Lens 空间 L~n(p)的■_∧-群■_∧(L~n(p))

设η为 Lens 空间 L~n(p)上的典则复线丛,σ=η-1∈(?)(L~n(p))本文完全求出了元素 σ~i∈(?)(L~n(p))及(rσ)~i∈(?)(L~n(p))的阶.然后,我们把 k 理论中的 r~i 运算应用到 Lens 空间到欧氏空间的浸入和嵌入问题上,得出了新的结果.     

局部对称共形平坦黎曼流形中的极小子流形

对局部对称共形平坦黎曼流形中具有平坦法丛的极小子流形作了一些讨论，得到了极小子流形是全测地的两个充分条件。     

迷向映照和伪Veronese流形

本文讨论了伪Riemann流形之间的迷向映照。作为从伪Riemann球面到伪Riemann球面的极值浸入的新例子,本文从伪Riemann球面之间的迷向调和映照中确定了所有的伪Veronese流形。最后,利用某些几何量来刻划双曲类空的Veronese流形。     

Characterization of the Nanoscale Microstructure of an Immersion Silver on Sputtered Copper

1 INTRODUCTION Silver and its compounds have received much attention due to their current and potential applica- tions in many areas[1, 2]. As a metal with the highest electrical and thermal conductivities, silver was one of the most important noble metals used in electrical industries in the last century. Several decades ago, however, the development of silver application in electronic area seemed not so quick. The fear for some undesirable phenomena involving silver, like “electrochemi…     

一种模拟动边界绕流的锐利界面浸入边界法

When the structural wall moves over a fixed grid, the structure coverage will change, resulting in many dead and emerging elements. To avoid the influence of malformation and reconstruction of body-fitted grids on the calculation efficiency and accuracy of the fluid-structure interaction problems with coupled boundary movement on the fixed grid, an improved numerical method for describing the interaction between an immersed rigid body and fluid based on a sharp-interface is proposed. In this method, both the fluid and solid are regarded as pure fluid domains in the whole computational domain, and the solid boundary is divided into several Lagrangian grid points. The flow parameter or velocity is reconstructed by interpolation at the interface element, which is then directly used as the boundary condition of the flow field, thus reflecting the influence of the wall boundary conditions. The method constructs the calculation structure of “virtual point, force point and vertical foot point”, and the velocity of the virtual point is obtained by bilinear interpolation. Then, the velocity of the force point is calculated by forcing the solid boundary to meet the no-slip condition, and the equations of the coupling system based on the immersion boundary method are finally solved to realize the numerical simulation of the flow with a complex moving boundary. The numerical program for this immersed boundary method is established using C++, then the accuracy and reliability of the proposed method are validated by comparison with the literature and experimental results of the basic numerical example of flow around a cylinder. Furthermore, the effects of the structural shape and the angle of attack on the trailing vortex structure, the vortex shedding frequency, and the lift/ coefficient characteristics of the flow around the elliptical cylinder have been analyzed. The anti-symmetric S-type, “P+S” Ⅰ-type and “P+S” Ⅱ-type trailing vortex shedding modes, as well as the variation laws of the vortex structure size, vortex shedding frequency and lift-drag coefficients ratio with axis ratio and angle of attack, are captured. The critical angle of attack (25°) corresponding to the maximum lift-drag ratio is determined as 25°.     

不可压粘性流体浸入边界直接力法及软件实现

浸入边界法通过在N-S方程中施加体积力模拟不可滑移固壁边界及动边界,避免生成复杂贴体网格及动网格,极大地节省了网格建模时间及动网格计算消耗。本文提出一种新型附加体积力简化计算方法,将简化附加体积力以源项形式嵌入动量方程迭代中,通过用户自定义函数对CFD软件FLUENT二次开发,实现了浸入边界法和通用流体力学求解器的耦合计算。通过静止圆柱和动圆柱绕流数值模拟进行了验证,并探讨了插值函数对计算精度的影响。研究表明,通过引入浸入边界模型,能够提高计算效率,并实现结构网格背景下复杂边界和动边界的高效建模。     

斑海豹胡须涡激振动及其尾流循迹机理直接数值模拟

在视力和听力受到限制的条件下,斑海豹可以通过具有特殊外形的胡须识别和追踪水中游鱼的尾迹.从仿生学的角度,对斑海豹胡须在尾迹流场中的振动特性和循迹机理进行研究,有助于开发研制新型水下探测器.本文采用嵌入式迭代浸入边界法,在雷诺数Re=300和折合流速Ur=6.0的条件下,对均匀流场和尾迹流场中斑海豹胡须模型的涡激振动进行...     

Cayley射影平面的浸入Kaehler曲面

得到了Cayley射影平面的全复浸入Kaehler曲面的一些有趣的拓扑限制。     

曲面到Kaehler流形的共形极小分支浸入

对曲面到Ｋａｅｈｌｅｒ流菜的共形极小分支浸入的分支点给一种（ｑ，ｒ）型分类，进而研究到复射影空间的共形极小扫支浸入，得知相应的α－变换和α－变换在分支点的性态。     

关于Dold流形的浸入的某些结果

在Ucci[1]中曾得到不少关于Dold流形在欧氏空间中的浸入的定理。本文将给出在这一方面的某些新结果并修正[1]中的一个错误。我们先作一些准备。用S~m表示m维球面,CP_n表示n维复投影空间。把S~m×CP_n中的点(x,z)与(x,z)迭合,所得的商流形即是Dold流形P(m,n),它具有维数,n+2n。 P(m,n)有胞腔分解如下:对每一对满足i,j≥0,i+2j=k≤m+2n的整数对(i,