压剪联合冲击下K9玻璃中的失效波

对K9玻璃进行了冲击速度为150~400 m/s,倾斜角为10、15的纵剖试样斜撞击实验。结果表明,在加载剪切横波(S+)和卸载纵波(P-)之间有波速超过了纵波波速的波阵面存在,此波的存在对卸载纵波和卸载横波的幅值有一定的影响。由于失效波的产生与材料的表面性质密切相关,为消除纵剖试样中间界面的影响,模拟VISAR的实验条件,进行了冲击速度为70~300 m/s、倾斜角为10的横剖试样斜撞击实验。可以确定在此冲击范围失效波的波速在0.98~1.4 km/s,产生失效波的临界状态为：压应力0.86~1.01 GPa,对应剪应力0.053~0.071 GPa。表明剪应力的存在极大降低了失效波产生的阈值。在此基础上初步分析了撞击面的动摩擦因数和相对滑移速度。     

冲击压缩下氧化铝陶瓷中破坏阵面的传播

进行了平面冲击波压缩下氧化铝陶瓷中破坏阵面的实验测试和理论探索. 通过氧 化铝陶瓷的平板碰撞实验,借助VISAR测试系统测量了试件自由面的质点速度历程,并对回 收试件进行了电镜扫描观察. 质点自由面速度历程曲线表明,氧化铝陶瓷材料中存在破坏阵 面的传播. 考察了破坏阵面的传播特性,给出了陶瓷材料的动态破坏模型,并对破坏阵面的 传播进行了数值分析.     

PVC夹芯板在冲击载荷下的动态响应与失效模式

通过开展对泡沫金属子弹撞击加载聚氯乙烯(polyvinyl chloride, PVC)夹芯板的实验,结合三维数字图像相关性(three dimensional digital image correlation, DIC-3D)技术,研究固支夹芯板在撞击加载条件下的动态响应,获得夹芯板受撞击及响应的变形过程,并结合图像分别分析夹芯板整体及三层结构的变形和失效模式;研究子弹冲量与背板最终变形之间的关系和相似冲量下等面密度不同芯层密度的夹芯结构的抗撞击性能。结果表明:夹芯板的破坏和失效主要集中在泡沫金属子弹直接作用区域,背板挠度由中间向固定端逐渐减小,子弹冲量与背板变形近似成线性关系。在等质量的条件下,降低芯层密度、增加芯层厚度可以有效降低背板的变形,实验结果对聚合物夹芯结构的工程优化设计具有一定的参考意义。     

压剪复合冲击下氧化铝陶瓷的剪切响应实验研究

通过对92.93%氧化铝陶瓷进行倾斜板碰撞实验,研究了多晶陶瓷材料在压剪复合冲击下的非弹性变形响应和剪切波传播规律。压剪复合冲击实验由57 mm开槽气体炮驱动铜飞片对陶瓷靶板加载,通过试件内埋植的电磁速度计来测量内部质点速度历程。将纵向粒子速度从感应电动势曲线中分离后得到横向粒子速度历程,发现在压剪复合冲击下由于材料剪切刚度的降低而引起的剪切波衰减。冲击软回收试件的扫描电子显微镜（SEM）观察表明,冲击载荷低于屈服强度时,多晶氧化铝陶瓷中存在沿晶界、气孔的微裂纹成核与扩展,在高于屈服强度的冲击加载下进一步产生了穿晶微裂纹,微裂纹系统导致了材料在卸载后的显著的体积膨胀。     

Finite deformations of Ogden's materials under impact loading

The present paper is devoted to the modeling of finite deformations of a hyperelastic body described by Ogden's model under contact/impact conditions. Frictional contact problems are solved by means of the bi-potential method. The first order algorithm is applied to integrate the equation of motion. The total Lagrangian formulation is adopted to describe the geometrically non-linear behavior. For the finite element implementation, the explicit expression of the tangent operator is derived including the case of repeated eigenvalues. A numerical example is given to illustrate efficiency and accuracy of the method.     

平板撞击下C30混凝土中冲击波的传播特性

采用1级气炮加载技术和锰铜应力计多点测试技术,开展了C30混凝土在平板撞击条件下的冲击压缩实验研究。基于锰铜应力计实测的应力波形,研究了混凝土中冲击波的传播特性,结果显示冲击波的应力峰值随传播距离呈现明显的衰减特性,衰减过程可分为2个阶段。在早期阶段,卸载波没有赶上前面传播的冲击波,冲击波应力峰值衰减较慢,主要是混凝土材料的本构粘性效应所引起的;而后期阶段应力峰值的快速衰减则归因于混凝土材料的本构粘性效应、后续的来自飞片自由面的反射波追赶卸载、边侧稀疏波卸载及波传播的几何弥散效应的共同作用;另外,冲击波在混凝土中传播的升时也随着传播距离逐渐增大,即由强间断波逐渐转化为弱间断波。     

A DAMAGE ACCUMULATING MODELING OF FAILURE WAVES IN GLASS UNDER HIGH VELOCITY IMPACT

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Nonstationary deformation of an elastic plate with a notch under the action of a shock wave

The behavior of a thin elastic plate with a rectilinear notch under the action a weak shock wave in air is studied experimentally. A technique is developed for this purpose. The effect of the notch on the strain state of the plate is analyzed __________ Translated from Prikladnaya Mekhanika, Vol. 43, No. 11, pp. 99–104, November 2007.     

粘结单元在模拟FRP层合板低速冲击响应中的应用

纤维增强树脂基复合材料层合板(fibre reinforced plastic composites,FRP)在航空、航天、交通、造船等诸多工程中得到了日益广泛的应用,而其在冲击载荷下的响应和破坏特别是分层一直为学术界所关注。本文中对FRP层合板在冲击载荷下的响应和破坏进行数值模拟,并通过引入粘结层重点研究其分层破坏。首先,介绍一种基于改进的粘结区域方法的粘结层损伤模型;其次,详细介绍了有限元模型建模过程和建模细节;最后,对有限元模型进行验证,并分析分层损伤发生的原因。模拟结果表明,该模型不仅能准确预测FRP层合板在低速冲击载荷下的载荷-时间曲线和载荷-位移曲线,还能成功地预测其分层破坏。     

工程陶瓷引弧微爆炸加工冲击力建模及实验分析

介绍了引弧微爆炸加工过程中冲击力产生的原因,利用单因素实验确定影响冲击力的主要工艺参数,利用正交实验和回归分析的方法建立了冲击力指数型经验模型,得出工艺参数对冲击力的影响规律。实验结果表明:工作电流、工作气压和微爆炸发生器喷嘴直径是影响冲击力大小的主要工艺参数,冲击力随着工作电流的增大而减小,随着工作气压和喷嘴直径的增大而增大,而工作脉宽和工作距离对冲击力大小影响不显著;建立的冲击力模型与实验结果吻合良好。研究结果可以为引弧微爆炸加工过程的控制提供参考依据。     

侧向撞击荷载作用下内八边形空心钢筋混凝土柱的动力响应

相比于实心钢筋混凝土柱,空心钢筋混凝土柱具有自重轻和截面扩展好等优点,被广泛地用作桥墩,由此其不可避免地会受到船舶的撞击。本文中进行6根内八边形空心钢筋混凝土柱和4根内衬八边形钢管空心钢筋混凝土柱的动力响应的实验。在实验中记录了构件破坏形态、撞击力时程曲线和跨中位移时程曲线,并从撞击高度、边界条件和钢板厚度等方面分析了构件的耐撞性能。结果表明:内八边形钢筋混凝土柱和内衬八边形钢管空心钢筋混凝土柱在撞击荷载作用下的破坏形态主要分为两种破坏类型,分别为局部型破坏和整体型破坏;撞击高度越大构件破坏越严重;两端固定对构件的耐撞击性能有提升作用;钢管厚度对构件的耐撞击性能有较明显的提升作用。     

Failure loads of spot weld specimens under impact opening and shear loading conditions

Failure loads of spot weld specimens are investigated under impact combined loading conditions. A set of test fixtures was designed and used to obtain failure loads of mild steel spot weld specimens under combined opening and shear loading conditions. Three different impact speeds were applied to examine the effects of separation speed on failure loads. Micrographs of the cross-sections of failed spot welds were obtained to understand the failure processes in mild steel specimens under different impact combined loads. The experimental results indicate that the failure mechanisms of spot welds are very similar for mild steel specimens at various impact speeds. These micrographs show that the sheet thickness can affect the failure mechanisms. For 1.0 mm specimens, the failure occurs near the base metal in a necking/shear failure mode. For 1.5 mm specimens, the failure occurs near the heat-affected zone in a shear failure mode. Based on the experimental results, the effects of the inertia force, the separation speed, and the loading angle on the failure loads of spot welds are investigated. Failure criteria are proposed to characterize the failure loads of spot welds under impact combined opening and shear loads for engineering applications. The failure load can be expressed as a function of the tensile strength of the base metal, the nugget size, the sheet thickness, the maximum separation speed, the loading angle, and empirical coefficients for a given welding schedule.     

非均匀泡沫金属材料在冲击载荷下的变形模拟

提出一种二维非线性弹塑性质量-弹簧-连杆模型,该模型将泡沫金属材料离散成许多质量块,质量块在受载方向由非线性弹塑性弹簧连接,垂直于受载方向由可延伸的弹性连杆铰接。采用该模型模拟并分析了层非均匀泡沫金属材料及局部不均匀泡沫金属材料在冲击载荷下的变形特性,说明了非均匀性对泡沫金属材料冲击变形的影响。     

Al2O3陶瓷动静态压缩下碎片形貌与破坏机理分析

为探究Al₂O₃陶瓷的宏观力学响应与破坏机理,分别利用材料试验机和分离式霍普金森压杆对其进行准静态和动态压缩实验,同时通过原位光学成像观测试样的破坏过程,并利用同步辐射CT和扫描电镜（SEM）对回收碎片的尺寸和形状以及微观破坏模式进行表征分析。宏观强度数据表明,Al₂O₃陶瓷的抗压强度符合Weibull分布,且与加载应变率呈现指数增长关系。原位光学成像和SEM回收分析共同揭示了动静态加载下裂纹成核与扩展模式存在明显差异。准静态加载时材料微观上更易发生沿晶断裂,宏观表现为劈裂裂纹较少,且倾向于沿加载方向传播并贯穿整个试样;而动态加载时穿晶断裂占主导地位,劈裂裂纹明显增加并发生相互作用,因此在传播过程中容易分叉而形成大量次生裂纹,提高了试样内裂纹密度。这与碎片的CT表征结果一致,即碎片平均球形度和伸长、扁平指数等均随应变率对数线性增加。破坏模式的改变最终导致高应变率下陶瓷材料应变率敏感性显著增强。

     

Dynamics of stress wave propagation in a chain of photoelastic discs impacted by a planar shock wave; Part I, experimental investigation

The propagation of stress waves through a chain of discs has been studied experimentally. Optically transparent 20-mm diameter discs, made of epoxy, were loaded dynamically by head-on collision with an incident planar shock wave. The loading was done in a vertical shock tube. The head-on collision between the punch-plate, placed on top of the chain of discs, and the incident shock wave resulted in a head-on reflected shock wave inducing behind it a fairly uniform step-wise pressure pulse having duration of about 6 ms. The recorded fringe patterns of the stress field, in the discs-chain, show that the input pressure pulse was broken into several oscillating cycles. The back and forth bouncing of stress waves gave rise to two different modes of the contact stress oscillations, which continued until the overall stress reaches equilibrium with the input conditions. The registered propagation velocity of the stress wave was significantly lower than the appropriate speed of sound in the material from which the discs were made.      

Dynamics of stress wave propagation in a chain of photoelastic discs impacted by a planar shock wave: Part II, numerical investigation

The propagation of stress waves through a chain of discs has been studied experimentally in Part I (Glam et al. [1]) and is completed here with numerical investigation using the standard package ABAQUS. A fair agreement is found between experimental findings and their simulations. Based on this agreement, parametric study of wave propagation through disc-chains was conducted. Specifically, effects associated with changes in the disc diameter, material density, stiffness/rigidity and the number of discs in the chain on the stressed chain have been studied. It was found that the propagation velocity of the evolved waves increases with improving contacts between the chain’s discs by exposing the chain to a static load before its dynamic loading. The wave- propagation velocity decreases with increase in the discs material density and it increases when its diameter increases. In case of a chain composed of small diameter discs and/or small material density, the transmitted stress wave is first strengthened and only at discs further down the chain it starts decaying. When checking the influence of the dynamic-loading duration it was found that long dynamic-load duration dissolves quickly into short pulses. It was also found that there is a ‘characteristic’ wave for a given chain. This wave propagates with minimal dispersion. Dynamic loads having shorter time duration than the ‘characteristic’ one experiences significant attenuation.     

高速破片撞击充液容器时容器壁面的损伤

为研究高速破片(钨球)撞击充液容器(贯穿前后壁面)时容器壁面的毁伤情况,利用ANSYS/LSDYNA对该过程进行了数值模拟,分析了破片撞击动能对充液容器前后壁面毁伤程度的影响,并进行实验验证。结果表明:高速破片撞击充液容器形成的液压水锤对充液容器前后壁面的破坏程度可分为3个等级,即前后壁面均未出现裂纹、前壁面没有出现裂纹后壁面出现裂纹和前后壁面均出现裂纹且后壁面呈花瓣式开裂;破片撞击充液容器过程中,前后壁面的最大变形量和前后壁面的裂纹总数随破片撞击动能的增加而增大。     

爆炸荷载作用下钢筋混凝土梁的动力响应及破坏形态分析

对基于Timoshenko梁理论建立的非线性动力有限元法作了改进。根据压区理论得到混凝土的平均剪应力和平均剪应变关系,建立了能反映箍筋的抗剪作用的材料模型;此外,对结构在爆炸荷载作用下可能出现的各种响应现象进行了描述,以准确地预测梁破坏时不同位置截面上钢筋和混凝土的受力、变形及破坏情况。应用改进的材料模型,对爆炸荷载作用下的五个钢筋混凝土试验梁的动力响应和破坏形态进行了数值模拟,结果表明,该数值方法能较好地模拟钢筋混凝土梁的弯曲、弯剪和剪切等破坏形态。     

基于DIC技术的爆炸应力波过异质界面应变场演化规律实验研究

采用氯仿粘结聚碳酸酯（polycarbonate, PC）板和聚甲基丙烯酸甲酯（polymethylmethacrylate, PMMA）板模拟含异质界面模型;在PC介质中布置柱状炮孔并与界面呈一定角度,根据炮孔端部与界面相对位置,分别于柱状炮孔两个端部设置起爆点,起爆点远离界面端部时定义为孔口起爆,靠近界面端部时定义为孔底起爆;借助数字图像相关实验系统,研究爆炸应力波通过异质界面后PMMA介质应变场演化过程及炮孔底部区域拉、压应变变化规律。实验结果表明,异质界面改变了爆炸应力波过界面后的传播形态。孔口起爆时,异质界面受爆破荷载作用后易形成应力集中区,界面处产生开裂,横向拉伸波作用是造成异质界面开裂的主要原因。起爆方式对过界面后介质PMMA的横/纵向拉、压应变场作用贡献不同,主要体现在应变场强度、拉/压应变场位置分布2个方面。在炮孔底部区域,起爆方式对应变场时程特性的影响主要体现在作用时效长短和应变强度2个方面。孔口起爆时,横/纵向应变体现出短时效、高强度的变化特征。就应变强度而言,起爆方式对横向压应变的影响显著强于其对纵向拉应变的影响。对空间分布特性影响主要体现在衰减程度,起爆方式对纵向应变衰减程度影响较大。无论采用何种起爆方式,爆炸应变场在PC介质中衰减速度较快,进入PMMA介质后衰减速度显著降低。

     

金属薄板在圆锥头弹体正冲击下的破裂模式

临界破裂速度下（圆板产生破裂的最小速度）,对四种不同材料的薄金属圆板在不同圆锥半角的圆锥头子弹正冲击下的破裂模式进行了试验。研究发现随着圆锥半角的增加,板的破裂模式分别有刺透型、花瓣型和剪切型。通过试验分析,建立了在不同圆锥头子弹以临界破裂速度正冲击下,金属薄板的破裂模式和子弹圆锥半角及金属薄板材料性能的关系。分析中考虑了子弹和板壁接触区域内的局部变形,给出一临界圆锥半角c=arcsin exp(-0.5f)(f是金属薄板材料的真实破裂应变）。由此得到：临界破裂速度正冲击下,圆锥半角30时,薄板破裂由子弹直接刺透板壁引起;＞c且30时,薄板破裂模式是剪切型;当 30＜＜c时,薄板破裂模式是花瓣型。