• 文献检索
  • 文档翻译
  • 深度研究
  • 学术资讯
  • Suppr Zotero 插件Zotero 插件
  • 邀请有礼
  • 套餐&价格
  • 历史记录
应用&插件
Suppr Zotero 插件Zotero 插件浏览器插件Mac 客户端Windows 客户端微信小程序
定价
高级版会员购买积分包购买API积分包
服务
文献检索文档翻译深度研究API 文档MCP 服务
关于我们
关于 Suppr公司介绍联系我们用户协议隐私条款
关注我们

Suppr 超能文献

核心技术专利:CN118964589B侵权必究
粤ICP备2023148730 号-1Suppr @ 2026

文献检索

告别复杂PubMed语法,用中文像聊天一样搜索,搜遍4000万医学文献。AI智能推荐,让科研检索更轻松。

立即免费搜索

文件翻译

保留排版,准确专业,支持PDF/Word/PPT等文件格式,支持 12+语言互译。

免费翻译文档

深度研究

AI帮你快速写综述,25分钟生成高质量综述,智能提取关键信息,辅助科研写作。

立即免费体验

Zr 基非晶合金射流的研究。

Research on non-cohesive jet formed by Zr-based amorphous alloys.

机构信息

School of Mechanical Engineering, Nanjing University of Science and Technology, Nanjing, 210094, People's Republic of China.

College of Field Engineering, Army Engineering University of PLA, Nanjing, 210007, People's Republic of China.

出版信息

Sci Rep. 2023 Mar 13;13(1):4149. doi: 10.1038/s41598-023-30836-0.

DOI:10.1038/s41598-023-30836-0
PMID:36914724
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10011371/
Abstract

The shaped charge jet formation of a Zr-based amorphous alloy and the applicability of different numerical algorithms to describe the jet formed were experimentally and numerically investigated. X-ray experiments were performed to study jet characteristics. The numerical results for the Zr-based amorphous alloy jet formed via the Euler and smooth particle hydrodynamics (SPH) algorithms were compared and analyzed using the Autodyn hydrocode. Particle motion was examined based on material properties. The Zr-based amorphous alloy formed a noncohesive jet driven by an 8701 explosive. Both the Euler and SPH algorithms achieved high accuracy for the determination of jet velocity. When the improved Johnson-Holmquist constitutive model (JH-2) was used, numerical results confirmed the model's suitability for the Zr-based amorphous alloy. The Euler algorithm effectively reflected jet shape within a short computing time, whereas the SPH algorithm was highly suitable for showing the shape of the jet tail within a long computing time. In the 3D Euler model, the flared jet mouth indicated radial particle dispersion; however, in the 2D model, particle dispersion in the head was directly observed by using the JH-2 material model. The brittle fracture of the material reduced the proportion of particles near the liner apex forming a jet. Furthermore, a new method in which stagnation pressure was used to predict jet formation and its coherence was proposed since the collapse angle was difficult to obtain.

摘要

采用实验和数值模拟的方法研究了 Zr 基非晶合金的聚能射流形成过程以及不同数值算法在描述射流形成过程中的适用性。采用 X 射线实验研究射流特性。利用 Autodyn 软件,对比并分析了 Zr 基非晶合金射流通过 Euler 和光滑粒子流体动力学(SPH)算法形成的数值结果。基于材料特性研究了颗粒运动。在 8701 炸药的驱动下,Zr 基非晶合金形成了无粘性射流。Euler 和 SPH 算法都能精确地确定射流速度。当使用改进的 Johnson-Holmquist 本构模型(JH-2)时,数值结果证实了该模型对 Zr 基非晶合金的适用性。Euler 算法在短计算时间内有效地反映了射流形状,而 SPH 算法在长计算时间内非常适合显示射流尾部的形状。在 3D Euler 模型中,喇叭形射流口表明了径向颗粒弥散;然而,在 2D 模型中,通过使用 JH-2 材料模型可以直接观察到头部的颗粒弥散。材料的脆性断裂减少了靠近衬垫顶点形成射流的颗粒比例。此外,由于难以获得坍塌角,提出了一种利用驻点压力预测射流形成及其连贯性的新方法。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/00454c80c341/41598_2023_30836_Fig21_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/f560093c356e/41598_2023_30836_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/dbcef9982069/41598_2023_30836_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/bd28378171f1/41598_2023_30836_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/4dabd8acad30/41598_2023_30836_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/31f445737e80/41598_2023_30836_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/3a5cfb1fdebb/41598_2023_30836_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/b26e48968d1a/41598_2023_30836_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/43130e68e263/41598_2023_30836_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/73bc91bd3011/41598_2023_30836_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/979798ca5e8c/41598_2023_30836_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/7a24521d79c8/41598_2023_30836_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/9d3964712564/41598_2023_30836_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/39b4c5e1a8ed/41598_2023_30836_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/fed2a42c2c08/41598_2023_30836_Fig14_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/dff3b21f3dec/41598_2023_30836_Fig15_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/3c55d478c2c7/41598_2023_30836_Fig16_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/d2da9884f02b/41598_2023_30836_Fig17_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/d03e59a73c8f/41598_2023_30836_Fig18_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/44b67e58a4d0/41598_2023_30836_Fig19_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/ea2dd305054d/41598_2023_30836_Fig20_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/00454c80c341/41598_2023_30836_Fig21_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/f560093c356e/41598_2023_30836_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/dbcef9982069/41598_2023_30836_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/bd28378171f1/41598_2023_30836_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/4dabd8acad30/41598_2023_30836_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/31f445737e80/41598_2023_30836_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/3a5cfb1fdebb/41598_2023_30836_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/b26e48968d1a/41598_2023_30836_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/43130e68e263/41598_2023_30836_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/73bc91bd3011/41598_2023_30836_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/979798ca5e8c/41598_2023_30836_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/7a24521d79c8/41598_2023_30836_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/9d3964712564/41598_2023_30836_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/39b4c5e1a8ed/41598_2023_30836_Fig13_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/fed2a42c2c08/41598_2023_30836_Fig14_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/dff3b21f3dec/41598_2023_30836_Fig15_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/3c55d478c2c7/41598_2023_30836_Fig16_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/d2da9884f02b/41598_2023_30836_Fig17_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/d03e59a73c8f/41598_2023_30836_Fig18_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/44b67e58a4d0/41598_2023_30836_Fig19_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/ea2dd305054d/41598_2023_30836_Fig20_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f8dd/10011371/00454c80c341/41598_2023_30836_Fig21_HTML.jpg

相似文献

1
Research on non-cohesive jet formed by Zr-based amorphous alloys.Zr 基非晶合金射流的研究。
Sci Rep. 2023 Mar 13;13(1):4149. doi: 10.1038/s41598-023-30836-0.
2
Formation and Penetration Properties of a Shaped Charge with ZrTiCuNiBe Liner.带有ZrTiCuNiBe药型罩的聚能装药的形成及侵彻特性
Nanomaterials (Basel). 2022 Nov 9;12(22):3947. doi: 10.3390/nano12223947.
3
Simulation Study on Expansive Jet Formation Characteristics of Polymer Liner.聚合物衬垫膨胀射流形成特性的模拟研究
Materials (Basel). 2019 Mar 4;12(5):744. doi: 10.3390/ma12050744.
4
Investigation of Penetration Performance of Zr-based Amorphous Alloy Liner Compared with Copper.锆基非晶合金内衬与铜的侵彻性能对比研究
Materials (Basel). 2020 Feb 19;13(4):912. doi: 10.3390/ma13040912.
5
Formation Behavior and Reaction Characteristic of a PTFE/Al Reactive Jet.聚四氟乙烯/铝反应射流的形成行为及反应特性
Materials (Basel). 2022 Feb 8;15(3):1268. doi: 10.3390/ma15031268.
6
Penetration and Cratering of Steel Target by Jets from Titanium Alloy Shaped Charge Liners.钛合金聚能装药药型罩射流对钢靶的侵彻与成坑
Materials (Basel). 2022 Jul 18;15(14):5000. doi: 10.3390/ma15145000.
7
Experimental and numerical study on micro-blasting process of 3A dental implant titanium alloy: A comparison between finite element method and smoothed particle hydrodynamics.3A 牙科种植体钛合金微喷砂工艺的实验与数值研究:有限元法与光滑粒子流体动力学的比较。
J Mech Behav Biomed Mater. 2022 Aug;132:105269. doi: 10.1016/j.jmbbm.2022.105269. Epub 2022 May 18.
8
Simulation Study on Jet Formability and Damage Characteristics of a Low-Density Material Liner.低密度材料药型罩射流可成型性与损伤特性的仿真研究
Materials (Basel). 2018 Jan 4;11(1):72. doi: 10.3390/ma11010072.
9
Study on the forming characteristics of polytetrafluoroethylene/copper jet with different preparation processes.不同制备工艺下聚四氟乙烯/铜射流形成特性的研究
Sci Rep. 2023 Sep 20;13(1):15659. doi: 10.1038/s41598-023-43053-6.
10
Study on Forming Law and Penetration of a Spherical Cone Composite Structure Liner Based on the Explosion Pressure-Coupling Constraint Principle.基于爆炸压力耦合约束原理的球锥复合结构药型罩成型规律及侵彻研究
Materials (Basel). 2022 Jul 7;15(14):4750. doi: 10.3390/ma15144750.

本文引用的文献

1
Compressive Behavior of (CuZrAl)Dy Bulk Metallic Glass at Different Strain Rates.不同应变速率下(CuZrAl)Dy块体金属玻璃的压缩行为
Materials (Basel). 2020 Dec 21;13(24):5828. doi: 10.3390/ma13245828.
2
Structural rearrangements that govern flow in colloidal glasses.控制胶体玻璃中流动的结构重排。
Science. 2007 Dec 21;318(5858):1895-9. doi: 10.1126/science.1149308.
3
A universal criterion for plastic yielding of metallic glasses with a (T/Tg) 2/3 temperature dependence.一种具有(T/Tg)2/3温度依赖性的金属玻璃塑性屈服通用准则。
Phys Rev Lett. 2005 Nov 4;95(19):195501. doi: 10.1103/PhysRevLett.95.195501. Epub 2005 Nov 3.