金属高速斜碰撞的观测

A. Mori
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Introduction Explosive welding technique is known well as the welding method to weld strongly for the two metal plates of similar and/or dissimilar material combinations. In explosive welding technique, a metal flyer plate is accelerated by the detonation of explosive and is collided to another metal plate (base plate) with a certain angle at high velocity. A good welding is achieved with generating the interfacial waves in the welded interface and the metal jet at the collision point when the velocity and the angle collided are within the suitable range [1, 2]. Therefore, to achieve the optimal welding conditions for the difficult-to-weld materials, it is necessary to know the parameters and the collision phenomena, such as the metal jet generations and the interfacial waves. The mechanism of interfacial waves and the metal jet generation have been studied theoretically and/or numerically by many researchers [3-5]. Onzawa et al. [6] reported about the characteristics of metal jet generated by the collision of similar and dissimilar metals set on parallel and angular arrangement using a high-speed streak camera. The observation for the metal jet generation is difficult by the optical observation system because the detonation gas spreads out rapidly with the high velocity which is faster than the flying velocity of metal. From the weldability window proposed by Wittman [7] and Deribas [8], claddings same as explosive welding can be obtained when a metal plate collides obliquely at high velocity. To know the inclined collision, same as the phenomena of explosive welding, a powder gun was applied to observe the high-speed oblique collision, which is same as the phenomena of explosive welding, without the influence of detonation gas. And the numerical simulation using SPH solver in ANSYS AUTODYN software was used to understand the material behavior in the high-speed oblique collision, comparing with the experimental results. Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 74-78 https://doi.org/10.21741/9781644900338-13 75 Experimental Procedure Experimental setup to observe the high-speed oblique collision is shown in Figure 1. A powder gun set on Institute of Pulsed Power Science in Kumamoto University was used to accelerate the metal plate. A pure copper and magnesium alloy AZ31, which diameter were 32 mm and thickness was 3 mm or 5 mm, were applied as the flyer and target plate. The flyer plate was combined the sabot made by Ultra high molecular weight polyethylene (UHPE) as the projectile. The projectile was set in the barrel of the powder chamber side. The copper weight-control plate was placed behind the flyer plate to control the flying velocity of projectile. The target plate put into a PMMA target holder was arranged on the target stand with an inclined angle (θ = 7, 10, 15, 20) in the target chamber. For the optical observation of the oblique collision, High-speed video camera (HPV-1, Shimadzu corp., capable of recording up to 1 million fps) was placed at the side of the target chamber and was located in the opposite side of the light across the target chamber. Smokeless and the black gunpowder were set in the powder chamber. After the target chamber was in a vacuum, the black gunpowder was ignited. Numerical Analysis Explicit dynamics software ANSYS AUTODYN was used and the 2-dimensional planer symmetry was applied to know the detail of the oblique collision at high velocity numerically. A target plate and a projectile were modeled by two solvers, which were the Smoothed Particle Hydrodynamics (SPH) solver and the Lagrangian solver. The 60% thickness part on the collision side of the metal plate was modeled by the SPH solver, and the remaining 40% was applied by the Lagrangian. The particle size of SPH solver and the mesh size of Lagragian solver were fixed at 0.05 mm and 0.03 mm when the thickness of metal plates was 5 mm and 3 mm respectively. The Mie-Grüneisen form shock equation of stat and the Johnson-Cook strength model were applied for each material. The material parameters for each equation are referred from the reports [9, 10]. 6000 mm Flyer metal plate Trigger pin φ32 mm φ40 mm Sabot Barrel Target plate Target holder Target stand θ Controller High-speed video camera Light","PeriodicalId":415881,"journal":{"name":"Explosion Shock Waves and High Strain Rate Phenomena","volume":"136 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Observation for the High-Speed Oblique Collision of Metals\",\"authors\":\"A. Mori\",\"doi\":\"10.21741/9781644900338-13\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In explosive welding, it is known well that the collision angle and collision velocity are the important parameters to achieve good welding. In addition, generations of a metal jet and the interfacial waves are important for the explosive welding conditions. To know the parameters and the collision conditions, the optical observation and the numerical simulation for the oblique collision using a powder gun were done by the authors. A metal jet was observed clearly by using a powder gun and wavy interface was generated without the intermetallic layer for the reactive materials by controlling the welding conditions. In this investigation, the results of the optical observations and the numerical analysis for similar and dissimilar material combinations were reported. Introduction Explosive welding technique is known well as the welding method to weld strongly for the two metal plates of similar and/or dissimilar material combinations. In explosive welding technique, a metal flyer plate is accelerated by the detonation of explosive and is collided to another metal plate (base plate) with a certain angle at high velocity. A good welding is achieved with generating the interfacial waves in the welded interface and the metal jet at the collision point when the velocity and the angle collided are within the suitable range [1, 2]. Therefore, to achieve the optimal welding conditions for the difficult-to-weld materials, it is necessary to know the parameters and the collision phenomena, such as the metal jet generations and the interfacial waves. The mechanism of interfacial waves and the metal jet generation have been studied theoretically and/or numerically by many researchers [3-5]. Onzawa et al. [6] reported about the characteristics of metal jet generated by the collision of similar and dissimilar metals set on parallel and angular arrangement using a high-speed streak camera. The observation for the metal jet generation is difficult by the optical observation system because the detonation gas spreads out rapidly with the high velocity which is faster than the flying velocity of metal. From the weldability window proposed by Wittman [7] and Deribas [8], claddings same as explosive welding can be obtained when a metal plate collides obliquely at high velocity. To know the inclined collision, same as the phenomena of explosive welding, a powder gun was applied to observe the high-speed oblique collision, which is same as the phenomena of explosive welding, without the influence of detonation gas. And the numerical simulation using SPH solver in ANSYS AUTODYN software was used to understand the material behavior in the high-speed oblique collision, comparing with the experimental results. Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 74-78 https://doi.org/10.21741/9781644900338-13 75 Experimental Procedure Experimental setup to observe the high-speed oblique collision is shown in Figure 1. A powder gun set on Institute of Pulsed Power Science in Kumamoto University was used to accelerate the metal plate. A pure copper and magnesium alloy AZ31, which diameter were 32 mm and thickness was 3 mm or 5 mm, were applied as the flyer and target plate. The flyer plate was combined the sabot made by Ultra high molecular weight polyethylene (UHPE) as the projectile. The projectile was set in the barrel of the powder chamber side. The copper weight-control plate was placed behind the flyer plate to control the flying velocity of projectile. The target plate put into a PMMA target holder was arranged on the target stand with an inclined angle (θ = 7, 10, 15, 20) in the target chamber. For the optical observation of the oblique collision, High-speed video camera (HPV-1, Shimadzu corp., capable of recording up to 1 million fps) was placed at the side of the target chamber and was located in the opposite side of the light across the target chamber. Smokeless and the black gunpowder were set in the powder chamber. After the target chamber was in a vacuum, the black gunpowder was ignited. Numerical Analysis Explicit dynamics software ANSYS AUTODYN was used and the 2-dimensional planer symmetry was applied to know the detail of the oblique collision at high velocity numerically. A target plate and a projectile were modeled by two solvers, which were the Smoothed Particle Hydrodynamics (SPH) solver and the Lagrangian solver. The 60% thickness part on the collision side of the metal plate was modeled by the SPH solver, and the remaining 40% was applied by the Lagrangian. The particle size of SPH solver and the mesh size of Lagragian solver were fixed at 0.05 mm and 0.03 mm when the thickness of metal plates was 5 mm and 3 mm respectively. The Mie-Grüneisen form shock equation of stat and the Johnson-Cook strength model were applied for each material. 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引用次数: 1

摘要

在爆炸焊接中,碰撞角和碰撞速度是实现良好焊接的重要参数。此外,金属射流和界面波的生成对爆炸焊接条件也有重要影响。为了了解这些参数和碰撞条件,作者进行了用粉末枪进行斜碰撞的光学观测和数值模拟。用粉末枪观察到明显的金属射流,通过控制焊接条件,反应材料形成无金属间层的波浪形界面。本文报道了相似和不同材料组合的光学观测和数值分析结果。爆炸焊接技术是一种将相似或不同材料组合的两块金属板进行强焊接的焊接方法。在爆炸焊接技术中,金属飞片受炸药的爆炸加速,以一定的速度与另一金属板(底板)形成一定角度的碰撞。当碰撞速度和碰撞角度在适当范围内时,在焊接界面产生界面波,在碰撞点产生金属射流,即可获得良好的焊接效果[1,2]。因此,为了实现难焊材料的最佳焊接条件,有必要了解金属射流生成和界面波等参数和碰撞现象。界面波和金属射流产生的机理已经被许多研究者从理论上和/或数值上进行了研究[3-5]。Onzawa等人[6]利用高速条纹相机研究了相似金属和异种金属在平行和角度排列时碰撞产生的金属射流特性。由于爆轰气体扩散速度快于金属的飞行速度,光学观测系统对金属射流产生的观测存在一定的困难。根据Wittman[7]和der[8]提出的可焊性窗口,在金属板高速斜碰撞时,可以得到与爆炸焊接相同的熔覆层。为了了解与爆炸焊接现象相同的倾斜碰撞,在没有爆轰气体影响的情况下,使用粉末枪观察与爆炸焊接现象相同的高速倾斜碰撞。利用ANSYS AUTODYN软件中的SPH求解器进行数值模拟,了解材料在高速斜碰撞中的行为,并与实验结果进行对比。爆炸冲击波与高应变率现象材料研究论坛LLC材料研究学报第13期(2019)74-78 https://doi.org/10.21741/9781644900338-13 75实验步骤观察高速斜碰撞的实验装置如图1所示。利用熊本大学脉冲功率研究所的粉末炮对金属板进行加速。采用直径为32 mm,厚度为3 mm或5 mm的纯铜镁合金AZ31作为飞片和靶板。飞行板是将超高分子量聚乙烯(UHPE)制成的弹丸结合在一起的。弹丸被设置在火药室一侧的枪管中。在飞片后放置铜重量控制板,控制弹丸的飞行速度。将装入PMMA靶架的靶板以倾斜角度(θ = 7、10、15、20)布置在靶室的靶架上。为了对倾斜碰撞进行光学观察,高速摄像机(HPV-1,岛足公司,能够记录高达100万帧/秒)被放置在目标室的一侧,位于穿过目标室的光线的另一侧。无烟火药和黑火药被放置在火药室里。在靶室处于真空状态后,点燃黑火药。采用显式动力学软件ANSYS AUTODYN,采用二维平面对称性对高速斜碰撞的细节进行数值分析。采用光滑粒子流体力学(SPH)和拉格朗日求解器对靶板和弹体进行了建模。金属板碰撞侧60%厚度部分采用SPH求解器建模,其余40%厚度部分采用拉格朗日量求解。当金属板厚度为5 mm和3 mm时,SPH求解器的粒径和Lagragian求解器的孔径分别固定为0.05 mm和0.03 mm。对每种材料采用了mie - grig - neisen形式的冲击方程和Johnson-Cook强度模型。各方程的材料参数参考文献[9,10]。 6000mm飞翼金属板扳机销φ 32mm φ 40mm炮管靶板靶架靶架θ控制器高速摄像机灯
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Observation for the High-Speed Oblique Collision of Metals
In explosive welding, it is known well that the collision angle and collision velocity are the important parameters to achieve good welding. In addition, generations of a metal jet and the interfacial waves are important for the explosive welding conditions. To know the parameters and the collision conditions, the optical observation and the numerical simulation for the oblique collision using a powder gun were done by the authors. A metal jet was observed clearly by using a powder gun and wavy interface was generated without the intermetallic layer for the reactive materials by controlling the welding conditions. In this investigation, the results of the optical observations and the numerical analysis for similar and dissimilar material combinations were reported. Introduction Explosive welding technique is known well as the welding method to weld strongly for the two metal plates of similar and/or dissimilar material combinations. In explosive welding technique, a metal flyer plate is accelerated by the detonation of explosive and is collided to another metal plate (base plate) with a certain angle at high velocity. A good welding is achieved with generating the interfacial waves in the welded interface and the metal jet at the collision point when the velocity and the angle collided are within the suitable range [1, 2]. Therefore, to achieve the optimal welding conditions for the difficult-to-weld materials, it is necessary to know the parameters and the collision phenomena, such as the metal jet generations and the interfacial waves. The mechanism of interfacial waves and the metal jet generation have been studied theoretically and/or numerically by many researchers [3-5]. Onzawa et al. [6] reported about the characteristics of metal jet generated by the collision of similar and dissimilar metals set on parallel and angular arrangement using a high-speed streak camera. The observation for the metal jet generation is difficult by the optical observation system because the detonation gas spreads out rapidly with the high velocity which is faster than the flying velocity of metal. From the weldability window proposed by Wittman [7] and Deribas [8], claddings same as explosive welding can be obtained when a metal plate collides obliquely at high velocity. To know the inclined collision, same as the phenomena of explosive welding, a powder gun was applied to observe the high-speed oblique collision, which is same as the phenomena of explosive welding, without the influence of detonation gas. And the numerical simulation using SPH solver in ANSYS AUTODYN software was used to understand the material behavior in the high-speed oblique collision, comparing with the experimental results. Explosion Shock Waves and High Strain Rate Phenomena Materials Research Forum LLC Materials Research Proceedings 13 (2019) 74-78 https://doi.org/10.21741/9781644900338-13 75 Experimental Procedure Experimental setup to observe the high-speed oblique collision is shown in Figure 1. A powder gun set on Institute of Pulsed Power Science in Kumamoto University was used to accelerate the metal plate. A pure copper and magnesium alloy AZ31, which diameter were 32 mm and thickness was 3 mm or 5 mm, were applied as the flyer and target plate. The flyer plate was combined the sabot made by Ultra high molecular weight polyethylene (UHPE) as the projectile. The projectile was set in the barrel of the powder chamber side. The copper weight-control plate was placed behind the flyer plate to control the flying velocity of projectile. The target plate put into a PMMA target holder was arranged on the target stand with an inclined angle (θ = 7, 10, 15, 20) in the target chamber. For the optical observation of the oblique collision, High-speed video camera (HPV-1, Shimadzu corp., capable of recording up to 1 million fps) was placed at the side of the target chamber and was located in the opposite side of the light across the target chamber. Smokeless and the black gunpowder were set in the powder chamber. After the target chamber was in a vacuum, the black gunpowder was ignited. Numerical Analysis Explicit dynamics software ANSYS AUTODYN was used and the 2-dimensional planer symmetry was applied to know the detail of the oblique collision at high velocity numerically. A target plate and a projectile were modeled by two solvers, which were the Smoothed Particle Hydrodynamics (SPH) solver and the Lagrangian solver. The 60% thickness part on the collision side of the metal plate was modeled by the SPH solver, and the remaining 40% was applied by the Lagrangian. The particle size of SPH solver and the mesh size of Lagragian solver were fixed at 0.05 mm and 0.03 mm when the thickness of metal plates was 5 mm and 3 mm respectively. The Mie-Grüneisen form shock equation of stat and the Johnson-Cook strength model were applied for each material. The material parameters for each equation are referred from the reports [9, 10]. 6000 mm Flyer metal plate Trigger pin φ32 mm φ40 mm Sabot Barrel Target plate Target holder Target stand θ Controller High-speed video camera Light
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