确定威布尔分布三参数的相关系数优化法

 根据本文给出的确定威布尔分布三参数的相关系数优化法求得的威布尔三参数,能使试验数据在威布尔概率坐标纸上最大限度地呈现为线性关系。     

固体火箭喷管排气中的粒子分布

1.前言 现代的固体火箭发动机为提高推进剂的能量特性及抑制不稳定燃烧，常常在推进剂中添加金属粉末，最常见的是加金属铝粉。在发动机工作时，铝粉燃烧形成凝聚相的氧化铝粒子。这些粒子在喷管中的流动过程中，温度、速度等方面的变化滞后于燃·气本身的变     

初始缺陷尺寸分布的尺寸效应研究

疲劳结构可能的开裂区域面积不同引起结构可能萌生裂纹的初始缺陷尺寸分布各异是造成"疲劳尺寸效应" 的一个可能解释。研究了试样测试部分尺寸大小与萌生裂纹的初始缺陷尺寸分布的关系,并建立了分析模型。模型利用已知的小尺寸试样的初始缺陷尺寸分布和大小试样的开裂面积比,推导出了相同条件下未知大尺寸试样的初始缺陷尺寸分布。这为结构完整性研究以及基于小裂纹扩展理论大尺寸试样的耐久性分析和疲劳全寿命预测打下基础,并为进一步研究"疲劳尺寸效应"创造了条件。     

Alfvénic Electron Acceleration in Aurora Occurs in Global Alfvén Resonosphere Region

Auroral emission caused by electron precipitation (Hardy et al., 1987, J. Geophys. Res. 92, 12275–12294) is powered by magnetospheric driving processes. It is not yet fully understood how the energy transfer mechanisms are responsible for the electron precipitation. It has been proposed (Hasegawa, 1976, J. Geophys. Res. 81, 5083–5090) that Alfvén waves coming from the magnetosphere play some role in powering the aurora (Wygant et al., 2000, J. Geophys. Res. 105, 18675–18692, Keiling et al., 2003, Science 299, 383–386). Alfvén-wave-induced electron acceleration is shown to be confined in a rather narrow radial distance range of 4–5 R _E (Earth radii) and its importance, relative to other electron acceleration mechanisms, depends strongly on the magnetic disturbance level so that it represents 10% of all electron precipitation power during quiet conditions and increased to 40% during disturbed conditions. Our observations suggest that an electron Landau resonance mechanism operating in the “Alfvén resonosphere” is responsible for the energy transfer.     

EB-PVD制备箔材的厚度均匀性研究

从真空蒸镀中使用的小平面蒸发源理论出发,针对电子束物理气相沉积中为改善箔材厚度分布所须旋转大基板进行蒸镀的情况,建立了该过程的数学模型;并利用该模型对不同的坩埚位置所沉积的箔材厚度进行了定性分析,从而实现了对坩埚与基板相对位置的优化,使基板上沉积的箔材厚度分布可以达到最均匀的状态.最后通过K值的提出使理论和实际箔材厚度的结果趋于一致,即证明所建立的数学模型是合理的.     

基于SFEM的SRM纤维缠绕结构的可靠性分析

采用纽曼级数展开的蒙特卡罗随机有限元方法(SFEM),分析了固体火箭发动机(SRM)复合材料缠绕的燃烧室在内压正态变化下的应力响应,然后利用应力强度干涉原理分析计算其可靠性.     

基于对数正态分布第k试验寿命的分散系数法

针对发动机构件寿命试验评估中对寿命分散系数计算公式与不同取值的需求,本文导出了寿命符合对数正态分布、基于任意第k试验寿命分散系数计算公式。并给出置信度为0.95、可靠度为99.87%、母体对数正态标准差lσgN=0.13时的寿命分散系数。本文基于最差试件寿命的分散系数与已有文献一致,而基于最好试件寿命分散系数较已有文献更为合理;采用本文公式可得到任意给定置信度、可靠度、寿命分散条件下的寿命分散系数,可供工程上评估构件寿命时使用。      

光盘形结构风荷载的风洞实验研究

应用风洞模拟实验研究了光盘形状结构的风荷载特性.风洞实验结果表明,在没有周围建筑物影响时,由于光盘形结构的截面具有对称翼型,上、下表面受到风荷载基本上都是负压分布,叠加后作用在光盘结构上的总体风荷载很小.周围建筑的存在对光盘形的风荷载影响很大,有周围建筑时光盘形结构所受的升力要比没有周围建筑时的值大1～3倍以上.特别有趣的是单独光盘形结构的整体风荷载除了受到一个升力的作用外,还受到了一个迎风低头的翻转力矩,为类似结构的风荷载设计提供了有益的启示.     

一种涡轮发动机加速控制规律设计的新方法

 提出了一种涡喷、涡扇发动机加速控制规律快速设计的新方法：在发动机稳态特性计算模型的基础上,通过额外增加转子提取功率,使得发动机稳态工作点（线）靠近喘振边界,在同时考虑燃烧室富油熄火边界、涡轮进口总温限制以及压气机喘振裕度限制的条件下,利用适当的控制规律描述形式并结合发动机工程研制中的经验,能够快速而准确地获得涡喷、涡扇发动机加速控制规律。对某型涡喷发动机加速控制规律的改进的计算结果表明,提出的加速控制规律的设计方法准确而有效。     

MESSENGER: Exploring Mercury’s Magnetosphere

The MErcury Surface, Space ENvironment, GEochemistry, and Ranging (MESSENGER) mission to Mercury offers our first opportunity to explore this planet’s miniature magnetosphere since the brief flybys of Mariner 10. Mercury’s magnetosphere is unique in many respects. The magnetosphere of Mercury is among the smallest in the solar system; its magnetic field typically stands off the solar wind only ∼1000 to 2000 km above the surface. For this reason there are no closed drift paths for energetic particles and, hence, no radiation belts. Magnetic reconnection at the dayside magnetopause may erode the subsolar magnetosphere, allowing solar wind ions to impact directly the regolith. Inductive currents in Mercury’s interior may act to modify the solar wind interaction by resisting changes due to solar wind pressure variations. Indeed, observations of these induction effects may be an important source of information on the state of Mercury’s interior. In addition, Mercury’s magnetosphere is the only one with its defining magnetic flux tubes rooted beneath the solid surface as opposed to an atmosphere with a conductive ionospheric layer. This lack of an ionosphere is probably the underlying reason for the brevity of the very intense, but short-lived, ∼1–2 min, substorm-like energetic particle events observed by Mariner 10 during its first traversal of Mercury’s magnetic tail. Because of Mercury’s proximity to the sun, 0.3–0.5 AU, this magnetosphere experiences the most extreme driving forces in the solar system. All of these factors are expected to produce complicated interactions involving the exchange and recycling of neutrals and ions among the solar wind, magnetosphere, and regolith. The electrodynamics of Mercury’s magnetosphere are expected to be equally complex, with strong forcing by the solar wind, magnetic reconnection, and pick-up of planetary ions all playing roles in the generation of field-aligned electric currents. However, these field-aligned currents do not close in an ionosphere, but in some other manner. In addition to the insights into magnetospheric physics offered by study of the solar wind–Mercury system, quantitative specification of the “external” magnetic field generated by magnetospheric currents is necessary for accurate determination of the strength and multi-polar decomposition of Mercury’s intrinsic magnetic field. MESSENGER’s highly capable instrumentation and broad orbital coverage will greatly advance our understanding of both the origin of Mercury’s magnetic field and the acceleration of charged particles in small magnetospheres. In this article, we review what is known about Mercury’s magnetosphere and describe the MESSENGER science team’s strategy for obtaining answers to the outstanding science questions surrounding the interaction of the solar wind with Mercury and its small, but dynamic, magnetosphere.