Experimental study on liquid metal free surface flow under magnetic and electric field for nuclear fusion. (1st March 2022)

• Record Type: Journal Article
• Authors: Meng, Xu; Wang, Zenghui; Zhang, Dengke
• Is Part Of: Nuclear fusion. Volume 62:Number 3(2022)
• Publication Date: 2022-03-01
• Subjects: flowing liquid metal -- magnetic field -- electric field -- fusion reactor; Nuclear fusion -- Periodicals; 621.48405
• DOI: 10.1088/1741-4326/ac4b9c
• Languages: English
• ISSNs: 0029-5515

Abstract

Abstract: In the future application of nuclear fusion, the liquid metal flows are considered to be an attractive option of the first wall of the tokamak which can effectively remove impurities and improve the confinement of plasma. Moreover, the flowing liquid metal can solve the problem of the corrosion of the solid first wall due to high thermal load and particle discharge. In the magnetic confinement fusion reactor, the liquid metal flow experiences strong magnetic and electric, fields from plasma. In the present paper, an experiment has been conducted to explore the influence of electric and magnetic fields on liquid metal flow. The direction of electric current is perpendicular to that of the magnetic field direction, and thus the Lorentz force is upward or downward. A laser profilometer based on the laser triangulation technique is used to measure the thickness of the liquid film of Galinstan. The phenomenon of the liquid column from the free surface is observed by the high-speed camera under various flow rates, intensities of magnetic field and electric field. Under a constant external magnetic field, the liquid column appears at the position of the incident current once the external current exceeds a critical value, which is inversely proportional to the magnetic field. The thickness of the flowing liquid film increases with the intensities of magnetic field, electric field, and Reynolds number. The thickness of the liquid film at the incident current position reaches a maximum value when the force is upward. The distribution of liquid metal in the channel presents a parabolic shape with high central and low marginal. Additionally, the splashing, i.e. the detachment of liquid metal is not observed in the present experiment, which suggests a higher critical current for splashing to occur.