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Numerical simulations of a cylinder wake under a strong axial magnetic field

机译:强轴向磁场作用下圆柱尾流的数值模拟

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We study the flow of a liquid metal in a square duct past a circular cylinder in a strong externally imposed magnetic field. In these conditions, the flow is quasi-two-dimensional, which allows us to model it using a two-dimensional (2D) model. We perform a parametric study by varying the two control parameters Re and Ha (Ha(2) is the ratio of Lorentz to viscous forces) in the ranges [0...6000] and [0...2160], respectively. The flow is found to exhibit a sequence of four regimes. The first three regimes are similar to those of the non-magnetohydrodynamic (non-MHD) 2D circular wake, with transitions controlled by the friction parameter Re/Ha. The fourth one is characterized by vortices raising from boundary layer separations at the duct side walls, which strongly disturbs the Karman vortex street. This provides the first explanation for the breakup of the 2D Karman vortex street first observed experimentally by Frank, Barleon, and Muller [Phys. Fluids 13, 2287 (2001)]. We also show that, for high values of Ha (Ha >= 1120), the transition to the fourth regime occurs for Re proportional to 0.56Ha, and that it is accompanied by a sudden drop in the Strouhal number. In the first three regimes, we show that the drag coefficient and the length of the steady recirculation regions located behind the cylinder are controlled by the parameter Re/Ha(4/5). Also, the free shear layer that separates the recirculation region from the free stream is similar to a free MHD parallel layer, with a thickness of the order of Ha(-1/2) that is quite different to that of the non-MHD case, and therefore strongly influences the dynamics of this region. We also present one case at Re=3x10(4) and Ha=1120, where this layer undergoes an instability of the Kelvin-Helmholtz-type. (C) 2008 American Institute of Physics.
机译:我们研究了强外部施加的磁场中液态金属在方管中流过圆柱体的过程,该圆柱体经过圆柱体。在这些条件下,流是准二维的,这使我们可以使用二维(2D)模型对其进行建模。我们通过分别在[0 ... 6000]和[0 ... 2160]范围内改变两个控制参数Re和Ha(Ha(2)是洛伦兹与粘性力之比)来进行参数研究。发现该流表现出四个方案的序列。前三个状态类似于非磁流体动力学(非MHD)的2D圆形尾流,其过渡由摩擦参数Re / Ha控制。第四个特征是涡流从管道侧壁处的边界层分离处升起,这严重干扰了卡曼涡街。这为弗兰克(Frank),巴里昂(Barleon)和穆勒(Muller)[实验]首次通过实验观察到的二维卡尔曼涡街破裂提供了第一个解释。流体13,2287(2001)]。我们还表明,对于高的Ha值(Ha> = 1120),对于Re与0.56Ha成比例的Re,会发生向第四态的过渡,并且伴随有Strouhal数的突然下降。在前三个状态中,我们显示了阻力系数和位于圆柱体后方的稳定再循环区域的长度由参数Re / Ha(4/5)控制。此外,将再循环区域与自由流区分开的自由剪切层类似于自由MHD平行层,其Ha(-1/2)量级的厚度与非MHD情况的厚度完全不同,因此强烈影响该区域的动态。我们还提出了Re = 3x10(4)和Ha = 1120的一种情况,其中该层经历了Kelvin-Helmholtz类型的不稳定性。 (C)2008美国物理研究所。

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