模拟长杆弹侵彻混凝土靶的MCA方法

采用改进的移动元胞自动机法数值软件,对长杆弹侵彻混凝土靶进行了二维数值模拟,给出了弹靶的破坏变形过程,得到了侵彻深度与冲击速度的关系曲线。数值模拟结果与已有的实验现象吻合较好,说明该计算方法可以有效地计算和模拟高速侵彻问题。     

水下爆炸特性的二维数值模拟研究

 对带有3 mm左右厚铝壳或钢壳的柱形TNT、RS-211、T/Γ（35/65）以及ROT901装药在水下采用一端点起爆后,水中冲击波超压分布进行了二维数值模拟研究。对该四种炸药的每一种,分别考虑了药量为1 kg、3 kg、5 kg和8 kg四种TNT当量的柱形装药情况。柱形装药的长径比为L/D=1.5左右。计算使用的程序为二维欧拉多流体网格法流体力学计算程序MFIC。给出了水中冲击波超压的空间和时间分布;对铝壳和钢壳两种情况的结果进行了分析、比较;同时给出了缩比模型与1∶1模型之间相应物理量之间的缩比关系。     

柱形装药水中爆炸近场径向压力测试初探

 针对端面起爆柱形装药水中爆炸近场冲击波阵面呈现非球形传播的特点,采用分幅相机记录了炸药起爆36 μs内近场冲击波的传播情况,分析了冲击波在不同时间和不同位置的形状;采用两台高速扫描相机测量了侧边任意一点的冲击波速度,结合Rankine-Hugoniot关系,得到了冲击波阵面的压力;同时用LS-DYNA方法对侧边任意一点的压力进行了数值模拟,两者得到的结果基本一致。     

刚体与SPH耦合的三维数值方法研究

 研究了刚性体与SPH（Smoothed Particle Hydrodynamics）方法相耦合的计算方法和技术,以此技术为核心,在原有三维综合拉氏程序CL3D的基础上,研制了适用于斜侵彻问题数值研究的刚性弹体与SPH靶体耦合计算的拉氏三维数值模拟程序CRSPH3D。针对金属材料编入了Johnson-Cook本构模型计算模块,针对混凝土材料编入了Johnson-Holmquist本构模型及与之配套的损伤模型和状态方程等的计算模块。用研制的计算程序对弹体分别正碰和斜碰穿透中厚铝靶和侵彻厚混凝土靶的过程进行了数值模拟计算和分析。结果表明,对于铝靶穿透问题,模拟计算得到的弹体剩余速度、弹体动能损失和贯穿图像与实验结果符合得较好。对于混凝土靶的侵彻问题也得到了与实验现象一致的、定性合理的图像。     

点对点移动水声通信技术研究

点对点移动水声通信是实现由活动和静止节点共同构成的水声数据通信网的关键技术之一. 对移动水声通信声信道特性进行了分析,指出不同途径到达的声线对应的多普勒频偏不一致,进一步加大了多途扩展产生的码间干扰的复杂性,不利于水声通信. 提出单阵元被动式相位共轭镜信道均衡技术,可实时自动补偿多普勒频偏,并聚焦多途信号. 将单阵元被动式相位共轭应用于Pattern时延差编码移动水声通信系统,进行了移动水声通信试验,湖试结果验证了其消除码间干扰性能及本文水声通信系统的鲁棒性. 关键词： 移动水声通信 被动式相位共轭镜 时变信道 码间干扰     

聚乙烯薄膜中X射线穿透深度计算方法的验证

通过银镜反应在聚乙烯薄膜一面镀银膜,用不同入射角进行掠入射X射线衍射测量,利用对应银的衍射峰出现的条件验证了X射线穿透深度计算公式在进行高分子薄膜表征中的可行性.     

基于光子图海水点扩展函数的估计

海水中粒子对光的散射是水下图像模糊的主要原因。点扩展函数能够反映海水中光的空间扩散程度,使用点扩展函数,水下图像能被恢复或增强。提出了一种基于光子图海水点扩展函数的估计方法,该方法通过用光子图求解辐射传输方程,对光场内任意点的辐射强度进行估计。通过与蒙特卡洛仿真点扩展函数的方法相比较,结果表明两者具有较好的一致性。     

A hybrid VOF and PIC multi-material interface treatment method and its application in the penetration

A hybrid VOF and PIC multi-material interface treatment method for Eulerian method is presented in this study in order to solve the problem that the Eulerian method is not robust enough to treat the dynamic fracture of material. This treatment method is used in the important computational region such as the material interface,large deformation region and fracture region where more particles are added for calculation,while the continuous transport method is used in the other regions. Through this method,a se...     

Effect of surface defects on vortex penetration in small superconducting squares

We report the dependence of the vortex penetration on the number and positions of surface defects in mesoscopic superconducting squares. The vortex penetration is detected by the change in the transport properties of small tunnel junctions attached to the sample (small-tunnel-junction method). We find that for vorticities L = 0 and 1, a defect at the center of a side facilitate the vortex penetration, while a defect at a corner does not affect the vortex penetration field. For higher vorticities, the influence of defects becomes complicated, indicating that not only the existence of surface defects but also the vortex arrangement influences the vortex penetration. Simple explanation for this mesoscopic vortex penetration effect is given.     

Doping dependence of Meissner effect in cuprate superconductors

Within the t–t′–J model, the doping dependence of the Meissner effect in cuprate superconductors is studied based on the kinetic energy driven superconducting mechanism. Following the linear response theory, it is shown that the electromagnetic response consists of two parts, the diamagnetic current and the paramagnetic current, which exactly cancels the diamagnetic term in the normal state, and then the Meissner effect is obtained for all the temperature T ? T_c throughout the superconducting dome. By considering the two-dimensional geometry of cuprate superconductors within the specular reflection model, the main features of the doping and temperature dependence of the local magnetic field profile, the magnetic field penetration depth, and the superfluid density observed on cuprate superconductors are well reproduced. In particular, it is shown that in analogy to the domelike shape of the doping dependent superconducting transition temperature, the maximal superfluid density occurs around the critical doping δ ≈ 0.195, and then decreases in both lower doped and higher doped regimes.