Abstract

Many researchers have investigated the impact factors of the bath–metal flow in an aluminum reduction cell using the simulation method. However, only a few have coupled their models with transient electromagnetic force, which makes the model closer to realistic conditions. In this work, coupling with the transient electromagnetic force, a three dimensional bath–metal two-phase quasi-steady flow model for a full 500 kA cell was built, and the model was validated with the metal velocity and the bath–metal interface deformation measurement in industrial cells. The impacts of local cathode electrical cut-off (LCEC) on the melt flow field were simulated according to six industrial cases. We found that the LCEC has little impact on the general pattern of the melt flow field, but the local metal velocity and the interface deformation would be changed to a certain extent. LCEC at positions A2A3 and A10A11 (as introduced in the full text) could suppress the interface hump at the central downstream area of the cell, with the anode cathode distance (ACD) increased by 3% and 7.5%, respectively. LCEC at positions A18A19 and A22A23 would deteriorate the interface hump condition, with the ACD decreased by 4% and 3%, respectively. The solution given in this paper is to cut the cathode flexes partially at abnormal positions to stabilize the melt flow field.

Highlights

  • The electromagnetic force is composed of the electric field and the magnetic field

  • This paper investigates the development of a proper simulation model for the evaluation of the melt flow field to improve the cell magnetohydrodynamics (MHD) stability

  • Under the condition of a static magnetic field coupled with a dynamic electric field, a three dimensional bath–metal two-phase quasi-steady flow model for a 500 kA full cell was built to study the impact of realistic local cathode electrical cut-off (LCEC) on the melt flow field

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Summary

Introduction

The electromagnetic force is composed of the electric field and the magnetic field. The electromagnetic field causes a vigorous agitation of the liquid metal layer and fluctuation of the bath–metal interface in an industrial aluminum reduction cell. With the rapid development of computer technology, increasing numbers of researchers have used various types of numerical simulation software to study bath–metal flow in the cell, such as ESTER/PHOENICS [8,9], MHD-Valdis [10,11], CFX [12,13,14], and Fluent [15,16,17], et al In most of the cases, the static electromagnetic force was calculated from the Metals 2020, 10, 110; doi:10.3390/met10010110 www.mdpi.com/journal/metals. According to Hua’s investigation [17], in the aluminum reduction cell, the local induced current density due to melt flow did not change the overall interface deformation. The simulation results were validated by the measured metal velocity and interface deformation in the industrial cells.

Physical
Multiphase Model
Turbulence Model
MHD Model
Simulation
Comparison of-6interface between2simulation
Simulation for Abnormal State
Two-phase
Conclusions
Full Text
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