纤维增强复合材料圆柱壳的屈曲计算

本文利用各向异性多层扁壳的大挠度方程,探讨了正交各向异性多层圆柱壳,在考虑偶合效应和沿厚度方向剪切变形时的轴压,外压及其联合作用下的稳定性问题.用逆解法,给出正交各向异性多层圆柱壳在薄膜力作用下的临界载荷算式.进行了实例计算,并与国内、外实例的实验值比较,符合得相当好.     

国有企业产权交易中应注意的问题

现代产权制度的重要内容之一是产权要具有可交易性。对资不抵债、无规模效益、重复建设、资产闲置的国有企业实施出售、兼并、股份转让等产权交易 ,可实现资源的有效配置 ,完成国有经济的战略性调整。在产权交易过程中 ,为防止国有资产的流失 ,提高社会经济效益 ,保护国家和人民的利益 ,应充分注意国有企业产权交易中的资产定价、资产有价证券化、资本市场及产权交易效率等问题     

网上考试系统的设计与实现

本文讨论了一种新的考试方法———网上考试 ,并讨论了一种基于B/S系统实现网上考试的思路和设计方法 ,并对实现网上考试系统的部分关键技术进行了分析     

基于双口RAM的智能429总线接口卡设计

利用89C52单片机和双口RAM IDT7132设计了智能ARINC429总线接口卡。采用单片机使接口卡具有了自动数据处理能力，实现了智能化；采取双口RAM作为单片机和ISA总线数据交互媒介，提高了传输速率。讨论了双口RAM的地址空间分配和数据共享冲突仲裁问题，对接口卡的软件设计做了介绍。应用表明，所设计的接口卡具有传输速率高、可靠性好等优点。     

民机数据总线信号综合测试仪

介绍的民机数据总线信号测试仪综合了当前民机上主要采用的ARINC429、ARINC419、CSDB和RS232等数字式航空数据总线规范的接口，具有和这些总线接口设备通讯的能力，可以灵活方便地应用于机载设备检测，装机交联实验当中。     

TiAl合金不同钛铝比层片组织的稳定性

对钛铝比为１．１７４、１．１０５和１．０４１的（ＴｉＡｌ）－２．５Ｖ－１Ｃｒ（ａｔ％）合金层片组织在１３２３Ｋ热暴露中的组织变化进行了观察和分析。发现钛铝比对ＴｉＡｌ合金层片组织的稳定性和失稳分解机理有重要影响，钦铝比适当大于１：１（如１．１０５）的合金可以得到稳定性更好的层片组织。     

基于超声波的复合材料层间剪切强度表征分析

采用数字采样、相关分析、频谱分析等方法,结合部分复合材料层板剪切强度试验,验证材料性能与分析结果的对应性、研究分析参数的选择,为无损表征复合材料剪切强度的可行性做了有益的探索.     

靶场测控通信系统可靠性分析

首先确定了测控通信系统可靠性分析框架，然后针对系统构型为串并联系统、试验信息为成败型数据／寿命型数据的情况，研究了可靠性信息融合的Bayes方法，最后讨论了系统可靠性的Bayes统计推断问题，包括点估计、置信估计和假设检验。     

基于FW-H方程的旋翼气动声学计算研究

由流体力学N S方程导出的非齐次波动方程———FfowcsWilliams Hawkings方程(简称FW H方程),可以精确地描述在静止流体中运动的物体与流体相互作用的发声问题。以FW H方程为理论模型,将旋翼桨叶运动发声问题等效为包含桨叶的任意运动控制面(声源面)的声辐射问题,并在旋翼绕流Euler方程数值模拟的基础上,在时域内计算了悬停旋翼和前飞旋翼的声场。应用于UH 1H和AH 1/OLS两种旋翼模型的气动声学计算表明:计算结果与噪声实验值符合良好;所研制的程序不仅能够较准确地计算单极子噪声和偶极子噪声,而且具有较强的跨音速四极子噪声预测能力。     

Deep Impact: Working Properties for the Target Nucleus – Comet 9P/Tempel 1

In 1998, Comet 9P/Tempel 1 was chosen as the target of the Deep Impact mission (A’Hearn, M. F., Belton, M. J. S., and Delamere, A., Space Sci. Rev., 2005) even though very little was known about its physical properties. Efforts were immediately begun to improve this situation by the Deep Impact Science Team leading to the founding of a worldwide observing campaign (Meech et al., Space Sci. Rev., 2005a). This campaign has already produced a great deal of information on the global properties of the comet’s nucleus (summarized in Table I) that is vital to the planning and the assessment of the chances of success at the impact and encounter. Since the mission was begun the successful encounters of the Deep Space 1 spacecraft at Comet 19P/Borrelly and the Stardust spacecraft at Comet 81P/Wild 2 have occurred yielding new information on the state of the nuclei of these two comets. This information, together with earlier results on the nucleus of comet 1P/Halley from the European Space Agency’s Giotto, the Soviet Vega mission, and various ground-based observational and theoretical studies, is used as a basis for conjectures on the morphological, geological, mechanical, and compositional properties of the surface and subsurface that Deep Impact may find at 9P/Tempel 1. We adopt the following working values (circa December 2004) for the nucleus parameters of prime importance to Deep Impact as follows: mean effective radius = 3.25± 0.2 km, shape – irregular triaxial ellipsoid with a/b = 3.2± 0.4 and overall dimensions of ∼14.4 × 4.4 × 4.4 km, principal axis rotation with period = 41.85± 0.1 hr, pole directions (RA, Dec, J2000) = 46± 10, 73± 10 deg (Pole 1) or 287± 14, 16.5± 10 deg (Pole 2) (the two poles are photometrically, but not geometrically, equivalent), Kron-Cousins (V-R) color = 0.56± 0.02, V-band geometric albedo = 0.04± 0.01, R-band geometric albedo = 0.05± 0.01, R-band H(1,1,0) = 14.441± 0.067, and mass ∼7×10¹³ kg assuming a bulk density of 500 kg m⁻³. As these are working values, {i.e.}, based on preliminary analyses, it is expected that adjustments to their values may be made before encounter as improved estimates become available through further analysis of the large database being made available by the Deep Impact observing campaign. Given the parameters listed above the impact will occur in an environment where the local gravity is estimated at 0.027–0.04 cm s⁻² and the escape velocity between 1.4 and 2 m s⁻¹. For both of the rotation poles found here, the Deep Impact spacecraft on approach to encounter will find the rotation axis close to the plane of the sky (aspect angles 82.2 and 69.7 deg. for pole 1 and 2, respectively). However, until the rotation period estimate is substantially improved, it will remain uncertain whether the impactor will collide with the broadside or the ends of the nucleus.