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Linear stability of magnetohydrodynamic flow in a square duct with thin conducting walls

机译:薄壁方形导管中磁流体动力学流动的线性稳定性   导墙

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摘要

This study is concerned with numerical linear stability analysis of liquidmetal flow in a square duct with thin electrically conducting walls subject toa uniform transverse magnetic field. We derive an asymptotic solution for thebase flow which is valid not only for high but also moderate magnetic fields.This solution shows that for low wall conductance ratios $c\ll1,$ an extremelystrong magnetic field with the Hartmann number $Ha\sim c^{-4}$ is required toattain the asymptotic flow regime considered in the previous studies. We use avector stream function/vorticity formulation and a Chebyshev collocation methodto solve the eigenvalue problem for three-dimensional small-amplitudeperturbations in ducts with realistic wall conductance ratios $c=1,0.1,0.01$and Hartmann numbers up to $10^{4}.$ As for similar flows, instability in asufficiently strong magnetic field is found to occur in the side-wall jets withthe characteristic thickness $\delta\sim Ha^{-1/2}.$ This results in thecritical Reynolds number and wavenumber increasing asymptotically with themagnetic field as $Re_{c}\sim110Ha^{1/2}$ and $k_{c}\sim0.5Ha^{1/2}.$ Therespective critical Reynolds number based on the total volume flux in a squareduct with $c\ll1$ is $\bar{Re}_{c}\approx520.$ Although this value is somewhatlarger than$\bar{Re}_{c}\approx313$ found by Ting et al. (1991) for theasymptotic side-wall jet profile, it still appears significantly lower than theReynolds numbers at which turbulence is observed in experiments as well as indirect numerical simulations of this type of flows.
机译:这项研究涉及在具有均匀横向磁场的薄壁导电壁的方管中液态金属流动的数值线性稳定性分析。我们导出了基本流的渐近解,该解不仅对于高磁场而且对于中等磁场都是有效的。该解决方案表明,对于低壁电导率$ c \ ll1,$具有哈特曼数$ Ha \ sim c ^的极强磁场为了达到先前研究中考虑的渐近流动状态,需要{-4} $。我们使用向量流函数/涡度公式和Chebyshev搭配方法来解决具有实际壁电导比$ c = 1,0.1,0.01 $和Hartmann数不超过$ 10 ^ {4}的管道中的三维小振幅扰动的特征值问题对于相似的流动,发现在具有特征厚度$ \ delta \ sim Ha ^ {-1/2}的侧壁射流中,在足够强的磁场中会发生不稳定。$这导致临界雷诺数和波数增加磁场渐近地为$ Re_ {c} \ sim110Ha ^ {1/2} $和$ k_ {c} \ sim0.5Ha ^ {1/2}。$相应的临界雷诺数基于方波管中的总体积通量$ c \ ll1 $的值为$ \ bar {Re} _ {c} \ approx520。$尽管此值比Ting等人发现的$ \ bar {Re} _ {c} \ approx313 $稍大。 (1991)对于渐近的侧壁射流剖面,它仍然明显低于雷诺数,在雷诺数时在实验以及这种流动的间接数值模拟中都观察到了湍流。

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