共查询到19条相似文献,搜索用时 167 毫秒
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爆轰波波形与药型罩结构匹配对杆式射流成形的影响 总被引:1,自引:0,他引:1
为提高杆式射流对钢靶的侵彻能力,设计了一种偏心亚半球药型罩,通过爆轰波碰撞理论推导出药型罩压垮速度,并结合改进的PER理论建立了杆式射流成形的模型。分析了药型罩结构参数对爆轰波碰撞压力的影响规律,获得了等质量变壁厚药型罩射流质量及速度分布的变化规律。结果表明:马赫反射压力随偏心距的增大而增大,随外壁曲率半径的增大而减小,而正规斜反射压力与马赫反射压力变化规律相反,且马赫反射压力受药型罩结构影响较大;通过对比不同方案,罩顶与罩口部厚、中间薄形状药型罩形成的射流质量提高了29.5%,头部速度提高了21.3%,且速度梯度最大,相同炸高条件下侵彻深度提高了约2倍装药直径。针对优化结构进行了数值模拟和实验验证,通过对爆轰波波形与药型罩结构合理的匹配设计,使形成的杆式射流成形及侵彻性能得到显著提升。 相似文献
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以球型空腔膨胀理论为基础,提出了一个计算陶瓷靶板阻力的损伤模型,该模型考虑了损伤因子对陶瓷靶板弹道性能的影响.结合不可压缩流体力学理论,对射流侵彻陶瓷靶板的侵彻速度进行了理论值计算,并与未考虑损伤的侵彻速度进行了比较,该模型的计算结果更接近实验结果.建立了射流侵彻陶瓷靶板的数值计算模型,对铜射流侵彻陶瓷靶的动态破坏过程进行了研究,讨论了药型罩的锥角、壁厚对射流侵彻结果的影响,结果表明:相同锥角的药型罩,壁厚对陶瓷靶板孔径的影响较小;同壁厚的药型罩,随着锥角的增大,侵彻孔径增大.侵彻速度的数值模拟结果与理论结果进行了比较,得到了较好的一致性. 相似文献
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高熵合金药型罩射流成型与稳定性 总被引:2,自引:0,他引:2
近年迅速兴起的多主元高熵合金因其具有很宽的成分-性能调控范围及一系列优异力学性能, 有望替代紫铜成为新一代药型罩材料. 本文基于CrMnFeCoNi五元高熵合金动态力学性能实验和数值模拟, 探索该合金用作药型罩的适用性. 基于分离式霍普金森拉杆和材料试验机研究了高熵合金不同应变率及温度下的力学行为, 获得了高熵合金Johnson-Cook热黏塑性动态本构. 利用流动速度与临界压垮角关系对凝聚性高熵合金射流形成边界进行界定. 结合数值模拟验证了高熵合金射流形成边界的合理性, 并进一步揭示了射流高速拉伸断裂演化规律. 研究表明: 射流断裂时间与材料强度成负相关, 材料动态强度增大, 将会引起射流断裂时间下降. 本工作可为新型高熵合金药型罩结构设计提供参考. 相似文献
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瞬态空化泡演变过程的数值模拟 总被引:8,自引:0,他引:8
采用边界积分方程方法,对无粘流体中三个空化泡以及自由面附近二个空化泡相互作用的演变过程进行了数值模拟。计算中边界用二阶有限元离散,影响系数矩阵非对角线元素用六点高斯数值积分方法计算,对第一类、第二类完全椭圆积分用高次多项式近似,对计算系数矩阵对角线元素中遇到的奇异积分进行了特殊处理。结果表明,在不同的给定参数下,空化泡的溃灭形态各异,柱状射流和环形射流都有可能发生,使空化泡演变成双泡或环形泡。 相似文献
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S. V. Fedorov 《Journal of Applied Mechanics and Technical Physics》2016,57(3):483-493
This paper presents an analysis of the possibility of increasing the ultimate stretching and penetration capability of metallic shaped-charge jets in the presence of an axial magnetic field in the shaped-charge liner due to heating and thermal softening of the jet material as a result of a sharp increase in the magnetic-field induction in the jet formation region upon liner collapse. This process is studied by numerical simulation in a quasi-two-dimensional formulation taking into account the inertial stretching of the conductive rigid-plastic rod in the presence of a longitudinal magnetic field in it. 相似文献
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超空化燃油射流使得喷雾中部分燃油分裂液滴内含有空化气泡;空化气泡的生长及溃灭对液滴的分裂与雾化具有重要影响. 基于VOF 方法首次对超空化条件下燃油液滴内空化气泡的生长及溃灭过程进行了数值模拟. 通过研究发现,单液滴内空化气泡的生长过程可以按控制机理划分为表面张力控制阶段、综合竞争阶段和惯性力控制阶段;在第I 阶段,空泡的生长主要受表面张力的控制作用,惯性力对空泡生长的促进作用及黏性力对空泡生长的抑制作用可以忽略;在第II 阶段,空泡的生长受表面张力、惯性力及黏性力三者的综合作用,空泡的生长速率是促进空泡生长的惯性力和抑制空泡生长的表面张力及黏性力相互竞争、共同作用的结果;在第III 阶段,空泡的生长主要受惯性力的控制作用,抑制空泡生长的表面张力及黏性力的作用基本可以忽略. 单液滴内空化气泡的溃灭过程由多个溃灭阶段和反弹阶段构成,类似于有阻尼弹簧振子的振动过程;根据每个溃灭周期结束时空泡半径随时间的变化历程,可以将空泡的溃灭分为快速溃灭期、缓慢溃灭期以及稳定期;溃灭初期空泡溃灭压力的变化非常剧烈,但空泡溃灭体积的变化则要相对平缓得多;空泡反弹压力随时间的变化与空泡反弹体积随时间的变化基本对应. 相似文献
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认识带尾喷流和自然超空泡的水下高速航行体流体动力特性并发展其预报与控制方法仍是水动力学领域极具挑战性的课题.本研究采用CFD方法对尾喷流和自然超空泡之间的相互作用进行了数值研究.针对发动机欠膨胀超音速喷流,采用现有实验结果验证了基于两方程湍流模型的二维轴对称流动数值模型的可靠性.尾喷流在空气和蒸汽环境中流动的数值计算结果表明,由于蒸汽环境中背压较低,欠膨胀尾喷流无法及时形成压缩波,使得蒸汽环境中尾喷流的过膨胀区和气相扩散区的体积比空气中大;尾喷流很难形成规则的激波格栅,波系结构相对简单.针对携尾喷流的平头航行体超空泡流状态的数值模拟结果表明,尾喷流注入超空泡后迅速充满航行体周围的空腔区域;尾喷流与超空泡尾迹区域形成的回射流相互作用最终导致超空泡断裂,断裂过程中伴随着燃气泡的下泄现象;受空泡壁面约束,尾喷流难以在狭窄的超空泡空腔内完全膨胀,尾喷流的激波波系结构有显著的变化:在喷嘴附近受到压缩,在远离喷嘴区域受到超空泡水汽掺混的破坏;空泡内压强基本维持在饱和蒸汽压附近,没有显著增加. 相似文献
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O. A. Druzhinin 《Fluid Dynamics》2009,44(2):213-223
The process of generation of internal waves by an initially cylindrical, turbulent jet with a Gaussian profile of the average horizontal velocity component in a fluid with stable linear density stratification is investigated by direct numerical simulation. It is shown that on time intervals Nt < 30, where N is the buoyancy frequency, the vertical velocity pulsations collapse, which is accompanied by the generation of internal waves whose spatial period is close to the wavelength of the spiral mode of jet instability in a homogeneous fluid. The wave dynamics and kinematics can be satisfactorily described by the linear theory for a pulsed source and their parameters are in good agreement with the parameters of the “coherent” internal waves generated by a stratified wake in a laboratory experiment. At large times the wave generation ceases and the variations of the fluid density are localized in the neighborhood of the centers of large-scale vortices formed in the horizontal plane in the neighborhood of the jet. 相似文献
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由于存在强冲击、多相界面复杂运动等强非线性效应,目前对于水下爆炸气泡运动的计算方法无法给出较为可信的水射流运动特征及其载荷形式.本文基于多相可压缩流体的five-equation计算模型,引入界面函数和界面密度压缩技术,采用5阶WENO重构与HLLC近似Riemann求解器进行空间离散,时间离散采用3阶TVD Runge-Kutta法.通过上述方法来提高水下爆炸气泡溃灭过程中气-液界面的计算精度,捕捉水射流的产生、发展以及水锤冲击等典型演化过程.计算结果表明,新的计算方法能够对水下近壁面爆炸气泡的溃灭过程进行有效的模拟,初步揭示了水射流直接载荷的特征,为水射流的产生机理及其损伤效应的研究提供技术支撑. 相似文献
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This study utilizes a U-shape platform device to generate a single cavitation bubble for a detailed analysis of the flow field
characteristics and the cause of the counter jet during the process of bubble collapse caused by sending a pressure wave.
A high speed camera is used to record the flow field of the bubble collapse at different distances from a solid boundary.
It is found that a Kelvin–Helmholtz vortex is formed when a liquid jet penetrates the bubble surface after the bubble is compressed
and deformed. If the bubble center to the solid boundary is within one to three times the bubble’s radius, a stagnation ring
will form on the boundary when impinged by the liquid jet. The fluid inside the stagnation ring will be squeezed toward the
center of the ring to form a counter jet after the bubble collapses. At the critical position, where the bubble center from
the solid boundary is about three times the bubble’s radius, the bubble collapse flow will vary. Depending on the strengths
of the pressure waves applied, the collapse can produce a Kelvin–Helmholtz vortex, the Richtmyer–Meshkov instability, or the
generation of a counter jet flow. If the bubble surface is in contact with the solid boundary, the liquid jet can only move
inside-out without producing the stagnation ring and the counter jet; thus, the bubble collapses along the radial direction.
The complex phenomenon of cavitation bubble collapse flows is clearly manifested in this study. 相似文献
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Jet formation and penetration mechanism of W typed shaped charge 总被引:1,自引:0,他引:1
Existing classical shaped charges are well known for their longer jets capable of achieving large hole depth to hole diameter ratios in metallic targets. However, in some situations, there arises demand to obtain 1:1 ratio for hole depth to hole diameter which is beyond normal shaped charges capability. A new variant of shape charge, named W typed shape charge (WSC), is proposed in this paper, which can meet the demand of 1:1 ratio, and is based on the geometry that can produce annular jets upon proper initiation scheme. In this paper, we present formation and penetration results of WSC based on three different schemes. We also show that not all WSC designs can form annular jets, only annularly initiated WSC, which also fulfils the "Internal-External Liners Equal-Impulse" criterion, has the capability to form annular jet. The experimental and numerical results show that when the ratio between annular initiation ring diameter and the charge diameter is 0.75, an annular jet is formed, which was also supported by high speed photographs performed in vacuum. 2D numerical simulations are performed with indigenously developed simulation software, where Eulerian approach with multi-material interface tracking algorithm is utilized, to find various mechanisms involved during jet formation process. The calculation results are found in good agreement with the experimental results, indicating that the interface treatment algorithm proposed in this paper can not only deal with large deformation problem, but also depict clearly the variation of materials interface. It is especially suitable for simulation of the process from liner collapse to formation of shaped charge jet. 相似文献