一维声子晶体中声波能带的解析研究

为了对一维声子晶体的能带进行解析研究,采用一维声子晶体的色散法,推导出一维声子晶体禁带频率和通带频率的解析公式;并利用此式对一维声子晶体的能带结构进行了解析研究,得到了禁带和导带的频率中心、频率宽度分别随介质厚度和声阻抗两者的变化规律,并与转移矩阵方法的计算结果进行了比较.研究结果表明:两种方法得到的结论相同,但解析法能更准确、更深刻地反映出一维声子晶体的能带随介质厚度和声阻抗等因素的变化规律;并且解析法克服了转移矩阵法等其他方法不能对能带结构进行解析研究的不足,是一种研究一维声子晶体能带更有效的方法.     

正负折射率的一维圆形受限光子晶体特性研究

对正负折射率材料构成的一维光子晶体,在横向圆形受限的条件下,推出了光波在其中传播时模式所满足的条件,并利用特征矩阵法研究了正负折射率绝对值相同时,光波在不同模式和不同介质厚度可见光能实现透射波和零反射。正负折射率绝对值不等时,得出介质厚度为半波长时透射波出现在中心波长处;随着模式数即入射角增大,透射波曲线向短波方向移动;介质折射率差的绝对值越大、周期数增加都使透射波谱宽度变窄。     

SH波在局部非均匀声子晶体中的传播

使用传输矩阵法,研究了水平剪切波(SH波)在一维局部材料非均匀声子晶体中的传播。首先使用皮亚诺方程给出了SH波在特定非均匀梯度介质声场的传输矩阵。然后使用传输矩阵和布洛赫定律给出了该声子晶体的禁带结构和传输系数。通过具体计算,发现这种非均匀性能明显影响声子晶体的频散曲线和禁带结构。然后比较了幂指数取不同值时,禁带结构与归一化频率和填充比的关系。发现幂指数不同,声子晶体的禁带不同。     

一维固液介质准周期结构声子晶体的传输特性

针对一维固液介质的Fibonacci序列准周期声子晶体,利用传输矩阵法研究了弹性纵波在准周期结构中的透射特性。计算结果表明：准周期结构具有比周期结构更宽的禁带,并伴随带边谐振;序列越高,带边谐振越强,并在较低序列的禁带中心出现谐振模;弹性波以0.1rad斜入射时,透射谱向高频方向移动;当固液介质波阻抗接近时,出现等间距的谐振模,同时禁带消失。     

光子晶体应变片的基本原理

光子晶体是人造的周期性结构材料。作为一种复合材料,各组份的介电性质及其空间排列方式决定了光子晶体具有独特的光带隙性能。光子晶体受力变形后必然会改变各组份的空间排列方式,从而改变其光带隙性能。本文利用数值方法模拟了一维光子晶体承受正应变时对其光带隙性能的影响,发现应变的大小与禁带起始波长及截止波长之间存在简单的线性关系。既通过测量光子晶体的光带隙性能就可以得知应变的大小,从而验证了制造光子晶体应变片的可行性。这种应变片的优点是不需要导线相联,而且没有活动部件。     

折射率介质在制栅和云纹干涉法中的应用

本文在已有的高折射率介质制栅方法的基础上提出了一种新的制作超高频全息光栅的方法,该方法制栅准确、简单、方便,其特点是所制光栅的频率与激光波长及介质的折射率无直接关系,而是等于制栅光路所得频率与两倍母栅频率之和.该制栅原理同时被推广应用于云纹干涉法中.     

弹性波斜入射声子晶体的传输特性

引入四维波矢的概念,推导出弹性波斜入射到多层介质系统的转移矩阵以及透射系数和反射系数公式.利用这些公式计算了横波和纵波斜入射一维声子晶体时横渡和纵波的透射系数,得出横波斜入射,透射波中的横波和纵波在一定频率范围内都会出现禁带,纵波斜入射时也有类似的结果.透射波中横波与纵波的相互转型随着入射角的增大而越加明显.     

一种三芯液晶光子晶体光纤的特性

针对三轴光纤陀螺共用光源问题,提出了一种新型的多芯液晶光子晶体光纤,该光纤具有三个呈等边三角形几何形状排列的液晶纤芯.利用有限元法对其功率分布、模场、有效折射率和色散特性进行了数值分析,结果表明,这种三芯液晶光子晶体光纤可将传输光完全等分为三束光,且具有平坦色散特性,在波长为1.45μm～1.75μm之间的色散变化小于2 ps·km-1·nm-1.此外,该光纤在大约150 nm的波长范围内显示出超平坦的色散,并且可以通过改变中心空气孔的直径来调整超平坦色散的波长范围.研究成果对液晶光子晶体光纤、三轴光纤陀螺和三相光纤电流互感器的等光分束器、1×3多芯光子晶体耦合器和平坦色散光纤的进一步发展具有重要意义.     

一种三芯液晶光子晶体光纤的特性（英文）

针对三轴光纤陀螺共用光源问题,提出了一种新型的多芯液晶光子晶体光纤,该光纤具有三个呈等边三角形几何形状排列的液晶纤芯。利用有限元法对其功率分布、模场、有效折射率和色散特性进行了数值分析,结果表明,这种三芯液晶光子晶体光纤可将传输光完全等分为三束光,且具有平坦色散特性,在波长为1.45μm~1.75μm之间的色散变化小于2 ps·km~(-1)·nm~(-1)。此外,该光纤在大约150 nm的波长范围内显示出超平坦的色散,并且可以通过改变中心空气孔的直径来调整超平坦色散的波长范围。研究成果对液晶光子晶体光纤、三轴光纤陀螺和三相光纤电流互感器的等光分束器、1×3多芯光子晶体耦合器和平坦色散光纤的进一步发展具有重要意义。     

一维声子晶体带隙的非局部辛分析

周期性弹性复合结构(声子晶体)中传播的弹性波存在特殊的色散关系:弹性波只能在某段频率范围内无损耗的传播,该频率范围称为通带.一维声子晶体的色散问题可以看作分层介质中弹性波的传播问题,利用二维弹性理论予以分析.为了研究非局部效应对声子晶体带隙特性的影响,将Eringen的二维非局部弹性理论引入到Hamilton体系下,利用精细积分与扩展的Wittrick Williams算法可获取任意频率范围内的本征解.通过对不同算例的数值计算,分析和对比了非局部理论方法与传统局部理论方法的差别.并进一步指出了该套算法的适用性和优势所在.     

The 7th International Conference on Fluid Mechanics May 24-27,2015,Qingdao,China

正http://www.icfm7.org First Announcement and Call for PapersThe objective of International Conference on Fluid Mechanics(ICFM)is to provide a forum for researchers to exchange new ideas and recent advances in the fields of theoretical,experimental,computational Fluid Mechanics as well as interdisciplinary subjects.It was successfully convened by the Chinese Society of Theoretical and Applied Mechanics(CSTAM)in Beijing(1987,     

INFORMATION FOR CONTRIBUTORS

Contributions： The Journal, Acta Mechanica Solida Sinica, is pleased to receive papers from engineers and scientists working in various aspects of solid mechanics. All contributions are subject to critical review prior to acceptance and publication.     

Preface

This special issue of PARTICUOLOGY is devoted to the first UK-China Particle Technology Forum taking place in Leeds, UK, on 1-3 April 2007. The forum was initiated by a number of UK and Chinese leading academics and organised by the University of Leeds in collaboration with Chinese Society of Particuology, Particle Technology Subject Group （PTSG） of the Institution of Chemical Engineers （IChemE）, Particle Characterisation Interest Group （PCIG） of the Royal Society of Chemistry （RSC） and International Fine Particle Research Institute （IFPRI）. The forum was supported financially by the Engineering and Physics Sciences Research Council （EPSRC） of United Kingdom,     

基于鲁棒滤波的捷联导引头视线角速度估计方法

针对捷联导引头无法直接获取视线角速度等信息的问题,研究了鲁棒滤波在大气层外飞行器捷联导引头视线角速度估计中的应用。为了建立非线性滤波估计模型,考虑目标视线角速度的慢变特性,采用一阶马尔科夫模型建立了状态方程;推导了视线角速度的解耦模型,并建立了量测方程;考虑到实际应用中存在系统噪声统计特性失准的问题,基于Huber-Based鲁棒滤波方法,设计了视线角速度滤波器,并完成了基于Huber-Based滤波方法和扩展卡尔曼滤波方法的数学仿真。仿真结果表明Huber-Based滤波方法的视线角、视线角速度及视线角加速度估计精度分别达到0.1140'、0.1423'/s、0.0203'/s2,而扩展卡尔曼滤波方法的视线角、视线角速度及视线角加速度估计精度仅分别为0.6577'、0.6415'/s、0.0979'/s~2。仿真结果证明了该方法可以有效地估计出相对视线角速度等信息,并且在非高斯噪声的条件下,依然可获得较高的估计精度,具有一定的鲁棒性。     

Guide for authors

正Each of the sections below provides essential information for authors.We recommend that you take the time to read them before submitting a contribution to Acta Mechanica Sinica.We hope our guide to authors may help you navigate to the appropriate section.How to prepare a submission This document provides an outline of the editorial process involved in publishing a scientific paper in Acta Mechanica     

Use specification of multiscale materials for life spanned over macro-, micro-, nano-, and pico-scale

Multiscale material intends to enhance the strength and life of mechanical systems by matching the transmitted spatiotemporal energy distribution to the constituents at the different scale, say—macro, micro, nano, and pico,—, depending on the needs. Lower scale entities are, particularly, critical to small size systems. Large structures are less sensitive to microscopic effects. Scale shifting laws will be developed for relating test data from nano-, micro-, and macro-specimens. The benefit of reinforcement at the lower scale constituents needs to be justified at the macroscopic scale. Filling the void and space in regions of high energy density is considered.Material inhomogeneity interacts with specimen size. Their combined effect is non-equilibrium. Energy exchange between the environment and specimen becomes increasingly more significant as the specimen size is reduced. Perturbation of the operational conditions can further aggravate the situation. Scale transitional functions and/or f_j/j+1 are introduced to quantify these characteristics. They are represented, respectively, by , and (f_mi/ma,f_na/mi,f_pi/na). The abbreviations pi, na, mi, and ma refer to pico, nano, micro and macro.Local damage is assumed to initiate at a small scale, grows to a larger scale, and terminate at an even larger scale. The mechanism of energy absorption and dissipation will be introduced to develop a consistent book keeping system. Compaction of mass density for constituents of size 10⁻¹², 10⁻⁹, 10⁻⁶, 10⁻³ m, will be considered. Energy dissipation at all scales must be accounted for. Dissipations at the smaller scale must not only be included but they must abide by the same physical and mathematical interpretation, in order to avoid inconsistencies when making connections with those at the larger scale where dissipations are eminent.Three fundamental Problems I, II, and III are stated. They correspond to the commonly used service conditions. Reference is made to a Representative Tip (RT), the location where energy absorption and dissipation takes place. The RT can be a crack tip or a particle. At the larger size scales, RT can refer to a region. Scale shifting of results from the very small to the very large is needed to identify the benefit of using multiscale materials.