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Redistribution of Gaseous Phase of Liquid Metal Two-Phase Flow in a Strong Magnetic Field

机译:液态金属两相流在强磁场中的气相重分布

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In the previous paper, the authors pointed out the motion of bubble or gaseous phase in the direction to the both side walls due to the pinch effect caused by the induced magnetic field in the liquid metal two-phase flow under the strong magnetic field. In the present paper, to clarify the existence of the pinch effect experimentally, an experi-mental study was performed.Firstly the distributions of the void fraction in the cross section perpendicular to the flow were measured at three locations in the flow direction for the various strength of the applied magnetic field. Secondly a magnetic field was superposed on the induced magnetic field by the outer coil to disturb the pinch effect by the cancel of the induced magnetic field with the superposed one, resulting in the evident redistribution of the void-fraction profile obtained above.From these experiments it is concluded that the pinch effect will play an important role to redistribute the bubble or gaseous phase in the liquid metal two-phase flow under the strong magnetic field and that the effect is more promoted with increasing magnetic interaction number defined as a ratio of the electromagnetic force to the inertia of the fluid.
机译:在前一篇论文中,作者指出由于强磁场作用下液态金属两相流中的感应磁场引起的收缩效应,气泡或气相在朝向两个侧壁的方向上运动。在本文中,为了通过实验弄清夹缩效应的存在,进行了一项实验研究:首先,在不同流动方向的三个位置上,测量了垂直于流动方向的横截面中空隙率的分布。施加磁场的强度。其次,外层线圈将磁场叠加在感应磁场上,通过消除叠加的感应磁场来扰乱夹缩效应,从而导致上述获得的空隙率分布明显重新分布。结论是,在强磁场下,收缩效应将在液态金属两相流中的气泡或气相重新分布中起重要作用,并且随着磁相互作用数的增加,该收缩效应会得到进一步促进,磁相互作用数定义为:电磁力使流体惯性变大。

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