球头弹低速斜侵彻下薄板穿甲破坏机理研究

为探讨球头弹低速斜侵彻下靶板的破坏机理,通过系列弹道试验,对比分析了不同初始速度下弹体的变形,靶板的破坏模式,以及靶板的破口大小及形状；同时采用ANSYS/LS-DYNA对弹靶作用过程进行了数值模拟。结果表明：低速斜侵彻下靶板响应非完全对称,根据受力特征可将靶板划分为四个不同区域,即接触区,弯曲区,拉伸区和对称区；薄板的穿甲破坏可分为四个不同的阶段,即隆起变形,碟形变形,弯曲变形,弹体贯穿阶段；不同初始速度下靶板出现四种典型的穿甲破坏模式,随着初始速度的增加依次为隆起—碟形变形,隆起—碟形变形—拉弯撕裂破坏,隆起—碟形变形—拉弯剪切破坏,隆起—拉弯剪切破坏。斜侵彻下靶板破口形状为椭圆形,随着初始速度的增加,破口长径不断减小,形状由椭圆形向卵形过渡。     

解析方法与数值模拟相结合求解炸药在容器内部爆炸产生的壁面载荷

本文采用总变差递减（TVD）数值方法与强爆炸解析解相结合的手段,求解了炸药在爆炸容器内部产生的作用载荷。计算结果与实验值在几个典型位置进行了比较,二者有良好的符合。与单纯的数值方法相比,本文所探索的方法能有效地克服对称轴附近的数值振荡,不失为确定爆炸载荷的一种新途径。     

微结构连续损伤理论

本文从微结构理论出发,用相对变形描述微结构之间的微空隙和微裂纹引起的材料损伤的影响,得到用损伤张量描述的各向异性损伤的微结构连续损伤力学理论。该微结构损伤模型可化简为目前公认的几种主要损伤模型:如J.P. Cordebojs和F. Sidoroff的弹性各向异性损伤模型,D. Krajcino-vic和G.U.Fonseka的脆性材料平面裂纹损伤模型,J. Lemaitre的各向同性损伤理论及Kachanov的以面积减少为变量的损伤模型等。作者运用这一理论对混凝土材料的单向拉、压基本受载情形进行了数值分析,并与D. Krajcinovic的损伤模型计算结果及实验结果作了比较,所得结果与实验值比较吻合,特别是在失稳后阶段给出了较好描述,初步表明了本理论的有效性和实用性。     

串联战斗部前后级作用关系数值模拟研究

利用Autodyn有限元软件采取三维数值仿真的方法,对串联战斗部前后级的作用关系开展研究。基于串联战斗部轴对称的特点,建立了1/2有限元仿真简化模型,通过设置前后级飞行速度0 m/s、100 m/s、200 m/s以及前后级间距10 mm、30 mm、50 mm,利用控制变量法,分析了前后级相对速度、前后级间距对随进子弹受力状态的影响规律。得出了随着前后级相对速度的增大或者前后级间距的减小,随进子弹各点的受力及速度降都会增大的变化规律。仿真结果可以为相关串联战斗部的优化设计提供参考。     

顶部开口条件下油罐油气爆炸数值模拟

根据油罐油气爆炸特性,基于RNG k-ε湍流模型、Finate-Rate/Eddy-Dissipation化学反应模型和相应的控制方程,采用SIMPLE算法对顶部开口条件下油气爆炸发生与发展过程进行了数值模拟。基于数值模拟结果分析了顶部开口条件下油罐油气爆炸罐外超压和火焰特征,与实验结果吻合良好,该模型可以用来预测顶部开口条件下油罐油气爆炸强度。     

穿甲子弹偏心入射陶瓷/钢复合靶板试验

设计并进行了7.62mm穿甲子弹侵彻陶瓷/低碳钢复合靶板的弹道试验,得到了极限速度及陶瓷锥底部半径等数据。分析了锥底半径与入射速度、面板及背板厚度的关系,着重分析了偏心入射时靶板的抗弹机理。结果表明:陶瓷锥可分为破碎区和粉碎区,粉碎区半径约为面板厚度与弹丸半径之和;当弹着点距离陶瓷面板边缘大于5mm时,靶板的抗弹性能变化不大,而弹着点位于距陶瓷面板边缘小于5mm的板边区时,抗弹性能明显降低,靶板的有效防护面积应扣除板边区。     

黄葛增压站噪声治理工艺措施

为解决黄葛增压站内4台室外整体式天然气压缩机组造成的噪声污染问题,结合生产运行要求、周边环境状况、噪声源分布及噪声特性,综合吸声、隔声、消声、阻尼减振、通风和泄压等技术,采用半密闭式降噪厂房和阻抗复合排气消声器等治理措施。治理后厂界噪声从64.2～72.1 dB(A)降至49.7～55.0 dB(A),距厂房最近厂界25 Hz声压值从97.9 dB降至84.2 dB,排气消声器出口噪声从84.3 dB(A)降至72.6 dB(A)且25Hz声压值从124.7 dB降至97 dB。厂界噪声达到GB 12348—2008《工业企业厂界环境噪声排放标准》3类要求,中、低频噪声强度减弱,解决了厂界噪声超标和噪声扰民问题。同时,为整体式天然气压缩机组噪声治理开辟了一条新途径,为日后降噪厂房和阻抗复合排气消声器广泛应用奠定了实践基础,为压缩机组噪声治理设计积累了宝贵经验。     

球形破片侵彻明胶运动模型及破片参数敏感性分析

为揭示球形破片对人体组织致伤机理,以明胶作为人体组织的替代物,基于动态空腔膨胀理论,考虑球形破片未完全侵入阶段的速度衰减,建立了球形破片侵彻明胶的分段运动理论模型,研究了球形破片侵彻明胶的运动规律。通过钢球和钨球侵彻明胶的实验验证了模型的正确性,求解了模型中的最优阻力系数。分析了理论计算过程中的误差来源,并推导得到了无量纲侵彻深度的表达式。利用Sobol′法进行了球形破片参数(直径、密度和速度)对侵彻深度影响的敏感性分析。结果表明：运动模型能够较好地模拟球形破片的运动规律;低密度的球形破片在未完全侵入阶段的速度衰减不能忽略;球形破片参数对侵彻深度影响的敏感性由高到低依次是速度、密度和直径。     

Research on the intermediate phase of 40CrMnSiB steel shell under different heat treatments

In this study, 40CrMnSiB steel cylindrical shells were tempered at 350, 500 and 600 ℃ to study the effect of tempering temperature on the dynamic process of expansion and fracture of the metal shell. A mid-explosion recovery experiment for the metal cylinder under internal explosive loading was designed, and the wreckage of the casings at the intermediate phase was obtained. The effects of different tempering temperatures on the macroscopic and microscopic fracture characteristics of 40CrMnSiB steel were studied. The influence of tempering temperatures on the fracture characteristic parameters of the recovered wreckage were measured and analyzed, including the circumferential divide size, the thick-ness and the number of the circumferential divisions. The results show that as the tempering temper-ature was increased from 350 to 600 ℃, at first, the degree of fragmentation and the fracture characteristic parameters of the recovered wreckage changed significantly and then became essentially consistent. Scanning electron microscopy analysis revealed flow-like structure characteristics caused by adiabatic shear on different fracture surfaces. At the detonation initiation end of the casing, fracturing was formed by tearing along the crack, which existed a distance from the initiation end and propagated along the axis direction. In contrast, the fracturing near the middle position consists of a plurality of radial shear fracture units. The amount of alloy carbide that was precipitated during the tempering process increased continuously with tempering temperature, leading to an increasing number of spherical carbide particles scattered around the fracture surface.     

Deformation,fragmentation and acceleration of a controlled fragmentation charge casing

Two different finite element software, LS-DYNA and Impetus, have been evaluated to test their ability to predict the deformation, fragmentation and acceleration of a controlled fragmentation charge casing. The general-purpose program LS-DYNA was used with a multi-material ALE formulation and a mass-preserving erosion criterion coupled to a Johnson-Cook fracture criterion. In the Impetus simulations, a third order Lagrangian element formulation was used for the casing and a node-splitting element erosion treatment coupled to a Cockcroft-Latham failure criterion was used to describe casing fracture. The high-explosive gases were described by a discrete particle formalism.In order to acquire data to validate our computational tools and constitutive models, a series of experiments have been performed using a laboratory charge with an internal grooved casing. In the test series, the charge geometry was fixed except that the groove depth were varied from very shallow to very deep resulting in different deformation patterns, fracture modes and terminal velocities. Various diagnostic tools captured the different stages of the expansion and fragmentation of the casing. A high-speed framing camera depicted the deformation pattern before fragmentation and was used to determine the moment when the casing failed. Three different complementary techniques were used to follow the acceleration of the fragments; a Photon Doppler velocimetry to determine the initial acceleration of the casing, double exposed radiographs to estimate the fragment velocity after break-up and a high-speed video to determine the terminal velocity of the fragment after leaving the fireball. In addition, the fragments were soft recovered in a set of sawdust pit tests and their final shape and weight were measured. A SEM was used to characterise the fracture surfaces and to determine the modus of fracture (tensile or shear failure).Comparisons to experiments show that both software can predict the change in deformation behaviour when the groove depth increases, from tangential necking for shallow grooves to radial punching for deep groves. Both software could also reasonable well predict the acceleration of the fragments, though both overestimates the terminal velocity for the charge with the deepest grooves.