A NEW CRITERION OF COMBINED TYPE CRACK—THE CRITERION OF MINIMUM DISTANCE(r_(min))IN PLASTIC REGION

The existence of the plastic area around the crack tip is an important factor against thecracking.In this plastic region.the cracking most likely develops in such a direction alongwhich the distance from the existant crack tip to the plastic region edge is the shortest one.Substituting the stress components at the crack tip for a combined cracking into R.Von.Mises equation of yielding condition,the boundary equation of the plastic regionaround the crack tip can be expressed as:where r is the distance from the crack tip to the boundary of plastic region.The direction inwhich the cracking develops can be determined by following conditions:One form of the material failures is the slipping under the action of shear stress.Underthe conditions of complex stress,the octahedral shear stress on a point around the crack tipis here.B devotes the.factor of the octahedral shear stress,which relates to the size. pattern ofcrack and the exerted stress.Its magnitude reflects the strength of the stress field aroundthe c     

点式压电智能结构的模型修正与振动主动控制

提出了在点式压电智能结构中应用摄动有限元方法对结构的有限元模型进行修正 ,从而达到提高建模精度 ,改善实际结构振动主动控制效果的目的。通过对一悬臂梁在模型修正前后进行振动主动控制的不同的控制效果验证了该方法的有效性     

雅砻江锦屏水电站工程区活动构造研究及地壳稳定性评价

北东向的锦屏山-小金河断裂带从北东到南西斜穿整个锦屏水电站工程区。在它的东南和西北分别有北北西走向的羊坪子-纸厂沟断层组和北西走向的前波、高牛场等断层。锦屏山-小金河断裂带的马山头-周家坪断层组、瓦科断层组和北西向前波断层等晚第四纪继续活动, 但活动强度很弱。工程区新构造运动以整体抬升为主, 兼水平滑移和旋转运动。历史至今, 工程区地震活动微弱, 是地壳相对稳定的地区。     

考虑地基-结构-散粒体相互作用时贮仓结构的静、动力研究[Ⅱ]--有限元分析

对贮仓结构的静、动力问题进行了系统的分析计算：考虑到地基—结构—散粒体间的相互作用，引入新的计算模式，对不同地基上的贮仓结构模型进行了系统的有限元静、动力分析计算，并与作者所完成的试验结果进行了比较。结果表明，所提出的计算模式及有限元计算模型是正确的。     

4:1椭球体分离流动湍流特性的试验研究

使用六线涡量探头,对α=30°条件下绕（4:1）椭球体分离流动的湍动能u’2,v’2,w’2,雷诺应力u’v’和涡量Ωx等进行了详尽的测量.应用频谱分析的方法揭示了绕（4:1）椭球体分离流内主附着涡外缘剪切层上的离散小涡的特性.     

广义协调平板型矩形壳元

本文根据修正势能原理通过广义协调方法提出了一种列式简单的平板型矩形壳元ＧＣＲ２４。它在四个角点处各有六个自由度，总共二十四个自由度。作为一种极限协调元，单元的收敛性得到保证，并且不发生薄膜闭锁现象。通过标准问题的数值检验，表明本文提出的平板型矩形薄壳元是性能可靠、计算精度高的优质单元。     

Sulfur Immobilized in Hierarchically Porous Structured Carbon as Cathodes for Lithium–Sulfur Battery with Improved Electrochemical Performance

In order to overcome the main obstacles for lithium–sulfur batteries, such as poor conductivity of sulfur, polysulfide intermediate dissolution, and large volume change generated during the cycle process, a hard‐template route is developed to synthesize large‐surface area carbon with abundant micropores and mesopores to immobilize sulfur species. The microstructures of the C/S hybrids are investigated using field emission scanning electron microscopy, transmission electron microscopy, X‐ray diffraction, Raman spectroscopy, X‐ray photoelectron spectroscopy, nitrogen adsorption–desorption isotherms, and electrochemical impedance spectroscopy techniques. The large surface and porous structure can effectively alleviate large strain due to the lithiation/delithiation process. More importantly, the micropores can effectively confine small molecules of sulfur in the form of S_2–4, avoiding loss of active S species and dissolution of high‐order lithium polysulfides. The porous C/S hybrids show significantly enhanced electrochemical performance with good cycling stability, high specific capacity, and rate capability. The C/S‐39 hybrid with an optimal content of 39 wt% S shows a reversible capacity of 780 mA h g^?1 after 100 cycles at the current density of 100 mA g^?1. Even at a current density of 5 A g^?1, the reversible capacity of C/S‐39 can still maintain at 420 mA h g^?1 after 60 cycles. This strategy offers a new way for solving long‐term reversibility obstacle and designing new cathode electrode architectures.     

碲化铋取向纳米柱状薄膜热导率测量

将热电材料制作成纳米柱状薄膜结构是一种理论上能有效降低热导率、从而大幅提升热电优值的操控手段。但是随之而来的问题是纳米柱状薄膜热导率的精确获取困难,因为常规的热物性测试手段已无法适用于该类表面多孔、厚度为微米量级结构热输运特性的表征。本文提出利用3ω方法可实现Bi_2Te_3取向纳米柱状薄膜热导率实验表征的测量结构,并且获得了纳米柱状薄膜的热导率和热扩散率值。该方法有望用于微米厚纳米柱状薄膜结构热输运性能的实验评价。     

用波晶片相位板产生角动量可调的无衍射涡旋空心光束

本文提出了一种用波晶片产生无衍射涡旋空心光束的新方案. 根据晶体双折射的性质, 设计波晶片的厚度, 在一块晶体薄片上对o光和e光分别形成各自的四台阶相位板, 线偏振光入射到该相位板后, o光和e光衍射按强度叠加, 利用准伽利略望远镜系统聚焦, 得到近似无衍射涡旋空心光束. 光路简单, 调节方便. 在近轴条件下, 运用菲涅耳衍射理论和经典电磁场角动量理论, 数值模拟计算了周期数不同的两块波晶片相位板衍射光强和角动量的分布, 结果表明: 两块相位板都能在较长距离内产生近似无衍射涡旋空心光束, 光强和轨道角动量的分布与螺旋相位板产生的涡旋光束基本相同. 在衍射光路中加入相位补偿器, 调节o光和e光的相位差可以调节自旋角动量的大小, 从而可以调节总角动量密度和平均光子角动量的大小. 用这种空心光束导引冷原子或冷分子, 原子在与光子相互作用过程中可获得可调的转动力矩.