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Verified CAS / Academic Author2 Decoded Studies

Prof. You YAN

School of Energy Science and Engineering, Central South University, Changsha 410083, China

Research Publications & English Decoded Briefs

Showing 2 publications
Transactions of Nonferrous Metals Society of China (中国有色金属学报)2026DOI: 10.1016/S1003-6326(26)67070-7

CFD modeling of gas−liquid mixing and splashing in industrial-scale bottom-blowing furnace: Effects of melt viscosity

The co-processing of lead-containing waste materials in oxygen bottom-blowing lead smelting alters melt viscosity, which in turn governs gas−liquid mixing efficiency, splashing behavior, and furnace lining erosion. A multi-fluid volume of fluid (VOF) model, incorporating experimentally determined high-lead slag viscosity values, was applied to an industrial-scale bottom-blowing furnace to resolve these coupled phenomena. The simulations demonstrate that optimal gas−liquid mixing occurs at viscosity values of 0.01 and 0.5 Pa·s, whereas minimal splashing is confined to the viscosity range of 0.1−0.25 Pa·s, corresponding to temperatures of approximately 1076−1100 °C. The regions surrounding the oxygen lances are identified as the most susceptible to erosion. Shear stress increases with melt viscosity, rising particularly rapidly within the 0.1−0.25 Pa·s interval. To minimize erosion, the melt viscosity should be maintained within 0.01−0.1 Pa·s. These findings provide quantitative thresholds for viscosity control in industrial bottom-blowing furnaces processing lead-containing secondary materials, enabling trade-offs between mixing intensity, splashing suppression, and lining protection to be optimized on an operational basis.

Journal of Central South University2025DOI: 10.1007/s11771-025-6123-z

Experimental study and creep constitutive modeling for 2219 aluminum alloy under tension and compression conditions

The creep deformation and mechanical properties of 2219 aluminum alloy were experimentally investigated under both tension and compression at the temperature of 165 ℃ for different time. The results indicated that the creep deformation under tensile stress was greater than that under compressive stress. As the stress level increases, the compressive creep rate showed more significant increase. The yield strength after compressive stress creep-ageing was higher than that after stress-free ageing, with the lowest strength observed in the tensile-aged sample. Overall, the average phase length after compressive stress creep-ageing was larger than after tensile stress ageing. Under tensile stress, the number and size of precipitates at small angles to the stress direction were larger than those perpendicular to the stress direction. In contrast, under compressive stress, this relationship was reversed, and the preferential orientation of phases became more pronounced with ageing time. A unified, physics-based creep-ageing constitutive model, accounting for the orientation of precipitation, was developed for both tensile and compressive stress conditions. The predicted results were in good agreement with the experimental data. These findings, along with the developed model, provide a theoretical and simulation basis for precise creep-ageing forming of components under complex stresses.