Vacuum arc remelting (VAR) is a secondary melting process for production of metal ingots. [1] In the vacuum condition, the alloy ingot as an electrode was melted by the electric arc and then molten drops fell into the mold. The VAR process was extensively utilized to improve the cleanliness, chemical homogeneity, and mechanical property of metal ingots. [2,3] However, improper melting parameters may result in metallurgical defects, such as macrosegregation, porosities, and beta flecks. [4][5][6] Due to the high temperature of the smelting process, the experimental study was under restriction. The modeling study of the VAR process was used to obtain the optimal parameters for improving the quality of the ingot.Kondrashov et al. [7] developed a simple heat model of the VAR process neglecting the magnetohydrodynamic phenomena in the molten pool. The depth of the molten pool was predicted under different current intensities. Delzant et al. [1] established two models to calculate the thermal radiation of the ingot top during the VAR process. In the crude approach, only the radiative heat transfer between the ingot and the electrode tip was considered. In the detailed approach, all radiative exchanges between the ingot, electrode, and crucible wall were taken into account. Results of the detailed radiation model revealed that the radiative heat transfer of the ingot top was heavily dependent on the arc gap length and the electrode radius. Patel et al. [8] investigated the effect of processing parameters on molten pool profile, flow field, and segregation using a 2D mathematical VAR model. The molten pool profile was significantly affected by the magnetic field. The flow and overall segregation tendency increased with the increase in the magnetic field. Zagrebelnyy et al. [9] established a numerical model to study the segregation of the ingot during the VAR process. The strong flow field was induced by the high arc power resulting in severe macrosegregation. When the arc power was low, the flow was dominated by weaker buoyancy force, and less segregation was formed. Kou et al. [10] calculated the temperature field, fluid flow, and solidification structure of the Ti─6Al─4 V alloy ingot during the VAR process. When the heat radiation was considered, simulated columnar grains on the ingot top agreed well with the experimental results. Chapelle et al. [11] investigated the deformation of the free surface in the VAR process using CFD-based simulations. Two stirring modes were applied in the simulation. In the case of unidirectional stirring, the free surface was a concave dome shape. In the case of alternated stirring, periodic fluctuations of the liquid metal level were generated. Kermanpur et al. [12] established a multiscale