锌磷酸盐玻璃掺杂VO~(2+)吸收光谱和EPR谱研究

3d1离子(如VO2+,V4+)是一类非常重要的离子,其掺杂电子顺磁共振谱已有大量的研究,积累了丰富的实验数据。利用3d1离子在四角压缩八面体对称中EPR参量的高阶微扰公式,计算了锌磷酸盐玻璃晶体中掺杂VO2+的EPR参量(g因子g‖,g⊥和超精细结构常数A‖,A⊥)和光吸收谱。由于锌磷酸盐玻璃晶体中掺杂VO2+中配体O2-的自旋-轨道耦合参量ζ0p(≈150cm-1)与中心过渡金属3d1离子V4+的ζ0d(≈248cm-1)相差不太大,故来自配体的自旋-轨道耦合参量ζ0p对EPR参量和光吸收谱的贡献必须予以考虑。采用重叠模型建立了杂质中心结构参数与电子顺磁共振(EPR)参量以及光吸收谱之间的定量关系;通过拟合锌磷酸盐玻璃中V4+中心的EPR参量和光吸收谱理论与试验符合,获得了杂质中心[VO6]8-基团的局域结构;研究发现,[VO6]8-基团的平行和垂直于C4轴的键长分别为:R‖≈0.175nm,R⊥≈0.197nm,即[VO6]8-基团的局域结构为沿C4轴方向呈压缩的八面体结构;所得EPR参量和光吸收谱的理论值与实验符合很好,并对上述结果的合理性进行了讨论。这说明微扰法可以用来研究材料中掺杂3d1过渡金属离子的EPR参量和光吸收谱。此外,对超精细结构常数(A‖和A⊥)的研究发现,较大的芯区极化常数κ值说明VO2+中未配对的s电子对超精细结构常数有较大的贡献。     

机动方舱核爆炸冲击波动力响应和安定性分析

本文以核爆炸当量、高度、距离为参数，采用等超压圆给出了普通方舱和防核加固方舱结构在核冲击波下的安全域。研究了限制舱体倾斜的压力条件。本文还以冲击波压力的时间函数为激励，求解了方舱的动力响应。从试验结果推论和计算模拟两方面，分析了方舱承受冲击波的能力。     

Nonlinear analysis of a structure loaded by a stochastic excitation

For a non-linear system excited by a stochastic load which is expressed as a time series,a recursive method based on the Z-transform is presented.To identify the obtained response time series,a discrete wavelet transform (DWT) technique is proposed.     

随机扰动的同宿分岔系统研究

利用一维扩展过程的奇点理论并结合能量包络的随机平均法，考查“隐藏在余维２分岔点之后”的同宿分岔系统受参激白噪声影响的分岔行为。     

压力梯度对湍流逆梯度输运的影响

研究Birkhoff系统的一般Lie对称性导致的非Noether守恒量. 得到非Noether守恒 量的存在定理，举例说明结果的应用.     

非牛顿流体有限长粗糙轴承分析

本文采用H.Christense力提出的随机粗糙模型,推导了幂律型流体纵向粗糙型和横向粗糙型润滑雷诺方程和相应的承载力、流量系数和摩擦系数的计算公式.对有限长动载径向轴承纵向粗糙型雷诺方程,用差分方法进行数值求解,得到了粗糙度和幂律指数对轴承的压力分布、承载力、流量系数和摩擦系数影响曲线,并有表面粗糙度和润滑油的非牛顿特性独立地影响轴承油膜力学特性的结论.     

Characterization of particle-laden, confined swirling flows by phase-doppler anemometry and numerical calculation

The particle dispersion characteristics in a confined swirling flow with a swirl number of approx. 0.5 were studied in detail by performing measurements using phase-Doppler anemometry (PDA) and numerical predictions. A mixture of gas and particles was injected without swirl into the test section, while the swirling airstream was provided through a co-flowing annular inlet. Two cases with different primary jet exit velocities were considered. For these flow conditions, a closed central recirculation bubble was established just downstream of the inlet.

The PDA measurements allowed the correlation between particle size and velocity to be obtained and also the spatial change in the particle size distribution throughout the flow field. For these results, the behaviour of different size classes in the entire particle size spectrum, ranging from about 15 to 80 μm, could be studied, and the response of the particles to the mean flow and the gas turbulence could be characterized. Due to the response characteristics of particles with different diameters to the mean flow and the flow turbulence, a considerable separation of the particles was observed which resulted in a streamwise increase in the particle mean number diameter in the core region of the central recirculation bubble. For the lower particle inlet velocity (i.e. low primary jet exit velocity), this effect is more pronounced, since here the particles have more time to respond to the flow reversal and the swirl velocity component. This also gave a higher mass of recirculating particle material.

The numerical predictions of the gas flow were performed by solving the time-averaged Navier-Stokes equations in connection with the well known kε turbulence model. Although this turbulence model is based on the assumption of isotropic turbulence, the agreement of the calculated mean velocity profiles compared to the measured gas velocities is very good. The gas-phase turbulent kinetic energy, however, is considerably underpredicted in the initial mixing region. The particle dispersion characteristics were calculated by using the Lagrangian approach, where the influence of the particulate phase on the gas flow could be neglected, since only very low mass loadings were considered. The calculated results for the particle mean velocity and the mass flux are also in good agreement with the experiments. Furthermore, the change in the particle mean diameter throughout the flow field was predicted approximately, which shows that the applied simple stochastic dispersion model also gives good results for such very complex flows. The variation of the gas and particle velocity in the primary inlet had a considerable impact on the particle dispersion behaviour in the swirling flow and the particle residence time in the central recirculation bubble, which could be determined from the numerical calculations. For the lower particle inlet velocity, the maximum particle size-dependence residence time within the recirculation region was considerably shifted towards larger particles.     

星载张力索网天线结构混合变量的多目标优化

以纵向拉索调整力大小和可调整的纵向拉索数目为设计变量,可调整的纵向拉索数目最少和网状反射面的均方根误差最小为目标函数,应力和频率为约束条件,建立了大型空间网状可展开天线的形面调整的多目标优化数学模型,并用遗传算法进行了优化求解。优化结果表明:该方法在提高天线表面精度的同时,能有效地减少可调整的纵向拉索数目,降低了工程人员在网面调整中的繁杂劳动。并且,网面调整的总次数也远少于实际工程中的调整,对工程应用具有一定的指导意义。     

精细积分法在电报方程求解中的应用

将精细积分法应用到了二维的电报方程的数值计算之中。实例计算表明，该方法具有简单、计算精度高、无条件稳定、不需要进行复杂、费时的频域一时域转换及卷积积分，直接时域分析，处理非零初始值容易等优点。与传统的ＦＦＴ法及ＮＩＬＴ法相比，其效率更高，功能更强。     

Interval analysis method and convex models for impulsive response of structures with uncertain-but-bounded external loads

Two non-probabilistic, set-theoretical methods for determining the maximum and minimum impulsive responses of structures to uncertain-but-bounded impulses are presented. They are, respectively, based on the theories of interval mathematics and convex models. The uncertain-but-bounded impulses are assumed to be a convex set, hyper-rectangle or ellipsoid. For the two non-probabilistic methods, less prior information is required about the uncertain nature of impulses than the probabilistic model. Comparisons between the interval analysis method and the convex model, which are developed as an anti-optimization problem of finding the least favorable impulsive response and the most favorable impulsive response, are made through mathematical analyses and numerical calculations. The results of this study indicate that under the condition of the interval vector being determined from an ellipsoid containing the uncertain impulses, the width of the impulsive responses predicted by the interval analysis method is larger than that by the convex model; under the condition of the ellipsoid being determined from an interval vector containing the uncertain impulses, the width of the interval impulsive responses obtained by the interval analysis method is smaller than that by the convex model.The project supported by the National Outstanding Youth Science Foundation of China (10425208), the National Natural Science Foundation of China and Institute of Engineering Physics of China (10376002) The English text was polished by Keren Wang.