一类带容量限制的运输问题

考虑一类带容量限制的运输问题.采用构造辅助网络的方法,将运输网络中的每个配送中心均拆分成两个节点,构造出新弧,形成新的网络,把此类运输问题转换为最小费用流问题来解决.并在此基础上,考虑运输网络中配送中心的容量扩张问题.     

磁性合金A1-xBx相图的理论计算

采用变分累积展开方法,研究了块体磁性合金的相图.利用随机键海森堡模型计算了面心立方、体心立方的居里点和耐尔点,给出了磁性合金临界点的计算公式,进而分别给出自旋1/2和3/2情况下Tc-x相图,并加以分析.     

转速对动态旋流器流场影响的数值分析

根据计算流体力学方法,对采用不同转速的动态旋流器流场进行数值模拟,深入分析了转速对动态旋流器切向速度、静压以及湍动能的影响。计算采用雷诺应力模型和混合物模型。结果表明:转速对动态旋流器切向速度和静压影响非常大,不但影响其数值大小,对其分布趋势也产生明显影响;转速对动态旋流器湍动能的影响主要集中在旋转栅附近,在转筒后半段转速对湍动能的影响明显弱化,适当提高转速甚至有抑制湍流的作用。     

高速SpaceFibre总线节点的系统设计

为了实现SpaceFibre总线节点的高效数据传输,针对网络协议中关键问题和技术提出了一种基于现场可编程门阵列(Field Programmable Gate Array,FPGA)的SpaceFibre总线节点系统设计方案。其中,采用了轮询仲裁算法,解决了多路虚拟通道中流量控制字的申请冲突;设计了基于服务质量机制的高效处理状态机,实现了多路虚拟通道的服务质量调度;提出了一种并行的分区存储架构和重发控制算法,实现了基于错误检测隔离恢复机制的错误恢复;采用了不同的数据并行处理方案,实现了多种数据格式的循环冗余校验和伪随机序列的计算。通过ModelSim仿真平台对节点系统进行功能仿真,并在Virtex-6 FPGA上完成了系统验证。结果表明,该设计实现了SpaceFibre总线节点的功能,串行传输速度可达3.125 Gbit/s,能够满足高速数据传输需求。     

燃烧室前缘扩张角对旋转爆震冲压发动机的影响

针对圆柱形隔离段-燃烧室构型的旋转爆震冲压发动机,开展了总温为860 K、马赫数为2的来流条件下的直连式试验,探讨了燃烧室前缘扩张角(θ=30°,45°,60°,90°)对爆震波传播特性、工况范围及压力分布的影响。结果表明:当燃烧室前缘扩张角为90°时,燃烧模态均为爆燃燃烧;随着扩张角的减小,燃烧模态将会向锯齿波和混合模态(包含单波阶段)转换。当燃烧室前缘扩张角为30°时,旋转爆震的自持工况范围最宽且燃烧室压力最高;同时,随着燃烧室前缘扩张角减小,实现混合模态的当量比下限降低。此外,分析了燃烧模态对来流的影响,发现:锯齿波/混合模态燃烧室内存在的周期性高频压力扰动会使隔离段内的激波串位置前移;混合模态对超声速来流的影响最为显著。     

防空导弹平均速度分析

分析了防空导弹平均速度的计算方法。首先给出了水面舰艇编队防空作战中目指线和自卫线的计算模型,阐述了防空导弹平均速度在其中的重要影响,然后分析了防空导弹速度特性,在此基础上得出满足作战要求的计算方法,最后根据典型弹道参数对防空导弹平均速度进行了仿真计算。     

槽头式野战管线水击波速计算方法研究

按照弹性水击理论,管线内发生水力瞬变时,其水击波速取决于管子的弹性、流体的可压缩性和管子受约束的情况。对于给定的输送介质,焊接式固定输油管线的水击波速是一个常数。而槽头式野战管线采用连接器连接,胶圈密封,这种特殊的连接方式改变了管子整体的弹性摸量,从而使水击波速的常规计算方法不再适用。本文研究了野战管线连接器连接方式时水击波速的影响,实验研究了在受到约束时,橡胶的弹性模量随所受压力的变化而变化的规律,推导出野战管线水击波速平均计算方法,推导的公式表明:与焊接式固定管线不同,野战管线的水击波速随管线内压力的增大而增大。     

槽头式野战管线水击波速测量研究

液体管道的水击波速受流体压力、温度、分子结构、含气量及管线几何尺寸、管材等因素的影响,准确地确定管线的水击波速是一个相当困难的问题,通过实验测量水击波速是一个常用方法。管线水击波速的常用测量方法有波前法和周期法。综合运用波前法和周期法,设计了实验测量野战管线的水击波速,并将实验结果与笔者先前提出的水击波速计算公式的计算结果作了对比,验证了公式的有效性。     

船用柴油机PID神经网络控制系统的设计

给出了PID NN控制器的结构形式、计算公式,并将其应用于船舶柴油机的转速控制系统中.从仿真结果可知,该算法的控制性能和鲁棒稳定性良好,具有较好的自学习和自适应性.     

Resistance of grid steel-tube-confined concrete targets against projectile impact: Experimental investigation and analytical engineering model

Steel-tube-confined concrete (STCC) targets are provided with excellent anti-penetration performance over semi-infinite concrete (SIC) targets since the steel tube imposes passive restraint on the in-filled concrete during the penetration process. Grid STCC system with square steel tubes is a potential solution to protective structures. In this paper, experiments of 9-cell grid STCC targets penetrated by 12.7 mm Armor Piercing Projectile (APP) were performed. The influence of side length and thickness of steel tube, steel ratio and impact velocity on anti-penetration performance were taken into account. Additionally, single-cell square STCC targets were also designed and tested for comparison with the 9-cell grid STCC targets. Damage modes and parameters of the tested targets were measured and discussed. Moreover, the stiffness of radial confinement of grid STCC targets is achieved according to the elastic solution of infinite cylindrical shell in Winkler medium. Furthermore, the penetration resistance and depth of penetration (DOP) for grid STCC targets are obtained on the basis of the dynamic finite spherical cavity-expansion (FSCE) models including radial confinement effect. It is shown that the 9-cell grid STCC targets with optimal dimension match of thickness and side length of steel tube can reduce the DOP by about 17 % and 23 % in comparison with the SIC targets and single-cell square STCC targets, respectively, due to both the confinement of square steel tube to concrete in the impacted cell and the additional confinement of the surrounding cells to the impacted cell; the penetration resistance and DOP of the grid and cellular STCC targets with similar steel ratio is close, and thus the grid STCC targets with simpler manufacturing process and excellent in-plane expandability are preferred in engineering practice; moreover, the predicted results of DOP model based on the FSCE models agree well with the tested results with the maximum disparity less than 12 % and the proposed model is more applicable to the grid and cellular STCC targets with high radial confinement.