Deep Impact Mission Design

The Deep Impact mission is designed to provide the first opportunity to probe below the surface of a comet nucleus by a high-speed impact. This requires finding a suitable comet with launch and encounter conditions that allow a meaningful scientific experiment. The overall design requires the consideration of many factors ranging from environmental characteristics of the comet (nucleus size, dust levels, etc.), to launch dates fitting within the NASA Discovery program opportunities, to launch vehicle capability for a large impactor, to the observational conditions for the two approaching spacecraft and for telescopes on Earth.     

Deep Impact: A Large-Scale Active Experiment on a Cometary Nucleus

The Deep Impact mission will provide the first data on the interior of a cometary nucleus and a comparison of those data with data on the surface. Two spacecraft, an impactor and a flyby spacecraft, will arrive at comet 9P/Tempel 1 on 4 July 2005 to create and observe the formation and final properties of a large crater that is predicted to be approximately 30-m deep with the dimensions of a football stadium. The flyby and impactor instruments will yield images and near infrared spectra (1–5 μm) of the surface at unprecedented spatial resolutions both before and after the impact of a 350-kg spacecraft at 10.2 km/s. These data will provide unique information on the structure of the nucleus near the surface and its chemical composition. They will also used to interpret the evolutionary effects on remote sensing data and will indicate how those data can be used to better constrain conditions in the early solar system.     

The History and Dynamics of Comet 9P/Tempel 1

Since its discovery in 1867, periodic comet 9P/Tempel 1 has been observed at 10 returns to perihelion, including all its returns since 1967. The observations for the seven apparitions beginning in 1967 have been fit with an orbit that includes only radial and transverse nongravitational accelerations that model the rocket-like thrusting introduced by the outgassing of the cometary nucleus. The successful nongravitational acceleration model did not assume any change in the comet’s ability to outgas from one apparition to the next and the outgassing was assumed to reach a maximum at perihelion. The success of this model over the 1967–2003 interval suggests that the comet’s spin axis is currently stable. Rough calculations suggest that the collision of the impactor released by the Deep Impact spacecraft will not provide a noticeable perturbation on the comet’s orbit nor will any new vent that is opened as a result of the impact provide a noticeable change in the comet’s nongravitational acceleration history. The observing geometries prior to, and during, the impact will allow extensive Earth based observations to complement the in situ observations from the impactor and flyby spacecraft.     

模糊σ-代数上的模糊数值测度及应用(Ⅰ)

设(Χ,A,μ)是一个全有限测度空间,H为由A生成的模糊σ-代数。通过计算H中模糊子集的截集的测度,运用一维模糊数的嵌入定理,构造了一种定义在H上取值于一维模糊数空间的测度,这种测度限制在A上就是测度μ,并且具有可列可加性、下连续性、上连续性、自连续性等性质。这种测度取值一维模糊数,保留了模糊子集较多的信息,所以它可以更为细致地刻划模糊子集。作为在模糊聚类理论方面的应用,把(Χ,A,μ)上用于度量普通集合间不相似性的度量推广到了H上的模糊子集间,得到了一种基本的H上不相似度量。     

地球观测科学的发展以及空间站对地观测

综述了地球观测科学的发展以及空间站对地观测。对载人空间站在对地观测中的优势、类型和应用进行了重点论述。介绍了我国空间站对地观测应用的重要意义。最后，论述了以空间站为核心的天基信息网和遥感技术的快速发展是空间对地观测的主要发展趋势。     

飞行控制系统故障检测方法研究

以某型飞机为研究对象，论述了一种基于模型的自修复飞行控制系统故障检测方法。首先提出了通过等价空间法产生残差序列，并对残差序列进行概率比检测，以获得一定置信度下的检测结果。同时舵面损伤故障的概率比检测采用预警检验、校验检测与隔离检测相结合的方法。最后，对所设计的故障检测方法进行了数字仿真研究。仿真结果验证了该方法具有较高的准确性和实时性，为飞行控制系统故障检测提供了一种有效的手段。     

拓扑空间的泛函表示

本文首先指出并非所有的拓扑空间都能用连续函数表示，其次给出了一般拓扑空间的下半连续函数表示，并利用下半连续函数讨论了拓扑空间的一些性质。     

飞行控制系统舵面效率损失率估算方法研究

以某型飞机为研究对象，论述了一种基于模型的自修复飞行控制系统舵面效率损失率的估算方法。首次提出了采用多传感器信息融合来估算舵面效率损失率。因为舵面损伤故障采用全局滤波法检测，没有可直接测量其损伤程度的传感器，所以需要从飞控系统中多个传感器的测量信号综合判决来估算舵面损伤情况。最后，对所设计的舵面效率损失率的估算方法进行了数字仿真研究。仿真结果验证了该方法具有较高的准确性和实时性，为飞行控制系统舵面效率损失率的估算提供了一种有效的方法。     

N4SID辨识方法在航空发动机中的应用

针对在现代航空发动机的自适应控制和故障监控领域建立系统动态模型的需要 ,本文研究了基于状态空间模型的数字子空间状态空间系统辨识 (N4SID)方法 ,并在某型双转子涡喷发动机非线性气动热力学模型的“小偏离”状态上进行了仿真实验 ,结论表明 :该方法可以较准确地辨识发动机“小偏离”状态时的系统模型     

全尺寸二元喷管红外辐射特性研究

 设计了一种全尺寸二元收敛喷管,用涡轮喷气发动机 WP-6作为燃气发生器,在发动机处于最大状态时,用红外光谱仪对二元喷管及尾喷流的红外辐射进行了测试。研究结果表明,与基准喷管相比,在发动机产生相同推力的条件下,二元喷管改善了喷口和尾焰红外辐射的光谱分布,减小了红外源的尖峰辐射,明显降低了发动机的红外辐射强度。