检查2.90～8.01 km和14.65～19.76 km高度范围内归一化温度扰动谱的谱特性,并且将它们与模式谱比较.结果表明,在波数9.8×10-4～2.5×10-2m-1范围内,对流层的垂直波数谱有约-1.9的平均谱斜率;低平流层的垂直波数谱有约-2.2的平均谱斜率.这两个平均谱斜率大大偏离了目前饱和谱模式和普适大气谱模式表示的-3.0和-2.4谱斜率,并且认为是目前气球测量中曾经观测到的最平谱斜率.在波数9.8×10-4～2.5×10-2m-1范围内,对流层和低平流层的平均谱振幅比饱和谱模式的谱振幅分别大24倍和5倍,这也与饱和谱模式以及目前文献中的观测结果有很大不同.这些较大平均谱振幅与最平的平均谱斜率一道共同表明,观测的温度谱并不遵循目前的饱和谱模式和普适大气谱模式.      

北纬30°中层顶区域钠与铁原子层的结构和年际变化

基于武汉大学Na和Fe激光雷达在2004年1月至2011年12月期间的观测数据，得到武汉上空中层顶区域Na和Fe原子层的平均特性、夜间变化和季节变化特征.Na层平均质心高度为91.36km，平均RMS（均方根）宽度为4.64km.Fe层平均质心高度为88.99km，平均RMS宽度为4.57km.在充分考虑金属层夜间变化和季节变化对数据样本影响的基础上，获取了Na层和Fe层结构在此期间的年际变化特征.对Na层和Fe层质心高度及RMS宽度的年际变化进行线性拟合，发现Na层和Fe层在此期间均相对稳定，Na层质心高度在近8年间仅有约58m的下降，变化率为-7.91m·a-1，Na层RMS宽度减小约151m，变化率为-20.60m·a-1.同期，Fe层的质心高度下降了约230m，变化率为-31.36m·a-1，Fe层RMS宽度则有所增大，变化率为21.01m·a-1.      

Long term variability of total ozone yearly minima and maxima in the latitudinal belt from 20°N to 60°N derived from the merged satellite data in the period 1979–2008

This paper deals with the behavior of the annual cycle of total ozone (ACO3) and its amplitude (O3_AMP) in the latitudinal belt from 20°N to 60°N. The prominent feature of the O3_AMP spatial pattern is the sharp maximum over the north-east coast of Asia. The spatial correlation of O3_AMP with its highest/lowest value varies with location: in the middle latitudes it correlates predominantly with the values of annual maxima of total ozone, while in the lower latitudes, there is a strong negative correlation with the values of ACO3 minima. Regarding temporal evolution of O3_AMP we detected distinct negative trend in the period of 1979–1995 which is caused by stronger negative trend of maxima than the negative trend of minima in ACO3. In the period 1995–2008 we found the positive trend of ACO3 in most regions due to stronger positive trend of maxima than that of minima in ACO3 in the middle latitudes (especially over the central and northern Europe and the north-east Asia). In the lower latitudes a weak negative trend of O3_AMP was identified and linked to weaker positive trend of maxima than positive trend of minima in ACO3. The behavior of the temporal trends was linked to the changes in Brewer–Dobson circulation and to the trends of tropopause pressure.     

Stratospheric flights with large polyethylene baloons from equatorial latitudes

Starting with average 50% success for stratospheric balloon flights during 1959–1969 and attaining 100% success during 1972–1973, the success record dropped to 50% during 1974–1979. Through a critical analysis of 59 flights made from Hyderabad and 21 flights made from other equatorial bases, revised design criteria were proposed for balloons to be flown from equatorial latitudes, which were accepted by M/s Winzen International, Inc. (WII), U.S.A. and have again raised the success record to 93% for 15 flights made since April 1980. A revised analysis for 71 flights made from 1965 to 1984 has been presented. Stratospheric circulation over Hyderabad indicating predominance of easterlies with mesospheric westerlies descending occasionally into stratosphere has been discussed.     

Variations of mesopause temperatures in Europe

Mesopause temperatures were derived from ground measurements of the near infrared OH1 spectrum. Preliminary data are presented. Seasonal variations at Wuppertal (51° N, 7° E) are well represented if the Cole and Kantor (1978) model [1] is raised by 10 K and shifted by about 18 days. Latitudinal variations from 68° N to 51° N are found much smaller than the model variations. During a stratospheric warming, mesopause and stratosphere temperatures were found to be in anticorrelation only if a substantial longitudinal shift is introduced.     

平流层爆发性增温事件中大气准16日行星波

2014年1月上中旬高纬平流层发生弱增温事件,增温幅度约25K,纬向西风减弱并于2月初转向.行星波在平流层爆发性增温（SSW）事件产生中具有重要作用.利用北半球近东经120°链上中低纬5个流星雷达探测的风场数据,研究了此SSW事件发生前和发生期间中间层和低热层区（MLT）大气风场的行星波状况.结果显示,极区平流层增温前MLT区大气呈现出明显增强的准16日波动,增温达到最大时,16日波也最强,表明中低纬MLT区的行星波变化与SSW事件存在耦合关系.进一步利用欧洲中心平流层再分析资料数据,分析SSW期间北半球平流层的波动和零风线状况,发现平流层准16日波和零风线随时间由低纬向高纬移动,反映出16日波与SSW之间存在某种动力学联系.