由卫星阻力测定的大气密度值与MSIS和CIRA1972模式的部分比对

本文利用我国卫星的阻力资料测定的大气密度值, 分别与MSIS和CIRA1972模式进行比对.比对结果表明:在本文所计算的高度上, MSIS模式比CIRA1972更接近卫星阻力资料测定的密度值.      

Ozone reference models for CIRA

The ozone reference model which is to be incorporated in the COSPAR International Reference Atmosphere (CIRA) is described and compared with other measurements of the Earth's ozone distribution. Ozone vertical structure models from approximately 25 to 90 km are provided combining data from five recent satellite experiments (Nimbus-7 LIMS, Nimbus-7 SBUV, AE-2 SAGE, Solar Mesosphere Explorer (SME) UVS, and SME IR). The results include the latest improvements in the SBUV algorithms using the most recent estimates of ozone cross sections. Also, the latest refinements in SME algorithms are incorporated. These algorithm improvements have improved agreement between the satellite data sets. Standard deviations are provided of monthly zonal means, and an estimate of the interannual variability is given. The models based on satallite data compare well with the Krueger and Minzner mid-latitude model incorporated into the U. S. Standard Atmosphere which is based on rocket and balloon measurements. Other comparisons are shown with Umkehr and more recent balloon data. Models are also provided of total columnar ozone reflecting recent improved estimates of ozone cross section. Information is provided on semiannual and annual variations. Other systematic variations including estimates of diurnal variations in the mesosphere will be included in the CIRA document.     

A middle atmosphere temperature reference model from satellite measurements

Temperature fields in the stratosphere and mesosphere have been derived from radiance measurements made by the Nimbus 5 SCR, the Nimbus 6 PMR, and the Nimbus 7 SAMS and LIMS radiometers. These instruments cover different latitude and height ranges and different times during the 1973–1983 period. The problems of combining different data sets are discussed, and examples from a proposed model atmosphere for the stratosphere and mesosphere are presented. The model is given in terms of zonal means and amplitude and phase of zonal waves 1 and 2 for temperature and geopotential height, as functions of latitude and pressure for each calendar month. Comparisons are made with the CIRA 1972 and the Koshelkov Southern Hemisphere models and with the SAMS results and in-situ rocket/radio sondes.     

我国火箭探测资料与CIRA 1986稿的比较

本文用我国气象火箭探测获得的中层大气风、温度、密度和气压等数据,与国际参考大气模式CIRA 1986稿作了比较.结果看到,我国火箭探测温度数据值在模式给出的平均值剖面上下波动,符合的程度在国际比对偏差范围之内;用探测数据分析得到的风的季节性和声重波强度等与模式给出的描述都很符合.从而说明,用CIRA 1986稿来表征我国上空的中层大气结构是合适的.      

Solar,geomagnetic and long term effects on thermospheric neutral kinetic temperatures at midlatitude

Measurements of midlatitude thermospheric neutral kinetic temperatures obtained from 1972 to 1979 have been used to investigate the effects of solar and geomagnetic activity, as well as long term effects, on the thermosphere. With these data a simple power law relationship between the temperature and solar activity (expressed as the 2.8 GHz solar radio flux) has been found to give a high correlation. In addition, a linear relationship between temperature changes and geomagnetic activity (expressed as Ap), as well as annual and semiannual effects have been found. The annual variation is found to be indistinguishable in phase from the annual variation of the solar declination angle. The present four parameter formulation gives a better fit to the data than is obtained with available empirical models of the thermosphere, and this has allowed us to investigate the properties and postulates of some of these models.     

Properties of the mesosphere and thermosphere and comparison with CIRA 72

Exospheric temperatures of several reference atmosphere are reviewed and a recommendation is made for the exospheric temperature of a proposed mean CIRA. One of the deficiencies of CIRA 72 and other present thermospheric models is the representation of density changes with geomagnetic activity. This deficiency is illustrated with samples of data. The data show the effects of geomagnetic activity, particle precipitation, a solar proton event, and gravity waves. An empirical model developed from the unique AFGL satellite density data bank using multiple linear regression is reviewed. The present model is for low to moderate solar flux and quiet geomagnetic conditions, but it is planned to extend the model to active conditions. Good progress has been made since CIRA 72 was specified in our knowledge and understanding of the properties of the lower thermosphere, although there are still some unresolved problems. The biggest progress has been made in the theory of tidal effects and of particulate energy deposition and of electrojet heating. On the other hand, it is still not possible to define adequately the systematic variations of the lower boundary conditions of thermospheric models. This is due to lack of knowledge of the systematic variations of the structure properties in the 100 to 120 km altitude region and inadequate information on the mesospheric turbulence profile and variations in the turbopause altitude.     

Middle atmosphere temperature measurements as compared to atmospheric models

Two large sets of temperature data measured in Europe are compared to atmospheric models that were prepared for the NEW CIRA. The data were taken by rocket flights during the Energy Budget and MAP/Wine Campaigns, and during several years of operation of ground based OH* spectrometers. Monthly mean temperature profiles from 20 – 85 km are available for November, December, and January. They are in very good agreement with the new models. Seasonal and latitudinal variations of upper mesosphere temperatures are obtained from the OH* data. They are also in fair agreement with the new models. These are therefore found a definite improvement as compared to the older ones. On the basis of this general agreement it is concluded that finer details as variations with solar cycle, magnetic activity, etc. could come into reach of future models.     

Neutral temperatures from Thomson scatter measurements: Comparisons with the CIRA(1972)

Neutral exospheric and lower thermospheric (100–130 km) temperatures from Thomson scatter measurements at Millstone Hill (42°N) are compared with CIRA temperatures with a view towards identifying deficiencies in the CIRA and recommending revisions. CIRA models the observed diurnal mean temperatures (T₀) to within 10% over a wide range of solar conditions (75? F_10.7 ? 250), but consistently underestimates the diurnal temperatures with maximum deviations approaching 50% of observed amplitudes (180–240 K) at solar maximum (1200 K ? T₀ ? 1400 K). The observed semidiurnal amplitudes, which lie in the range of 20K–80K, are always underestimated and frequently by more than 50%. In the lower thermosphere, tidal oscillations of temperature of order 20K–40K occur which are not modelled by CIRA. In addition, an analysis of exospheric temperatures at Millstone Hill during a magnetic disturbance indicates a response within 1–2 hours from storm onset, whereas CIRA assumes a 6.7 hour delay. Although some of these deficiences are addressed by the more recent MSIS model, there exists a sufficient data base to recommend several additional revisions to the CIRA temperatures at this time.     

Some recent advances in thermospheric models

Since the publication of the last COSPAR International Reference Atmosphere (CIRA 1972) valuable progress has been achieved in improving our understanding of the terrestrial thermosphere. As a result, several empirical models are now available for numerous applications. The reliability of these models is discussed within the framework of known physical phenomena. The most recent published advances deal with longitudinal and universal time effects. Some general shortcomings are pointed out in order to stimulate farther progress.     

任意偏心率卫星的大气阻力的短周期摄动

通过本文采用的计算方法和CIRA 1972在160～2000公里高度围范的大气密度的分析模型,导出了人造地球卫星大气阻力短周期摄动的一种计算公式,它形式简单,收敛性好,适用于任意偏心率的卫星。     

广州地磁Z分量日变幅的谱特征

利用1972—1993年广州地磁资料，分析了Z分量日变幅的年平均、年变化和半年变化等低频成分的逐年变化，以及小于60天的短周期变化特征．同时对1972—1993年的F10.7日均值进行了谱分析．结果指出，广州地磁Z分量日变幅的年平均与太阳活动指数F10．7的年平均存在良好的线性相关；具有幅度大约5nT夏季极大的年变化，与太阳活动没有明显相关，是一种季节效应；存在春秋分极大的半年变化，幅度与太阳活动有关，高年的幅度明显大于低年；具有明显的与太阳自转相关的27天左右的变化和明显的与行星波有关的接近16日、10日、5日、2日等短周期变化．广州地磁Z分量日变幅的这些谱特征，有助于更深入地了解中低层大气对电离层影响的物理机制．     

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.      

A generalization of the Hines” dispersion relation

A simple dispersion relation which forms a generalization to the Hines' relation has been developed for the real atmosphere which fully allows for reflection and transmission at every height level. The relation is an analytic function of the Brunt frequency, the speed of sound profile and its derivatives and the variations in mean molecular mass (using CIRA 1972). The correction terms to the Hines' dispersion relation become important for gravity waves with frequencies close to the Brunt frequency.     

由大气密度的季变化所造成的中、低层大气电离率的季变化

本文对CIRA 1972 模式下的中、低层大气密度季变化所造成的电离率的季变化作了理论计算, 利用宇宙线电离源函数对全球中、低层大气的电离率作了数值计算.计算结果表明, 在70km以下的大气电离率的季变化幅度为百分之几十.在电离峰值高度(约15km)以下幅度为约百分之十, 高度越高变幅越大, 到70km处达35%.在20km以上电离率的季变化趋势与大气密度的季变化趋势大致相同, 夏季比冬季大, 20km以下变化稍为复杂.      

低纬地磁Z分量的半年变化

利用武汉、广州、泉州和琼中等4个低纬地磁站连续多年的地磁资料，计算了各月5个磁静日Z分量日均值与中午1100---1300时段平均值之差(Dz)，对每年12个Dz采用多元回归分析方法，得到各年的半年变化幅度和相位．结果表明：4个站的Dz每年都有半年变化现象；半年变化幅度与太阳活动有关，一般来说，太阳活动高年Dz半年变化幅度明显大于太阳活动低年；太阳活动本身的半年变化，对Dz半年变化幅度有显著的调制作用；Dz半年变化的相位在3—4月(或9—10月)，即极大值出现在分季；低纬地区地磁Z分量存在显著的半年变化，能够反映赤道电急流也有明显的半年变化，这再一次证明，赤道电急流幅度的半年变化，通过“喷泉效应”使得电离层，f0F2产生半年变化，其是产生，f0F2半年变化的一个主要因素．     

Proposed ozone reference models for the middle atmosphere

Since the publication of the last COSPAR International Reference Atmosphere (CIRA 72), large amounts of ozone data acquired from satellites have become available in addition to increasing quantities of rocketsonde, balloonsonde, Dobson, M83, and Umkehr measurements. From the available archived satellite data, models are developed for the new CIRA using 5 satellite experiments (Nimbus 7 SBUV and LIMS, AEM-2 SAGE, and SME IR and UVS) of the monthly latitudinal and altitudinal variations in the ozone mixing ratio in the middle atmosphere. Standard deviations and interannual variations are also quantified. The satellite models are shown to agree well with a previous reference model based on rocket and balloon measurements.     

The geomagnetic variation in the upper atmosphere

A brief review is given of the development of models of the geomagnetic variation in the thermosphere and exosphere, including some recent models based mainly on satellite-borne gas analyzer measurements. One recent model, derived from ESRO4 data, is described in detail and compared with the model in CIRA72. The limitations of this model are discussed. The model in the MSIS comprehensive model is also examined briefly. There appears to be a serious error in the amplitude of the exospheric temperature increase predicted by the MSIS model.     

Comparisons of winds at (44°S, 173°E), 65–110km,with CIRA 72

In the 95km height region of the atmosphere, ground-based techniques made an important contribution to the CIRA 72 [1] wind model. Recent wind measurements from a partial reflection experiment at 44S covering one and a half years are presented and compared with CIRA 72. The zonal wind component compares favourably, although the measured values are more easterly above 80km in autumn and winter; a feature of the autumn winds is a temporary easterly reversal above 90km. Winter mesospheric winds can be very disturbed. The summer mesosphere easterly maximum appears earlier in the season and at a higher altitude than the model. A much poorer comparison is shown between the measured meridional wind component and the 1969 model of Groves [2].     

Zonal mean temperature, pressure, zonal wind and geopotential height as functions of latitude

The new zonal mean COSPAR International Reference Atmosphere (CIRA-86) of temperature, zonal wind, and geopotential/geometric height is presented. This data can be used as a function of altitude or pressure and has nearly pole-to-pole coverage (80°S-80°N) extending from the ground to approximately 120 km. Data sources and methods of computation are described; in general, hydrostatic and thermal wind balance are maintained at all levels and latitudes. As shown by a series of cross sectional plots, the new CIRA accurately reproduces most of the characteristic features of the atmosphere such as the equatorial wind and the general structure of the tropopause, stratopause, and mesopause.     

Proposal for a reference model of the middle atmosphere of the southern hemisphere

Available rocketsonde information has been used to compile tables of monthly mean temperature, pressure, density and zonal wind for the middle atmosphere of the southern hemisphere with the purpose of revising similar tables presented to COSPAR earlier. The altitude range is 25 to 80 km in steps of 5 km. The latitude range is 0° to 70°S with a 10° step. The compatability of different sets of temperature measurements is discussed. Mean values of temperature, pressure and zonal wind obtained for the southern hemisphere are compared with northern hemisphere model values. Large differences between the hemispheres (up to 20°C in temperature, 20–30% in pressure, 30–50 m/s in wind) imply that reference atmospheres such as CIRA should be complemented by southern hemisphere climatology.