阶梯圆盘的设计及其声参数计算

由薄圆盘改进而来的阶梯型薄圆盘声波辐射器在空气中有着很好的应用,但由于阶梯的存在,需要根据在节线处位移连续、位移斜率连续、剪切力连续以及弯矩连续,加之其边界条件才能推导出频率方程。多一条节线,则多四个方程。变量多,方程系数复杂,频率方程难解。本文以单节线阶梯圆盘为例,提出了一种数值计算方法,编制了计算程序。计算结果与实验测试值符合较好。更进一步,可计算得到阶梯盘的声场分布、辐射阻抗等声学特性。本文为阶梯圆盘的设计和其声学性能的计算提供了一种方法。      

球冠型换能器声辐射指向性分析

为了研究球冠型换能器的声辐射特性,在分离变量法求解球面坐标系下波动方程的基础上,采用基于球谐基傅里叶变换及边界条件的求解模型,给出了球冠型换能器声辐射的远场声压计算表达式和远场指向性表达式;仿真计算了球冠换能器的远场指向性随球冠极角、球半径及振动频率变化的特性,球冠所在球障板的直径和介质中声波的波长比决定着球冠声辐射指向性,在低频或波长大于球障板直径时,球冠声辐射呈无指向性,随着频率的增高即波长的减小或者球障板直径的增大,球冠声辐射的指向性越明显,波束开角越趋向于球冠的开角,而且波束开角内出现波浪状起伏越明显;试制了高频球冠型换能器基阵,测试了换能器基阵300 kHz的指向性,测试结果与理论计算相符合,验证了理论计算表达式的正确性,可为设计球冠型换能器及基阵提供理论指导。      

Er_2O_3薄膜型热辐射体的制备与性能研究

调制辐射体的可见和近红外区域的辐射光谱与光伏电池吸收光谱的匹配是开发高性能热光伏电池技术的关键.采用电子束蒸发在单晶硅衬底上制备金属Er薄膜并进行后氧化处理制备Er_2O_3薄膜型辐射体.X射线衍射结果表明薄膜结晶良好,且Si基底对Er_2O_3薄膜的晶体结构没有显著影响.X射线光电子能谱拟合结果表明薄膜中Er元素和O元素符合Er_2O_3的化学计量比.高温近红外光谱测试结果表明,样品在1550 nm左右出现了明显的Er~(3+)离子的特征辐射峰,这与GaSb光电池的吸收光谱相匹配.     

指向性辐射器的简正波声场

本文讨论比较一般的指向性辐射器在分层介质中的声场,并将指向性概念应用于简正波计算。结果表明,对无方向性点源的简正波表示式补充以指向性激发函数,就可得到指向性辐射器的简正波声场,而指向性激发函数与辐射器的位置及指向特性有关。文中还分别计算了具有垂直对称性、反对称性、单边指向性以及尖锐指向性的辐射器的简正波声场。对于均匀水层中的垂直线阵,若源的分布函数正比于某一简正波的本征函数,则指向性激发函数的零点正好对应于其他简正波的本征射线的方向。 关键词：     

低频三阶超心形指向性声源设计

为提高圆周阵列主极大的指向性增益,提出基于圆周等间距六元密排阵的低频三阶超心形指向性声源,利用点源方法对其波束特性进行研究与分析,得到了指向性声源的优化方案。以具有弱互辐射效应的单边辐射弯张换能器作为圆周密排阵阵元,利用有限元方法分析了三阶超心形指向性声源的声辐射特性,相比单极子声源,其主极大方向指向性增益为8.0 dB,可达到提高增益的目的。研制了实验样机,经水池实验获得该声源的工作特性:谐振频率为0.92 kHz,对应发送电压响应级为139.0 dB,-3 dB波束宽度为56.0°,各旁瓣小于-15.0 dB。有限元计算与实测结果验证了优化方案的可行性,实现了低频三阶超心形指向性发射。     

一种紧凑型宽带高功率微波源设计与测试研究

设计了一款体积紧凑、工作在特高频波段的宽带高功率微波源,系统利用24 V蓄电池供电,Marx发生器作为驱动源,采用四分之一波长开关振荡器调制产生宽带电磁脉冲,激励高功率微带平板天线辐射,测试结果显示系统工作中心频率为425 MHz,远场辐射场强-距离积峰峰值为91.5 kV@1 m,该微波源体积尺寸为871 mm×370 mm×330 mm,含电池质量小于43 kg,拓展了宽带高功率微波技术在无人机、机器人等平台的应用前景。     

图像光谱技术实现精确测温

建立了一种以灰体辐射为基础测量温度的新方法,它不仅可以测定辐射体的实时温度,而且可以实现无接触和高精度测量。首先,利用多通道CCD图像光谱仪精确测量辐射体在较宽波段内的辐射光谱,作为该辐射体的指纹光谱,将其定义为一个等效的灰体;其次,通过对所测光谱的拟合确定该辐射体的灰体辐射模型的系数,从而确定待测辐射体的灰体辐射模型;最后,通过光谱技术与灰体辐射模型的结合确定给定辐射体的任意温度。通过对无火焰和有火焰这两类热辐射体的实验检验,表明该测温方法具有实时、准确和无接触等优点。     

板厚对无障薄板声辐射特性影响的分析

分析无障薄板的声辐射特性时通常忽略板厚对格林函数的影响而采用双层势计算.本文考虑板厚引起的声辐射阻抗,采用混合势计算结构表面声压与振速,并分析板厚对声辐射参数的影响。根据交界相容性条件,采用边界积分方程分别表示平板上下表面的声压和振速,并合并同类项.进一步将结构的动力方程代入混合势形式的振速方程中,离散声压差值和板的位移为振动模态叠加的形式,获得二重积分形式的声辐射阻抗,从而求解振动模态系数,确定声辐射特性参数.以水下简支矩形板为例计算对比了声辐射参数,并讨论了其对板厚的敏感性。结果表明:板厚引起的声辐射阻抗对声辐射参数的大小影响较小,但随着频率的增加致使共振频率发生较大偏移;在相同阶数的共振频率范围内,板厚度越大,采用双层势计算的误差越大。      

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。     

六方氮化铝纳米线本征缺陷和氧杂质的光致发光谱研究

利用AlCl3和NaN3直接反应合成出六方结构氮化铝纳米线.变温光致发光谱显示,在可见光范围内有两个半高宽大约为5 nm的尖锐辐射峰,中心波长分别位于413 nm和422 nm处.同时,在近紫外区还有一个较宽的辐射带,随着温度升高,该辐射峰发生了明显的红移现象,其中心波长随温度线性变化.理论和实验分析表明,413 nm辐射与AlN本身性质无关,而422 nm辐射峰是与A1有关的两种本征缺陷所致.     

Nodal line optimization and its application to violin top plate design

In the literature, most problems of structural vibration have been formulated to adjust a specific natural frequency: for example, to maximize the first natural frequency. In musical instruments like a violin; however, mode shapes are equally important because they are related to sound quality in the way that natural frequencies are related to the octave. The shapes of nodal lines, which represent the natural mode shapes, are generally known to have a unique feature for good violins. Among the few studies on mode shape optimization, one typical study addresses the optimization of nodal point location for reducing vibration in a one-dimensional beam structure. However, nodal line optimization, which is required in violin plate design, has not yet been considered. In this paper, the central idea of controlling the shape of the nodal lines is proposed and then applied to violin top plate design. Finite element model for a violin top plate was constructed using shell elements. Then, optimization was performed to minimize the square sum of the displacement of selected nodes located along the target nodal lines by varying the thicknesses of the top plate. We conducted nodal line optimization for the second and the fifth modes together at the same time, and the results showed that the nodal lines obtained match well with the target nodal lines. The information on plate thickness distribution from nodal line optimization would be valuable for tailored trimming of a violin top plate for the given performances.     

Effects of driving frequency of longitudinal transducer on the vibration characteristics of a stepped plate

The flexural vibration characteristics of a stepped plate, driven at its center by different frequency of longitudinal transducer with a certain area are investigated. The variation in the nodal circle, fundamental frequency and displacement distribution of the stepped plate are calculated by using finite element method (FEM) under different driving frequencies. The results show that the fundamental frequency and nodal circle of the flexural-vibration stepped plate (FVSP) increase with an increase in the driving frequency of the longitudinal vibration ultrasonic transducer (LVUT), before the second-order flexural vibration occurs. When the driving frequency is f = 28 kHz, the displacement amplitude of the stepped plate can achieve the maximum, and the nodal circle radius of the stepped plate is 2.61 cm which fits evenly the edge of stepped profile. Meanwhile, the directivity and radiation efficiency of the FVSP would be greatly improved in a special driving frequency. The conclusions agree with the experimental ones and are significant for both design and applications of the stepped plate.     

Vibration of moderately thick square orthotropic stepped thickness plates

Numerous studies that address the vibration of stepped thickness plates are reported in the literature. Predominately, classical plate theory has been used to formulate studies for both isotropic and anisotropic stepped plates. Mindlin plate theory has been employed to obtain results for thick isotropic stepped thickness plates. Exact solutions, Rayleigh-Ritz, differential quadrature and finite element methods have been employed to compute results for frequency of vibration. Results for frequency of vibration for thick orthotropic stepped thickness plates are presented here using orthorhombic material properties of aragonite. The finite element method has been used to compute frequencies and determine mode shapes for simply supported and clamped square Mindlin plates.     

Radiation efficiency of a guitar top plate linked with edge or corner modes and intercell cancellation

This paper was based on a theoretical framework to determine strong and weak radiation by a guitar top plate, vibrating through deflections hard to analyze: multipolar mode shapes. The air-structure interaction was examined in terms of edge modes or corner modes, and considering even or odd number modes. A numerical model was implemented and experimentally calibrated, exhibiting several advantages exploring the coupling between vibratory and acoustic waves in a top plate. Two analyses were applied detecting high or low radiation efficiency for the structure. First, the addition of volume velocity for odd numbers of poles and cancellation for even numbers were examined. In fact, both behaviors can happen at the same time, as it was shown for a corner radiator case used as an example. Second, the ratio between bending and acoustic wavenumbers was explored. To illustrate the importance of this ratio, some theoretical features of a more efficient radiator than the corner mode were exposed in an edge mode example. Labeling multipolar mode shapes as efficient or inefficient radiators showed to be a useful alternative analyzing the top plate behavior. It can be applied knowing the nodal lines of the vibration pattern and estimating the bending and acoustic wavelengths.     

Analysis of flexural wave velocity and vibration mode in thin cylindrical shell

The relationship between the flexural wave velocity and the excited vibration mode of a thin cylindrical shell is investigated. The natural frequency corresponding to the vibration mode is obtained as the solution of characteristic equation of thin cylindrical shell. However, all of these vibration modes are not excited actually. To estimate the excited vibration mode, the concept of "modified bending stiffness" is introduced, and the influence of each stress component upon the modified bending stiffness is analyzed. The excited mode is theoretically discriminated from the nonexcited mode based on the smallness of this modified bending stiffness. The validity of our theory is confirmed by an excellent agreement between theoretical and experimental results on flexural wave velocity.     

Exact solutions of in-plane natural vibration of a circular plate with outer edge restrained elastically

We solve exactly the equations of in-plane natural vibration for a circular plate whose outer edge is restrained elastically. The mode shapes are represented by trigonometric functions with a number of nodal diameters in the circumferential direction and mode functions in the radial direction. We present the exact frequency equations and mode functions and tabulate the frequency parameters satisfying the frequency equations. The corresponding mode functions and two-dimensional mode shapes are illustrated when both radial and tangential stiffness are zero (free edge), infinity (clamped edge), or medium. Comparisons with previous reported results confirm the accuracy of the present work.     

Study of a new type linear ultrasonic motor with double-driving feet

A new type linear USM with double-driving feet has been developed. The stator consists of eight piezoelectric ceramic plates and one brass plate. Piezoelectric ceramics plates are polarized along the thickness and are symmetrically bonded to the two surfaces of one rectangle brass plate. Double-driving feet are assembled on the same side of the brass plate. The working vibration mode is a composite in-plane bimode, which consists of the first longitudinal in-plane vibration mode and the second bending one. The basic size of the linear USM is determined carefully by FEA. The characteristics of the prototype motor were measured experimentally.     

Experimental investigation on the flow over normal flat plates with various corner shapes

The influence of corner modification on the flow over normal flat plates is experimentally investigated in a water tunnel. Particle image velocimetry measurement is performed at Re = 2240 based on the width of the plate. Besides the flat plate with sharp edges, others with chamfered corners, rounded corners and stepped corners at the windward side are studied. Although the flat plate is very thin compared with square cylinders, corner modification can also achieve a significant drag reduction. The mechanism for the drag reduction is explored based on the solid analysis of the vortical structures and the statistical parameters. With corner modification, the strength and the scale of the vortex are decreased, while the formation of the vortex is postponed, resulting in a weakened vortex-interaction process. Thus, the fluctuation intensity of the wake is weakened, the wake width is narrowed down with the recirculation region elongated, and the vortex shedding frequency becomes higher. These modifications interpret well how the drag of a normal plate could be reduced, which is confirmed by the drag estimation from the wake profiles.     

Complex vibration ultrasonic welding systems with large area welding tips

Vibration and welding characteristics of complex vibration ultrasonic welding systems of 27 and 40 kHz were studied. Complex vibration systems, which have elliptical to circular or rectangular to square locus, are effective for ultrasonic welding of various specimens including the same and different metal specimens, and for direct welding of semiconductor tips and packaging of various electronic devices without solder. The complex vibration systems consist of a one-dimensional longitudinal-torsional vibration converter with slitted part, a stepped horn and a longitudinal vibration transducer as a driving source. The complex vibration welding tips of 27 and 40 kHz have enough area of 6-8 mm square for various welding specimens. Aluminum plate specimens of 0.3-1.0 mm thickness were successfully joined with weld strengths almost equal to aluminum specimen strength, and independent to the specimen direction. Required vibration amplitude of 40 kHz is smaller than that of 27 kHz.