基于Nash-Pareto策略的两种改进算法及其应用

针对多目标、多设计变量的优化问题,提出了两种优化的新算法:一种是将多目标问题转化为单目标时,对目标权重的确定提出了新的途径;另一种是直接对多目标问题进行优化,并对Pareto遗传优化技术作了改进,以得到均匀分布的Pareto最优解集.两种新算法都是建立在Nash的系统分解与Pareto遗传算法的基础上,因此称这类算法为Nash-Pareto策略.借助于这类算法,文中以跨声速压气机双圆弧类叶型的气动优化为例,给出了气动优化的全过程.数值优化的实验表明所给出的改进算法是可行的、有效的.     

CO2脉冲激光与气体相互作用实验

实验研究采用波长为10.6μm的CO2脉冲激光器,N2,He,CO2等三种纯净气体及上述气体的相互混合气作为推进工质时,通过实验舱内的冲击摆装置对抛物形光船获得的冲量耦合系数Cm进行了测量。实验发现气体工质的获得的冲量耦合系数Cm随气压增高而增大,通常气体工质的分子量越大,冲量耦合系数Cm越大;在低气压条件下,分子量较大的气体所占的比例越高,混合气获得的冲量耦合系数Cm越高;在高气压条件下,混合气体工质获得的冲量耦合系数与混合气体的种类及比例密切相关。     

透射式水工质的高耦合效率激光推进模式

为了提高激光推进的耦合效率,防止光学器件污染,提出了透射式液体工质的激光推进模式。在这种推进模式中,Nd:YAG固体激光器中产生的450 mJ,7 ns激光穿过透明的玻璃基底后,与燃烧室中的液体推进剂相互作用,产生的等离子体在玻璃基底、燃烧室和液体推进剂的约束下膨胀,产生很高效率的动量转换,使靶获得初速度。纯水和黑墨水分别被用作推进剂,通过比较实验结果发现,在这种模式中墨水比水更适合做推进剂。通过改变燃烧室的长度和孔径,得到的耦合系数的最大值为17 858.3 N/MW。     

基于生存力分析的战斗机超视距空战效能评估

超视距空战已经成为现代空战的主要模式。本文通过对战斗机生存力进行分析,用概率分析法计算了敏感性概率和易损性概率,评估了飞机生存率和飞机损失比等作战效能指标,发展了一种新的超视距空战效能的计算方法。给出了战斗机一对一超视距空战效能评估的计算实例,验证了计算方法的有效性。     

三焦点张量的最小代数误差非迭代算法研究

通过普通数码相机获得的3幅未标定图像,采用RANSAC算法进行两两匹配获得3幅图像的一组兴趣点对,利用最小代数误差非迭代算法在MATLAB中计算出三焦点张量,提出一种最小代数误差非迭代算法。实验结果表明,该方法是一种有效的三焦点张量计算方法,计算复杂度小、实现效率高。能够得到较准确的三焦点张量,为下一步相机自动标定以及三维场景的自动重建和量测奠定了基础。     

三维Euler方程组隐式LU分解的高性能并行计算

许多非定常无粘流体力学问题的数值模拟都需要利用Euler方程组来进行计算,而由于在隐格式下,所选取的时间步长可以比在显格式下时大得多,所以隐格式越来越受到重视,其中隐式LU分解是最常用的方法之一。对三维Euler方程组,采用隐式LU分解进行计算时,网格点所在的各个对角阵面之间存在数据依赖关系,本文分析了采用区域分解且边界上用显格式代替隐格式进行计算的高效性,在长方体建筑物内的爆炸模拟表明,在有112个CPU的某MPP巨型机上,并行计算效率超过60%。本文还分析了计算结果与串行计算时的差异,以及利用区域重叠减小这种差异的方法,同时考虑了对处理器进行合理的逻辑组织,将计算网格映射到处理器网格,以最大限度减少通信开销的方法。文中最后以一个爆炸毁伤的例子实际说明了所述方法的可行性与高效性。     

基于约简遗传规划的线参数模型及在航空发动机起动建模中的应用

提出了一种新的约简遗传规划(PGP)算法和一种新的基于约简遗传规划的航空发动机起动动态线参数模型.这种模型采用遗传规划产生航空发动机起动模型的输入输出非线性模型集,并以二叉树结构表征函数项,运用正交最小二乘算法(OLS)估计二叉树分支(基本函数项)对于模型精度的贡献并去除复杂、冗余的函数项,从而加快遗传规划的收敛速度,最后通过GP进化可获得简单、可靠、准确的线参数非线性模型.发动机起动过程试车数据建模和与支持向量机的比较证明,这种方法可以产生适用性好、解析性强的线参数非线性模型,产生的模型可获得与支持向量机相当甚至更优的结果.     

Thermal Fatigue Behavior of Ni_3Al Based Superalloy IC6E

The thermal fatigue behavior of Ni3Al based superalloy IC6E during the cycles between 900 ℃/1 000 ℃ and the room tempera-ture was investigated. The experimental results indicate that the primary and secondary thermal fatigue cracks initiate inside or round the borides and then spread away along grain boundaries and/or in interdendritic areas. The fracture of borides and their separation from the matrix at interfaces are mainly responsible for the crack initiation and its spreading. At temperatures higher than 1 000 ℃, the grain boundary oxidation combined with cyclic stresses accelerates the crack growth.     

Combustion Synthesis of h-BN-SiC Ceramic Composites

The feasibility was demonstrated to fabricate h-BN-SiC ceramics through combustion synthesis of the mixture of boron carbide and silicon powders under 100 MPa nitrogen pressure. The mass fraction of BN and SiC in the combustion products were found to be 72 % and 28 % respectively. The thermodynamics of the synthesis reaction and the adiabatic combustion temperature were calculated on the theoretical ground. The bending strengths of the ceramics were measured to be 65.2 MPa at room temperature and 55 MPa at 1350 ℃. The phase composition and microstructure of the combustion products were identified by X-ray diffraction (XRD) and scanning electron microscopy (SEM).     

Kinetic Monte Carlo Simulation of EB-PVD Film:Effects of Substrate Temperature

The 2D kinetic Monte Carlo (KMC) simulation was used to study the effects of different substrate temperatures on the microstruc-ture of Ni-Cr films in the process of deposition by the electron beam physical vapor deposition (EB-PVD). In the KMC model, substrate was assumed to be a “surface” of tight-packed rows, and the simulation includes two phenomena: adatom-surface collision and adatom diffusion. While the interaction between atoms was described by the embedded atom method, the jumping energy was calculated by the molecular static (MS) calculation. The initial location of the adatom was defined by the Momentum Scheme. The results reveal that there exists a critical substrate temperature which means that the lowest packing density and the highest surface roughness structure will be achieved when the temperature is lower than the smaller critical value, while the roughness of both surfaces and the void contents keep decreasing with the substrate temperature increasing until it reaches the higher critical value. The results also indicate that the critical substrate temperature rises as the deposition rate increases.