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首页> 外文期刊>International Journal of Heat and Mass Transfer >Rotating Rayleigh-benard Convection Under The Influence Of Transverse Magnetic Field
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Rotating Rayleigh-benard Convection Under The Influence Of Transverse Magnetic Field

机译:横向磁场影响下的旋转瑞利-贝纳德对流

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In the present numerical study the effect of constant transverse magnetic field on convection of low Prandtl number liquid metal rotating in a cubical cavity with an aspect-ratio of 8:8:1 has been investigated. The bottom wall is heated while the top-wall is cooled and all the other walls are kept thermally insulated. The governing equations of mass, momentum, energy and magneto-hydrodynamic for a frame rotating with the enclosure, subject to Boussinesq approximation applied to gravity and centrifugal force terms, have been solved on a collocated grid using a semi-implicit finite difference method. The simulations have been carried out for liquid metal flows having a fixed Prandtl number Pr = 0.01, Rayleigh number Ra = 107, and magnetic Prandtl number Pm = 4.0 × 10~(-4) while Chandrasekhar number Q varies from 5.0625 × 10~4 to 1.21 × 10~6 and non-dimensional rotation rate Ω is varied from zero to 10~5.rnThe increase in strength of transverse magnetic field (from Q_1 - 5.0625 × 10~4 to Q_h = 1.21 × 10~6) till 2 ≌ Ta leads to slight increase in convective heat transfer as well as formation of two-dimensional coherent structures aligned along the direction of magnetic field. For cases pertaining to Q < Ta the two-dimensionality of the flow breaks down and the rolls distort in their alignment which leads to decrease in magnitude of vertical heat transfer. For cases where Q << Ta, the increased Coriolis forces lead to generation of large-scale circulation which forms a large cylindrical rotating column of fluid in consonance with Taylor-Proudman theorem. On increasing the strength of magnetic field the component of rms velocity in the direction of magnetic field gets suppressed while there is increase in other two components.
机译:在目前的数值研究中,研究了恒定横向磁场对纵横比为8:8:1的立方腔中旋转的低普朗特数液态金属对流的影响。底壁被加热,而顶壁被冷却,其他所有壁保持隔热。使用半隐式有限差分法,在并置网格上求解了随外壳旋转的框架的质量,动量,能量和磁流体动力学的控制方程式,该方程式适用于重力和离心力项的Boussinesq近似。对于具有固定的Prandtl数Pr = 0.01,瑞利数Ra = 107和磁性Prandtl数Pm = 4.0×10〜(-4),而Chandrasekhar数Q为5.0625×10〜4的液态金属流进行了模拟到1.21×10〜6且无量纲旋转速率Ω从零变化到10〜5.rn横向磁场强度的增加(从Q_1-5.0625×10〜4到Q_h = 1.21×10〜6)直到2 ≌Ta导致对流传热略有增加,并形成沿磁场方向排列的二维相干结构。对于与Q <Ta有关的情况,流的二维分解,并且辊的对齐方式变形,从而导致垂直传热的幅度减小。对于Q << Ta的情况,增加的科里奥利力会导致大规模循环的产生,从而形成与Taylor-Proudman定理一致的大型圆柱状旋转流体柱。随着磁场强度的增加,沿磁场方向的均方根速度分量被抑制,而另外两个分量则增加。

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