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Analysis of general unified MHD boundary-layer flow of a viscous fluid - a novel numerical approach through wavelets

机译:粘性流体的一般统一MHD边界层流动分析-一种通过小波进行数值模拟的新方法

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The common boundary-layer equations are derived in which the boundary-layer forms either due to the flow of a viscous fluid over a moving wedge or due to the stretching of the surface with a non-uniform velocity using the concept of the velocity ratio (free stream velocity to the stretching surface velocity). The extreme values of the velocity ratio parameter then characterize both former and latter boundary-layer flows. The model also considers the effect of uniform magnetic field which is applied normal to the flow. Once the mainstream flow is approximated either in the form of the power of distance along the wedge surface or as zero, the self-similar solutions exist. Using suitable transformations, the boundary-layer equations have been converted into the Falkner-Skan-type equation over the unbounded domain that accounts the velocity ratio parameter. The governing problem over an unbounded domain is solved using a novel numerical scheme which makes use of the power of Haar wavelets coupled with collocation method and quasilinearization technique. The wavelet solutions have been verified to be very accurate when compared with numerous previously observed results. Several interesting physical aspects of the considered problem are focused and justified through both theoretical as well as numerical approach. The results show that there are overand under-shoots in the solutions. Also, the flow divides into near-field (the solutions are confined to a viscous region) and far-field region (inviscid region). It is noticed that the boundary-layer thickness decreases for increasing pressure gradient and magnetic field parameters. Further, interestingly, our study leads to dual solutions for some range of physical parameters, which is explored for the first time through wavelet method in the literature. The physical hydrodynamics is explored and discussed. (C) 2019 International Association for Mathematics and Computers in Simulation (IMACS). Published by Elsevier B.V. All rights reserved.
机译:使用速度比的概念,得出了常见的边界层方程式,其中边界层的形成是由于粘性流体在活动楔块上的流动或由于表面以非均匀速度拉伸而引起的(自由流速度到拉伸表面速度)。速度比参数的极值然后表征前边界层流和后边界层流。该模型还考虑了垂直于流场施加的均匀磁场的影响。一旦主流流量以沿楔形表面的距离幂形式或为零而近似,则存在自相似解。使用适当的变换,边界层方程已在考虑速度比参数的无界域上转换为Falkner-Skan型方程。利用一种新颖的数值方案,解决了无界域上的控制问题,该方案利用了Haar小波的能量,并搭配了配置方法和拟线性化技术。与众多先前观察到的结果相比,小波解已被证明非常准确。通过理论和数值方法,重点关注并证明了所考虑问题的几个有趣的物理方面。结果表明,解决方案中存在过高和过低的问题。同样,流动分为近场(溶液局限于粘性区域)和远场区域(无粘性区域)。注意到边界层厚度随着压力梯度和磁场参数的增加而减小。此外,有趣的是,我们的研究导致对某些物理参数范围的双重解,这在文献中首次通过小波方法进行了探索。探索并讨论了物理流体动力学。 (C)2019国际模拟数学与计算机协会(IMACS)。由Elsevier B.V.发布。保留所有权利。

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