活性无序合金冲击的释能特性及在毁伤元中应用研究进展

侯先苇; 张先锋; 熊玮; 谈梦婷; 刘闯; 戴兰宏

doi:10.11883/bzycj-2023-0189

活性无序合金冲击的释能特性及在毁伤元中应用研究进展

doi: 10.11883/bzycj-2023-0189

侯先苇^1,,
张先锋^1, ,,
熊玮¹,
谈梦婷¹,
刘闯¹,
戴兰宏^{2, 3}

1.
南京理工大学机械工程学院，江苏南京 210094
2.
中国科学院力学研究所非线性力学国家重点实验室，北京 100190
3.
中国科学院大学工程科学学院，北京 101408

基金项目: 国家自然科学基金(11790292，12141202，12002170)

详细信息

作者简介:
侯先苇（1997—　），女，博士研究生，18260081681@163.com

通讯作者:
张先锋（1978—　），男，博士，教授，lynx@njust.edu.cn

中图分类号: O385
计量
- 文章访问数: 250
- HTML全文浏览量: 111
- PDF下载量: 136
- 被引次数: 0
出版历程
- 收稿日期: 2023-05-24
- 修回日期: 2023-08-28
- 网络出版日期: 2023-08-29
- 刊出日期: 2023-09-11

Research progress on impact energy release characteristics of reactive disordered alloy and its application in kill elements

1.
School of Mechanical Engineering, Nanjing University of Science and Technology, Nanjing, Jiangsu 210094, China
2.
State Key Laboratory of Nonlinear Mechanics, Institute of Mechanics, Chinese Academy of Sciences, Beijing 100190, China
3.
School of Engineering Science, University of Chinese Academy of Sciences, Beijing 101408, China

摘要

摘要: 无序合金是一种新型金属材料，突破了传统的合金设计理念，表现出不同于传统合金的优异力学性能、冲击释能及剪切自锐特性，在高温、高压、高应变率等环境具有良好的应用前景。分析活性无序合金的冲击释能特性对其应用于军事领域有着重要的指导作用，能为弹药战斗部的设计提供参考。本文阐述了静动态力学实验中典型无序合金的反应释能现象；总结了撞击速度与活性无序合金释能超压、释能效率之间的关系；讨论了撞击速度、材料破碎程度及靶标特征等因素对活性无序合金释能机理的影响；归纳了制备工艺及元素类型对活性无序合金释能特性的调控效果。进一步，本文梳理了活性无序合金在破片、穿甲弹芯和聚能装药战斗部三个方向的应用研究进展，分析了活性无序合金毁伤元的侵彻行为和作用机制。最后，针对活性无序合金材料未来的发展趋势和需求进行了展望。
- 无序合金 /
- 活性金属 /
- 冲击释能特性 /
- 高效毁伤
Abstract: Disordered alloy is a new kind of reactive material, which breaks through the design concept of traditional alloy and exhibits excellent mechanical properties, impact energy release characteristics and adiabatic shear sensitivity, showing good application prospects in high temperature, high pressure, high strain rates and other application environments. Analyzing the impact energy release characteristics of reactive disordered alloy has an important guiding role for its development in the military field and can provide the basis for the design and application of warheads for ammunition. In this paper, the impact energy release characteristics of reactive disordered alloys are introduced from four aspects, including the energy release phenomenon of chemical reaction, the energy release law induced by impacting, the energy release mechanism and the regulation of the energy release behaviors. The chemical reaction showing energy release phenomenon in static and dynamic mechanical experiments is described. The relationship between impact velocities and the energy release overpressures or the efficiency of energy release of reactive disordered alloys is obtained. The effect between impact velocities and crushing degree of the reactive disordered alloys or characteristics of the target on the energy release mechanism is discussed. At the same time, the regulation effects of preparation process and the kinds of element on energy release effect of disordered alloy materials are summarized. This kind of alloy own good impact energy release characteristics, presented an ideal energetic structural material. Furthermore, the research progress of reactive disordered alloys applied to warheads in military area is summarized from three directions, including fragment, armor-piercing core and shaped charge liner. The macro and micro penetration behavior and mechanism of warheads of reactive disordered alloys are analyzed under high-speed loading conditions. Via the design of the structure, the good penetration and damage performance benefit from the self-sharpening and energy release characteristics of the material. Finally, the further development trend and demands of reactive disordered alloy are prospected.
- disordered alloy /
- reactive metal /
- impact energy release characteristics /
- high efficiency damage

HTML全文

图 1 室温下空气中测试的锆基非晶合金试样断裂瞬间^[19]

Figure 1. Moment of fracturing a BAA specimen testedat room temperature in air^[19]

下载: 全尺寸图片幻灯片

图 2 摆锤冲击试验装置及空气环境中试验现象^[20]

Figure 2. Pendulum impact test device and test phenomena in air environment^[20]

下载: 全尺寸图片幻灯片

图 3 Zr_41.2Ti_13.8Cu_12.5Ni₁₀Be_22.5分子轨道能级谱^[20]

Figure 3. Molecular orbital energy spectrum of Zr_41.2Ti_13.8Cu_12.5Ni₁₀Be_22.5^[20]

下载: 全尺寸图片幻灯片

图 4 氮气环境中断裂后断口扫描电镜照片^[20]

Figure 4. Scanning electron microscope photos of fracture surface of the specimen fracturing in nitrogen environment^[20]

下载: 全尺寸图片幻灯片

图 5 准密闭容器试验^[25]

Figure 5. Quasi-sealed chamber test^[25]

下载: 全尺寸图片幻灯片

图 6 高速摄影图片及容器内超压时程曲线^[26]

Figure 6. Video frames and pressure curves inside the chamber^[26]

下载: 全尺寸图片幻灯片

图 7 破片撞击靶板后反应产物形貌与成分^[26]

Figure 7. Morphology and composition of the reaction products of fragment after impacting target^[26]

下载: 全尺寸图片幻灯片

图 8 高熵合金破片不同撞击速度下压力峰值^[33]

Figure 8. Peak overpressures at different impact velocities of the high-entropy alloy fragments^[33]

下载: 全尺寸图片幻灯片

图 9 多种活性材料的单位质量能量密度^[34]

Figure 9. Specific energy per unit mass of various reactive materials^[34]

下载: 全尺寸图片幻灯片

图 10 锆基非晶合金动态压缩高速摄影图像^[37]

Figure 10. High-speed photography of Zr-based amorphous alloy under dynamic compression^[37]

下载: 全尺寸图片幻灯片

图 11 锆基非晶合金动态压缩模拟损伤云图^[37]

Figure 11. Simulational damage contours of Zr-based amorphous alloy under dynamic compression^[37]

下载: 全尺寸图片幻灯片

图 12 氩气中不同撞击速度下动态破碎锆基非晶合金累积质量分布试验数据^[38]

Figure 12. Experimental data of cumulative mass distribution forZr-based amorphous alloy after dynamic fragmentation atdifferent impact velocities in argon atmosphere^[38]

下载: 全尺寸图片幻灯片

图 13 TiZrNbV高熵合金动态压缩背散射电子成像结果^[40]

Figure 13. BSE result of TiZrNbV high entropy alloy after dynamic compression^[40]

下载: 全尺寸图片幻灯片

图 14 不同撞击速度下回收试样的断口形貌^[40]

Figure 14. Fracture morphology of recovered specimen at different impact velocities^[40]

下载: 全尺寸图片幻灯片

图 15 原位晶化对锆基非晶合金能量释放行为的影响^[45]

Figure 15. Effect of in-situ crystalline phases on the energy release behaviors of Zr-based amorphous alloy^[45]

下载: 全尺寸图片幻灯片

图 16 NbZrTiTa高熵合金和HfZrTiTa_0.53合金弹丸在不同速度下撞击靶箱后的碎片^[50]

Figure 16. The fragments of NbZrTiTa high-entropy alloy and HfZrTiTa_0.53 high-entropy alloy projectilesimpacting the target at different velocities^[50]

下载: 全尺寸图片幻灯片

图 17 1200 m/s速度下NbZrTiTa高熵合金弹丸碎片的截面背散射电子成像^[50]

Figure 17. Cross-section BSE photos of NbZrTiTa high-entropy alloy projectile at 1200 m/s^[50]

下载: 全尺寸图片幻灯片

图 18 0.5 mm厚的盖板下破片不同撞击速度对应的压力-时间的曲线^[60]

Figure 18. Pressure as a function of time for a 0.5 mmcover target thicknesses^[60]

下载: 全尺寸图片幻灯片

图 19 不同靶板厚度下不同撞击速度对应的超压-时间曲线^[60]

Figure 19. Overpressure as a function of time for differentcover plate at different impact velocities^[60]

下载: 全尺寸图片幻灯片

图 20 超压-反应速率曲线^[60]

Figure 20. Reaction efficiency as a function of shock pressure^[60]

下载: 全尺寸图片幻灯片

图 21 冲击温度-反应速率曲线^[60]

Figure 21. Reaction efficiency as a function of shock temperature^[60]

下载: 全尺寸图片幻灯片

图 22 Zr₅₅Cu₃₀Ni₅Al₁₀非晶合金破片典型速度撞击间隔靶板高速摄影图片^[71]

Figure 22. High-speed photographs of Zr₅₅Cu₃₀Ni₅Al₁₀ amorphous fragments impacting spacing targets at typical velocity^[71]

下载: 全尺寸图片幻灯片

图 23 WFeNiMo高熵合金在不同速度下穿靶燃烧过程的高速摄影^[72]

Figure 23. High-speed video frames of combustion process of WFeNiMo HEA at different speeds^[72]

下载: 全尺寸图片幻灯片

图 24 高速撞击后高熵合金回收破片细观结构^[72]

Figure 24. Microstructure of high-entropy alloy fragments after high speed impact^[72]

下载: 全尺寸图片幻灯片

图 25 非晶破片毁伤后效仿真结果^[73]

Figure 25. Simulation results of amorphous fragmentation damage aftermath^[73]

下载: 全尺寸图片幻灯片

图 26 W/Zr基非晶合金预制破片^[11]

Figure 26. W/Zr-based amorphous alloy fragments^[11]

下载: 全尺寸图片幻灯片

图 27 预制破片布置方式^[11]

Figure 27. Arrangement of performed fragments^[11]

下载: 全尺寸图片幻灯片

图 28 典型时刻高速摄影图片^[11]

Figure 28. High-speed photographs at typical moments^[11]

下载: 全尺寸图片幻灯片

图 29 棉被和油箱毁伤情况^[11]

Figure 29. The damage of quilts and fuel tanks^[11]

下载: 全尺寸图片幻灯片

图 30 破片侵彻后油箱^[11]

Figure 30. The oil tank penetrated by fragments^[11]

下载: 全尺寸图片幻灯片

图 31 复合材料弹芯的“自锐”和钨合金弹芯的“镦粗”^[77]

Figure 31. “Self-sharpening” of composite core and the “upsetting” of tungsten alloy core^[77]

下载: 全尺寸图片幻灯片

图 32 弹芯残体照片^[82]

Figure 32. Pictures of penetrator residual^[82]

下载: 全尺寸图片幻灯片

图 33 钨丝/锆基非晶复合材料侵彻深度与着靶动能及长径比的关系曲线^{[80, 86]}

Figure 33. Curves of kinetic energy and penetration depth of Wf/Zr-MG and WHA rods^{[80, 86]}

下载: 全尺寸图片幻灯片

图 34 不同直径钨丝/锆基非晶复合材料着靶速度-侵彻深度关系^[86]

Figure 34. Relationship between penetration depth and impact velocities of different Zr-based composite materials^[86]

下载: 全尺寸图片幻灯片

图 35 多组分钨丝/锆基非晶合金复合材料杆弹横截面^[86]

Figure 35. The cross section of multi-component Wf/Zr-based amorphous composite rod projectiles^[86]

下载: 全尺寸图片幻灯片

图 36 分段式钨丝/锆基非晶合金复合材料杆弹及侵彻结果（单位：mm）^[86]

Figure 36. Segmented Wf/Zr-based amorphous composite rod projectiles and penetration results (unit: mm)^[86]

下载: 全尺寸图片幻灯片

图 37 弹体侵彻靶体的高速摄像^[88]

Figure 37. High-speed video photographs of the projectiles penetrating the targets^[88]

下载: 全尺寸图片幻灯片

图 38 长杆弹侵彻深度和撞击动能的关系^[88]

Figure 38. Relation between penetration depth and kineticenergy of long rod projectiles^[88]

下载: 全尺寸图片幻灯片

图 39 长杆弹弹孔体积和撞击动能的关系曲线^[88]

Figure 39. Relation between total penetration volume and kinetic energy of long rod projectiles^[88]

下载: 全尺寸图片幻灯片

图 40 弹体侵彻靶板典型过程^[89]

Figure 40. Typical frames of the projectiles penetrating the targets^[89]

下载: 全尺寸图片幻灯片

图 41 弹体侵彻后靶板表面毁伤效果^[89]

Figure 41. The targets damaged surface after the projectiles penetrating^[89]

下载: 全尺寸图片幻灯片

图 42 钨丝/锆基非晶合金复合材料自锐剪切失效的 4 种模式^[81]

Figure 42. Four modes of self-sharpening shear failure of Wf/Zr-based amorphous composites material^[81]

下载: 全尺寸图片幻灯片

图 43 钨丝增强金属玻璃复合材料弹残余弹体头部及其附近位置 SEM 图像^[79]

Figure 43. SEM images of tungsten wire reinforced metal glass composite residual projectile head and its vicinity^[79]

下载: 全尺寸图片幻灯片

图 44 回收弹体TEM测试结果^[90]

Figure 44. Transmission electron microscope (TEM) bright-field images of LRPs after impact^[90]

下载: 全尺寸图片幻灯片

图 45 回收弹体TEM明图中的变形孪晶和堆叠断层^[90]

Figure 45. TEM results showging the multiple deformation twins and the stack faults^[90]

下载: 全尺寸图片幻灯片

图 46 钨丝/锆基非晶合金复合材料杆弹不同着靶速度下的侵彻断裂模式^[86]

Figure 46. Fracture modes of Wf/Zr-based amorphous composite projectile at different impact velocities^[86]

下载: 全尺寸图片幻灯片

图 47 WFeNiMo和93W长杆弹对靶体的侵彻深度与动能关系^[9]

Figure 47. Depth of WFeNiMo rod and 93W rod penetrating targets versus kinetic energy^[9]

下载: 全尺寸图片幻灯片

图 48 等截面直管内两相的流动模型^[91]

Figure 48. Model of two-phase flow in a straight pipe with equal cross section^[91]

下载: 全尺寸图片幻灯片

图 49 不同初始浓度及密度对硬相浓度演化的影响^[91]

Figure 49. Effect of initial concentration on concentration evolution of hard phase^[91]

下载: 全尺寸图片幻灯片

图 50 Zr₅₇Cu_15.4Ni_12.6Al₁₀Nb₅非晶合金射流成型形态^[95]

Figure 50. Shape of Zr₅₇Cu_15.4Ni_12.6Al₁₀Nb₅ jet forming^[95]

下载: 全尺寸图片幻灯片

图 51 Zr_41.2Ti_13.8Cu_12.5Ni₁₀Be_22.5非晶合金射流成型形态^[96]

Figure 51. Shape of Zr_41.2Ti_13.8Cu_12.5Ni₁₀Be_22.5 jet forming^[96]

下载: 全尺寸图片幻灯片

图 52 塑性和脆性药型罩形成的射流^[98]

Figure 52. Jets by plastic and brittle liner^[98]

下载: 全尺寸图片幻灯片

图 53 两种材料杆式射流不同时刻下的成形状态^[99]

Figure 53. Shape of rod jets about two materials at different times^[99]

下载: 全尺寸图片幻灯片

图 54 CrMnFeCoNi与紫铜材料流动速度（V₂）与临界压垮角（β_c）关系^[100]

Figure 54. Relationship between flow velocity (V₂) and critical crushing angle (β_c) of CrMnFeCoNi and copper^[100]

下载: 全尺寸图片幻灯片

图 55 材料流动速度（V₂）与临界压垮角（β_c）曲线不同取值位置有限元仿真结果^[100]

Figure 55. Finite element simulation results of value positions of flow velocity (V₂) and critical crushing angle (β_c) curve^[100]

下载: 全尺寸图片幻灯片

图 56 不同硬化指数k下射流形态对比^[100]

Figure 56. Comparison of jet shape under different hardening index (k)^[100]

下载: 全尺寸图片幻灯片

图 57 不同炸高下药型罩侵彻深度^[105]

Figure 57. Penetration depths of liners under different stand off^[105]

下载: 全尺寸图片幻灯片

图 58 数值模拟模型及成型射流^[12]

Figure 58. Model and jet structure of numerical simulation^[12]

下载: 全尺寸图片幻灯片

图 59 聚能装药结构^[109]

Figure 59. Shaped charge^[109]

下载: 全尺寸图片幻灯片

图 60 靶板截面形貌和晶相^[12]

Figure 60. Cross-section profile and crystal phase of target plate^[12]

下载: 全尺寸图片幻灯片

图 61 残余射流区的XRD谱^[12]

Figure 61. XRD spectrum of residual zone^[12]

下载: 全尺寸图片幻灯片

图 62 残余射流区的EDS谱^[12]

Figure 62. EDS spectrum of residual zone^[12]

下载: 全尺寸图片幻灯片

图 63 射流侵彻后靶板的EBSD细观分析：(a)变形区IPF图；(a)中区域b的（b₁、b₂）IPF图和对应的KAM图；(a)中区域c的(c₁, c₂) IPF图和对应的KAM图^[113]

Figure 63. Microstructural analysis of the residual jet after penetration via EBSD: (a) IPF map of deformation zone; (b₁, b₂) IPF map and corresponding KAM map of region b in (a); (c₁, c₂) IPF map and corresponding KAM map of region c in (a)^[113]

下载: 全尺寸图片幻灯片

图 64 再结晶区的高倍BSE-SEM图像(a)及线扫描分析(b)：在(a)中显示的两个晶界上进行线扫描，其对应的位置在(b)中用虚线标记^[113]

Figure 64. High-magnification BSE-SEM images (a) and line scan analysis (b) of the recrystallization region: a line scan was conducted across two grain boundaries as displayed in (a), the corresponding locations of which are labeled with dashed lines in (b)^[113]

下载: 全尺寸图片幻灯片

图 65 CoCrNi残余射流侵彻后的TEM组织分析：(a) CoCrNi残余射流的TEM照片，其中的白色虚线标记了沿晶界的纳米尺寸沉淀；(b) 降水（图(a)中的红色矩形区域）的HAADF-TEM照片；(c～e) 图(b)中对应的Co、Cr、Ni元素分布；(f) 降水SAED图（区域I(b)），(g) 图(b)中Ⅰ，Ⅱ，Ⅲ，Ⅳ区域Co，Cr，Ni元素含量^[113]

Figure 65. Microstructural analysis of CoCrNi residual jet after penetration by TEM: (a) TEM images of CoCrNi residual jet, where the white dashed line marks the nanosized precipitations along grain boundaries; (b) HAADF-TEM image of the precipitation (red rectangle region in (a)); (c–e) Corresponding element distributions of Co, Cr, and Ni in (b); (f) SAED pattern ofprecipitation (region I in (b)); (g) Element content of Co, Cr, and Ni in region I, II, III, IV in (b)^[113]

下载: 全尺寸图片幻灯片

表 1 锆基非晶合金的冲击化学反应行为^[36]

Table 1. Impact-induced chemical reaction behavior of ZrTiNiCuBe^[36]

射击序号	靶板厚度/mm	撞击速度/（m·s⁻¹）	超压峰值/MPa	扩孔半径/mm	挠度/mm
1	3	1450	0.02	7～10	10～15
2	3	1560	0.04	10～15	15～20
3	2	1348	0.05	20～25	20～25
4	2	1218	0.024	8～12	10～15
5	4.5	1630	0.021	7～10	8～10

下载: 导出CSV

参考文献(115)

[1]	汪卫华. 非晶态物质的本质和特性 [J]. 物理学进展, 2013, 33(5): 177–351. WANG W H. The nature and properties of amorphous matter [J]. Progress in Physics, 2013, 33(5): 177–351.
[2]	FALK M L, KANGER J S. 类固体非晶态材料的变形与失效 [J]. 力学进展, 2021, 51(2): 406–426. DOI: 10.6052/1000-0992-21-034. FALK M L, KANGER J S. Deformation and failure of amorphous, solidlike materials [J]. Advances in Mechanics, 2021, 51(2): 406–426. DOI: 10.6052/1000-0992-21-034.
[3]	乔吉超, 张浪渟, 童钰, 等. 基于微观结构非均匀性的非晶合金力学行为 [J]. 力学进展, 2022, 529(1): 117–152. DOI: 10.6052/1000-0992-21-038. QIAO J C, ZHANG L T, TONG Y, et al. Mechancial properties of amorphous alloys: in the framework of the microstructure heterogeneity [J]. Advances in Mechanics, 2022, 529(1): 117–152. DOI: 10.6052/1000-0992-21-038.
[4]	LIU D, YU Q, KABRA S, et al. Exceptional fracture toughness of CrCoNi-based medium-and high-entropy alloys at 20 Kelvin [J]. Science, 2022, 378(6623): 978–983. DOI: 10.1126/science.abp8070.
[5]	卜叶强, 王宏涛. 多主元合金中的化学短程有序 [J]. 力学进展, 2021, 51(4): 915–919. DOI: 10.6052/1000-0992-21-027. BU Y Q, WANG H T. Short-range order in multicomponent alloys [J]. Advances in Mechanics, 2021, 51(4): 915–919. DOI: 10.6052/1000-0992-21-027.
[6]	陈曦, 杜成鑫, 程春, 等. Zr基非晶合金材料的冲击释能特性 [J]. 兵器材料科学与工程, 2018, 41(6): 44–49. DOI: 10.14024/j.cnki.1004-244x.20180717.002. CHEN X, DU C X, CHENG C, et al. Impact energy releasing characteristics of Zr-based amorphous alloy [J]. Ordnance Material Science and Engineering, 2018, 41(6): 44–49. DOI: 10.14024/j.cnki.1004-244x.20180717.002.
[7]	张周然. HfZrTiTa_x高熵合金含能结构材料的组织结构与力学性能研究 [D]. 长沙: 国防科技大学, 2017: 80–84. DOI: 10.27052/d.cnki.gzjgu.2017.000221. ZHANG Z R. Microstructure and mechanical properties of HfZrTiTa_x high-entropy alloys energetic structural materials [D]. Changsha: National University of Defense Technology, 2017: 80–84. DOI: 10.27052/d.cnki.gzjgu.2017.000221.
[8]	李继承, 陈小伟. 块体金属玻璃及其复合材料的压缩剪切特性和侵彻/穿甲“自锐”行为 [J]. 力学进展, 2011, 41(5): 480–518. DOI: 10.6052/1000-0992-2011-5-lxjzJ2011-056. LI J C, CHEN X W. Compressive-shear behavior and self-sharpening of bulk metallic glasses and their composite materials [J]. Advances in Mechanics, 2011, 41(5): 480–518. DOI: 10.6052/1000-0992-2011-5-lxjzJ2011-056.
[9]	LIU X F, TIAN Z L, ZHANG X F, et al. “Self-sharpening”tungsten high-entropy alloy [J]. Acta Materialia, 2020, 186: 257–266. DOI: 10.1016/j.actamat.2020.01.005.
[10]	LIU T W, LI T, DAI L H. Near-equiatomic µ phase in self-sharpening tungsten-based high-entropy alloy [J]. Metals, 2022, 12(7): 1130. DOI: 10.3390/met12071130.
[11]	张玉令, 施冬梅, 张云峰, 等. W骨架/Zr基非晶合金复合材料破片侵彻能力与后效研究 [J]. 爆炸与冲击, 2021, 41(5): 053301. DOI: 10.11883/bzycj-2020-0063. ZHANG Y L, SHI D M, ZHANG Y F, et al. Investigation of penetration ability and aftereffect of Zr-based metallic glass reinforced porous W matrix composite fragments [J]. Explosion and Shock Waves, 2021, 41(5): 053301. DOI: 10.11883/bzycj-2020-0063.
[12]	HAN J L, CHEN X, DU Z H, et al. Application of W/Zr amorphous alloy for shaped charge liner [J]. Materials Research Express, 2019, 6(11): 115209. DOI: 10.1088/2053-1591/ab47d7.
[13]	CONNER R D, DANDLIKER R B, SCRUGGS V, et al. Dynamic deformation behavior of tungsten-fiber/metallic-glass matrix composites [J]. International Journal of Impact Engineering, 2000, 24(5): 435–444. DOI: 10.1016/s0734-743x(99)00176-1.
[14]	SCHROERS J, JOHNSON W L. Highly processable bulk metallic glass-forming alloys in the Pt-Co-Ni-Cu-P system [J]. Applied Physics Letters, 2004, 84(18): 3666–3668. DOI: 10.1063/1.1738945.
[15]	胡宏伟, 宋浦, 邓国强, 等. 温压炸药的特性及发展现状 [J]. 力学进展, 2022, 52(1): 53–78. DOI: 10.6052/1000-0992-21-021. HU H W, SONG P, DENG G Q, et al. Characteristics of thermobaric explosives and their advances [J]. Advances in Mechanics, 2022, 52(1): 53–78. DOI: 10.6052/1000-0992-21-021.
[16]	INOUE A, ZHANG T, MASUMOTO T. Preparation of bulky amorphous Zr-Al-Co-Ni-Cu alloys by copper mold casting and their thermal and mechanical properties [J]. Materials Transactions, JIM, 1995, 36(3): 391–398. DOI: 10.2320/matertrans1989.36.391.
[17]	INOUE A, AMIYA K, KATSUYA A, et al. Mechanical properties and thermal stability of Ti- and Al-based amorphous wires prepared by a melt extraction method [J]. Materials Transactions, JIM, 1995, 36(7): 858–865. DOI: 10.2320/matertrans1989.36.858.
[18]	YOKOYAMA Y, INOUE A. Solidification condition of bulk glassy Zr₆₀Al₁₀Ni₁₀Cu₁₅Pd₅ alloy by unidirectional arc melting [J]. Materials Transactions, JIM, 1995, 36(11): 1398–1402. DOI: 10.2320/matertrans1989.36.1398.
[19]	LIU C T, HEATHERLY L, HORTON J A, et al. Test environments and mechanical properties of Zr-base bulk amorphous alloys [J]. Metallurgical and Materials Transactions A, 1998, 29(7): 1811–1820. DOI: 10.1007/s11661-998-0004-6.
[20]	GILBERT C J, AGER III J W, SCHROEDER V, et al. Light emission during fracture of a Zr-Ti-Ni-Cu-Be bulk metallic glass [J]. Applied Physics Letters, 1999, 74(25): 3809–3811. DOI: 10.1063/1.124187.
[21]	潘念侨. Zr基非晶合金材料动态本构关系及其释能效应研究 [D]. 南京: 南京理工大学, 2016: 36–54. DOI: 10.7666/d.Y3046370. PAN N Q. Dynamic Zr based amorphous alloy material constitutive relation and release energy effect reserch [D]. Nanjing: Nanjing University of Science and Technology, 2016: 36–54. DOI: 10.7666/d.Y3046370.
[22]	ZHANG Z R, ZHANG H, TANG Y, et al. Microstructure, mechanical properties and energetic characteristics of a novel high-entropy alloy HfZrTiTa_0.53 [J]. Materials & Design, 2017, 133: 435–443. DOI: 10.1016/j.matdes.2017.08.022.
[23]	AMES R. Vented chamber calorimetry for impact-initiated energetic materials [C]// Proceedings of the 43rd AIAA Aerospace Sciences Meeting and Exhibit. Reno: AIAA, 2005: 279. DOI: 10.2514/6.2005-279.
[24]	AMES R G. Energy release characteristics of impact-initiated energetic materials [J]. MRS Online Proceedings Library, 2005, 896(1): 308. DOI: 10.1557/PROC-0896-H03-08.
[25]	汪德武, 任柯融, 江增荣, 等. 活性材料冲击释能行为研究进展 [J]. 爆炸与冲击, 2021, 41(3): 031408. DOI: 10.11883/bzycj-2020-0337. WANG D W, REN K R, JIANG Z R, et al. Shock-induced energy release behaviors of reactive materials [J]. Explosion and Shock Waves, 2021, 41(3): 031408. DOI: 10.11883/bzycj-2020-0337.
[26]	WANG C T, HE Y, JI C, et al. Investigation on shock-induced reaction characteristics of a Zr-based metallic glass [J]. Intermetallics, 2018, 93: 383–388. DOI: 10.1016/j.intermet.2017.11.004.
[27]	GILBERT C J, AGER III J W, SCHROEDER V, et al. Mechanism for light emission during fracture of a Zr-Ti-Cu-Ni-Be bulk metallic glass: temperature measurements in air and nitrogen [J]. MRS Online Proceedings Library, 1998, 554(1): 191–196. DOI: 10.1557/PROC-554-191.
[28]	WEI H Y, YOO C S. Kinetics of small single particle combustion of zirconium alloy [J]. Journal of Applied Physics, 2012, 111(2): 023506. DOI: 10.1063/1.3677789.
[29]	WEI H Y, YOO C S. Dynamic responses of reactive metallic structures under thermal and mechanical ignitions [J]. Journal of Materials Research, 2012, 27(21): 2705–2717. DOI: 10.1557/jmr.2012.302.
[30]	尚春明, 施冬梅, 李文钊, 等. Zr基非晶合金燃烧热测试方法 [J]. 兵器装备工程学报, 2019, 40(8): 193–197. DOI: 10.11809/bqzbgcxb2019.08.038. SHANG C M, SHI D M, LI W Z, et al. Study on combustion heat method of Zr-based amorphous alloy [J]. Journal of Ordnance Equipment Engineering, 2019, 40(8): 193–197. DOI: 10.11809/bqzbgcxb2019.08.038.
[31]	TU J, QIAO L, SHAN Y, et al. Study on the impact-induced energy release characteristics of Zr_68.5Cu₁₂Ni₁₂Al_7.5 amorphous alloy [J]. Materials, 2021, 14(6): 1447. DOI: 10.3390/ma14061447.
[32]	尚春明, 施冬梅, 张云峰, 等. Zr基非晶合金的燃烧释能特性 [J]. 含能材料, 2020, 28(6): 564–568. DOI: 10.11943/CJEM2019219. SHANG C M, SHI D M, ZHANG Y F, et al. Combustion and energy release characteristics of Zr-based amorphous alloys [J]. Chinese Journal of Energetic Materials, 2020, 28(6): 564–568. DOI: 10.11943/CJEM2019219.
[33]	侯先苇, 熊玮, 陈海华, 等. 两种典型高熵合金冲击释能及毁伤特性研究 [J]. 力学学报, 2021, 53(9): 2528–2540. DOI: 10.6052/0459-1879-21-327. HOU X W, XIONG W, CHEN H H, et al. Impact energy release and damage characteristics of two high-entropy alloys [J]. Chinese Journal of Theoretical and Applied Mechanics, 2021, 53(9): 2528–2540. DOI: 10.6052/0459-1879-21-327.
[34]	张云峰, 刘国庆, 李晨, 等. 新型亚稳态合金材料冲击释能特性 [J]. 含能材料, 2019, 27(8): 692–697. DOI: 10.11943/CJEM2018170. ZHANG Y F, LIU G Q, LI C, et al. Shock energy release characteristics of novel metastable alloy materials [J]. Chinese Journal of Energetic Materials, 2019, 27(8): 692–697. DOI: 10.11943/CJEM2018170.
[35]	LUO P G, WANG Z C, JIANG C L, et al. Experimental study on impact-initiated characters of W/Zr energetic fragments [J]. Materials & Design, 2015, 84: 72–78. DOI: 10.1016/j.matdes.2015.06.107.
[36]	CHEN X, DU C X, CHENG C, et al. Impact-induced chemical reaction behavior of ZrTiNiCuBe bulk metallic glass fragments impacting on thin plates [J]. Materiali in Tehnologije, 2018, 52(6): 737–743. DOI: 10.17222/mit.2018.089.
[37]	张云峰, 罗兴柏, 施冬梅, 等. 动态压缩下Zr基非晶合金失效释能机理 [J]. 爆炸与冲击, 2019, 39(6): 063101. DOI: 10.11883/bzycj-2018-0114. ZHANG Y F, LUO X B, SHI D M, et al. Failure behavior and energy release of Zr-based amorphous alloy under dynamic compression [J]. Explosion and Shock Waves, 2019, 39(6): 063101. DOI: 10.11883/bzycj-2018-0114.
[38]	JI C, HE Y, WANG C T, et al. Effect of dynamic fragmentation on the reaction characteristics of a Zr-based metallic glass [J]. Journal of Non-Crystalline Solids, 2019, 515: 149–156. DOI: 10.1016/j.jnoncrysol.2019.04.022.
[39]	GRADY D E. Fragment size distributions from the dynamic fragmentation of brittle solids [J]. International Journal of Impact Engineering, 2008, 35(12): 1557–1562. DOI: 10.1016/j.ijimpeng.2008.07.042.
[40]	REN K R, LIU H Y, CHEN R, et al. Compression properties and impact energy release characteristics of TiZrNbV high-entropy alloy [J]. Materials Science and Engineering: A, 2021, 827: 142074. DOI: 10.1016/j.msea.2021.142074.
[41]	LOU H B, WANG X D, XU F, et al. 73 mm-diameter bulk metallic glass rod by copper mould casting [J]. Applied Physics Letters, 2011, 99(5): 051910. DOI: 10.1063/1.3621862.
[42]	INOUE A, ZHANG T. Fabrication of bulk glassy Zr₅₅Al₁₀Ni₅Cu₃₀ alloy of 30 mm in diameter by a suction casting method [J]. Materials Transactions, JIM, 1996, 37(2): 185–187. DOI: 10.2320/matertrans1989.37.185.
[43]	DONG W B, ZHANG H F, CAI J, et al. Enhanced plasticity in a Zr-based bulk metallic glass containing nanocrystalline precipitates [J]. Journal of Alloys and Compounds, 2006, 425(1/2): L1–L4. DOI: 10.1016/j.jallcom.2006.01.021.
[44]	黄彩敏. 金属型含能结构材料的组织调控与力、热特性研究 [D]. 长沙: 国防科技大学, 2020. DOI: 10.27052/d.cnki.gzjgu.2020.000084. HUANG C M. Research on prepartion, mechanical and thermal characteristics of metallic energetic structural materials [D]. Changsha: National University of Defense Technology, 2020. DOI: 10.27052/d.cnki.gzjgu.2020.000084.
[45]	HUANG C M, BAI S X, LI S, et al. Effect of in-situ crystalline phases on the mechanical properties and energy release behaviors of Zr₅₅Ni₅Al₁₀Cu₃₀ bulk metallic glasses [J]. Intermetallics, 2020, 119: 106720. DOI: 10.1016/j.intermet.2020.106720.
[46]	HUANG H L, WU Y, HE J Y, et al. Phase-transformation ductilization of brittle high-entropy alloys via metastability engineering [J]. Advanced Materials, 2017, 29(30): 1701678. DOI: 10.1002/adma.201701678.
[47]	SUH D W, RYU J H, JOO M S, et al. Medium-alloy manganese-rich transformation-induced plasticity steels [J]. Metallurgical and Materials Transactions A, 2013, 44(1): 286–293. DOI: 10.1007/s11661-012-1402-3.
[48]	LI Z M, PRADEEP K G, DENG Y, et al. Metastable high-entropy dual-phase alloys overcome the strength–ductility trade-off [J]. Nature, 2016, 534(7606): 227–230. DOI: 10.1038/nature17981.
[49]	LI X, CHEN L Q, ZHAO Y, et al. Influence of manganese content on ε-/ α′-martensitic transformation and tensile properties of low-C high-Mn TRIP steels [J]. Materials & Design, 2018, 142: 190–202. DOI: 10.1016/j.matdes.2018.01.026.
[50]	王睿鑫. NbZrTiTa高熵合金的组织结构演变及结构释能特性研究 [D]. 长沙: 国防科技大学, 2018. DOI: 10.27052/d.cnki.gzjgu.2018.001416. WANG R X. Microstructure evolution and energetic structural properties of NbZrTiTa high-entropy alloy [D]. Changsha: National University of Defense Technology, 2018. DOI: 10.27052/d.cnki.gzjgu.2018.001416.
[51]	TANG Y, WANG R X, XIAO B, et al. A review on the dynamic-mechanical behaviors of high-entropy alloys [J]. Progress in Materials Science, 2023, 135: 101090. DOI: 10.1016/j.pmatsci.2023.101090.
[52]	黄劲松, 刘咏, 陈仕奇, 等. 锆基非晶合金的研究进展与应用 [J]. 中国有色金属学报, 2003, 13(6): 1321–1332. DOI: 10.3321/j.issn:1004-0609.2003.06.001. HUANG J S, LIU Y, CHEN S Q, et al. Progress and application of Zr-based amorphous alloys [J]. The Chinese Journal of Nonferrous Metals, 2003, 13(6): 1321–1332. DOI: 10.3321/j.issn:1004-0609.2003.06.001.
[53]	马卫锋, 寇宏超, 李金山, 等. W纤维增强Zr基非晶复合材料的界面研究现状 [J]. 材料导报, 2006, 20(4): 64–66. DOI: 10.3321/j.issn:1005-023X.2006.04.018. MA W F, KOU H C, LI J S, et al. The present status of interface study of W fiber reinforced Zr-based amorphous matrix composite [J]. Materials Reports, 2006, 20(4): 64–66. DOI: 10.3321/j.issn:1005-023X.2006.04.018.
[54]	INOUE A. Stabilization of metallic supercooled liquid and bulk amorphous alloys [J]. Acta Materialia, 2000, 48(1): 279–306. DOI: 10.1016/s1359-6454(99)00300-6.
[55]	QIU K Q, WANG A M, ZHANG H F, et al. Mechanical properties of tungsten fiber reinforced ZrAlNiCuSi metallic glass matrix composite [J]. Intermetallics, 2002, 10(11/12): 1283–1288. DOI: 10.1016/s0966-9795(02)00136-x.
[56]	武晓峰, 邱克强, 张海峰, 等. SiC颗粒对Zr₅₅Al₁₀Ni₅Cu₃₀非晶形成能力和热稳定性的影响 [J]. 金属学报, 2003, 39(4): 414–418. DOI: 10.3321/j.issn:0412-1961.2003.04.016. WU X F, QIU K Q, ZHANG H F, et al. Effect of SiC_p on the glass forming ability and thermal stability of Zr₅₅Al₁₀Ni₅Cu₃₀ bulk metallic glass [J]. Acta Metallurgica Sinica, 2003, 39(4): 414–418. DOI: 10.3321/j.issn:0412-1961.2003.04.016.
[57]	XU Y K, XU J. Ceramics particulate reinforced Mg₆₅Cu₂₀Zn₅Y₁₀ bulk metallic glass composites [J]. Scripta Materialia, 2003, 49(9): 843–848. DOI: 10.1016/s1359-6462(03)00447-0.
[58]	寇生中, 郑宝超, 李娜, 等. 不同元素掺杂对Zr基非晶形成能力及力学性能的影响 [J]. 金属功能材料, 2011, 18(2): 1–5. DOI: 10.13228/j.boyuan.issn1005-8192.2011.02.009. KOU S Z, ZHENG B C, LI N, et al. Effects of additional different element on glass forming ability and mechanical properties of bulk Zr-based amorphous alloys [J]. Metallic Functional Materials, 2011, 18(2): 1–5. DOI: 10.13228/j.boyuan.issn1005-8192.2011.02.009.
[59]	张云峰, 罗兴柏, 施冬梅, 等. W骨架/Zr基非晶合金复合材料细观胞元重构 [J]. 稀有金属材料与工程, 2019, 48(1): 137–142. ZHANG Y F, LUO X B, SHI D M, et al. Reconstruction of meso-cells of Zr-based metallic glass reinforced porous W matrix composite [J]. Rare Metal Materials and Engineering, 2019, 48(1): 137–142.
[60]	张云峰, 罗兴柏, 刘国庆, 等. W骨架/Zr基非晶合金复合材料破片的冲击释能特性 [J]. 稀有金属材料与工程, 2020, 49(8): 2549–2556. ZHANG Y F, LUO X B, LIU G Q, et al. Shock-induced reaction characteristics of porous W/Zr-based metallic glass composite fragments [J]. Rare Metal Materials and Engineering, 2020, 49(8): 2549–2556.
[61]	MA Y S, ZHOU L, ZHANG K C, et al. Effects of cerium doping on the mechanical properties and energy-releasing behavior of high-entropy alloys [J]. Materials, 2022, 15(20): 7332. DOI: 10.3390/ma15207332.
[62]	MA Y S, HE J Y, ZHOU L, et al. Mechanical properties and impact energy release characteristics of Al_0.5NbZrTi_1.5Ta_0.8Ce_0.85 high-entropy alloy [J]. Materials Research Express, 2022, 9(11): 116510. DOI: 10.1088/2053-1591/ac9f04.
[63]	魏祥赛. Ni-M系高熵合金含能结构材料设计与力学性能 [D]. 大连: 大连理工大学, 2022: 16−73. DOI: 10.26991/d.cnki.gdllu.2022.000524. WEI X S. Design and mechanical properties of Ni-M high entropy alloy energetic structural materials [D]. Dalian: Dalian University of Technology, 2022: 16−73. DOI: 10.26991/d.cnki.gdllu.2022.000524.
[64]	高人奎. TiZrHf系高熵合金的冲击动力学特性及反应释能评价 [D]. 沈阳: 沈阳理工大学, 2022: 51−72. DOI: 10.27323/d.cnki.gsgyc.2022.000486. GAO R K. Impact dynamics properties and reaction energy release evaluation of TiZrHf based high entropy alloys [D]. Shenyang: Shenyang Ligong University, 2022: 51−72. DOI: 10.27323/d.cnki.gsgyc.2022.000486.
[65]	CHEN C, GAO R K, GUO K, et al. Quantitative determination of impact release energy for TiZrHfX_0.3 multicomponent materials in vacuum environment [J]. International Communications in Heat and Mass Transfer, 2022, 133: 105958. DOI: 10.1016/j.icheatmasstransfer.2022.105958.
[66]	TANG W Q, ZHANG K, CHEN T Y, et al. Microstructural evolution and energetic characteristics of TiZrHfTa_0.7W_0.3 high-entropy alloy under high strain rates and its application in high-velocity penetration [J]. Journal of Materials Science & Technology, 2023, 132: 144–153. DOI: 10.1016/j.jmst.2022.05.043.
[67]	MONTGOMERY JR H E. Reactive fragment: US3961576 [P]. 1976-06-08.
[68]	TRUITT R M, NIELSON D B, ASHCROFT B N, et al. Weapons and weapon components incorporating reactive materials: US11512058 [P]. 2006-08-29.
[69]	WILLIAM J F. Reactive fragrant warhead for enhanced neutralization of mortar, rocket, and missile threats: ONR-SBIR, N04-903 [R]. 2005.
[70]	REN S Y, ZHANG Q M, WU Q, et al. Influence of impact-induced reaction characteristics of reactive composites on hypervelocity impact resistance [J]. Materials & Design, 2020, 192: 108722. DOI: 10.1016/j.matdes.2020.108722.
[71]	郭磊, 王传婷, 何勇, 等. Zr₅₅Cu₃₀Ni₅Al₁₀活性破片对间隔防护结构破坏特性研究 [J]. 航天器环境工程, 2020, 37(6): 582–588. DOI: 10.12126/see.2020.06.008. GUO L, WANG C T, HE Y, et al. The failure characteristics of spacing protective structures impacted by Zr₅₅Cu₃₀Ni₅Al₁₀ active fragments [J]. Spacecraft Environment Engineering, 2020, 37(6): 582–588. DOI: 10.12126/see.2020.06.008.
[72]	陈海华, 张先锋, 熊玮, 等. WFeNiMo高熵合金动态力学行为及侵彻性能研究 [J]. 力学学报, 2020, 52(5): 1443–1453. DOI: 10.6052/0459-1879-20-166. CHEN H H, ZHANG X F, XIONG W, et al. Dynamic mechanical behavior and penetration performance of WFeNiMo high-entropy alloy [J]. Chinese Journal of Theoretical and Applied Mechanics, 2020, 52(5): 1443–1453. DOI: 10.6052/0459-1879-20-166.
[73]	杨林, 于述贤, 范群波. Zr_77.1Cu₁₃Ni_9.9非晶合金破片侵彻LY12铝合金及TC4钛合金靶板毁伤后效及机理对比研究 [J]. 北京理工大学学报, 2023, 43(4): 417–428. DOI: 10.15918/j.tbit1001-0645.2022.092. YANG L, YU S X, FAN Q B. Damage effect and mechanism of Zr_77.1Cu₁₃Ni_9.9 bulk metallic glasses fragment penetrating LY12 aluminum alloy and TC4 titanium alloy target plate [J]. Transactions of Beijing Institute of Technology, 2023, 43(4): 417–428. DOI: 10.15918/j.tbit1001-0645.2022.092.
[74]	LEHR H F, WOLLMAN E, KOERBER G. Experiments with jacketed rods of high fineness ratio [J]. International Journal of Impact Engineering, 1995, 17(4/5/6): 517–526. DOI: 10.1016/0734-743x(95)99876-s.
[75]	BACKMAN M E. Terminal ballistics: AD-A021 833 [R]. China Lake, California: Naval Weapons Center, 1976.
[76]	CHEN X W, WEI L M, LI J C. Experimental research on the long rod penetration of tungsten-fiber/Zr-based metallic glass matrix composite into Q235 steel target [J]. International Journal of Impact Engineering, 2015, 79: 102–116. DOI: 10.1016/j.ijimpeng.2014.11.007.
[77]	RONG G, HUANG D W, YANG M C. Penetrating behaviors of Zr-based metallic glass composite rods reinforced by tungsten fibers [J]. Theoretical and Applied Fracture Mechanics, 2012, 58(1): 21–27. DOI: 10.1016/j.tafmec.2012.02.003.
[78]	张明星, 黄晓霞. 钨合金穿甲弹芯材料强化技术及材料技术国外研究分析 [J]. 四川兵工学报, 2015, 36(12): 114–117. DOI: 10.11809/scbgxb2015.12.028. ZHANG M X, HUANG X X. Foreign research and analysis on strengthening technology and material technology of tungsten alloy piercing projectile [J]. Journal of Ordnance Equipment Engineering, 2015, 36(12): 114–117. DOI: 10.11809/scbgxb2015.12.028.
[79]	荣光, 黄德武. 钨纤维复合材料穿甲弹芯侵彻时的自锐现象 [J]. 爆炸与冲击, 2009, 29(4): 351–355. DOI: 10.11883/1001-1455(2009)04-0351-05. RONG G, HUANG D W. Self-sharpening phenomena of tungsten fiber composite material penetrators during penetration [J]. Explosion and Shock Waves, 2009, 29(4): 351–355. DOI: 10.11883/1001-1455(2009)04-0351-05.
[80]	杜忠华, 杜成鑫, 朱正旺, 等. 钨丝/锆基非晶复合材料长杆体弹芯穿甲实验研究 [J]. 稀有金属材料与工程, 2016, 45(5): 1308–1313. DU Z H, DU C X, ZHU Z W, et al. An experimental study on perforation behavior of pole penetrator prepared from W_F/Zr-based bulk metallic glass matrix composite [J]. Rare Metal Materials and Engineering, 2016, 45(5): 1308–1313.
[81]	陈小伟, 李继承, 张方举, 等. 钨纤维增强金属玻璃复合材料弹穿甲钢靶的实验研究 [J]. 爆炸与冲击, 2012, 32(4): 346–354. DOI: 10.11883/1001-1455(2012)04-0346-09. CHEN X W, LI J C, ZHANG F J, et al. Experimental research on the penetration of tungsten-fiber/metallic glass-matrix composite material penetrator into steel target [J]. Explosion and Shock Waves, 2012, 32(4): 346–354. DOI: 10.11883/1001-1455(2012)04-0346-09.
[82]	杜忠华, 杜成鑫, 朱正旺, 等. 分段结构的钨丝/锆基非晶复合材料弹芯穿甲实验研究 [J]. 稀有金属材料与工程, 2016, 45(9): 2359–2365. DU Z H, DU C X, ZHU Z W, et al. An experimental study on perforation behavior of segmented W_f/Zr-based bulk metallic glass matrix composite [J]. Rare Metal Materials and Engineering, 2016, 45(9): 2359–2365.
[83]	杜成鑫, 杜忠华, 朱正旺. 着靶速度和钨丝直径对钨丝/锆基非晶复合材料弹芯侵彻性能的影响 [J]. 稀有金属材料与工程, 2017, 46(6): 1632–1637. DU C X, DU Z H, ZHU Z W. Effect of impact velocity and diameter of tungsten fiber on penetration ability of W_f/Zr-based metallic glass composite penetrator [J]. Rare Metal Materials and Engineering, 2017, 46(6): 1632–1637.
[84]	杜成鑫, 杜忠华, 朱正旺. 钨丝直径对锆基复合非晶材料穿甲性能的影响 [J]. 稀有金属材料与工程, 2017, 46(4): 1080–1085. DU C X, DU Z H, ZHU Z W. Effect of tungsten fiber diameter on penetration ability of Zr-based metallic glass composites [J]. Rare Metal Materials and Engineering, 2017, 46(4): 1080–1085.
[85]	JIANG F, CHEN G, WANG Z H, et al. Mechanical properties of tungsten fiber reinforced (Zr_41.2Ti_13.8Cu_12.5Ni₁₀Be_22.5)_{100- x}Nb_x bulk metallic glass composites [J]. Rare Metal Materials and Engineering, 2011, 40(2): 206–208. DOI: 10.1016/S1875-5372(11)60016-7.
[86]	杜成鑫. Wf/Zr基非晶复合材料杆弹准细观侵彻机理及优化设计 [D]. 南京: 南京理工大学, 2020: 39−62. DOI: 10.27241/d.cnki.gnjgu.2020.000070. DU C X. Research on penetration mechanism and optimization design of Wf/Zr-based bulk metallic glass matrix composite rod [D]. Nanjing: Nanjing University of Science & Technology, 2020: 39−62. DOI: 10.27241/d.cnki.gnjgu.2020.000070.
[87]	SORENSEN B R, KIMSEY K D, SILSBY G F, et al. High velocity penetration of steel targets [J]. International Journal of Impact Engineering, 1991, 11(1): 107–119. DOI: 10.1016/0734-743X(91)90034-D.
[88]	林琨富, 张先锋, 陈海华, 等. Hf基非晶合金夹芯结构长杆弹的侵彻行为 [J]. 爆炸与冲击, 2021, 41(2): 023301. DOI: 10.11883/bzycj-2020-0181. LIN K F, ZHANG X F, CHEN H H, et al. Penetration behaviors of Hf-based amorphous alloy jacketed rods [J]. Explosion and Shock Waves, 2021, 41(2): 023301. DOI: 10.11883/bzycj-2020-0181.
[89]	HOU X W, ZHANG X F, XIONG W, et al. Study on energy release characteristics and penetration effects to concrete targets of Hf-based amorphous alloys [J]. Journal of Non-Crystalline Solids, 2022, 581: 121438. DOI: 10.1016/j.jnoncrysol.2022.121438.
[90]	HOU X W, ZHANG X F, LIU C, et al. Effects of annealing temperatures on mechanical behavior and penetration characteristics of FeNiCoCr high-entropy alloys [J]. Metals, 2022, 12(11): 1885. DOI: 10.3390/met12111885.
[91]	陈海华, 张先锋, 赵文杰, 等. W₂₅Fe₂₅Ni₂₅Mo₂₅高熵合金高速侵彻细观结构演化特性 [J]. 力学学报, 2022, 54(8): 2140–2151. DOI: 10.6052/0459-1879-22-128. CHEN H H, ZHANG X F, ZHAO W J, et al. Effect of microstructure on flow behavior during penetration of W₂₅Fe₂₅Ni₂₅Mo₂₅ high-entropy alloy projectile [J]. Chinese Journal of Theoretical and Applied Mechanics, 2022, 54(8): 2140–2151. DOI: 10.6052/0459-1879-22-128.
[92]	赵腾, 罗虹, 贾万明, 等. 药型罩材料技术基本要素探讨 [J]. 兵器材料科学与工程, 2007, 30(5): 77–82. DOI: 10.3969/j.issn.1004-244X.2007.05.022. ZHAO T, LUO H, JIA W M, et al. Discussion on the basic elements of shaped charge liner material [J]. Ordnance Material Science and Engineering, 2007, 30(5): 77–82. DOI: 10.3969/j.issn.1004-244X.2007.05.022.
[93]	张雪朋. 活性射流作用钢靶侵彻爆炸联合毁伤效应研究 [D]. 北京: 北京理工大学, 2016: 1−6. ZHANG X P. Research on penetration and blast combined damage effects of reactive material jet against steel target [D]. Beijing: Beijing Institute of Technology, 2016: 1−6.
[94]	张雪朋, 肖建光, 余庆波, 等. 活性药型罩聚能装药破甲后效超压特性 [J]. 兵工学报, 2016, 37(8): 1388–1394. DOI: 10.3969/j.issn.1000-1093.2016.08.007. ZHANG X P, XIAO J G, YU Q B, et al. Armor penetration aftereffect overpressure produced by reactive material liner shaped charge [J]. Acta Armamentarii, 2016, 37(8): 1388–1394. DOI: 10.3969/j.issn.1000-1093.2016.08.007.
[95]	WALTERS W P, KECSKES L J, PRITCHETT J E. Investigation of a bulk metallic glass as a shaped charge liner material [R]. Aberdeen Proving Ground: Army Research Laboratory, 2006.
[96]	SHI J, HUANG Z X, ZU X D, et al. Experimental and numerical investigation of jet performance based on Johnson-Cook model of liner material [J]. International Journal of Impact Engineering, 2022, 170: 104343. DOI: 10.1016/j.ijimpeng.2022.104343.
[97]	SHI J, HUANG Z X, ZU X D, et al. Experimental investigation of Zr-Based amorphous alloy as a shaped charge liner [J]. Propellants, Explosives, Pyrotechnics, 2022, 47(11): e202200063. DOI: 10.1002/prep.202200063.
[98]	CUI P, GAO X B, XU J Q, et al. Simulation and experimental study on jet velocity of Zr-based amorphous alloy liner [J]. Metals, 2022, 12(6): 978. DOI: 10.3390/met12060978.
[99]	周秉文, 孟凡迪, 张全孝, 等. 铜基非晶合金的动态性能及杆式射流仿真研究 [J]. 兵器材料科学与工程, 2020, 43(6): 1–5. DOI: 10.14024/j.cnki.1004-244x.20200612.001. ZHOU B W, MENG F D, ZHANG Q X, et al. Dynamic properties and rod jet simulation of copper-based bulk metallic glasses [J]. Ordnance Material Science and Engineering, 2020, 43(6): 1–5. DOI: 10.14024/j.cnki.1004-244x.20200612.001.
[100]	鄢阿敏, 乔禹, 戴兰宏. 高熵合金药型罩射流成型与稳定性 [J]. 力学学报, 2022, 54(8): 2119–2130. DOI: 10.6052/0459-1879-22-274. YAN A M, QIAO Y, DAI L H. Formation and stability of shaped charge liner jet of CrMnFeCoNi high-entropy alloy [J]. Chinese Journal of Theoretical and Applied Mechanics, 2022, 54(8): 2119–2130. DOI: 10.6052/0459-1879-22-274.
[101]	郑哲敏. 聚能射流的稳定性问题 [M]// 郑哲敏. 郑哲敏文集. 北京: 科学出版社, 2004: 12.
[102]	郑哲敏. 关于射流侵彻的几个问题 [J]. 兵工学报, 1980(1): 13–22. ZHENG Z M. Several problems on jet penetration [J]. Acta Armamentarii, 1980(1): 13–22.
[103]	CHOU P C, CARLEONE J. The stability of shaped-charge jets [J]. Journal of Applied Physics, 1977, 48(10): 4187–4195. DOI: 10.1063/1.323456.
[104]	CUI P, SHI D M, XU J Q, et al. Investigation of explosion simulation on jet forming of ZrCuNiAlAg amorphous alloy liner with eccentric sub-hemisphere structure [J]. IOP Conference Series: Materials Science and Engineering, 2020, 964: 012020. DOI: 10.1088/1757-899x/964/1/012020.
[105]	CUI P, WANG D S, SHI D M, et al. Investigation of penetration performance of Zr-based amorphous alloy liner compared with copper [J]. Materials, 2020, 13(4): 912. DOI: 10.3390/ma13040912.
[106]	CUI P, SHI D M, ZHANG Y L, et al. Numerical simulation and experimental study on jet forming and penetration performance of Zr-based amorphous alloy liner [J]. Engineering Letters, 2021, 29(1): 151–157.
[107]	CUI P, SHI D M, XU J Q, et al. Numerical simulation on jet forming and penetration performance of several amorphous energetic alloy liner with typical structures [J]. Journal of Physics: Conference Series, 2021, 1948: 012186. DOI: 10.1088/1742-6596/1948/1/012186.
[108]	芦永进, 梁增友, 邓德志, 等. 铜基非晶合金双层药型罩射流形成及侵彻性能 [J]. 火炮发射与控制学报, 2022, 43(1): 14–20, 28. DOI: 10.19323/j.issn.1673-6524.2022.01.003. LU Y J, LIANG Z Y, DENG D Z, et al. Jet formation and penetration performance of a Cu-based amorphous alloy double-layer charge liner [J]. Journal of Gun Launch & Control, 2022, 43(1): 14–20, 28. DOI: 10.19323/j.issn.1673-6524.2022.01.003.
[109]	HAN J L, CHEN X, DU Z H, et al. Design and penetration of a new W-particle/Zr-based amorphous alloy composite liner [J]. Journal of the Brazilian Society of Mechanical Sciences and Engineering, 2020, 42(7): 364. DOI: 10.1007/s40430-020-02359-6.
[110]	LÜ J X, ZHANG J L, SHEK C. Corrosion of glassy (Ni₈Nb₅)_99.5Sb_0.5 alloy and stability of passive film [J]. Rare Metal Materials and Engineering, 2013, 42(3): 447–451. DOI: 10.1016/S1875-5372(13)60045-4.
[111]	ZHAO Z Y, LIU J X, GUO W Q, et al. Effect of Zn and Ni added in W-Cu alloy on penetration performance and penetration mechanism of shaped charge liner [J]. International Journal of Refractory Metals and Hard Materials, 2016, 54: 90–97. DOI: 10.1016/j.ijrmhm.2015.07.022.
[112]	BAI X, LIU J X, LI S K, et al. Effect of interaction mechanism between jet and target on penetration performance of shaped charge liner [J]. Materials Science and Engineering: A, 2012, 553: 142–148. DOI: 10.1016/j.msea.2012.06.003.
[113]	CHEN J, LIU T W, CAO F H, et al. Deformation behavior and microstructure evolution of CoCrNi medium-entropy alloy shaped charge liners [J]. Metals, 2022, 12(5): 811. DOI: 10.3390/met12050811.
[114]	GUO W Q, LIU J X, XIAO Y, et al. Comparison of penetration performance and penetration mechanism of W-Cu shaped charge liner against three kinds of target: pure copper, carbon steel and Ti-6Al-4V alloy [J]. International Journal of Refractory Metals and Hard Materials, 2016, 60: 147–153. DOI: 10.1016/j.ijrmhm.2016.07.015.
[115]	ZHANG S C, JIANG Z H, LI H B, et al. Precipitation behavior and phase transformation mechanism of super austenitic stainless steel S32654 during isothermal aging [J]. Materials Characterization, 2018, 137: 244–255. DOI: 10.1016/j.matchar.2018.01.040.