Preservation of unimodality under shock models

A number of results pertaining to preservation of aging properties (IFR, IFRA etc.) under various shock models are available in the literature. Our aim in this paper is to examine in the same spirit, the preservation of unimodality under various shock models. For example, it is proved that in a non-homogeneous Poisson shock model if {p_k}_K≥0, the sequence of probabilities with which the device fails on the kth shock, is unimodal then under some suitable conditions on the mean value function Λ (t), the corresponding survival function is also unimodal. The other shock models under which the preservation of unimodality is considered in this paper are pure birth shock model and a more general shock model in which shocks occur according to a general counting process. © 1999 John Wiley & Sons, Inc. Naval Research Logistics 46: 952–957, 1999     

Experimental study on explosion dispersion process of a multi-layer composite charge under different initiation modes

The influence of initiation modes on the explosive dispersion process of the multi-layer composite charge (MCC) was studied. Overpressure sensors and high-speed photography system were used to investigate the energy release process of an MCC with a specific structure. The shock wave pressure and explosive dispersion characteristics of the MCC under different initiation modes were compared. The forming and expanding process of the shock wave of the composite charge under different initiation modes was determined. The separation position of the shock wave and fireball interface was determined. The calculation formulas of the shock radius and overpressure of the composite charge are presented. The radius of the shock wave of the composite charge was significantly affected by the initiation mode. Moreover, the development process of the composite explosive fireball under different initiation modes was analyzed, the variation rules of the composite charge dispersion radius and fireball dispersion velocity with time were obtained under the different initiation modes, the explosion energy release rate of composite charge under simultaneous initiation modes was the highest, and the peak overpressure under the simultaneous initiation mode was 1.61 times that of central single-point initiation.     

Investigation on energy output structure of explosives near-ground explosion

In order to give the energy output structure of typical explosives near-ground explosion in real ground conditions, the free-field shockwave, ground reflection shockwave and Mach wave overpressure time history of composition B explosive, RDX explosive and aluminized explosive were measured by air pressure sensors and ground pressure sensors. The shape of the free-field shock wave, ground reflection shock wave, and Mach wave and explosion flame were captured by high-speed camera. The experimental results show that, at the same horizontal distance from the initiation point, the peak overpressure of explosive shock wave of composition B explosive, both in the air and on the ground, is less than that of RDX and aluminized explosives. At a distance of 3.0 m from the initiation point, the peak overpressure of aluminized explosives is slightly less than that of RDX explosives. Owing to the exothermic effect of aluminum powder, the pressure drop of aluminized explosives is slower than that of RDX explosives. At 5.0 m from the initiation point, the peak overpressure of aluminized explosives is larger than that of RDX explosives. At the same position from the initiation point, among the three kinds of explosives, the impulse of aluminized explosives is the maximum and the impulse of composition B explosives is the minimum. With the increase of the horizontal distance from the initiation point, the height of Mach triple-points (Mach steam) of the three explosives increases gradually. At the same horizontal distance from the initiation point, there is poorly difference in the height of Mach triple-points between aluminized explosive and RDX explosive, and the height of Mach triple-points of composition B explosive is much smaller than that of other two explosives. The maximum diameter and duration of the fireball formed by aluminized explosives are the largest, followed by composition B explosive, and the maximum diameter and duration of the fireball formed by RDX explosive are the smallest.     

Effect of microstructure on short pulse duration shock initiation of TATB and initial response mechanism

Micro-TATB particles with different sizes and 3D nanoporous TATB architectures with different specific surface areas were prepared through recrystallization to study short pulse duration shock initiation properties by electric gun technology. For micro-TATB, the initiation threshold significantly decreases with TATB average size ranging from 79.7 μm to 0.5 μm. For 3D nanoporous TATB architecture, the initiation threshold decreases and then increases with specific surface areas increased from 9.6 m²/g to 36.2 m²/g. The lowest initiation thresholds are obtained for the micro-TATB with average sizes of 1.3 μm and 0.5 μm, and 3D nanoporous TATB architecture with specific surface area of 22.4 m²/g. The shock initiation thresholds of micro-TATB and 3D nanoporous TATB architectures show significantly decreases with the porosity increased. The decomposition reaction and thermal conductivity properties were further investigated to understand the initial response mechanism. High porosity provides more collapse sites to generate high temperature for formation of hot spots. The low thermal conductivity and decomposition temperature could enhance the formation and ignition of the hot spots, and initial decomposition reaction of TATB. The effect of the decomposition temperature is higher than that of the thermal conductivity on the shock initiation properties. The enhanced decomposition reaction could promote energy release and transfer process from the ignition to the combustion. This work offers a new insight to understand the effects of microstructure on the shock initiation properties and the initial response mechanism of TATB.     

辐射叶加载的短波宽带鞭状天线优化设计

提出一款具有多层辐射叶结构的新型鞭状天线,在10 m鞭状天线体上设置不同的辐射叶层数、半径、长度、分支数、仰角及其分布情况,研究其对天线辐射性能的影响,综合考虑选择一套最合适的辐射叶结构,并为天线进行双加载和宽带匹配网络的算法优化。仿真结果表明,与现有的普通宽带鞭状天线相比,增益和效率得到了普遍提高,在低频段增益最高提高了3 dB,效率最高提高了5%;在高频段增益最高提高了5 dB,效率最高提高了35%,方向图上翘也得到了一定的抑制,为改善现有的宽带鞭状天线提供一种新的结构设计方法。     

界面改性对SiCp/Cu复合材料导热性能的影响

采用磁控溅射法结合结晶化热处理工艺在SiC颗粒表面成功制备了金属Mo涂层,分析Mo涂层的成分和形貌;采用热压烧结工艺制备SiCp/Cu复合材料,重点对比分析Mo界面阻挡层厚度对复合材料导热性能的影响。结果表明:磁控溅射法能够在SiC颗粒表面沉积得到Mo涂层,随溅射时间的延长,Mo涂层的厚度增加、粗糙度增大,且磁控溅射后SiC颗粒表面直接得到的Mo涂层为非晶态,结晶化热处理后,变为致密平整的晶态Mo涂层。磁控溅射时间对Mo涂层厚度和复合材料导热性能影响明显。随磁控溅射时间的增加,复合材料的热导率呈先增后减趋势。采用磁控溅射9h镀Mo改性并经过800℃结晶化热处理的SiC复合粉体在850℃下热压烧结制备的SiCp/Cu复合材料(VSiC=50%),其热导率达到了最高值274.056W/(m·K)。     

石墨烯微片尺寸对石墨烯纸热导率的影响

石墨烯热导率远高于传统金属薄膜等导热材料,可用作热扩散材料。石墨烯纸由石墨烯微片组装而成,石墨烯微片尺寸大小对其组装方式微观结构以及宏观导热性能等具有重要影响。采用溶液过滤自组装方法制备了分散均匀的氧化石墨烯纸,然后在Ar/H2气氛下对氧化石墨烯纸进行热还原处理,得到了石墨烯纸。结果表明,大尺寸石墨烯微片组成的石墨烯纸结构更加致密、结晶度更高;0.5μm~3μm和50μm~100μm的氧化石墨烯所制备的石墨烯纸的热导率分别为632.8 W/m K和683.7 W/m K,大尺寸石墨烯微片组成的石墨烯纸热导率提高了8%。     

基于磁致伸缩式超声导波测温技术基础研究

温度是科学研究中最普遍的物理量,也是生产精密仪器的重要参数,然而国内对于高温环境除热电偶测温传感器外尚无可靠的原位测试方法。依据超声导波测温的原理,设计出一套基于磁致伸缩效应的超声导波测温装置,测试了该装置在常温以及常温(12℃)~600℃的运行情况。实验表明,该装置可以在高温环境下稳定运行,并且得到常温(12℃)~600℃范围内的起始声波和端面回波之间时间间隔△t与介质温度之间的对应关系,为2 000℃以上的高温测量奠定了基础。     

地波雷达组网探测高空目标优化布站

针对高空无人机等目标,建立基于高频地波雷达为主的2D雷达探测网,以目标高度估计和协同补盲为约束条件,对2D雷达网的优化布站问题进行理论计算和实例仿真,实验结果证明布站方法的有效性。     

基于改进 Gerstner 波的岛礁近岸波浪实时仿真?

为了实现岛礁附近波浪实时仿真,结合 Gerstner 波和水波动力学知识,提出了一种能够模拟波浪卷曲和折射绕射现象的波浪建模与绘制方法。首先,建立 Gerstner 波参数随水深变化关系,构建模拟波浪卷曲过程的几何模型;然后,定义岛礁地形对波浪传播的阻障和遮挡系数,并据此修正波浪传播的波向和波高,实现折射和绕射现象的仿真;最后,应用着色器缓存技术完成计算的硬件加速,并构建了基于视点的波浪传播多分辨率绘制策略。实验结果表明,该方法对波浪的卷曲和折射绕射现象取得了较好的仿真效果,绘制效率能够满足实时性要求。