两个等径蛋白质气泡在Bingham流体中振动特性

利用黏弹性膜构成的蛋白质气泡有限变形方程,并考虑一个气泡在Bingham流体中振动产生的Bjerknes力对另一个气泡振动特性的影响,建立了两个等径蛋白质气泡在Bingham流体中振动的非线性方程.利用数值计算方法求解该方程,结果表明,增加Bingham流体的塑性黏度,蛋白质气泡振幅衰减速度加快,振动周期增加,频率减小;当两个气泡间的距离减小时,气泡振动频率会增加,振幅衰减速度加快;初始半径小的气泡振动频率高,振幅衰减快,而且振动的频率和振幅衰减的速率越大;与单个气泡相比,两个蛋白质气泡在Bingham流体中振动时,振动具有更高的振动频率,而且振幅衰减速度更快.     

低频振动管外流动与传热特性研究

采用数值模拟与实验相结合的方法,研究了低频振动管外的流动与传热特性,分析了不同参数对换热性能的影响.数值计算结果的场协同理论分析与实验表明:振动有利于强化传热,且其强化传热的效果随着振动频率与振幅升高而增强.在半周期内,时相位为90°时管外的换热性能最好,在一定范围内协同角余弦值随振动频率的变化与振幅基本无关.对比不同管型,沿椭圆管短轴方向振动的协同角余弦值最高,传热效果最好.     

基于希尔伯特变化的微小振动激光多普勒信号处理

为了实现对固体目标微小振动参数的测量,建立了微小振动的激光多普勒信号模型。采用希尔伯特数字运算,将激光多普勒振动信号的即时信号采样转化为信号的谱采样。通过频谱计算得到每个振动周期中瞬时频率的平均数,应用差值采样序列积分计算得到振动频率,最后根据振动信号频率变化与振幅的关系得到振幅。采用希尔伯特方法对实验测试结果进行处理验证,并分析了误差来源。实验结果表明：实验测量目标的振动振幅约为1.85×10-4m,转动的圆频率约为170 Hz。因此,应用希尔伯特变换方法处理测量的目标微小振动信号,获取目标运动的参数是可行的。     

垂直振动床中的能量传递与耗散

本文采用数值方法分析了一维垂直振动床内颗粒动能/温度、能量耗散以及体积分数的分布规律.离散元模拟结果表明:当床底做低频、小振幅振动时,床层内颗粒整体随床底上下运动,沿床高方向颗粒动能逐渐增加;对于高频振动,床层内的颗粒做无规则的运动,沿床高方向颗粒动能逐渐降低.在不同振动频率(高频、低频)下体积分数、能量耗散也表现出不同的分布规律.将离散元模拟结果与动力学理论计算值对比,当系统做高频振动时,两模型所得结果基本吻合;而对于低频、小振幅振动,所得结果存在较大差异.由于低频、小振幅振动时床内颗粒并非做无规则运动,动力学理论的适用性需进一步完善.     

水声作用下矩形弹性-粘弹性复合板的振动和散射声近场(Ⅱ)——矩形弹性-粘弹性复合板散射声近场研究

本文根据作者前一篇文章导出的复合粘-弹性薄板弯曲振动方程给出板振动简正模式的级数解,计算和分析了声波入射时,矩形复合粘弹性障板的振动;研究了密介质中,复合板简正模振动和其二次辐射场之间作用,以及不同模式振动之间由于辐射场引起的互耦合作用;数值计算了简支矩形板各号简正模的自耦合和互耦合系数随kl_1的变化关系,(r=l_2/l_1作为参变量,k为波数,l_1,l_2分别为板的两对边边长);并计算了复合障板在不同频率声波作用下各号模的复数振幅值;进而计算了不同频率声波作用下,板振动二次辐射声的近场声压分布。     

Frenkel-Kontorova模型中基底势振动的影响

基于一维Frenkel-Kontorova模型, 研究了振动的基底势对系统纳米摩擦现象的影响. 分别在相邻原子间的距离与周期势场的周期比为不公度(incommensurate)、可公度(commensurate)两种情形下, 探讨了基底势振动的振幅和频率对滞回现象(hysteresis)、最大静摩擦力以及超滑现象的作用机理. 两种情形下, 固定频率, 随着振幅的增大, 滞回区域的面积以及最大静摩擦力都将减小, 对于不同的频率, 减小的趋势不同. 系统甚至产生了超滑现象. 但当频率过大时, 振幅的改变不会影响滞回区域的面积以及最大静摩擦力的大小, 此时与基底不加振动时的情形一致; 当振幅固定, 随着频率的增大, 滞回区域的面积将增大, 对于不同振幅, 增大的趋势不同. 特别地, 对于某些固定的振幅, 最大静摩擦力随着振动频率的增大先逐步减小直至出现超滑现象, 再进一步增大频率, 最大静摩擦力又转而逐步增大. 这一现象类似于共振, 表明存在最佳的振动频率促进系统内所有原子的共同运动, 使得整个系统的最大静摩擦力几乎消失. 另外, 两种情形的区别是, 对于某些固定的频率(如ω= 0.5)和不同的小振幅, 不可公度情形往往具有相同的平均终止速度, 而可公度情形则不同, 表明相同前提下后者具有更复杂的动力学行为. 关键词： Frenkel-Kontorova模型 滞回 最大静摩擦力 超润滑     

振动对面形测量误差的影响分析

振动会使高精度面形测量产生误差。建立了振动对干涉测量面形的误差模型,应用13步移相算法分析了在振幅为63 nm时的误差情况。分析结果表明,当面形测量误差的敏感频率为12 Hz时,振动引起的面形均方根(RMS)误差约为12 nm。通过实验进行了验证,仿真分析结果和实验结果基本相同。实验分析了在12 Hz时,振幅为5~63 nm时,对应的测量面形RMS误差为1~7.1 nm,振幅和RMS误差线性增大。为不同振动频率和振幅引起的面形RMS的误差分析和高精度面形测量的振动环境控制提供了一定的参考。     

光泵磁共振信号幅度与射频场振幅的关系

在光泵磁共振实验中观测到单量子跃迁共振信号幅度随射频场振幅增加而迅速增加,并很快达到饱和,然后单调缓慢下降的关系.当射频场振幅更大时(约大于3.5V),观测到双量子跃迁共振信号,信号幅度与射频场振幅成二次函数关系.本文对实验结果进行了分析和解释.     

正弦振动下动态调制传递函数分析与研究

振动导致航空相机成像分辨率下降,常采用动态调制传递函数(MTF)评价振动对成像质量的影响。根据线性光学系统的传递函数理论,针对任意频率的正弦振动,提出一种基于第一类贝塞尔函数的动态MTF计算方法,并以奈奎斯特频率处动态MTF不小于0.9为条件,得出低频振动的振幅容限随频率增加而减小,高频振动的振幅容限为0.2 pixel。通过对刀口靶标进行正弦振动下动态成像实验,得出理论计算结果与实验结果间相对误差小于4.25%,相比以往相关文献的分析结果,计算精度最大可提高18.5倍,因此该方法可用于预估和评价振动环境下航空相机的成像质量,对视轴稳定系统的设计具有指导意义。     

振荡场作用下聚合物/纳米棒混合体系的自组装

采用元胞动力学和布朗动力学联用方法研究了振荡场作用下两嵌段共聚物/均聚物/纳米棒混合体系的自组装相行为.通过计算模拟,探讨了振荡场的振幅和频率对混合体系相形貌形成和演化的影响.研究发现振荡场对体系有序结构的形成和转变有重要作用,随着外加振荡场频率的增大,混合体系形貌从平行于场方向的条纹结构过渡到斜层状结构再转变为垂直于场方向的条纹结构.进一步分析了振荡场作用下体系畴尺寸的演化及纳米棒取向角的变化情况.研究结果为制备和调控聚合物纳米复合材料有序结构提供了新的方法和参考.     

Online Research on Plasticizing Process of Starch Under Superimposed Vibration Field

A novel testing machine, integrating plastic vibration processing with molding, based on a multipass rheometer, was used to investigate the effect of the complex force field on plasticization of taro and wheat thermoplastic starch (TPS) melts. Various kinds of continuous vibration fields could be tested by controlling the movement of pistons. A superimposed vibration field, combining the effects of vibration and shear, was obtained by adding a high-frequency low-amplitude oscillation on a low-frequency high-amplitude oscillation. The rheological properties of starch were directly monitored during and after the plasticization process without removing the starch melts out of the testing machine. The apparent viscosity of the TPS melts were obtained for different high-frequency oscillation conditions by monitoring the pressure difference in the cavity. The plasticization preparation time was used to characterize the benefit provided by the superimposed vibration field. The results showed the decrease of the percentage of the average plasticizing preparation time for taro starch was 3.4%, while that for wheat starch was 1.6% compared to single, low-frequency, high-amplitude oscillation. Comparison of the plasticizing preparation time under different vibration frequencies showed that the plasticization was promoted by applying the superposed vibration field, and the effective degree was related to the vibration frequency and starch type. Both TPS exhibited shear-thinning behavior after the plasticization, and samples of both types of starch which were plasticized under higher vibration frequency presented lower apparent viscosities at certain shear rates.     

Improving Melt Flow Behavior via Melt Vibration

A self‐made melt vibration extrusion device was used to study the melt flow behavior in a vibration field. A pulse pressure was superimposed on the flowing melt during extrusion, called vibration assisted extrusion (VAE); conventional extrusion (CE) was studied for comparison. A die (L/D=17.5) was attached to the device to study melt flow behavior of an amorphous polymer (polystyrene) and semi‐crystalline polymers (high density and linear low polyethylene). Results show that the melt vibration technique is an effective processing tool to improve polymer melt flow behavior for both crystalline and amorphous polymers. Increasing with vibration frequency for extrusion at constant vibration pressure amplitude, the viscosity decreases sharply, and also with increasing vibration pressure amplitude at a constant vibration frequency. The effect of vibration field on melt flow behavior depends greatly on the melt temperature, with the largest change in viscosity obtained at low temperature. Increasing with vibration frequency at constant pressure vibration amplitude, the maximum decrease percentages of viscosities are 82.9, 66.7, and 48.9%, for HDPE, LLDPE, and PS, respectively; increasing with pressure vibration amplitude at a constant vibration frequency, the maximum decrease percentage of viscosities are 99.0, 94.3, and 99.0%, for HDPE, LLDPE, and PS, respectively.     

Self-Reinforced High-Density Polyethylene Prepared by Low-Frequency,Vibration-Assisted Injection Molding. 1. Processing Conditions and Physical Properties

Using a low-frequency, vibration-assisted injection molding (VAIM) device, the effects of vibration variables (frequency and amplitude) on mechanical properties and thermal softening temperature of high-density polyethylene (HDPE) injection moldings were investigated. For VAIM-processed samples, the mechanical properties can be improved by changing vibration frequency and vibration pressure amplitude. Injected at a constant vibration pressure amplitude, a low range of frequency (below 0.7 Hz) was favorable for increasing yield strength; in the high range of frequency (0.7 Hz < f < 2.33 Hz) the yield strength remained at a plateau. Injected at a constant frequency (0.7 Hz) the yield strength increased sharply with decreased elongation when applying large vibration pressure amplitude. The maximal yield strength and Young's modulus were 60.6 MPa and 2.1 GPa for a VAIM sample compared with 39.8 MPa and 1.0 GPa for a conventional injection-molded (CIM) sample, respectively; there was also a 10°C increase in Vicat softening point temperature.     

Melt Vibration Improved Melt Flow Behavior and Mechanical Properties of High Density Polyethylene

A pulse pressure was superimposed on the melt flow resulting in melt vibration. With application of the melt vibration technology, the melt flow behavior and mechanical properties of high‐density polyethylene were studied. For vibration‐assisted extrusion (VAE) at constant vibration pressure amplitude, the viscosity decreases sharply with increasing vibration frequency, and also does so when increasing vibration pressure amplitude for VAE at constant vibration frequency. The effect of vibration field on melt rheological behavior is also related to the melt temperature; a large decease in viscosity is obtained at low melt temperature. Compared with the mechanical properties obtained by conventional injection molding (CIM), the mechanical properties for vibration‐assisted injection molding (VAIM) samples were improved by changing the vibration frequency and vibration pressure amplitude. Injected at constant low vibration pressure amplitude, the VAIM sample prepared at high vibration frequency shows large elongation at break; injected at constant low vibration frequency, the VAIM sample prepared at high vibration pressure amplitude shows greatly improved yield strength. The above two VAIM processing routes produce different VAIM samples with different fracture behaviors; a distinct layered structure for VAIM samples was observed by SEM.     

Direct energy flow measurement in magneto-sensitive vibration isolator systems

The effectiveness of highly nonlinear, frequency, amplitude and magnetic field dependent magneto-sensitive natural rubber components applied in a vibration isolation system is experimentally investigated by measuring the energy flow into the foundation. The energy flow, including both force and velocity of the foundation, is a suitable measure of the effectiveness of a real vibration isolation system where the foundation is not perfectly rigid. The vibration isolation system in this study consists of a solid aluminium mass supported on four magneto-sensitive rubber components and is excited by an electro-dynamic shaker while applying various excitation signals, amplitudes and positions in the frequency range of 20–200 Hz and using magneto-sensitive components at zero-field and at magnetic saturation. The energy flow through the magneto-sensitive rubber isolators is directly measured by inserting a force transducer below each isolator and an accelerometer on the foundation close to each isolator. This investigation provides novel practical insights into the potential of using magneto-sensitive material isolators in noise and vibration control, including their advantages compared to traditional vibration isolators. Finally, nonlinear features of magneto-sensitive components are experimentally verified.     

一种采用双换能器和摆式结构的宽频振动能量采集器

针对悬臂梁振动能量采集器在大振幅振动下梁容易断裂的缺点,本文提出了一种基于摆式结构的具有宽频和倍频特性的振动能量采集器,该采集器由两个Terfenol-D/PMN-PT/Terfenol-D磁电换能器和嵌有六个磁铁的旋转摆构成.文中建立了摆式结构的摆动方程,分析了采集器的频率响应特性以及谐振时的机-磁-电转换特性,并对采集器输出电压波形进行了频谱分析.理论和实验研究表明:该采集器具有宽频和倍频特性,采集器样机在1 g(1 g=9.8 m/s~2)有效值加速度振动下,向下扫频时的半功率带宽达到4.8 Hz,且能在f=16.9 Hz的振动下获得3.569 mW的负载功率.利用双换能器以及采集器的倍频和宽频特性,能有效地提高低频时采集器的输出功率.     

目标物材料特性对激光语音获取的影响研究

为了扩大激光语音检测系统的应用场景,分析目标物材料参数对系统语音获取的影响,在完善语音获取中,语音信号从产生到与目标物作用的信号流程基础上,对目标物进行声致振动建模,以Sewell-Sharp-Cremer模型为基础,提出目标物声致振动幅度计算方法,并根据Matlab分析计算和实验对比了铁、铝、塑料、纸4种目标物的振幅及其对激光语音获取的影响。仿真及实验结果表明:目标物振幅在300 Hz～1 000 Hz呈指数型衰减,在1 000 Hz以上衰减趋于平缓;300 Hz处非金属材料振幅为69 nm和62 nm,高于金属材料的30 nm和10 nm。金属材料较非金属材料动态范围小,频率敏感度低,更适合作为语音获取的目标物。     

Molecular Constants of MnF6 −2 Anion

Abstract

The normal coordinate analysis of XY₆ type of anions and molecules employing different force fields is well established.^1,2 Recently, the vibrational spectra and complete frequency assignment of MnF₆ ^?2 has been reported by Flint.³ Using the available vibrational data the force constants have been evaluated employing three potential models viz. general valence force field (GVFF), Urey-Bradley force field (UBFF) and orbital valence force field (OVFF). The mean amplitudes of vibration and Bastiansen-Morino shrinkages have also been computed at two temperatures.     

Biaxially Self-Reinforced High-Density Polyethylene Prepared by Vibration-Assisted Injection Molding. I. Processing Conditions and Physical Properties

A pulse pressure was imposed on the melt in the injection molding cavity during the injection and holding pressure stages, called vibration-assisted injection molding (VAIM) technology. With the VAIM technology, biaxially self-reinforced high-density polyethylene (HDPE) samples were prepared and the physical properties affected by the vibration processing conditions were studied. The tensile properties can be improved in both the machine direction (MD) and the transverse direction (TD) by changing the vibration frequency and vibration pressure amplitude, respectively. The elongation at break increased with increasing the vibration frequency for the VAIM sample processed at constant low vibration pressure amplitude; the yield strength increased with increasing the vibration pressure amplitude for the VAIM sample prepared at constant low vibration frequency. The softening point temperature for the VAIM sample increased by 8°C compared with a conventional injection-molded (CIM) sample.     

磁场对量子阱中弱耦合束缚极化子性质的影响

采用线性组合算符及幺正变换方法研究了磁场对量子阱中弱耦合束缚极化子的性质的影响。导出了量子阱中束缚极化子的基态能量与振动频率、库仑束缚势、磁场和阱宽之间的变化关系。同时也讨论了振动频率与库仑束缚势、磁场之间的变化关系。通过数值计算结果表明:量子阱中束缚极化子的基态能量因振动频率、库仑束缚势、磁场和阱宽的不同而不同,它随振动频率和磁场的增加而增大,随库仑束缚势和阱宽的增大而减小。量子阱中束缚磁极化子的基态能量与振动频率无关,随库仑束缚势和阱宽的增大而减小,随磁场的增大而增大。