首页> 外文会议>ASME/JSME Thermal Engineering Joint Conference >NATURAL CONVECTION OF LIQUID METAL IN A CUBE WITH UNIFORM FLUX HEATING FROM A SIDE WALL UNDER HORIZONTAL MAGNETIC FIELDS
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NATURAL CONVECTION OF LIQUID METAL IN A CUBE WITH UNIFORM FLUX HEATING FROM A SIDE WALL UNDER HORIZONTAL MAGNETIC FIELDS

机译:在水平磁场下的侧壁中加热均匀焊剂的立方体中的自然对流

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Three-dimensional numerical calculations were carried out for the natural convection of liquid metal in a cube heated from a vertical wall with uniform heat flux and cooled from an opposing vertical wall isothermally under various strengths of horizontal magnetic field. The direction of the magnetic fields are in the X-coordinate (horizontal and perpendicular to the heated wall) or in the Y-coordinate(horizontal and parallel to the heated wall). Computational parameters are Pr (Prandtl number) = 0.025, Ra{sup}* (modified Rayleigh number) = 10{sup}5 - 5×10{sup}6, and Ha (Hartmann number) = 0 - 500. Numerical results are compared with previous experimental results. Under the X-directional magnetic field, the average Nusselt number decreased with the magnetic strength and agreed favorably with the previous experiments for any value of the Hartmann numbers studied. However, under the Y-directional magnetic field, the average Nusselt numbers slightly increased at moderate strength of the magnetic field, then gradually decreased with the magnetic field. This general tendency agrees with previous experiments. Figure A shows perspective views of velocity vectors for various cases. At Ha = 0, the velocity profiles are not uniform along the Y-direction. This non-uniform velocity profile has not been obtained for the Prandtl number greater than 0.7. At Ha = 200Y, the velocity profiles along the Y-direction are almost uniform. The Y-directional magnetic field appears to rectify the flow, while suppressing the convection weakly. The X-directional magnetic fields suppress the convection extensively.
机译:对从具有均匀热通量加热的立方体中的液态金属的自然对流进行三维数值计算,并从相对的垂直壁在水平磁场的各种强度下从相对的垂直壁冷却。磁场的方向在X坐标(水平且垂直于加热壁)中或在Y坐标(水平和平行于所述加热壁)中。计算参数是PR(PRANDTL编号)= 0.025,RA {SUP} *(修改的RAYLEIGH号)= 10 {SUP} 5 - 5×10 {SUP} 6,HA(HARTMANN NUMBER)= 0 - 500.数值结果是与先前的实验结果相比。在X方向磁场下,平均泡沫数量随磁强度降低,并且在先前的研究中,有利地商定了所研究的HARTMANN号的任何值的实验。然而,在Y方向磁场下,在磁场的中等强度下略微增加平均露天数,然后用磁场逐渐降低。这种普遍趋势同意以前的实验。图A示出了各种情况的速度向量的透视图。在HA = 0,速度轮廓沿Y方向不均匀。对于大于0.7的Prandtl号而未获得该不均匀速度曲线。在HA = 200℃时,沿Y方向的速度分布几乎是均匀的。 y方向磁场似乎纠正了流量,同时削弱了对流弱。 X方向磁场广泛抑制对流。

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