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1.
本文借助Nazarchuk的扩散理论模型和有关资料, 分析了1986年1月4日哈雷彗星等离子体彗尾的尾轴方向及其垂直方向的相对亮度分布, 推算出CO+离子的平均寿命、纵向(沿尾轴)和横向扩散系数, 估算了磁场强度, 最后进行一些讨论.   相似文献   

2.
本文对用于新机主动控制技术ACT电/光传飞行操纵系统的一种采用三冗余加一备份方案的容错计算机配置作了一般性介绍;并对其系统可靠性进行了分析与计算。包括,可靠度R(t)、失效率λ(t)及平均寿命MTTF的数学模型建立与数值估算;并应用网络分析法进行了验证,估算出故障覆盖率对系统可靠度的影响。最后,对软件可靠性问题作了一般性讨论。  相似文献   

3.
在以往,卫星成本的估算都是依据过去已经发射卫星的经验数据作参考,以推算一个新型号卫星的成本。近几年来,又比较着重各种部件和主要设备的成本核算,以改善卫星成本估算的准确性。然而,对于卫星初步方案设计阶段,由于设计的详细情况还不很清楚,要进行卫星整星的成本估算,确是一件不容易的事。为此,曾经提出过一些成本估算模式。几年来,美国有关部门有目的地收集了各种卫星的成本及有关的技术资料。加利福尼亚州埃尔·塞贡多航宇公司,根据这些资料,分析和整理了一项“卫星整星成本估算关系式”。只要知道卫星的任务和装什么样的有效载荷、卫星的重量以及  相似文献   

4.
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.   相似文献   

5.
介绍了建立卫星成本估算关系式所用的回归分析法;重点给出了以近年来29颗国外小卫星的实际成本数据为依据,用回归分析法拟合,得出小卫星的成本估算关系式;除了给出最常见的以卫星干质量为自变量的成本估算关系式外,还给出了以其他功能、性能参数为自变量的、多种形式的成本估算关系式;并以实例,对不同的自变量计算出成本估算值,取他们的带权平均值得到最后的小卫星成本估算值;最后给出了含双自变量的小卫星成本估算关系式。  相似文献   

6.
本文计算了地球中层大气的钠层模式。在此模式中,流星蒸发是形成钠层的源而尘埃的吸附足汇。本文考虑和比较了有关钠层形成机制的已往工作中所出现过的所有光化学反应,选出了四十个合理而重要的化学反应作为本模式的化学基础。模式也考虑进了高度变化的涡流扩散和带电粒子受地磁场作用的向下飘移等机制。本文对各化学反应和模式中各个因素的重要性作了比较和评价。本文计算结果表明,在各高度上中层大气中的钠及其化合物的相对浓度主要取决于化学反应过程本身,与源、汇及各层间扩散机制等关系不大。虽然在钠层模式计算中必须考虑到十种钠成分,但105公里以上主要成分足钠离子(Na+)。80公里以下主要成分是氢氧化钠(NaOH)。80公里到105公里间主要成分是中性钠原子(Na)。所有成分的总浓度主要地取决于源和汇随高度的分布。大气背景及电离常数的变化可以引起钠层相当显著的季变化和周日变化。理论计算结果与历年来的观测结果作比较后可以看到两者大体上符合得相当好。   相似文献   

7.
万爽  易帆 《空间科学学报》2006,26(5):357-363
采用特征分析方法计算中层大气Fe和Na层的化学特征时间,同时计算了它们被流星烟粒吸附和被垂直输运的特征时间.结果表明,(1)在Fe层数密度峰值高度附近,其EA化学特征时间为数日,远大于传统定义的数分钟;(2)比较Fe的输运特征时间(w=1 m/s)和化学特征时间,得出在84 km以下化学过程占优势,而在84km以上,垂直输运过程占主导地位,与Na层结果相同;(3)通过将各自化学特征时间与垂直输运和流星烟粒吸附的特征时间比较,以及考察流星金属注入率对Fe和Na原子分布的影响,发现最有可能使Fe和Na层下边沿截止高度重合的原因是流星烟粒的吸附效应.   相似文献   

8.
空间材料Kapton的真空紫外与 原子氧复合效应研究   总被引:7,自引:0,他引:7  
对空间常用聚合物材料Kapton开展了真空紫外辐射及其与原子氧复合效应的地面模拟试验研究,总结了试验前后试样外观、质量、表面形貌、光学参数和表面成分的变化规律,并对反应机理作了初步的分析.结果表明:在原子氧的作用下,Kapton的剥蚀主要是碳氮等元素的氧化所致.而在真空紫外辐射的作用下,Kapton表面会交联形成大分子,从而提高了试样的抗原子氧剥蚀性能.但是,随着原子氧累积通量的增大,这层大分子会逐渐被剥蚀掉,而真空紫外辐射,对Kapton的原子氧效应试验结果没有影响.   相似文献   

9.
使用原子氧效应地面模拟设备对硅橡胶材料O型圈进行了原子氧暴露实验;用测压法进行了O型圈在原子氧暴露前后的泄漏率比对实验,并对实验前后O型圈表面形貌特征作了扫描电镜分析.实验表明:原子氧对O型圈表面有很大的剥蚀效应;O型圈经过原子氧暴露后,质量减少、泄漏率明显增大;暴露时间越长,表面形貌受到的损坏越严重、质量减少量越多,泄漏率也就越大.   相似文献   

10.
对光抽运小铯束管的光频移进行了测量 ,并对结果进行了简要的分析 ,估算了射入Ramsey腔的相应光强。导致光频移的光源是抽运光和检测光通过漫反射进入微波腔的部分和原子束中的铯原子自发辐射所产生的荧光。  相似文献   

11.
利用Helios2飞船的数据,对太阳风速度分布中质子束流部分与整个质子的密度之比随日心距离的变化做了分析.为了排除碰撞因素的影响,有针对性地分析了太阳风高速流(600相似文献   

12.
太阳神飞船观测表明,太阳风高速流中质子束分量相对于核分量的密度随日心距离增加而增加.提出解释这一观测现象的机理并给出二维数值模拟结果.由于阿尔芬波速随日心距离增加而减少,第二支左旋波将与更多的质子共振,把部分原来属于核分布的质子拉到束分布中来.用数值模拟方程方法求解回旋波共振导致的准线性扩散方程,数值结果与观测结果相符合.  相似文献   

13.
For extrasolar space exploration it might be very convenient to take advantage of space environmental effects such as solar radiation heating to accelerate a solar sail coated by materials that undergo thermal desorption at a particular temperature. Thermal desorption can provide additional thrust as heating liberates atoms, embedded on the surface of the solar sail. We are considering orbital dynamics of a solar sail coated with materials that undergo thermal desorption at a specific temperature, as a result of heating by solar radiation at a particular heliocentric distance, and focus on two scenarios that only differ in the way the sail approaches the Sun. For each scenario once the perihelion is reached, the sail coat undergoes thermal desorption. When the desorption process ends, the sail then escapes the Solar System having the conventional acceleration due to solar radiation pressure. We study the dependence of a cruise speed of a solar sail on perihelion of the orbit where the solar sail is deployed. The following scenarios are considered and analyzed: (1) Hohmann transfer plus thermal desorption. In this scenario the sail would be carried as a payload to the perihelion with a conventional propulsion system by a Hohmann transfer from Earth’s orbit to an orbit very close to the Sun and then be deployed. Our calculations show that the cruise speed of the solar sail varies from 173?km/s to 325?km/s that corresponds to perihelion 0.3?AU and 0.1 AU, respectively. (2) Elliptical transfer plus Slingshot plus thermal desorption. In this scenario the transfer occurs from Earth’s orbit to Jupiter’s orbit; then a Jupiter’s fly-by leads to the orbit close to the Sun, where the sail is deployed and thermal desorption comes active. In this case the cruise speed of the solar sail varies from 187?km/s to 331?km/s depending on the perihelion of the orbit. Our study analyses and compares the different scenarios in which thermal desorption comes beside traditional propulsion systems for extrasolar space exploration.  相似文献   

14.
In order to prepare infrared sounding of comet Halley from the flyby VEGA probes, we have computed the synthetic spectrum between 2.5 and 15 μ of a typical comet at a heliocentric distance of ~ 0.8 AU. The present paper is particularly devoted to the contribution from the cometary gases. For a selection of 20 possible parent molecules, the most efficient excitation process is resonant fluorescence by the solar radiation field. The H2O, CO, CO2, CH4, NH3 and H2CO molecules are the best candidates for detection by the IKS infrared spectrometers aboard the VEGA probes. For the water molecule, collisions are too rare to ensure thermal equilibrium in the whole coma ; therefore a limited number of fluorescence lines are expected to be present in the H2O vibrational bands.  相似文献   

15.
Recent results of theoretical investigations related to generation of high-energy (0.1-1 keV) photons in comets due to production of high-temperature (3×105-107 K) plasma clots from collisions of cometary and interplanetary grains at high relative velocities (70-700 km s−1 at heliocentric distances R=0.01-1 AU) are summarized and main features of the process are marked.  相似文献   

16.
Based on the computed equilibrium temperature of evaporating dirty water-ice grains, dirty water-ice halo is examined, taking into account of a size dependence of terminal velocity of dust at P/Halley. It is found that due to an enhanced grain's temperature caused by dirtiness, icy halo cannot extend over 100 km from the nucleus when comet approaches inside a solar distance r of 1 AU. Therefore, it is unlikely that the ice bands in the near infrared wavelengths could be detected in the cometary coma at r<1 AU.  相似文献   

17.
On 15th February 1992, ISAS space engineering satellite HITEN was successfully inserted into an elliptical orbit around the moon with perilune between some 100 km and 8000 km and apolune of about 50.000 km. On board was a small scientific experiment designed to detect cosmic dust particles, MDC - Munich Dust Counter. During a period of more than one year, until Hiten's hard landing on the moon surface at 10th of April 1993 (UTC), measurements of impact velocity, mass and crude flight direction of micrometeoroid particles have been performed. In total 150 cosmic dust impacts were detected and evaluated. From these measurements, the impact rate versus time and the dust flux versus distance from the moon are derived. The evidence of moon ejecta and some indications of particles which are orbiting the moon will be discussed. The spatial distribution of the measured particles is shown in lunarcentric as well as in heliocentric coordinate systems. The directional distribution is also given, showing the different populations of cosmic dust particles. Finally, the gathered data will be compared with previous results from measurements in the vicinity of the Earth and in the geomagnetic tail region.  相似文献   

18.
文章分析了I型彗尾风差角的大量资料, 得出其变化和日心距离的关系是不大的;但对日心黄纬, 却显示出逐渐减小的趋向.文章还得出, 风差角的变化随着彗星的切向速度而单调上升, 从而进一步证实了动力风差原理是形成风差角的主要因素.在此基础上, 分析了太阳风速度场的分布特性, 得出了平均太阳风速度随日心距离的变化是不明显的, 而随日心黄纬有着缓慢增强的趋势.   相似文献   

19.
Results of investigations of cosmogenic isotope radioactivity in chondrites fallen to earth during two solar cycles are presented. The data obtained on radial and latitudinal gradients cover the period 1955–1976, heliocentric distances from 1.03 AU to 3.33 AU, and heliographic latitudes from 23°S to 16°N. The dependence of radial and latitudinal gradients on the phase of solar activity is established, as well as a north-south asymmetry during a certain period after the inversion of the general solar magnetic field in 1969.  相似文献   

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