用PDA测量两相湍流流场时固体粒子的选择

激光法测量两相流是近年来开发的一项新技术，测量过程中需要存在合适的粒子。本文研究了用三维粒子动态分析仪（ＰＤＡ）测量气固两相湍流流场时固体粒子的选择问题。试验过程中，运用几种不同的粒子作为煤粉粒子的模拟粒子进行测量和比较，结果表明：（１）粒子的特性参数是影响测量精度的重要因素之一；（２）测最气固两相湍流流场中粒子的运动特征时，应尽可能选择形状较规则、折射率大、尺寸分布合理、不易粘结且易于收集同时接近所要模拟的粒子性能的固体粒子，必要的时侯应结合粒子性能对测量结果进行修正．     

双参数指数分布下定时截尾恒加试验的统计分析

设产品寿命服从双参数指数分布ε（λ，μ），其中λ＞０为尺度参数（失效率），μ＞０为位置参数（保证寿命）。在加速应力水平Ｓｉ下，失效率和保证寿命的加速模型分别为 ｌｎθｉ＝β０＋β１ψ１（Ｓｉ）＋β２ψ２（Ｓｉ） μｉ＝α０－α１ｆ（Ｓｉ），ｉ＝１，２，…，ｋ 本文给出了定时截尾情形下对由恒定应力加速寿命试验得到的数据进行统计分析的方法。获     

中点箝位型光伏并网逆变器调制策略及效率对比

传统三电平中点箝位(Three-level neutral point clamped,3L-NPC)半桥逆变器在高压大功率条件下,由于开关器件损耗不均衡而使其容量受限,因此衍生了多种NPC型三电平半桥拓扑。为了优化选取NPC型拓扑及调制策略,对4种3L-NPC型拓扑(二极管NPC、有源式NPC、层叠式NPC及有源层叠式NPC)的调制策略及开关器件损耗分布进行了对比分析,并研制了一台5kW的NPC型统一实验平台,进行了效率测试。理论分析与实验结果表明:(1)根据零电平续流路径的配置不同,NPC型拓扑主要有4种调制策略;(2)选取合理的NPC型拓扑及调制策略,不仅可以均衡器件损耗,而且系统效率基本不变,为逆变器的扩容奠定了基础。     

窄分布纳米级HMX的制备及粒度分析

通过撞击法成功地制备了窄分布的纳米级HMX。实验结果表明，分散剂1和分散剂2能改善HMX的粒度分布。在分散剂1存在的条件下，用撞击法可制备出粒度分布较窄的纳米HMX颗粒，其d50分别为70．1nm和68．9nm，分布范围分别为0．9nm和1．4nm。     

低轨道带可变翼的平板型极高真空分子屏

本文计算了在低轨道自由飞行的平板型分子屏（ＷａｋｅＳｈｉｅｌｄＦａｃｉｌｉｔｙ）加了可变翼后，分子屏后实验区的压力分布。计算中考虑了分子屏和翼材料出气对实验区压力的影响。本文并对加可变翼和不加可变翼、考虑出气和不考虑出气几种情形进行了计算和比较。我们的结果表明：给轨道分子屏加上可变翼后，其实验区的压力可比不加可变翼降低一个数量级以上，压力达１０－１３Ｐａ。本文的研究表明，这种给轨道分子屏加可变翼的模型对更好的利用分子屏环境是非常有利的。     

Tether Satellite System Collision Study

A study was performed to determine the probability of collision with resident space objects and untrackable debris for the tether component of the Tethered Satellite System (TSS) after it broke away from the Space Shuttle orbiter (mission STS-75) in February 1996. Both an analytical and a numerical approach were used in this study, and the results obtained with these two methods were found to be in good agreement. These results show that the deployed tether is expected to have been impacted by several particles 0.1mm or larger in size. The probability of collision with objects 10cm in size or larger was on the order of 10^–3 per month. Since the severed tether reentered within one month after deployment, the collision hazard to other objects while in orbit was small. The analytical methods used in this study are useful for tether collision evaluations in general.     

高压金属软管应力及参数敏感度分析

某型号发动机热试车考核中高压金属软管多次出现破坏。通过建立软管有限元模型,采用非线性有限元分析了软管应力分布和各部分承载特点,判断波峰处轴向应力是影响软管结构强度的主要因素,有限元计算结果和试验破坏部位一致,表明有限元模型的合理性。在此基础上,通过参数化建模、设计中心复合实验和进行参数敏感度分析,得出影响波峰处最大轴向应力的敏感参数,为结构参数优化提供了依据。     

Experimental study of a flush wall scramjet combustor equipped with strut/wall fuel injection

In this study a flush wall scramjet combustor is tested in a supersonic incoming air flow with the Mach number of 3 which is generated by an air vitiation heater producing the stagnation temperature of 1505 K. Using liquid kerosene as the fuel, the flame is stabilized by means of a centrally mounted O₂ pilot strut after being ignited by a plasma torch. During experimental measurements, the fuel is injected with a constant equivalence ratio of 0.8 according to specified strut/wall injection ratios, i.e., a portion of the fuel amount is injected from the strut while the rest is injected from the wall. The strut and wall injectors are arranged at the same axial position. The combustion performance and wall temperature gradients are evaluated with various fuel feeding ratios between the wall and the strut. Experimental results show, when the equivalence ratio is constant and the axial injection position is fixed, the combustion characteristics vary significantly with the strut/wall fuel feeding ratio, especially when this ratio is close to its lowest and highest limits. Among the four fuel feeding ratios examined, the strut only injection mode and the average distributed strut/wall injection mode show the best combustion performance. However, the strut/wall injection mode produces a smaller wall temperature gradient compared to the strut only injection mode, which is due to the significant film cooling effect caused by the wall injected liquid kerosene.     

小半径弯管弯胀复合成形研究

为解决小半径弯管内侧起皱、外侧减薄的成形缺陷,提出了一种弯胀复合成形的方法。通过几何关系解析了初始弯曲半径和初始管坯直径与最终管径和最终弯曲半径之间的关系,确定了初始弯曲半径的取值范围。采用有限元与实验相结合的方式研究了不同初始弯曲半径对零件壁厚分布的影响,分析了胀形过程中零件弯曲处及直壁处的变形规律。最终发现:初始弯曲半径越大,零件的最终减薄越小,胀形过程中弯曲处内外侧发生均匀减薄,直壁处内侧减薄明显大于外侧减薄。     

部分球壳分布离子流激发的电磁不稳定性

在离子环束流和低频电磁波相互作用的过程中廓了环束流将演化成具有投掷角展宽的部分球壳速度分布离子流,其投掷角展宽随时间增大,低频右旋电磁不稳定性增长率峰值,总的说来也逐渐增大,并向高频短波方向移动,与此相反,低频左旋电磁不稳定性增长率峰值,当投掷 角展宽等于０时,大于右旋不稳定性峰值,但随着投掷角展宽增加而迅速低于右 性增长率峰值,并向工波方向移动。