Abstract

Herein, a 2D unified model coupling a plasma arc–molten bath–cavity in a direct current electric arc furnace was developed for a characteristic analysis of the fluid flow and heating rate of the molten bath. The ‘local thermodynamic equilibrium–diffusion approximation’ method was employed for the physical phenomenon at the plasma arc/molten bath interface, and the volume-of-fluid method was used to track the free surface. After ensuring model validation, the formation processes of the cavity and the flow field and heating rate of the molten bath were investigated by utilizing the unified model. The numerical results showed that the formation processes of the cavity contained three stages, namely the expansion, compression, and dynamic equilibrium stages. The arc pressure and plasma shear stress both contributed to the cavity formation, and dominated the expansion of the cavity depth and diameter, respectively. Under plasma arc jet impingement, there were two flow patterns inside the molten bath: (i) a clockwise eddy on the top surface and lateral part of molten bath dominated by plasma shear stress, and (ii) a counter-clockwise eddy in the bottom part of the molten bath dominated by the electromagnetic force. Meanwhile, the main heated region of the molten bath with the plasma arc–molten bath–cavity coupling was in the radial range of 0.2–0.6 m, and a high-temperature region was formed on the top surface of the molten bath caused by plasma shear stress.

Highlights

  • Increasingly efficient technologies have been developed to reduce the tapto-tap time of electric arc furnace (EAF) steelmaking [1,2,3], including the ‘large hot heel’ operation and scrap-preheating technology

  • A large amount of molten steel is left in the bottom of the furnace from the prior heating to assist in the melting of fresh scrap entering the direct current (DC) EAF [5]

  • The fluid flow and heating rate of the molten steel is dominated by both complex energy and momentum transfer at the interface between the molten steel and plasma arc [7,8,9,10,11,12,13], which is closely related to the steelmaking productivity of EAFs using a large hot heel operation

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Summary

Introduction

Increasingly efficient technologies have been developed to reduce the tapto-tap time of electric arc furnace (EAF) steelmaking [1,2,3], including the ‘large hot heel’ operation and scrap-preheating technology. In the large hot heel operation, the plasma arc is utilized to heat the molten steel at first, and to melt the scrap through a heat exchange between the molten steel and scrap. The fluid flow and heating rate of the molten steel is dominated by both complex energy and momentum transfer at the interface between the molten steel and plasma arc [7,8,9,10,11,12,13], which is closely related to the steelmaking productivity of EAFs using a large hot heel operation. It is well known that both the plasma arc and molten bath interact with each other during the steelmaking process in a DC EAF. It is essential to develop a unified model coupling the plasma arc, molten bath, and cavity in a DC EAF

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