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首页> 外文期刊>Physical review, B >Extended asymmetric hot region formation due to shockwave interactions following void collapse in shocked high explosive
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Extended asymmetric hot region formation due to shockwave interactions following void collapse in shocked high explosive

机译:冲击高爆炸药中空隙塌陷后由于冲击波相互作用而引起的扩展的不对称热区形成

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In both continuum hydrodynamics simulations and also multimillion atom reactive molecular dynamics simulations of shockwave propagation in single crystal pentaerythritol tetranitrate (PETN) containing a cylindrical void, we observed the formation of an initial radially symmetric hot spot. By extending the simulation time to the nanosecond scale, however, we observed the transformation of the small symmetric hot spot into a longitudinally asymmetric hot region extending over a much larger volume. Performing reactive molecular dynamics shock simulations using the reactive force field (ReaxFF) as implemented in the LAMMPS molecular dynamics package, we showed that the longitudinally asymmetric hot region was formed by coalescence of the primary radially symmetric hot spot with a secondary triangular hot zone. We showed that the triangular hot zone coincided with a double-shocked region where the primary planar shockwave was overtaken by a secondary cylindrical shockwave. The secondary cylindrical shockwave originated in void collapse after the primary planar shockwave had passed over the void. A similar phenomenon was observed in continuum hydrodynamics shock simulations using the CTH hydrodynamics package. The formation and growth of extended asymmetric hot regions on nanosecond timescales has important implications for shock initiation thresholds in energetic materials.
机译:在连续流体动力学模拟和数百万个原子反应分子动力学模拟中,冲击波在含有圆柱形空隙的单结晶季戊四醇四硝酸酯(PETN)中传播时,我们观察到了初始径向对称热点的形成。但是,通过将仿真时间扩展到纳秒级,我们观察到了小对称热点向在更大体积上延伸的纵向非对称热点区域的转变。使用LAMMPS分子动力学软件包中实现的反作用力场(ReaxFF)进行反应性分子动力学冲击模拟,我们表明,纵向不对称热区是由主要径向对称热点与次要三角形热区的聚结形成的。我们表明,三角形的高温区域与双冲击区域相吻合,在该区域中,主要的平面冲击波被次要的圆柱形冲击波所取代。在主平面冲击波经过空隙之后,第二圆柱冲击波起源于空隙塌陷。在使用CTH流体动力学软件包的连续流体动力学冲击模拟中观察到了类似的现象。纳秒级尺度上扩展的不对称热区的形成和增长对高能材料中的激波起始阈值具有重要意义。

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