首页> 外文会议>Fundamental Issues and Applications of Shock-Wave and High-Strain-Rate Phenomena >Comparison of tungsten carbide penetrator impact behavior in soft and hard copper targets
【24h】

Comparison of tungsten carbide penetrator impact behavior in soft and hard copper targets

机译:硬质和硬质铜靶中碳化钨穿透剂冲击行为的比较

获取原文
获取原文并翻译 | 示例

摘要

The cratering effects of dense tungsten carbide spheres (3.175 mm diameter and a density of 15 g/cm~3) impacting hard (0.89 GPa) and soft (0.7 GPa) copper targets (density of 8.9 g/cm~3) at velocities from 0.55 km/s to 2 km/s have been examined in comparison to similar impact conditions for soda-lime glass (2.2 g/cm~3) and ferritic stainless steel (7.8 g/cm~3) projectiles in previous studies. This range of impact velocities (0.55 to 2 km/s) illustrates a penetration anomaly where maximum values of crater depth (p) to crater diameter (D_c) ratio (or p/D_c) near 1 km/s are roughly 1.4 and 1.7 for hard and soft copper respectively. This is in contrast to an expected threshold or steady-state value of < 1 at hypervelocities ( > 5 km/s). These values also differ greatly from p/D_c values of ~0.9 at 1 km/s impact velocity for the stainless steel/copper system, where the hypervelocity threshold was observed to be p/D_c = 0.6. The hard copper targets were characterized by an equiaxed grain size of 85 μm and a dislocation density of ~10~(10) cm~(-2) while the soft plates were cast copper plates with a large, columnar grain structure (grain size 3.2 mm) and a dislocation density roughly two orders of magnitude less than the hard copper target The microstructures (observed by light metallography and transmission electron microscopy) surrounding the crater walls are characterized by dynamic recrystallization zones and microbands extending away from this narrow flow zone, and these zone widths increased with impact velocity and corresponding shock pressures. Residual hardness mapping was also performed on selected samples. These maps reveal a difference in affected zone size between hard and soft copper, as does the microstructure.
机译:密集的碳化钨球(直径为3.175 mm,密度为15 g / cm〜3)的弹坑效应,以下列速度撞击硬(0.89 GPa)和软(0.7 GPa)的铜靶(密度为8.9 g / cm〜3)。与之前研究中的钠钙玻璃(2.2 g / cm〜3)和铁素体不锈钢(7.8 g / cm〜3)的抛射物相似的冲击条件相比,测试了0.55 km / s至2 km / s。该冲击速度范围(0.55至2 km / s)说明了一个穿透异常,其中1 km / s附近的坑深(p)与坑直径(D_c)之比(或p / D_c)的最大值约为1.4和1.7硬铜和软铜。这与超高速(> 5 km / s)时的预期阈值或稳态值<1相反。这些值也与不锈钢/铜系统在1 km / s的冲击速度下p / D_c值(在0.9 km / s时)大不相同,在超高速阈值下观察到的p / D_c = 0.6。硬铜靶的特征是等轴晶尺寸为85μm,位错密度为〜10〜(10)cm〜(-2),而软板则是具有大的柱状晶粒结构(晶粒尺寸为3.2)的铸铜板。毫米)和位错密度,大约比硬铜靶低两个数量级。火山口壁周围的微观结构(通过光金相和透射电子显微镜观察)的特征是动态再结晶区和从该狭窄流动区延伸的微带,以及这些区域宽度随冲击速度和相应的冲击压力而增加。还对选定的样品进行了残留硬度图。这些图揭示了硬铜和软铜之间受影响区域大小的差异,以及微观结构也是如此。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号