三峡库区泄滩滑坡滑带土特征研究

在滑坡地质灾害勘察过程中,如何准确地辨识滑带土的特征和确定滑动面的具体位置,是让大多数工程技术人员都感到头痛的问题。本文以三峡库区泄滩古滑坡为例,较为详细地介绍了泄滩滑坡滑体的结构特征,以及通过勘探平硐、钻孔岩芯和地表露头等多种手段揭露的滑带土的基本特征。研究结果表明,泄滩滑坡滑带土中不仅可见明显的擦痕、镜面以及碎块石印模,而且在个别钻孔可见滑带土呈糜棱岩化现象,地表露头还可见到滑带土在地下水和高速下滑过程中被碾压、搓揉原有结构被破坏后又重新胶结的痕迹。同时,在滑带以下还存在一层特殊的滑坡影响带。泄滩滑坡滑带土特征非常典型,具有一定的代表性,可供同行在实际工作中确定滑面时参考。     

MRD与滑移隔震混合控制结构及其优化设计

为了改善滑移隔震结构的减震效果和适用范围,提出3种磁流变阻尼器(MRD)与滑移隔震混合方案,建立了MRD与滑移隔震混合控制结构的动力分析模型,对6层MRD与滑移隔震混合控制结构进行地震反应分析。MRD与滑移隔震混合结构的3种混合方案的相对加速度峰值、相对速度峰值、相对位移峰值和层间剪力峰值分别比滑移隔震结构有不同程度的降低,而混合方案3的控制效果更加明显。在此基础上,建立了MRD与滑移隔震混合结构优化设计模型,采用IHGA程序对结构进行优化设计。结果表明,MRD与滑移隔震混合结构的各项地震反应均得到了更好地控制。     

Non-uniform frictional sliding under cyclic loading with frictional characteristics changing in the process of sliding

Frictional sliding on a crack with non-uniform frictional characteristics is considered. The present work continues the investigation of Gorbatikh et al. [Int. J. Solids Struct., in press] and focuses on the cyclic loading. The evolution of the sliding process in loading–reloading–unloading cycles is analyzed. We also extend the analysis to the important case when the frictional resistance changes in the process of sliding (such changes may model “degradation” of the sliding surface during sliding, as well as other physical factors, not necessarily related to the sliding itself).     

界面接触特性对两种自组装分子膜摩擦特性的影响

利用多功能微摩擦磨损试验机，在不同滑动速度和载荷条件下，采用不同摩擦副分析了界面接触特性对自组装分子膜摩擦特性的影响，同时采用Lennard-Jone势对铜和镍与三氯十八硅烷(OTS)和3-氨基丙基-三甲氧基硅烷(APS)自组装分子膜之间的相互作用进行了比较。结果表明，镍同OTS和APS对摩的摩擦系数均大于铜同2种自组装分子膜对摩的摩擦系数，这是因为镍与自组装分子膜间具有较强的相互作用所致。铜和镍与OTS对摩的摩擦系数随滑动速度的增加而增大，随载荷增加而减小；铜与APS对摩的摩擦系数随滑动速度的增加而减小，载荷对摩擦系数的影响则很小；而镍与APS对摩的摩擦系数随滑动速度增加而增大，随载荷增加而减小．可以用分子弛豫来解释2种自组装分子膜的摩擦特性差异。     

西宁市林家崖滑坡稳定性研究

林家崖滑坡是一个具有上下两个滑体的滑坡系统，本文首先阐述其特性，对其变形控制因素及机理进行分析研究，并将常规Sarma法和基于Sarma法的基本原理的一种新的计算公式结合起来对该滑坡系统的稳定性进行了分析研究。指出，对于这种双层滑体滑坡，在进行稳定性分析时应视情况而增加考虑上滑体滑动效应，以使结果更合理，为滑坡治理设计提供更科学的依据。     

Sliding homoclinic orbits and bifurcations of three-dimensional piecewise affine systems

Sliding dynamics is a peculiar phenomenon to discontinuous dynamical systems, while homoclinic orbits play a role in studying the global dynamics of dynamical systems. This paper provides a method to ensure the existence of sliding homoclinic orbits of three-dimensional piecewise affine systems. In addition, sliding cycles are obtained by bifurcations of the systems with sliding homoclinic orbits to saddles. Two examples with simulations of sliding homoclinic orbits and sliding cycles are provided to illustrate the effectiveness of the results.

     

粉末冶金Cu-Fe复合材料的摩擦磨损行为

研究了 Ｆｅ 含量、施加载荷和滑动速度对粉末冶金 Ｃｕ Ｆｅ 复合材料摩擦磨损性能的影响,并用电子显微镜和 Ｘ 射线能谱分析了 Ｃｕ Ｆｅ 复合材料的磨损机理．结果表明：载荷和滑动速度对摩擦系数影响不大, Ｃｕ Ｆｅ 复合材料的摩擦系数随 Ｆｅ 含量的增加略有增加;在低载荷下,随 Ｆｅ 含量的增加, Ｃｕ Ｆｅ 复合材料的耐磨性提高;当载荷大于 ２００ Ｎ 时,含 Ｆｅ 量高的复合材料的耐磨性反而降低;在低载荷高速滑动条件下,随滑动速度的增加, Ｃｕ Ｆｅ 复合材料磨损率下降     

微/纳尺度粘着滑动接触的多尺度分析

采用分子动力学与有限元耦合的多尺度方法,求解二维刚性圆柱表面压头与弹性平面的微/纳尺度粘着滑动接触问题,通过与全分子动力学模拟结果的比较验证了多尺度方法的有效性。对压头半径、滑动速度、下压深度以及是否考虑粘着效应等对滑动接触性能的影响进行了全面研究,通过不同条件下摩擦力及接触力分布的比较,揭示了上述各参数对粘着滑动接触...     

边坡大距离整体滑移的模拟研究

边坡整体滑移模拟是迄今未被解决的一个课题。文章通过构制一个专门的滑面单元, 采用数值模拟的原理实现了对粘滑类边坡失稳的大距离滑移模拟; 采用分析模拟法实现了对脆性滑移类边坡失稳滑移的模拟, 并开发了相应的软件。     

高速干摩擦条件下铝基复合材料的摩擦磨损行为研究

在MMS-1G型高速干滑动摩擦磨损试验机上,采用铝基复合材料和蠕墨铸铁作为销试样,研究了速度和接触压力对摩擦副摩擦磨损特性的影响.结果表明:摩擦副的摩擦磨损特性受控于所产生的摩擦热、材料的导热能力以及材料保持一定塑性变形抗力的温度条件三者之间的耦合作用;随着速度与接触压力的增加,摩擦副的摩擦系数显著降低;不同材料表现出不同的磨损行为;接触压力愈高,材料的摩擦磨损性能差异愈小;在本文试验条件下,当摩擦速度较低(＜100 m/s)时,蠕墨铸铁表现出良好的摩擦磨损特性,而速度较高(＞100 m/s)时, 铝基复合材料表现出较优良的摩擦磨损性能.     

不同滑动干摩擦条件下钢／铁摩擦副的摩擦磨损性能与表面形貌特征研究

考察了不同滑动速度与接触压力条件下蠕墨铸铁的摩擦学性能及其三维表面形貌特征。结果表明：在与40Cr钢配副时,蠕墨铸铁的摩擦磨损性能与滑动速度和接触压力之积（pv值）呈现出良好的相关性;不同摩擦条件下的三维磨损表面形貌具有不同的特点,且主要表面形貌参数与pv值之间呈现出较好的相关性。     

碳钢表面碳—氮共渗层在高速干摩擦条件下的摩擦学性能研究

对 2 0 # 钢试样进行碳 -氮共渗热处理 ,考察了共渗层在高速干摩擦条件下的摩擦学性能 ,并用扫描电子显微镜和X射线光电子能谱仪对其磨损表面形貌和元素化学状态进行了分析 .结果表明 :随着滑动速度的增加 ,2 0 # 钢表面碳 -氮共渗层的磨损率逐渐降低 ,当滑动速度达到 35m/s左右时 ,磨损率显著增大 .扫描电子显微镜和X射线光电子能谱分析结果表明 ,高速轻载干摩擦条件下 2 0 # 钢表面碳 -氮共渗层的摩擦学性能同磨损表面氧化物的形成和剥落密切相关 ,而磨损率的显著增加是由于磨损表面氧化物类型发生从Fe2 O3 到FeO的转变所致 .     

锻压过程宏-细观跨尺度仿真研究

采用基于Voronoi图的微结构模型,针对Cr5锻件锻压过程中晶体之间滑移趋势进行了有限元仿真研究。并根据晶粒接触滑移角度的不同,对锻压过程中不同应力区域晶粒应力、滑移剪切力的不均匀分布进行了统计和分析。将宏观有限元分析的特定区域的分析结果耦合成相应尺寸的细观模型的边界条件,从而实现了针对应力集中区域的宏-细观跨尺度的仿真。所得结果表明,材料内部滑移趋势受接触滑移角度影响很大,位于宏观滑移区的材料,在细观模型中的滑移趋势同样明显。     

The Sliding Bifurcations in Planar Piecewise Smooth Differential Systems

In this paper we are mainly interested in the bifurcation phenomena for a class of planar piecewise smooth differential systems, where a new phenomenon, i.e. sliding heteroclinic bifurcation, is found. Furthermore we will show that the involved systems can present many interesting bifurcation phenomena, such as the (sliding) heteroclinic bifurcation, sliding (homoclinic) cycle bifurcation and semistable limit cycle bifurcation and so on. The system can have two hyperbolic limit cycles, which are bifurcated in one way from a semistable limit cycle, and in another way from a heteroclinic cycle and a sliding cycle. In the proof of our main results, we will use the geometric singular perturbation theory to analyze the dynamics near the sliding region.     

A finite element study of the deformations, forces, stress formations, and energy losses in sliding cylindrical contacts

This work presents the results of a finite element analysis (FEA) used to simulate two-dimensional (2D) sliding between two interfering elasto-plastic cylinders. The material for the cylinders is modeled as elastic-perfectly plastic and follows the von Mises yield criterion. The FEA provides trends in the deformations, reaction forces, stresses, and net energy losses as a function of the interference and sliding distance between the cylinders. Results are presented for both frictionless and frictional sliding and comparisons are drawn. The effects of plasticity and friction on energy loss during sliding are isolated. This work also presents empirical equations thatt relate the net energy loss due to sliding under an elasto-plastic deformation as a function of the sliding distance. Contour plots of the von Mises stresses are presented to show the formation and distribution of stresses with increasing plastic deformation as sliding progresses. This work shows that for the plastic loading cases the ratio of the horizontal force to the vertical reaction force is non-zero at the point where the cylinders are perfectly aligned about the vertical axis. In addition, a “load ratio” of the horizontal tugging force to the vertical reaction force is defined. Although this is analogous to the common definition of the coefficient of friction between sliding surfaces, it just contains the effect of energy loss in plasticity. The values of the contact half-width are obtained for different vertical interferences as sliding progresses.     

Adaptive terminal sliding mode control for nonlinear differential inclusion systems with disturbance

This paper deals with the adaptive terminal sliding mode control for nonlinear differential inclusion systems subjected to disturbance. The upper bound of the disturbance is unknown. First, the fast terminal sliding mode surface is established and sufficient condition for fast convergence is given. Then the adaptive sliding mode controller is designed to make the state of system arrive at the sliding mode in finite time. A numerical example is provided to show the effectiveness of the proposed method.     

On partial sliding along a planar crack: the case of a circular sliding zone

Summary A problem of partial sliding along a planar crack with a local drop in frictional resistance is investigated. A sliding zone initiates in the area of reduced friction, and then propagates as the applied shear load is monotonously increased. The problem is formulated in general terms, and then solved for the case when sliding spreads as a penny-shaped zone. Conditions under which the front of the zone stays circular during sliding are analyzed. It is observed that the axisymmetry of the profile of frictional resistance does not necessarily guarantee uniform propagation of sliding in the radial direction. The circular shape becomes the most favorable growth condition only if the shear modes are related in a certain way. The problem is studied based on the criterion of propagation that stress intensity factors(SIFs) for II and III modes vanish on the boundary of the sliding zone. The singular integrals in expressions for the SIFs are reduced to non-singular ones. Analytical solutions are derived for a number of special cases where the radius of the sliding zone is related to the applied shear load.This work is supported by the National Science Foundation through grant DGE-0209543 to the University of New Mexico.     

单晶硅滑动磨损性能及其相变研究

考察了单晶硅在室温和低接触应力条件下的摩擦磨损行为随速度的变化情况．结果表明，单晶硅的摩擦系数和磨损率随滑动速度的提高而呈现降低趋势；单品硅在低速、短滑动时间下的磨损表面形貌特征以微断裂为主，并伴有一定程度的塑性变形;随着滑动时间的延长，塑性变形特征逐渐减弱，塑性变形同具有金属延性特征的p—Sn(简称si—II)相密切相关，Si—II在滑动过程中可转变为体心立方结构(简称Si-III)、斜方六面体结构(简称Si—XII)和非晶硅相;在高速条件下，单晶硅磨损表面呈现微断裂和较弱的塑性变形特征；尽管通过Raman分析证实磨损表面存在si—III相，但其对磨损机制的影响有待于进一步研究．     

Experimental investigations of granular shape effects on the generation of electrostatic charge

In solid processing systems, electrostatic problems are commonly observed for granules of various shapes. However, a complete understanding of the basic dependence of electrostatic charge generation on particle shape has yet to be established. This observation motivated the present study on examining the effect of granular shape on electrostatics. In this study, polyvinyl chloride （PVC） granules （diameter 1.1-4.1 ram, in the shape of a triangle or trapezium） were first discharged to remove any residual charges and sub- sequently their electrostatic charging characteristics were studied by allowing a granule to slide along a pipe wall. Several factors such as granular front-facing angle, length-ratio, sliding area, sliding orienta- tion, sliding times, and relative humidity were considered when studying their effects on the electrostatic charging of granules. It was found that triangular granules with smaller front-facing angles tended to generate more electrostatic charge. The amount of electrostatic charge increased with granular length- ratio and sliding area but decreased with humidity. In addition, granular sliding in the orientation of the front-facing angle （for triangular granules） or the short side （for trapezoidal granules） generated more electrostatic charge than that in the orientation of the long side. For both granule shapes, the elec- trostatic charge increased with granular sliding times and reached a saturated state after around 8-9 sliding movements. The saturated electrostatic charge increased with either granular length ratio or sliding area.