SHPB混凝土实验中试件尺寸的影响（英文）

分离式霍普金森压杆(SHPB)实验常被用来获得混凝土类材料的动态压缩强度,所得数据对建立本构方程有重要作用,因此需要对其进行正确解释或分析。利用最新的混凝土材料模型研究了SHPB实验中试件尺寸的影响。藉由混凝土试件的体积考虑动态尺寸效应的影响,并提出了一个计算由于惯性(约束)效应引起的动态增强因子的新经验公式。结果表明:新经验公式与不同尺寸混凝土的SHPB模拟结果吻合得很好,且惯性(约束)效应引起的动态增强因子随着试件尺寸的增大而增大。     

混凝土类材料在SHPB实验中惯性效应的数值模拟研究（英文）

分离式霍普金森压杆(SHPB)被广泛应用于测试混凝土类材料在高应变率(10~103 s-1)下的动态增强效应。为更好地理解这类问题,进行了数值模拟研究,采用J2本构模型研究SHPB试验中的纵向惯性效应,线性Drucker-Prager模型研究SHPB试验中的径向惯性效应。研究结果表明:纵向惯性效应不影响动态增强因子;径向惯性效应对动态增强因子有影响,但不是混凝土类材料在高应变率下动态增强因子提高的最主要原因。     

高温SHPB冲击实验技术及其应用

 为研究高温下材料的动态力学性能,研制了一套适用于分离式霍普金森压杆（Split Hopkinson Pressure Bar,SHPB）高温冲击实验的温控系统。利用该温控系统和Φ100 mm常规SHPB装置,对混凝土在高温下的动态力学性能进行了实验研究,实验温度分别为20、200、400、600、800和1 000 ℃。结果表明：由管式实时加热装置和箱式预加热炉组成的温控系统操作方便,实验效率高,试件组装方法简便可行;热传导导致的试件温度分布不均匀和压杆局部温升对实验结果产生的影响可以忽略,实验技术可靠;高温下混凝土动态力学性能的温度效应十分明显,相同冲击速率下,随温度升高,平均应变率逐渐增大,动态应力-应变曲线逐渐表现出塑性特性,动态抗压强度随温度升高先增大后减小,动态峰值应变随温度升高不断增大。     

无机玻璃动态压缩破坏的离散元模拟

利用离散元软件PFC~(2D)(Particle Flow Code)建立了分离式霍普金森压杆(SHPB)系统,模拟了无机玻璃圆柱和圆盘试件在冲击压缩下的动态力学行为和失效破坏模式。结果表明:无机玻璃作为典型的脆性材料,其抗压强度具有明显的应变率效应,而杨氏模量则对应变率不敏感;无机玻璃圆柱的破坏过程受纵向压力、端面摩擦力以及横向惯性力的影响,初期微裂纹呈三角状分布,随着纵向应力水平的提高,出现明显的泊松效应,产生横向张应力,致使微裂纹沿纵向扩展,最终试件发生沿轴向的劈裂断裂;摩擦系数和泊松比对试件破坏模式及强度有一定影响。将建立的SHPB数值实验平台用于模拟无机玻璃巴西圆盘试验,揭示了圆盘发生中心开裂的拉伸特征及拉伸强度的应变率相关性。     

气垫导轨上的磁阻尼效应实验

为了克服摩擦力对运动磁体与非磁性导体相互作用产生的磁阻尼效应的影响,在铝合金气垫导轨上进行磁阻尼效应实验,推导了相互作用过程中各物理量间的解析关系,并运用自己开发的专用实验设备,获得了与理论推导一致的实验结果.     

基于地质聚合物混凝土的SHPB实验参数控制

为有效地测试地质聚合物混凝土的冲击力学特性,以矿渣、粉煤灰为原材料,制备了高流态的C30地质聚合物混凝土,探索了此类混凝土的霍普金森压杆(SHPB)实验技术参数的控制规律,得到了射弹速度、整形器直径与最佳近似恒应变率之间的关系。结果表明:波形整形技术消除了波形振荡现象,有效地降低了弥散效应;整形后应力波形的前沿升时远远高于传统矩形波的前沿升时,保证了应力的均匀性;通过组合控制射弹速度和整形器直径,实现了恒应变率加载。     

高温高应变率下混凝土材料的损伤演化方程

采用?74 mm大口径分离式霍普金森压杆(SHPB)对不同温度(20、200、400℃)下的C45混凝土材料进行动态力学性能实验,得到了不同温度、不同应变率下混凝土材料的应力-应变曲线。实验结果表明:在20~400℃温度范围内,混凝土材料具有温度硬化和应变率硬化现象。基于上述实验数据给出了损伤变量关于塑性应变的关系式,并通过相关实验数据确定了不同温度、不同应变率下损伤演化方程的材料参数。将该损伤演化方程应用于混凝土材料的本构关系中,预测结果与实验数据具有较好的一致性,证明了所提出的高温、高应变率下混凝土材料损伤演化方程的合理性。     

基于数值模拟的SHPB实验数据处理方法（英文）北大核心CSCD

在分离式霍普金森压杆(SHPB)实验中,可以精确测得加载试件边界上的应力和速度。然而,基于这些测量结果得到一条精确的应力应变曲线有一定难度。根据SHPB实验技术的原理,有3组公式可以处理实验数据,并且3组公式都对波头的选择敏感。由于波动效应的影响以及选择波头的误差,3种方法得到的应力-应变曲线缺乏一致性。为了解决正确对齐波头的问题,编写了三波耦合法的数据处理程序。该方法基于动量守恒,可以得到更可靠的应力-应变曲线。为了证明该方法的正确性,进行SHPB的数值模拟实验。结果显示,利用这种方法可以得到唯一的应力-应变曲线。这种方法可以避免对齐波头时的误差,而传统的两波法或三波法则不能。     

基于数值模拟的SHPB实验数据处理方法（英文）

在分离式霍普金森压杆(SHPB)实验中,可以精确测得加载试件边界上的应力和速度。然而,基于这些测量结果得到一条精确的应力应变曲线有一定难度。根据SHPB实验技术的原理,有3组公式可以处理实验数据,并且3组公式都对波头的选择敏感。由于波动效应的影响以及选择波头的误差,3种方法得到的应力-应变曲线缺乏一致性。为了解决正确对齐波头的问题,编写了三波耦合法的数据处理程序。该方法基于动量守恒,可以得到更可靠的应力-应变曲线。为了证明该方法的正确性,进行SHPB的数值模拟实验。结果显示,利用这种方法可以得到唯一的应力-应变曲线。这种方法可以避免对齐波头时的误差,而传统的两波法或三波法则不能。     

组合式隔热陶瓷短杆高温SHPB实验技术

讨论和分析了当前高温分离式霍普金森压杆(SHPB)实验技术,为了获得材料在高温下可靠的动态力学性能,建立了一套在压杆和试件之间添加隔热陶瓷短杆的高温SHPB实验系统。相比于传统接触式高温SHPB方案,该系统可以使用在更高的冲击载荷和温度下,与机械对杆方案相比,实验装置及其控制要简便许多。结合有限元模拟,对陶瓷短杆及温度场对压杆中应力波传播的影响进行了相应的评估,并利用这套实验系统得到了800℃下HR2抗氢钢的动态压缩应力-应变曲线。     

陶瓷纤维对普通硅酸盐混凝土的强韧化效应

 采用液压试验机和Φ100 mm分离式霍普金森压杆实验装置,研究了体积分数为0.1%、0.2%和0.3%的陶瓷纤维混凝土的准静态和动态力学性能,分析了陶瓷纤维的增强机理,并将其与相同纤维体积分数的碳纤维混凝土进行对比。结果表明：陶瓷纤维改善了普通硅酸盐混凝土的准静态力学性能;纤维体积分数为0.3%时,抗压强度提高15.0%,劈裂抗拉强度提高8.5%,抗折强度提高12.7%。冲击荷载作用下,陶瓷纤维混凝土的动态抗压强度和比能量吸收随平均应变率的增加近似线性增长;体积分数为0.2%时,陶瓷纤维的增强、增韧效果最佳。陶瓷纤维对普通硅酸盐混凝土的增强、增韧效果总体上优于碳纤维。     

Al-0.5%Cu合金中表现反常振幅效应的低频位错内耗

用低频扭摆的方法,系统地研究了能够较有把握地观测到在Al-0.5％Cu合金中所出现的反常位错内耗的实验程序。结果指出,把试样在拉力试验机上预先拉伸到某一适当的形变量后,立即测量它在某一适当温度下时效的过程中的内耗,可以在内耗-时效时间曲线上观察到一个表现反常振幅效应(即内耗-振幅曲线上出现一个峯值)的时效内耗峯。用经过充分时效而内耗已经达到稳定值的试样,逐渐增加振幅,测量内耗,也可以观察到一个应变振幅内耗峯(当内耗表示为应变振幅的函数时)。此外,用一定的应变振幅在较高温度下,测量经过充分时效的试样的内耗时,也可以观察到一个表现反常振幅效应的温度内耗峯(当内耗表示为温度的函数时)。这些实验结果肯定地指出,在一定测量温度下的振幅内耗峯和表现反常振幅效应的温度内耗峯是存在的。为了找出以前在Al-0.5％Cu中所观察到的反常内耗现象重复性不好的原因,系统地研究了测量内耗所用的应变振幅对于出现振幅内耗峯的影响以及预形变量对于出现时效内耗峯和温度内耗峯的影响。对于出现反常内耗现象的实验条件进行了分析。所观察到的关于反常内耗现象的实验结果,都可用位错拖着溶质原子气团运动的模型来作定性的解释。具体的模型和理论分析将另行报导。     

器壁滑动摩擦力对受振颗粒体系中冲击力倍周期分岔过程的影响

颗粒物质由离散的固体颗粒组成, 受到周期性振动时可以表现出复杂的动力学行为. 这些行为往往受众多因素的影响, 如空气阻力和器壁摩擦力等. 针对受振颗粒体系中冲击力的倍周期分岔现象, 通过抽真空或将容器底镂空消除空气阻力, 单独研究器壁滑动摩擦力的影响. 结果表明在仅有器壁摩擦力作用的情况下, 倍周期分岔过程仅受约化振动加速度的控制, 与颗粒的尺寸、颗粒层数及振动频率无关. 将器壁摩擦力处理成一个大小恒定、方向与颗粒和器壁相对速度反向的阻力, 并包含到完全非弹性蹦球模型中, 能够对所观察到的现象给出很好的解释. 通过对倍周期分岔点测量平均值的拟合, 得到器壁滑动摩擦力的大小约为颗粒总重量的10%. 关键词： 颗粒物质 器壁摩擦力 倍周期分岔 冲击力     

Ultrasonically controlled particle size distribution of explosives: a safe method

Size reduction of the high energy materials (HEM's) by conventional methods (mechanical means) is not safe as they are very sensitive to friction and impact. Modified crystallization techniques can be used for the same purpose. The solute is dissolved in the solvent and crystallized via cooling or is precipitated out using an antisolvent. The various crystallization parameters such as temperature, antisolvent addition rate and agitation are adjusted to get the required final crystal size and morphology. The solvent-antisolvent ratio, time of crystallization and yield of the product are the key factors for controlling antisolvent based precipitation process. The advantages of cavitationally induced nucleation can be coupled with the conventional crystallization process. This study includes the effect of the ultrasonically generated acoustic cavitation phenomenon on the solvent antisolvent based precipitation process. CL20, a high-energy explosive compound, is a polyazapolycyclic caged polynitramine. CL-20 has greater energy output than existing (in-use) energetic ingredients while having an acceptable level of insensitivity to shock and other external stimuli. The size control and size distribution manipulation of the high energy material (CL20) has been successfully carried out safely and quickly along with an increase in the final mass yield, compared to the conventional antisolvent based precipitation process.     

An equivalent method of jet impact loading from collapsing near-wall acoustic bubbles: A preliminary study

Cavitation damage is a micro, high-speed, multi-phase complex phenomenon caused by the near-wall bubble group collapse. The current numerical simulation method of cavitation mainly focuses on the collapse impact of a single cavitation bubble. The large-scale simulation of the cavitation bubble group collapse is difficult to perform and has not been studied, to the best of our knowledge. In this study, the equivalent model of impact loading of acoustic bubble collapse micro-jets is proposed to study the cavitation erosion damage of materials. Based on the theory of the micro-jet and the water hammer effect of the liquid–solid impact, an equivalent model of impact loading of a single acoustic bubble collapse micro-jet is established under the principle of deformation equivalence. Since the acoustic bubbles can be considered uniformly distributed in a small enough area, an equivalent model of impact loading of multiple acoustic bubble collapse micro-jets in a micro-segment can be derived based on the equivalent results of impact loading of a single acoustic bubble collapse micro-jet. In fact, the equivalent methods of cavitation damage loading for single and multiple near-wall acoustic bubble collapse micro-jets are formed. The verification results show the law of cavitation deformation of concrete using equivalent loading is consistent with that of a micro-jet simulation, and the average relative errors and the mean square errors are insignificant. The equivalent method of impact loading proposed in this paper has high accuracy and can greatly improve the calculation efficiency, which provides technical support for numerical simulation of concrete cavitation.     

传输矩阵法在行波管内部反射引起的增益波动计算中的应用

本文分析了由于行波管慢波结构制造误差引入的多个不连续点对小信号增益的影响.行波管内部反射对增益波动的影响,须采用考虑反射波的四阶模型进行分析,用传输矩阵法对节点处的自左至右入射和自右至左入射两种散射类型建立传输矩阵,研究在不同空间电荷参量下,慢波电路的单个反射节点以及慢波电路的皮尔斯速度参量b和增益参量C的多个随机分布不连续性对行波管小信号增益的影响,计算结果与Chernin模型具有很好的一致性.并以G波段行波管为例分析了慢波结构周期长度分布有两个不连续点和周期长度的多个随机分布不连续性带来的小信号增益波动.结果表明,制造误差越大,周期长度分布的两个不连续点相距越远,小信号增益波动越大,多个小的不连续性可以引起较大的增益波动.     

Optimized pulse parameters for reducing quantitation errors due to saturation factor changes in magnetic resonance spectroscopy

We present an analysis of the effects of chemical exchange and changes in T(1) on metabolite quantitation for heart, skeletal muscle, and brain using the one-pulse experiment for a sample which is subject to temporal variation. We use an optimization algorithm to calculate interpulse delay times, TRs, and flip angles, theta, resulting in maximal root-mean-squared signal-to-noise per unit time (S/N) for all exchanging species under 5 and 10% constraints on quantitation errors. The optimization yields TR and theta pairs giving signal-to-noise per unit time close or superior to typical literature values. Additional simulations were performed to demonstrate explicitly the dependence of the quantitation errors on pulse parameters and variations in the properties of the sample, such as may occur after an intervention. We find that (i) correction for partial saturation in accordance with the usual analysis neglecting variations in metabolite concentrations and rate constants may readily result in quantitation errors of 15% or more; the exact degree of error depends upon the details of the system under consideration; (ii) if T(1)'s vary as well, significantly larger quantitation errors may occur; and (iii) optimal values of pulse parameters may minimize errors in quantitation with minimal S/N loss.     

Investigation on ultrasonic volume effects: Stress superposition,acoustic softening and dynamic impact

Conventional high power ultrasonic vibration has been widely used to improve manufacturing processes like surface treatment and metal forming. Ultrasonic vibration affects material properties, leading to a flow stress reduction, which is called ultrasonic volume effect. The volume effect contains multi-mechanisms such as stress superposition due to oscillatory stress, acoustic softening by easier dislocation motion and dynamic impact leading to extra surface plastic deformation. However, most researches ignored the stress superposition for the convenience of measurement, and few studies considered ultrasonic dynamic impact since the relatively low ultrasonic energy in macro scale. The purpose of this study is to investigate the characteristics and mechanisms of different ultrasonic volume effects in micro-forming. A 60 kHz longitudinal ultrasonic-assisted compression test system was developed and a series of ultrasonic-assisted compression tests at different amplitudes on commercially pure aluminum A1100 in micro-scale were carried out combining the surface analysis by SEM, EDX and micro-hardness test. Three different ultrasonic volume effects, stress superposition, acoustic softening and dynamic impact, were confirmed in the ultrasonic-assisted compression tests. In order to quantitatively predict stress superposition, a hybrid model for stress superposition is developed considering the elastic deformation of experimental apparatus in practice, the evolution of the modeling results fitted well with the experimental results. With low ultrasonic amplitude, stress superposition and acoustic softening occurred because vibrated punch contacted with the specimen all the time during compression. However, with higher amplitude, due to the extra surface plastic deformation by larger ultrasonic energy, forming stress was further reduced by the ultrasonic dynamic impact. A possible method to distinguish the effects of dynamic impact and acoustic softening is to analyze the waveform of the oscillatory stress in the process. In the case of ultrasonic dynamic impact effect, a higher amount of oxidation was observed on the specimen surface, which could be the result of local heating by surface plastic deformation and surface friction when the vibrated punch detached from the specimen. The findings of this study provide an instructive understanding of the underlying mechanisms of volume effects in ultrasonic-assisted micro-forming.