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61.
空间微小碎片撞击对太阳能电池性能影响   总被引:1,自引:1,他引:0  
文章利用中国科学院空间科学与应用研究中心的等离子体驱动微小碎片加速器,进行了空间微小碎片累积撞击太阳能电池的模拟试验。之后,利用体式显微镜统计出太阳能电池表面的撞击坑,并测量了撞击前后太阳能电池的开路电压、短路电流、最大输出功率等参数的变化。试验结果与理论分析揭示了引起太阳能电池功率衰减的主要原因是碎片累积撞击导致的太阳能电池表面损伤。  相似文献   
62.
超高速撞击中的弹丸形状效应数值模拟研究   总被引:2,自引:0,他引:2  
文章用AUTODYN仿真软件对球形、圆锥形、圆柱形和盘形4种不同形状弹丸超高速撞击Whipple防护结构所产生的碎片云形貌特征及对后墙的毁伤程度进行了数值仿真研究。对比分析结果指出:质量与速度相等的4种不同形状弹丸撞击缓冲屏所产生的碎片云有明显差异;弹丸长径比越小,穿过缓冲屏后的破碎程度越大;在5 km/s撞击速度下,球形弹丸对后墙的毁伤程度最小,而圆柱形弹丸的毁伤程度最大。这说明弹丸的形状对超高速撞击结果有显著影响,在航天器超高速撞击风险评估和防护工程设计中应充分考虑弹丸的形状效应。球形弹丸的弹道极限曲线在防护结构的碎片防护能力评价时存在高估的问题,在实际工作中要特别注意这一点。  相似文献   
63.
为研究超高速碰撞过程中所产生碎片云的特性,在中国空气动力研究与发展中心超高速所碰撞靶上发展了四序列激光阴影照相系统.该系统由YAG激光光源、阴影仪、成像系统和控制系统组成,在采用多光源空间分离、偏振分光、光束角放大、补偿式滤光等技术后,获得了撞击速度v=4. 6km/s时碎片云的四序列阴影照片.笔者对该系统的工作原理、调试情况及试验结果进行了介绍.调试及试验结果表明:(1)该系统可以获得最小间隔为1μs、曝光时间为10ns的4个不同时刻的超高速碰撞碎片云图像,满足碰撞试验中对碎片云照相的要求;(2)该技术可以发展为更多序列激光阴影照相系统,并应用于其它超高速瞬态过程的测量显示.  相似文献   
64.
天基照相跟踪空间碎片批处理轨道确定研究   总被引:1,自引:0,他引:1  
随着国内外天基观测空间碎片研究的展开,文章提出了利用跟踪卫星的CCD(Charge
Coupled Device)相机对空间碎片进行轨道探测的方法,首先建立了CCD照相观测模型和基于 照相观测 的空间碎片批处理轨道确定模型。通过对CCD相机底片归算方法的分析可知,利用
CCD相机所获得的观测数据与跟踪卫星的姿态无关,且其精度只与测量和坐标转换计算的精 度有关,在测量和计算中可获得较高的精度。分别对分布密度较高的低轨道和地球同步 轨道区域的空间碎片进行了定轨分析。仿真结果表明,定轨时采用两个跟踪弧段的照相数据 定轨精度大大高于一个弧段照相数据的定轨精度;跟踪卫星距离空间碎片越近,定轨精度越 高;低轨道空间碎片的定轨精度高于地球同步轨道上的空间碎片定轨精度。
  相似文献   
65.
飞机设计中发动机转子碎片非包容性设计   总被引:2,自引:0,他引:2  
基于一种双发常规布局飞机进行飞机设计中发动机转子碎片非包容失效设计的研究,通过研究相关适航规章,以及相关咨询通告等文件,得出第3节到第7节所描述的对咨询通告AC20-128A适当裁剪的工程方法和步骤,并在实例机型设计中进行验证,缩短了飞机研制周期的同时,也表明在发动机转子碎片非包容失效事故发生后,飞机系统及机体结构等采取的设计措施、防范措施符合相关适航条例要求,也即结构剩余的强度、灾难性事件发生概率等满足AC20-128A第10条c中的定性和定量要求,表明该型实例飞机完全满足相关适航条例的要求,并获得中国民用航空局(CAAC)和美国联邦航空局(FAA)的认可。  相似文献   
66.
This paper presents a new method for estimating ballistic coefficients (BCs) of low perigee debris objects from their historical two line elements (TLEs). The method uses the drag perturbation equation of the semi-major axis of the orbit. For an object with perigee altitude below 700 km, the variation in the mean semi-major axis derived from the TLE is mainly caused by the atmospheric drag effect, and therefore is used as the source in the estimation of the ballistic coefficient. The method is tested using the GRACE satellites, and a number of debris objects with external ballistic coefficient values, and agreements of about 10% are achieved.  相似文献   
67.
In order to test laser ranging possibilities to space debris objects, the Satellite Laser Ranging (SLR) Station Graz installed a frequency doubled Nd:YAG pulse laser with a 1 kHz repetition rate, a pulse width of 10 ns, and a pulse energy of 25 mJ at 532 nm (on loan from German Aerospace Center Stuttgart – DLR). We developed and built low-noise single-photon detection units to enable laser ranging to targets with inaccurate orbit predictions, and adapted our standard SLR software to include a few hundred space debris targets. With this configuration, we successfully tracked – within 13 early-evening sessions of each about 1.5 h – 85 passes of 43 different space debris targets, in distances between 600 km and up to more than 2500 km, with radar cross sections from >15 m2 down to <0.3 m2, and measured their distances with an average precision of about 0.7 m RMS.  相似文献   
68.
Breakup model is the key area of space debris environment modeling. NASA standard breakup model is currently the most widely used for general-purpose. It is a statistical model found based on space surveillance data and a few ground-based test data. NASA model takes the mass, impact velocity magnitude for input and provides the fragment size, area-to-mass ratio, velocity magnitude distributions for output. A more precise approach for spacecraft disintegration fragment analysis is presented in this paper. This approach is based on hypervelocity impact dynamics and takes the shape, material, internal structure and impact location etc. of spacecraft and impactor, which might greatly affect the fragment distribution, into consideration. The approach is a combination of finite element and particle methods, entitled finite element reconstruction (FER). By reconstructing elements from the particle debris cloud, reliable individual fragments are identified. Fragment distribution is generated with undirected graph conversion and connected component analysis. Ground-based test from literature is introduced for verification. In the simulation satellite targets and impactors are modeled in detail including the shape, material, internal structure and so on. FER output includes the total number of fragments and the mass, size and velocity vector of each fragment. The reported fragment distribution of FER shows good agreement with the test, and has good accuracy for small fragments.  相似文献   
69.
Under ESA contract an industrial consortium including Aboa Space Research Oy (ASRO), the Astronomical Institute of the University of Bern (AIUB), and the Dutch National Aerospace Laboratory (NLR), proposed the observation concept, developed a suitable sensor architecture, and assessed the performance of a space-based optical (SBO) telescope in 2005. The goal of the SBO study was to analyse how the existing knowledge gap in the space debris population in the millimetre and centimetre regime may be closed by means of a passive optical instrument. The SBO instrument was requested to provide statistical information on the space debris population in terms of number of objects and size distribution. The SBO instrument was considered to be a cost-efficient with 20 cm aperture and 6° field-of-view and having flexible integration requirements. It should be possible to integrate the SBO instrument easily as a secondary payload on satellites launched into low-Earth orbits (LEO), or into geostationary orbit (GEO). Thus the selected mission concept only allowed for fix-mounted telescopes, and the pointing direction could be requested freely. Since 2007 ESA focuses space surveillance and tracking activities in the Space Situational Awareness (SSA) preparatory program. Ground-based radars and optical telescopes are studied for the build-up and maintenance of a catalogue of objects. In this paper we analyse how the proposed SBO architecture could contribute to the space surveillance tasks survey and tracking. We assume that the SBO instrumentation is placed into a circular sun-synchronous orbit at 800 km altitude. We discuss the observation conditions of objects at higher altitude, and select an orbit close to the terminator plane. A pointing of the sensor orthogonal to the orbital plane with optimal elevation slightly in positive direction (0° and +5°) is found optimal for accessing the entire GEO regime within one day, implying a very good coverage of controlled objects in GEO, too. Simulations using ESA’s Program for Radar and Optical Observation Forecasting (PROOF) in the version 2005 and a GEO reference population extracted from DISCOS revealed that the proposed pointing scenario provides low phase angles together with low angular velocities of the objects crossing the field-of-view. Radiometric simulations show that the optimal exposure time is 1–2 s, and that spherical objects in GEO with a diameter of below 1 m can be detected. The GEO population can be covered under proper illumination nearly completely, but seasonal drops of the coverage are possible. Subsequent observations of objects are on average at least every 1.5 days, not exceeding 3 days at maximum. A single observation arc spans 3° to 5° on average. Using a simulation environment that connects PROOF to AIUB’s program system CelMech we verify the consistency of the initial orbit determination for five selected test objects on subsequent days as a function of realistic astrometric noise levels. The initial orbit determination is possible. We define requirements for a correlator process essential for catalogue build-up and maintenance. Each single observation should provide an astrometric accuracy of at least 1”–1.5” so that the initially determined orbits are consistent within a few hundred kilometres for the semi-major axis, 0.01 for the eccentricity, and 0.1° for the inclination.  相似文献   
70.
One of the primary mission risks tracked in the development of all spacecraft is that due to micro-meteoroids and orbital debris (MMOD). Both types of particles, especially those larger than 0.1 mm in diameter, contain sufficient kinetic energy due to their combined mass and velocities to cause serious damage to crew members and spacecraft. The process used to assess MMOD risk consists of three elements: environment, damage prediction, and damage tolerance. Orbital debris risk assessments for the Orion vehicle, as well as the Shuttle, Space Station and other satellites use ballistic limit equations (BLEs) that have been developed using high speed impact test data and results from numerical simulations that have used spherical projectiles. However, spheres are not expected to be a common shape for orbital debris; rather, orbital debris fragments might be better represented by other regular or irregular solids. In this paper we examine the general construction of NASA’s current orbital debris (OD) model, explore the potential variations in orbital debris mass and shape that are possible when using particle characteristic length to define particle size (instead of assuming spherical particles), and, considering specifically the Orion vehicle, perform an orbital debris risk sensitivity study taking into account variations in particle mass and shape as noted above. While the results of the work performed for this study are preliminary, they do show that continuing to use aluminum spheres in spacecraft risk assessments could result in an over-design of its MMOD protection systems. In such a case, the spacecraft could be heavier than needed, could cost more than needed, and could cost more to put into orbit than needed. The results obtained in this study also show the need to incorporate effects of mass and shape in mission risk assessment prior to first flight of any spacecraft as well as the need to continue to develop/refine BLEs so that they more accurately reflect the shape and material density variations inherent to the actual debris environment.  相似文献   
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