水平均布荷载作用在地基内部时的土中应力公式

本文根据半无限体内受水平集中力作用的明德林公式，通过积分而首次完整地推导出水平矩形均布荷载作用在地基内部时的土中应力分量的解析表达式，以便工程设计人员在设计时使用。     

安全壳再循环地坑滤网应力分析

安全壳再循环地坑滤网是核电厂安全系统的重要设备,再循环工况下它的工作状况直接影响到安全注射系统(应急堆芯冷却系统)、安全壳喷淋系统的正常运行.本文对滤网结构进行在自重和接管载荷下的静态分析、模态分析和地震谱分析.并对结构各使用限制条件下的应力进行组合和评定.结果显示,滤网结构满足ASMEⅢ的规范要求.文章也阐述了结构各方面参数对结构抗震性能的影响.     

PORE STRUCTURE CHARACTERISTICS OF DEPOSITS FORMED DURING FIBER BUNDLE MEDIA FILTRATION

Scanning electronic microscope was adopted to investigate the pore structure of deposits formed during polypropylene fiber bundle filtration.The effects of flocculants.cationic polyacrylamide and polyaluminumchloride,on the pore structure and filtration process were examined.It is found from experimental results that the filter deposit has a self-similarity pore structure.which can be described in fractal dimensions.     

Designing a forwarder operation considering tolerable soil disturbance and minimum total cost

A model is developed to minimize the sum of road construction plus forwarding costs with the constraint that rut depth caused by the forwarder cannot exceed a maximum depth during the anticipated season of operation. Road spacing, forwarder trail spacing, forwarder size, forwarder load capacity, and tire inflation pressures are used as decision variables in developing the transportation plan. The total cost was minimized using the optimum road spacing approach. The model identifies whether the cumulative rut depth caused by the forwarder exceeds the maximum allowable rut depth at the point of or prior to the spacing that minimizes the cost, and if so, the rut depth limits the road spacing. If the road spacing at the point of minimum cost is less than the road spacing at the maximum allowable rut depth, road spacing is not constrained by rut depth. This model will help logging managers to evaluate the trade-offs between specified decision variables and then to design an optimum forwarder operation with tolerable soil disturbance and minimum total cost. The solution procedure of the model is described and a computer program is used to apply this model using a numerical example.     

明渠梯形断面临界水深的近似计算公式

本文用摄动法求得了明渠梯形断面临界水深的近似计算公式,其理论较文献[1]严密.     

有限深抛物势量子盘中极化子的激发态性质

量子点作为一种重要的低维纳米结构, 近年来在单光子光源和新型量子点单光子探测器的研究引起了人们的广泛关注, 对各种势阱中量子点性质的研究已取得了重要成果. 但是大多理论研究都局限于无限深势阱, 而有限深势阱更具有实际意义. 利用平面波展开、幺正变换和变分相结合的方法研究了有限深势阱中极化子激发态能量及激发能随势阱形状和量子盘大小的变化规律. 数值计算结果表明: 极化子的激发态能量、激发能随势垒高度或宽度的增大而增大, 原因是势垒愈高、愈宽, 电子穿透势垒的可能性愈小, 电子在阱内运动的可能性愈大, 进而导致极化子的激发态能量和激发能均随势垒高度和宽度的增大而增大; 极化子的激发态能量和激发能随量子盘半径的增大而减小, 表明量子盘具有显著的量子尺寸效应; 极化子的激发态能量随有效受限长度的增加而减小, 原因是有效受限长度愈大, 有效受限强度愈小, 电子受到的束缚愈弱、振动愈慢、势能愈小, 进而导致基态能量、激发态能量减小; 同时由于激发态能量较基态能量减小慢, 使得激发能随之增加. 研究结果对量子点的应用具有一定的理论指导意义.     

非中心对称超导序参量研究

非中心对称超导体是近年发现的一类新型超导材料. 在这类材料中, 非中心对称的晶体势场产生一个有效的反对称自旋-轨道耦合(ASOC)并导致自旋简并的能级发生分裂, 从而在超导配对态中允许自旋单态和自旋三重态混合. 这一性质有别于先前研究的大部分超导体, 需要从概念上突破BCS理论框架. 此外, 理论研究还表明非中心对称超导可能还是一类潜在的拓扑超导材料. 这些独特的物理性质已激发了广泛的研究兴趣, 并且越来越受到关注.#br#超导序参量的对称性是认识和理解超导形成机理的一个重要物理量. 本文将介绍基于隧道二极管的伦敦穿透深度测量技术, 并简要综述非中心对称超导的研究现状以及穿透深度测量在非中心对称超导序参量研究中的应用. 通过对比研究具有不同反对称自旋-轨道耦合强度的非中心对称超导材料, 我们发现其混合超导配对态与反对称自旋-轨道耦合强度缺乏简单的对应关系, 但与能带劈裂(E_ASOC)相对于超导转变温度(T_c)的比值(E_r=E_ASOC/T_c)紧密相关.     

Surface morphology and amide concentration depth profile of aminolyzed poly(ethylene terephthalate) films

Surface of biaxially oriented poly(ethylene terephthalate) films was chemically modified by exposure to ethylenediamine (EDA), triethylenetetramine (TETA), and tetraethylenepentamine (TEPA) for different treatment times. Variable angle attenuated total reflection Fourier transform infrared (ATR‐FTIR) spectroscopy was used in conjunction with weight loss measurements, scanning electron microscopy (SEM), and atomic force microscopy to establish the surface modification and to draw the depth profile of the newly created species, with emphasis on amide group. A clear differentiation was found between the effects of the three amines studied: EDA produces the highest amidation degree but, because of its deep penetration into the film, leads to delamination of rather thick layers, TETA reacts at and near surface and develops surface cracks without delamination, and TEPA is the mildest reactant, generating amide groups on the surface without visible deterioration of the sample. It was proved that the amide II absorption band became weaker with increasing analyzed depth, with a pronounced heterogeneity near the surface. SEM micrographs showed the development of cracks onto the surface at longer aminolysis time, which allowed a better understanding of ATR‐FTIR observations. Assuming an exponential decay for the depth profile spectrally obtained, the surface concentration of amide groups and the decay constant were determined for the amines and reaction times used. © 2010 Wiley Periodicals, Inc. J Polym Sci Part A: Polym Chem, 2010     

Ultra-elongated depth of focus of plasmonic lenses with concentric elliptical slits under Gaussian beam illumination

In this paper, we discuss the influence of ratio of minor to major axis on the propagation property and focusing performance of a plasmonic lens with variant periodic concentric elliptical slits illuminating under a Gaussian beam. In order to analyse the influence theoretically, a finite-difference time-domain （FDTD） numerical algorithm is adopted for the computational numerical calculation and the design of the plasmonic structure. The structure is flanked with penetrated slits through a 200-nm metal film （Au） which is coated on a quartz substrate. Tunability of focusing capability of the plasmonic lenses is studied by tailoring the ratio. Our calculation results demonstrate that the ratio of the elliptical slits greatly affects the focusing capability of the lense. The plasmonic lenses with concentric elliptical slits illuminating under a Gaussian beam have ultra-elongated depth of focus. These results are very encouraging for the future study of the plasmonic lens-based applications.     

Depth‐integrated free‐surface flow with a two‐layer non‐hydrostatic formulation

This paper presents the derivation of a depth‐integrated wave propagation and runup model from a system of governing equations for two‐layer non‐hydrostatic flows. The governing equations are transformed into an equivalent, depth‐integrated system, which separately describes the flux‐dominated and dispersion‐dominated processes. The depth‐integrated system reproduces the linear dispersion relation within a 5 error for water depth parameter up to kd = 11, while allowing direct implementation of a momentum conservation scheme to model wave breaking and a moving‐waterline technique for runup calculation. A staggered finite‐difference scheme discretizes the governing equations in the horizontal dimension and the Keller box scheme reconstructs the non‐hydrostatic terms in the vertical direction. An semi‐implicit scheme integrates the depth‐integrated flow in time with the non‐hydrostatic pressure determined from a Poisson‐type equation. The model is verified with solitary wave propagation in a channel of uniform depth and validated with previous laboratory experiments for wave transformation over a submerged bar, a plane beach, and fringing reefs. Copyright © 2011 John Wiley & Sons, Ltd.