爆炸冲击作用下铝蜂窝板失稳研究

基于非线性动力学软件AUTODYN,对铝蜂窝夹芯板在爆炸冲击载荷作用下的失稳过程进行三维数值模拟。通过建立不同参数规格的铝蜂窝夹芯板的实体模型,研究其前、后面板在TNT爆炸冲击作用下的动态响应及塑性阶段的失稳变形。计算结果表明:随着铝蜂窝板前、后面板厚度,夹芯层铝箔高度和厚度的增加,铝蜂窝板在爆炸冲击载荷下的最终残余变形量均明显减小,抵抗变形的能力增强;对于夹芯层胞元形状不同但相对密度相同的铝蜂窝板,因冲击载荷下单轴压缩"惯性效应"差异较小,其面板在爆炸载荷作用下的最终残余变形量差异不大。     

水下爆炸冲击波作用下空化区域形成的特性研究

对水下爆炸冲击波作用下的局部空化和区域空化形成特性进行了理论和实验研究.引入平面冲击波假设,理论分析了结构几何尺度及冲击波参数的变化对空化区域形成的影响,并在直径5 m的圆柱形水箱中,对边长1 m、厚度2 mm的方形钢板在50 g TNT炸药、1 m爆距条件下进行了水下爆炸冲击实验,以验证局部空化理论.研究结果表明:在相同的冲击条件下,结构尺度的变化对局部空化的形成具有较大影响;炸药质量及爆深的变化会改变区域空化的形状及范围;实验结果与局部空化理论计算结果基本一致.     

接枝聚合物对小分子的选择性吸附研究

文章应用密度泛函理论研究接枝于壁面的方阱链对二元小分子混合物的选择性吸附特性. 系统的Helmholtz剩余自由能泛函被表示为硬球排斥和方阱吸引两部分贡献之和,分别由硬球链流体状态方程和变阱宽方阱链流体状态方程的简单加权密度近似来进行计算. 用此理论方法,分别考察了接枝聚合物的结构性质,以及不同温度下接枝分子层对二元方阱流体的选择性吸附性能. 结果表明:分子刷厚度随接枝密度线性增长而随温度非线性增加,并且在高温下趋于饱和;在较低温度下,接枝聚合物刷能表现出很好的选择性吸附能力,当聚合物刷被加热到高于饱和温度时,该能力将大幅度地减弱. 关键词： 密度泛函理论 接枝聚合物 选择性吸附 方阱链     

双泡耦合声空化动力学过程模拟

为了对双泡耦合的声空化过程进行模拟,本文从流体动力学控制方程和流体体积分数模型出发,在Fluent软件中构建双泡耦合超声空化三维有限元仿真模型,对超声波驱动下流体中双泡耦合声空化动力学过程进行数值模拟,并通过对空化气泡周围声场的变化进行分析研究双泡耦合声空化的非线性动力学特性.结果显示:在超声波驱动下,球形气泡先缓慢扩张,扩张到最大半径后迅速收缩直至溃灭;耦合双气泡间存在相互作用力,使得空化气泡的扩张受到抑制、气泡收缩时间增长;空化气泡在收缩阶段的能量转换能力增强,相比单气泡声空化,耦合双气泡溃灭时气泡内部的压强更大.本文分析结果将为超声空化泡群的动力学过程模拟提供参考.     

液力涡轮内部的强约束流动与空化现象

为描述液力涡轮制动器内的流动特征及流动对制动器力矩性能的影响,采用计算流体动力学方法对制动器内的流动结构及空化现象进行了研究,获得了涡轮制动器瞬态启动和停止过程中转轮及挡板附近的流动参数分布,捕捉了制动器封闭腔体内的空化区位置和形态,求解了挡板上受到的流体载荷。结果表明,制动器腔体内存在着大尺度流动结构,其随着挡板与转轮之间的轴向距离增加而沿轴向发展;空化区出现在转轮叶片背面及根部附近,空化相体积份额随转轮转速增加而增大,但未对制动器的力矩系数造成明显影响;作用在挡板上的轴向流体作用力的合力方向始终指向转轮侧,该力的大小随转轮转速和叶轮与挡板间距增加而增加。     

超声在液体中的非线性传播及反常衰减

本文从广义的Navier-Stokes流体方程出发,考虑到流体介质的黏滞性和存在的热传导,导出了更接近实际流体的三维非线性声波动方程.鉴于声传播所涉及的空间和时间尺度的复杂性和多样性,文中针对一维情形下的非线性波动方程进行了求解和分析.由方程的二级近似解可以看出,声压振幅的衰减遵循几何级数规律,而且驱动声波的频率越高声压的衰减就越快.在满足条件ωb《ρ0c_0~2时,基波的衰减系数与驱动频率的平方及耗散系数的乘积成正比;二次谐波的衰减规律更加复杂,与频率的更高次幂相关.对声衰减系数及声压的分布进行数值计算发现,声压的分布还与初始的声压幅值及频率有关,初始的声压与频率越高衰减得越快.另外,当声压高于液体的空化阈值时,液体中就会出现大量的空化泡,文中模拟了单个空化泡的运动,发现随着声压的增大空化泡的振动越剧烈、空化泡所受的黏滞力变大,随着声波作用时间的增大黏滞力的幅值迅速增大并与驱动声压值同阶,因而空化泡的非线性径向运动引起的声衰减不容忽视.结果表明,驱动声压越高在空化区域附近引起的声衰减越快、输出的声压越低.     

近场爆炸冲击波对屏蔽压装TNT的冲击引爆试验和仿真

为研究近场强冲击波对屏蔽装药的冲击引爆效应,通过试验和LS-DYNA3D非线性有限元计算程序对屏蔽压装TNT的冲击引爆进行研究,得到了接触爆炸时压装TNT被引爆的临界屏蔽板厚度和非接触爆炸时屏蔽压装TNT的殉爆距离,分析了非接触爆炸时屏蔽板厚度对殉爆距离的影响,并通过非线性最小二乘法拟合得到屏蔽板厚度与殉爆距离的函数关系。结果表明:数值计算结果与试验结果基本一致;接触爆炸时临界起爆的屏蔽板厚度在20～23 mm之间;屏蔽板采用3 mm厚的45钢时,非接触爆炸作用下压装TNT的殉爆距离在12～15 mm之间;非接触爆炸时殉爆距离随着屏蔽板厚度的增加而减小,当无屏蔽板时,压装TNT的殉爆距离为79 mm,当屏蔽板厚度从1 mm加大到9 mm时,殉爆距离从51 mm减为1.5 mm,被发装药的屏蔽板对冲击波有显著的防护作用。     

微尺度振荡Couette流的格子Boltzmann模拟

采用有效多松弛时间-格子Boltzmann方法(Effective MRT-LBM)数值模拟了微尺度条件下的振荡Couette和Poiseuille流动. 在微流动LBM中引入Knudsen边界层模型,对松弛时间进行修正. 模拟时平板或外力以正弦周期振动,Couette流中考虑了单平板振动、上下板同相振动这两类情况. 研究结果表明,修正后的MRT-LBM模型能有效用于这类非平衡的微尺度流动模拟;对于Couette流,随着Kn数的增大,壁面滑移效应变得越明显. St越大,板间速度剖面的非线性特性越剧烈;两板同相振荡时,若Kn,St均较小,板间流体受到平板拖动剪切的影响很小,板间速度几乎重叠在一起;在振荡Poiseuille流动中,St数增大到一定值时,相位滞后现象减弱;相对于Kn数,St数对振荡Couette 和Poiseuille流中不同位置处速度相位差的产生有较大影响. 关键词： 格子Boltzmann方法 有效MRT模型 Knudsen层 振荡流     

强冲击载荷下边界对固支方板的毁伤破坏试验

冲击载荷作用下边界条件对方板的毁伤破坏具有很大影响。利用落锤试验机开展了不同边界支撑下固支方板的冲击试验,为获取固支方板边界撕裂的典型破坏模式,专门设计加工了与固支方板尺寸相当的冲击锤头和可改变倒角的方板支撑框架。研究结果表明:(1)冲击载荷作用下,固支方板呈现出塑性大变形、单边撕裂、双边撕裂等典型破坏模式,倒角越小,方板越容易撕裂;(2)边界支撑对固支方板中心位移、整体变形轮廓影响较小,但对方板的撕裂长度、临界撕裂阈值存在较大影响;(3)不同边界支撑主要改变方板边界处的剪切应变,边界支撑倒角越小,剪切效果越明显,方板边界临界撕裂应变位于[0.191,0.241]区间。     

非线性介质的表面等离子体波导设计和优化

设计了一种基于非线性介质Si-NC/SiO2的混合表面等离子体波导,利用有限元方法定量分析了这种波导所支持基模的能流密度分布、有效折射率、传播长度和有效面积与几何结构参数以及非线性介质的依赖关系.分析结果表明,光场主要被限制在非线性区域,通过调节非线性层的厚度以及非线性比例因子,可以实现模式的有效折射率和传播长度等传输特性参数的调节.固定非线性介质比例因子,有效折射率和传播距离随非线性层厚度增加而增大;固定波导尺寸,有效折射率随比例因子增大而增大,传播距离和有效面积较小.最后,根据分析结果对非线性效应进行优化,优化后波导最优结构尺寸为波导宽度为250nm,非线性材料层厚度为100nm,硅层厚度为150nm.     

基于离散元方法的颗粒材料缓冲性能及影响因素分析

在冲击荷载作用下, 颗粒材料通过颗粒间的摩擦及非弹性碰撞可有效进行能量耗散实现缓冲作用. 本文采用离散元方法对冲击载荷下颗粒材料的缓冲过程进行数值分析, 研究不同厚度下颗粒材料的缓冲性能. 计算结果表明: 颗粒层厚度H是影响颗粒材料缓冲性能的关键因素, 并存在一个临界厚度H_c. 当H < H_c时, 冲击力随H的增加而降低; 当H > H_c时, 冲击力对H的变化不敏感并趋于稳定值. 此外, 在不同颗粒摩擦系数和初始密集度下对缓冲过程的离散元分析表明, 光滑和疏松颗粒材料具有更好的缓冲性能. 最后, 对颗粒材料在冲击过程中的力链结构和底板的压力分布进行了讨论, 以揭示颗粒材料缓冲性能的内在机理.     

正则系综条件下空化空泡形成的分子动力学模拟

液体中空化现象的研究对减少空蚀破坏, 提高空化空泡的有效利用具有重要意义.本文采用分子动力学模拟的方法, 对正则系综条件下系统中空化的发生特性进行研究, 分析空化发生的机理, 讨论温度、数密度等因素对空化发生的影响, 并与格子Boltzmann方法进行了比较.模拟结果表明: 温度和数密度的变化, 都对系统中的空化产生显著影响.其中, 温度升高, 使系统中空化空泡的形成由稳定变得不稳定, 最终难以形成.数密度降低, 则会促进空化空泡的形成.随着数密度的减小, 温度对空化空泡形成的影响程度下降.     

Modelling drying pathways of an evaporating soft matter droplet

Micro-droplets of soft matter solutions have different morphologies upon drying, and can become wrinkled, buckled or cavitated particles. We investigate the morphology evolution of a drying soft matter droplet in this work: at the early stage of drying, wrinkling or cavitation instability can occur in the droplet, depending on the comparison between the critical wrinkling and cavitation pressure; at a later stage of drying, no wrinkles will appear if cavitation happens first, while cavitation can still occur if wrinkling happens first. A three-dimensional phase diagram in the space of elastic length, gel layer thickness and weight loss is provided to illustrate the drying pathways of a soft matter droplet. This diagram can help guide future fabrications of micro-particles with desired morphologies.     

Numerical simulations of the flapping of a three-dimensional flexible plate in uniform flow

The self-sustained flapping of a three-dimensional flexible plate in a uniform viscous flow is numerically simulated with a fictitious domain method. The effects of the various non-dimensional control parameters including the Reynolds number, the density ratio, the dimensionless shear modulus, the length–thickness ratio, and the width–length ratio on the flapping of the plate are investigated. The results show that there exist two flapping modes: symmetrical and asymmetrical flapping about the centerline in the spanwise direction. Near the critical point a decrease in the plate width–length ratio, or the increase in the Reynolds number or the reduced velocity (a combination of the density ratio, the dimensionless shear modulus, and the length–thickness ratio) can make symmetric (or nearly symmetric) flapping become asymmetric. It is found that the flapping amplitude is mainly controlled by the density ratio and the dimensionless elastic modulus, while the frequency by the density ratio and the length–thickness ratio. In addition, the flapping amplitude and frequency are affected significantly by the confinement effect of the computational domain, and normally enhanced as the confinement effect becomes stronger. The effects of the plate width and the mass ratio (i.e., the ratio of the length–thickness and density ratios) on the critical reduced velocities are examined. The results indicate that when the fluid–plate mass ratio (or the plate length–thickness ratio) is relatively small there exist two significantly different critical velocities for the flapping instability, depending on the strength of initial plate deformation, a hysteresis phenomenon. No obvious hysteresis can be observed when the fluid–plate mass ratio (or the plate length–thickness ratio) is large.     

基于高速摄像实验的开放腔体圆柱壳入水空泡流动研究

基于高速摄像方法,针对入水空泡流动特征和机理,进行了开放腔体圆柱壳垂直入水实验研究.通过对实验现象的观测,发现开放腔体圆柱壳入水运动会形成波动流动和云化流动两种流动方式,结合影像数据,分别描述了两种流动状态下的空泡形态特征,并获得了空泡波动参数的变化规律;对比不同入水速度实验,分析了入水速度对入水空泡流动方式和流动参数的影响;依据流体力学基本理论,分析了入水空泡波动和云化现象的形成机理.结果表明:随入水速度增加,入水空泡依次呈现波动和云化两种流动状态,波动频率与入水速度无关,闭合发生时间随入水速度增加而减小,与Froude数呈线性关系;入水导致开放空腔内部气体涨缩,引起开放端压力场和速度场周期性扰动,空泡截面扩展程度出现差异,形成空泡波动现象;空泡闭合后尾部形成回射流,回射流触及空泡壁面引起壁面流动转捩,形成空泡云化现象.     

A parametric review of sonochemistry: Control and augmentation of sonochemical activity in aqueous solutions

In this review the phenomenon of ultrasonic cavitation and associated sonochemistry is presented through system parameters. Primary parameters are defined and considered, namely; pressure amplitude, frequency and reactor design; including transducer type, signal type, vessel-transducer ratio, liquid flow, liquid height, liquid temperature and the presence of a reflective plate. Secondary parameters are similarly characterised and involve the use of gas and liquid additives to influence the chemical and physical environments. Each of the parameters are considered in terms of their effect on bubble characteristics and subsequent impact on sonochemical activity. Evidence suggests that via parametric variation, the reaction products and efficiency may be controlled. This is hypothesised to occur through manipulation of the structural stability of the bubble.     

Boiling-up of liquid argon at high superheatings under the impact of weak ultrasonic fields

The technique of lifetime measurement for metastable liquid and continuous depressurization technique were applied for study of kinetics of spontaneous cavitation in superheated liquid argon under impact of weak ultrasonic fields. It was demonstrated that acoustic cavitation may occur through the mechanism of homogeneous generation of vapor phase or through “swinging” of vapor bubbles generated by high-energy particles and/or other kinds of initiative factors. The thresholds of acoustic cavitation are described by the theory of homogeneous nucleation.     

Ultrasonic system for continuous washing of textiles in liquid layers

The use of ultrasonic energy for washing of textiles has been tried several times without achieving practical development. In fact, the softness of the fibres makes the cavitation to produce small erosion effect and the reticulate structure of the fabric favours the formation of air bubble layers which obstruct wave penetration. In addition, a high proportion of water with respect to the wash load and a certain water degassing is required to assure efficiency and homogeneity in the wash performance. Such requirements have hindered the commercial development of the ultrasonic washing machines for domestic purposes. For specific industrial applications, a great part of these limitations may be overcome. This article deals with a new process in which the fabric is exposed to the ultrasonic field in a flat format. Such process has been implemented at laboratory and at semi-industrial stage by using specially designed power ultrasonic transducers with rectangular plate radiators. The cleaning effect is produced by the intense cavitation field generated by the plate radiator within a thin layer of liquid where the fabric is introduced. The homogeneity of such effect is achieved by the successive exposure of all the fabric areas to the intense acoustic field. In this paper the structure and performance of the developed system are shown.     

Memory effect and redistribution of cavitation nuclei in a thin liquid layer

Temporal evolution and spatial distribution of acoustic cavitation structures in a thin liquid layer were investigated experimentally with high-speed photography. The inception and disappearance processes of cavitation bubble cloud revealed that the metastable cavitaton structures formed in the thin liquid layer caused a long-term “memory effect”. A factor which weakens the memory effect was identified. The distribution of cavitation nuclei was investigated by changing the temporal decay of the memory effect.     

Forced vibrations of a non-uniform thickness rectangular plate with two free sides

A forced vibration of a rectangular plate with thickness varying linearly in one direction is studied. The plate is simply supported along two opposite sides, and is free along the other sides. Approximate formulae are proposed for estimating the maximum deflection and surface stresses of a rectangular plate subject to a uniformly distributed harmonic lateral load. The accuracy of the formulae is discussed. The approximate formulae show the possibility that one can obtain solutions for the forced vibration of a plate with non-uniform thickness from those for the static bending of the same plate when the plate is subjected to a uniformly distributed load.