Chebyshev谱方法研究非稳态Maxwell流体在轴向余弦振荡圆柱上的斜驻点流动北大核心CSCD

研究了非稳态Maxwell流体斜撞击轴向余弦振荡圆柱的斜驻点流动.首先,基于斜驻点流动特性,在柱面坐标系下求得关于压力的二阶常微分方程,对压强进行修正,建立了非稳态Maxwell流体在振荡圆柱上斜驻点流动的边界层模型.接着,合理的相似变换将模型转化,使用Chebyshev谱方法求得模型的数值解.结果表明,在贴近圆柱表面的流体随着圆柱体做周期性运动;圆柱的曲率越大越会使在同一时刻同一位置处的流体质点的速度越大;相反,非稳态参数及流体的记忆特性也会在更靠近圆柱壁面处阻碍流体流动.     

双筒流变仪中粘弹性流体的解析解及运动特性分析

求得二阶流体和Maxwell流体在环管内不定常旋转运动问题的解析解.据此可以分析环管内旋转速度和切应力分布与变化特征.流体的物性常数、管道环隙大小等参数在解析公式中有明确反映,便于分析与讨论.本解可以用来分析类似的工程流动问题,尤其更具有针对性的是分析双筒流变仪中流动特征与应力状态,确定材料的粘弹性参数.通过计算,发现当外筒作简谐振动时,Maxwell流的速度和切应力变化曲线上有突变结,突变结上振幅和相位都发生突变.当外筒匀速旋转时,Maxwell流体的速度和切应力变化曲线分别呈斜方波和锯齿波形状.振动周期与材料常数H_a二次曲线相关.     

环空管内粘弹性流体不定常旋转流的解及流动特性分析

本文用Hankel积分变换法分别求得二阶流体和Maxwell流体在环管内不定常旋转流运动方程的解析解,据此可以分析环管内旋转速度和切应力的分布与变化特征;流体物性参数、管道环隙大小等参量在解析公式中有明确反映,便于定性分析和讨论,本解可以为钻探工程和高分子加工工艺的设计提供理论依据,另外还可用来分析双筒粘度计的流动状态和应力特征,拟合曲线,确定材料的粘弹性参数,在对这种流体进行特性分析时,我们发现,Maxwell流体的旋转流动在起动初期表现为方波振荡,振动的幅度和周期随Ha(物质常数)的增大而增大,此种现象还是首次发现,可能对实际应用有一定的意义。     

非牛顿流体管内不定常流的解析解

本文用积分变换方法分别给出了二阶流体和Maxwell流体管内不定常流运动方程的解析解.据此可以分析轴向速度和切应力分布与变化特征,为管道工程设计提供理论依据.     

多孔饱和矩形管中粘性随温度变化对熵产、热和流体流动的影响

研究了充填流体-饱和多孔介质的矩形管中,随温度变化的粘性对充分发展强迫对流的影响.采用Darcy流动模型并假设粘性-温度为倒线性关系.管壁视为均匀热通量,即Kays和Craw-ford称为的H边界条件.当流体粘性随温度升高而降低时,管壁的Nusselt数增大.求解速度和温度分布时,利用热力学第二定律求解了局部平均熵产率.根据Brinkman数、Péclet数、粘性变化数、无量纲管壁热通量和管道截面宽高比,给出了熵产率、Bejan数、传热不可逆性和流体流动不可逆性的表达式.这些表达式是该类问题参数研究的基础.可以看出,当管道截面宽高比的增大使熵产率减小时,方形管中流动产生的熵大于矩形管,这类似于Ratts和Raut研究的明流(clear flow)情况.     

非牛顿磁性纳米流体旋转流动

研究非牛顿磁性纳米磁体定常旋转流动。考虑到磁化强度的特殊贡献,应用修正的非牛顿磁性流体运动方程,磁场作用是纯扩散,不受流体运动速度场的影响。给出了多种流动的解析解。应用计算机符号运算技术,软件Maple16,可以得岀非牛顿上随体Maxwell磁性纳米流体和Oldroyd B磁性纳米流体非定常流动方程的各级近似解的常微分方程,获得解析和数值解。在研究中对纳米流体的物质常数作纳米修正。     

化学反应对高对流Maxwell流体在多孔面上作MHD流动和传质的影响

研究导电的高对流Maxwell流体在多孔表面上,作计及物质化学反应时的MHD流动及其传质.将非线性的偏微分控制方程及其相应的边界条件,变换为非线性的常微分方程,并利用Kel-ler-Box法进行数值求解.用图形给出了各种物理参数对流动和传质特性的影响,并对结果进行了讨论.可以看到,化学反应阶次提高了扩散边界层的厚度;还可以看到,传质率强烈地依赖于Schmidt数和反应率参数.此外,在特例情况下得到了以往文献中可供利用的结果.     

Maxwell流体在有限长管道中作不稳定的蠕动传输:食道吞咽进程分析

解析地研究了有限长管道中Maxwell流体的不稳定蠕动传输.管壁受到不超过静止边界的收缩波作用.对无量纲形式的方程,应用长波长近似进行分析.导出了轴向速度和径向速度的表达式,评估了沿波长和管道长度方向的压力.讨论了回流现象,确定了回流极限区域.对食道中咀嚼食物(如面包、蛋白等)传输的数学公式给出了物理上的解释.可以看出,与Newton流体相比,Maxwell流体有利于在食道中的流动.与Takahashi等[Rheology,1999,27:169-172]的实验结果相符合.进一步揭示了松弛时间既不影响剪应力,也不影响回流极限.发现了压力的峰值,对整数值波列是相同的,而对非整数值波列是不同的.     

径向磁场下电磁流体力学的柱对称定态严格通解

本文从最一般的电磁流体力学基本方程出发,导出了圆截面管道中不可压缩粘滞导电流体的走态流动问题的严格通解。可以证明,Globe和Arora找到的严格解,是本通解的两个特例,并讨论了三类典型的电磁流体力学定态流动问题,画出了不同参数下的流场和磁场分布曲线。     

滑移和感应磁场对Johnson-Segalman流体蠕动传输的影响

存在感应磁场和滑移条件下,研究Johnson-Segalman(J-S)流体在平面通道中的蠕动流.通道中的流动认为是对称的,并在剪切应力项中考虑了速度的滑移条件.首先给出问题的数学公式,然后在长波长和低Reynolds数近似下,求解该方程组得到摄动解,确定沿管道截面的压力增量、轴向速度、微转动分量、流函数、磁力函数、轴向感应磁场和电流密度分布公式.导出了小数值Weis-senberg数时解的表达式,分析并勾画出诸流动物理量的有趣变化.     

Flow through an oscillating rectangular duct for generalized Maxwell fluid with fractional derivatives

The velocity field and the associated shear stresses corresponding to the unsteady flow of generalized Maxwell fluid on oscillating rectangular duct have been determined by means of double finite Fourier sine and Laplace transforms. These solutions are also presented as a sum of the steady-state and transient solutions. The solutions corresponding to Maxwell fluids, performing the same motion, appear as limiting cases of the solutions obtained here. In the absence of w, namely the frequency, and making α → 1, all solutions that have been determined reduce to those corresponding to the Rayleigh Stokes problem on oscillating rectangular duct for Maxwell fluids. Finally, some graphical representations confirm the above assertions.     

Haar wavelet approximation for magnetohydrodynamic flow equations

This study proposes Haar wavelet (HW) approximation method for solving magnetohydrodynamic flow equations in a rectangular duct in presence of transverse external oblique magnetic field. The method is based on approximating the truncated double Haar wavelets series. Numerical solution of velocity and induced magnetic field is obtained for steady-state, fully developed, incompressible flow for a conducting fluid inside the duct. The calculations show that the accuracy of the Haar wavelet solutions is quite good even in the case of a small number of grid points. The HW approximation method may be used in a wide variety of high-order linear partial differential equations. Application of the HW approximation method showed that it is reliable, simple, fast, least computation at costs and flexible.     

A note on the flow induced by a constantly accelerating plate in an Oldroyd-B fluid

The velocity field and the adequate tangential stress that is induced by the flow due to a constantly accelerating plate in an Oldroyd-B fluid, are determined by means of Fourier sine transforms. The solutions corresponding to a Maxwell, Second grade and Navier–Stokes fluid appear as limiting cases of the solutions obtained here. However, in marked contrast to the solution for a Navier–Stokes fluid, in the case of an Oldroyd-B fluid oscillations are set up which decay exponentially with time.     

Exact analytic solutions for the unsteady flow of a non-Newtonian fluid between two cylinders with fractional derivative model

The velocity field and the associated shear stress corresponding to the torsional oscillatory flow of a generalized Maxwell fluid, between two infinite coaxial circular cylinders, are determined by means of the Laplace and Hankel transforms. Initially, the fluid and cylinders are at rest and after some time both cylinders suddenly begin to oscillate around their common axis with different angular frequencies of their velocities. The solutions that have been obtained are presented under integral and series forms in terms of generalized G and R functions. Moreover, these solutions satisfy the governing differential equation and all imposed initial and boundary conditions. The respective solutions for the motion between the cylinders, when one of them is at rest, can be obtained from our general solutions. Furthermore, the corresponding solutions for the similar flow of ordinary Maxwell fluid are also obtained as limiting cases of our general solutions. At the end, flows corresponding to the ordinary Maxwell and generalized Maxwell fluids are shown and compared graphically by plotting velocity profiles at different values of time and some important results are remarked.     

Flow of a generalized Maxwell fluid induced by a constantly accelerating plate between two side walls

The unsteady flow of a viscoelastic fluid with the fractional Maxwell model, induced by a constantly accelerating plate between two side walls perpendicular to the plate, is investigated by means of the integral transforms. Exact solutions for the velocity field are presented under integral and series forms in terms of the derivatives of generalized Mittag–Leffler functions. The corresponding solutions for Maxwell fluids are obtained as limiting cases for β → 1. In the absence of the side walls, all solutions that have been determined reduce to those corresponding to the motion over an infinite plate.      

Exact solutions for the flow of an Oldroyd-B fluid due to an infinite flat plate

The unsteady flow of an Oldroyd-B fluid due to an infinite flat plate, subject to a translation motion of linear time-dependent velocity in its plane, is studied by means of the Laplace transform. The velocity field and the associated tangential stress corresponding to the flow induced by the constantly accelerating plate as well as those produced by the impulsive motion of the plate are obtained as special cases. The solutions that have been determined, in all accordance with the solutions established using the Fourier transform, reduce to those for a Newtonian fluid as a limiting case. The similar solutions for a Maxwell fluid are also obtained.     

Exact solutions for electro-osmotic flow of viscoelastic fluids in rectangular micro-channels

Transient electro-osmotic flow of viscoelastic fluids in rectangular micro-channels is investigated. The general twofold series solution for the velocity distribution of electro-osmotic flow of viscoelastic fluids with generalized fractional Oldroyd-B constitutive model is obtained by using finite Fourier and Laplace transforms. Under three limiting cases, the generalized Oldroyd-B model simplifies to Newtonian model, fractional Maxwell model and generalized second grade model, where all the explicit exact solutions for velocity distribution are found through the discrete Laplace transform of the sequential fractional derivatives. These exact solutions may be able to predict the flow behavior of viscoelastic biological fluids in BioMEMS and Lab-on-a-chip devices and thus could benefit the design of these devices.     

Flow of a viscoelastic fluid with the fractional Maxwell model between two side walls perpendicular to a plate

The unsteady flow of a viscoelastic fluid with the fractional Maxwell model between two side walls perpendicular to a plate is investigated. Exact solutions for the velocity field are established by means of the Fourier and Laplace transforms. The similar solutions for Maxwell and Newtonian fluids can be obtained as limiting cases of our results. In the absence of side walls, all solutions that have been determined reduce to those corresponding to the motion over an infinite plate.     

Unsteady helical flows of Oldroyd-B fluids

The unsteady helical flow of an Oldroyd-B fluid, in an infinite circular cylinder, is studied by using finite Hankel transforms. The motion is produced by the cylinder that, at time t = 0⁺, is subject to torsional and longitudinal time-dependent shear stresses. The solutions that have been obtained, presented under series form, satisfy all imposed initial and boundary conditions. The corresponding solutions for Maxwell, second grade and Newtonian fluids are obtained as limiting cases of general solutions. Finally, the influence of the pertinent parameters on the fluid motion is underlined by graphical illustrations.