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Application of complex variables in electromagnetofluiddynamic, magnetofluiddynamic and fluid dynamic flows: Viscoelastic boundary-layer theory.

机译:复变量在电磁流体动力学,磁流体动力学和流体动力学流中的应用:粘弹性边界层理论。

摘要

This thesis is devoted to (a) a theoretical investigation of steady plane electromagnetofluiddynamic (EMFD), magnetofluiddynamic (MFD) and ordinary fluid dynamic flows and a numerical study of boundary-layer viscoelastic flows. In the theoretical study, the complex conjugate method is employed to obtain the geometries and solutions for various EMFD, MFD and non-MFD flows. Fluid motions with different assumptions such as isometry, circulation preserving, velocity magnitude being constant on each individual streamline and vorticity being a function of the real part of an analytic function of a complex variable are considered. The flow problems that have been considered in this part are: (1) Isometric orthogonal, constantly-inclined and aligned MFD flows of an electrically conducting incompressible second-grade fluid of finite electrical conductivity and of infinite electrical conductivity, (2) Isometric constantly-inclined EMFD flows of an electrically conducting incompressible second-grade fluid with non-zero charge density, (3) Circulation-preserving constantly-inclined, orthogonal and aligned EMFD flows of an electrically conducting incompressible second-grade fluid with non-zero charge density, (4) Circulation-preserving aligned MFD flows with finite electrical conductivity, (5) Constantly-inclined and aligned magnetogasdynamic and gas dynamic flows with the assumption that the velocity magnitude is constant on each individual streamline, and (6) Jeffery flows for incompressible viscous and second-grade fluids. The numerical study deals with viscoelastic steady plane boundary-layer flows. The model for viscoelastic fluid is taken to be the second-grade fluid. A general theory of viscoelastic boundary-layer theory is developed, and as illustrations, the shooting method and the Box scheme are adopted to obtain solutions for: (1) flow near a stagnation point with suction, (2) flow due to a stretching boundary with suction, (3) flow past a semi-infinite flat plate with zero pressure gradient and with exponential pressure gradient, (4) flow past a wedge, and (5) flow past a symmetrical circular cylinder. Finally, the viscoelastic boundary-layer flow is extended to study a magnetofluiddynamic boundary-layer motion due to the stretching of the wall.Dept. of Mathematics and Statistics. Paper copy at Leddy Library: Theses u26 Major Papers - Basement, West Bldg. / Call Number: Thesis1991 .N488. Source: Dissertation Abstracts International, Volume: 53-01, Section: B, page: 0350. Supervisor: O. P. Chandna. Thesis (Ph.D.)--University of Windsor (Canada), 1991.
机译:本文致力于(a)稳态平面电磁流体动力(EMFD),磁流体动力(MFD)和普通流体动力流动的理论研究,以及边界层粘弹性流动的数值研究。在理论研究中,采用复共轭方法获得各种EMFD,MFD和非MFD流动的几何形状和解。考虑具有不同假设的流体运动,例如等轴测图,保持循环,在每个单独的流线上恒定的速度大小以及涡旋是复杂变量的解析函数的实部的函数。本部分已考虑的流动问题是:(1)具有有限电导率和无限电导率的导电不可压缩二级流体的等轴测正交,恒定倾斜和对齐的MFD流量,(2)等轴测恒定-电荷密度为非零的不可压缩的导电二级流体的倾斜EMFD流量;(3)电荷密度为非零的不可压缩的导电二级流体的保持倾斜,正交且对齐的EMFD流通, (4)具有有限电导率的保持循环的对齐MFD流,(5)假设在每个单独的流线上速度幅度恒定,并且不断倾斜和对齐的磁动力和气体流,以及(6)对于不可压缩的粘性的Jeffery流和二级流体。数值研究涉及粘弹性稳态平面边界层流动。粘弹性流体的模型被认为是二级流体。提出了粘弹性边界层理论的一般理论,并以射击方法和Box方案为例进行说明,以得到以下解决方案:(1)吸力附近的滞流点;(2)拉伸边界引起的流动吸力作用下,(3)流过具有零压力梯度和指数压力梯度的半无限平板,(4)流过楔形物,(5)流过对称的圆柱体。最后,扩展了粘弹性边界层流,以研究由于壁的拉伸而产生的磁流体动力学边界层运动。数学和统计学。莱迪图书馆的纸质副本:论文主要论文-西楼地下室。 /电话:Thesis1991 .N488。资料来源:国际论文摘要,第53卷,第B部分,第0350页。主管:O。P. Chandna。论文(博士学位)-温莎大学(加拿大),1991。

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    Nguyen Phu Van.;

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