分散电极的制备及其分散差电池的电动势

物质超细化后除产生强烈的量子尺寸效应和宏观量子遂道效应外,还将产生强烈的表面效应和体积效应等。这些效应可改变其的电化学性质。早在1982年Plieth[1]就发现了金属颗粒的粒度对电极电势有影响,随后又在理论和实验方面做了许多工作[2,3]。后来人们又不断发现,组成电极的粉末     

长中半径水平井钻柱接触摩擦阻力分析

用整体钻柱静力模型和间隙元法,分析了长中半径水平井钻柱的接触非线性问题,算出了钻柱与井壁接触摩擦阻力的分布,为水平井井眼轨道设计和施工提供了重要参数。     

二硫化钼表面氧化行为的研究（Ⅱ）─—二硫化钼摩擦表面氧化与电子转移的研究

利用电子自旋共振谱和Ｘ射线光电子能谱研究了二硫化钼ＭｏＳ＿２摩擦表面的氧化和电子转移，发现ＭｏＳ＿２在摩擦过程中是以Ｍｏ￣（４＋）经由Ｍｏ￣（５＋）过渡态继而与氧作用生成稳定的Ｍｏ￣（６＋），并且是以ＭｏＯ＿３的形式存在，证明ＭｏＳ＿２的摩擦表面除有一般认为的Ｍｏ￣（４＋）和Ｍｏ￣（６＋）这两种化学状态以外，还有Ｍｏ￣（５＋）自由基离子这种从未发现的的中间态。Ｍｏ￣（５＋）是４ｄ￣１电子构型，其在室温下于空气或氧气中是稳定的，然而在摩擦环境或添加剂的作用下，Ｍｏ￣（５＋）所含不成对电子很容易发生转移而生成Ｍｏ￣（６＋），这种研究结果更加深入地揭示了ＭｏＳ＿２摩擦表面氧化过程的复杂性，因此，应当从摩擦化学角度重新认识ＭｏＳ＿２摩擦氧化产物及其形成机制，这于研究摩擦环境和添加剂对润滑剂的抗氧化协同效应具有重要意义。     

弹性接触问题线性互补法的摄动原理

为使弹性摩擦问题的线性互补法得到收敛性保证,提出一个摄动原理,证明了通过“摆脱摄动误差”可得到原离散模型的精确解。     

摩擦接触问题的比例边界等几何B可微方程组方法

摩擦接触问题是计算力学领域最具挑战性的问题之一,接触系统的泛函具有非线性、非光滑的特点,导致接触算法的收敛性与精确性难以保证.因此将比例边界等几何分析(scaled boundary isogeometric analysis,SBIGA)与B可微方程组(B dierential equation,BDE)相结合,提出了求解二维摩擦接触问题的比例边界等几何B可微方程组方法.在比例边界等几何坐标变换的基础上,通过虚功原理推导了关于边界控制点变量的接触平衡方程,表示成B可微方程组形式的接触条件可被严格满足,求解B可微方程组的算法的收敛性有理论保证.此比例边界等几何B可微方程组方法(SBIGA-BDE)只需在接触体边界进行等几何离散,使问题降低一维,能精确描述接触边界,并可通过节点插入算法进行真实接触区域的识别.此外,由于几何建模和数值分析使用相同的基函数,节约了划分网格的时间.以赫兹接触问题和悬臂梁摩擦接触问题为例,通过与解析解及数值计算软件ANSYS计算结果进行对比,验证了该方法求解二维摩擦接触问题的有效性及高精度等特点.      

Competition between fingers in Hele-Shaw flows

In experiments on the displacement of viscous fluids in a Hele-Shaw cell of channel type the catastrophic development of competition between fingers is sometimes observed: for a long time two fingers propagate almost side by side and then one of them suddenly suppresses the other. It is believed that this is a manifestation of the capillary forces on the phase interface [1]. Using the solution found in [2] for the problem in an idealized formulation, it is shown that this scenario is perfectly feasible without having to take capillary forces into account.     

Three-dimensional localization of atoms in the polychromatic optical superlattice

Quasiclassical kinetic theory of the light pressure force has been applied to describe the localization of atoms (or ions) with the transition F=1→F=0 in the three-dimensional (3D) dissipative optical superlattice of a new type. Its action is based on the effect of the gradient force rectification in the polychromatic field: superposition of the three color far-off-resonant field and partially coherent resonant field. An approximate explicit solution of the kinetic equation for 3D motion of atoms in such a (multicolor) field has been achieved. This solution demonstrates the capability of the polychromatic superlattice to provide efficient cooling and strong spatial localization of the particles and to form an atomic (or ionic) grating with highly controllable characteristics.     

Revealing sol-gel type main effects by exploring a molecular cluster behavior in model in-plane amphiphilic aggregations

In-plane (bio)matter aggregations of amphiphilic nature are modeled extensively by Monte Carlo simulation in their natural entropic contexts. The modeling starts by designing the aggregations at a molecular level, pointing to its well-known configuration vs conformation character. Then, the conformational behavior is distributed over the aggregations obtained, with the aim of revealing their main sol-gel type (viscoelastic) effects. The passage between the resulting sol and gel phases is not controlled by a scan in the temperature domain, on the contrary, the control parameter is selected to be the hydrophobic-interaction strength while the temperature remains unchanged. The distribution of ordered fringed micelles, and the overall crystalline inclusions of the gel phase, suggested a first-order phase change, reasonably conceivable in terms of Avrami-Kolmogorov formalism for such hydrophobic-force driven and percolation-in-nature systems. A phase transition diagram has been presented as a novel proposition to discern between sol vs gel phases. As specific results, also of high experimental value, a damped-oscillating cluster-involving effect on the resulting hydrophobic-polar matrices has been detected and analysed. Other additional intermolecular-sharing entropy-influenced effects on clustering, as seen in terms of chain-to-chain connectivities, have been addressed as being of sufficient relevance to the gelation mechanism described. The microcrystalline inclusions downgrade to some extent the overall picture of entropy-affected gelation, being all together suitable for experimental check-out.