Enhanced impact and wear properties of gear steel by supersonic fine particle bombardment modification technology

Shi, Lei; Cui, Xiufang; Li, Jian; Guo, Jingjie; Zhang, Xuerun; Wen, Xin; Tian, Hongjing

doi:10.1016/j.matchar.2022.112368

Cited by 5 publications

(1 citation statement)

References 43 publications

Supporting

Mentioning

Contrasting

Order By: Relevance

“…Gear steel needs to have high wear resistance, hardness, and contact fatigue strength, while being hard on the outside and tough on the inside, capable of withstanding high external impact loads. [1][2][3][4][5][6][7][8] The gear heat treatment process often encounters severe banded structures, which can result in uneven carburized layer depth and hardness, leading to issues such as mismatched gear steel structure and hardness. [9][10][11][12][13][14] Therefore, it is necessary to eliminate the banded structure in gear steel.…”

Section: Introductionmentioning

confidence: 99%

The Effect of Cooling Rate on the Banded Structure of 20CrMnTi Gear Steel Based on C Diffusion and Partitioning Analysis

Zhao,

Chen,

et al. 2023

steel research int.

View full text Add to dashboard Cite

This study, through experimental analysis and numerical calculations, not only identifies the critical cooling rate for eliminating banded structures in 20CrMnTi gear steel but also analyzes the impact of cooling rate on banded structures, including the mechanisms related to element distribution and interface migration. The results indicate that the fundamental cause of banded structure formation is the presence of chemical segregation bands, and increasing the cooling rate leads to a reduction in the grade of ferrite/pearlite banded structures, with a critical cooling rate of 0.55 °C s−1. Bainite and martensite banded structures are observed in samples cooled at rates of 3 and 5.8 °C s−1, respectively. As the cooling rate increases from 0.07 to 1 °C s−1. The ferrite phase transformation time in the solute‐poor zone is shortened from 171 to 12 s within the ferrite phase transformation temperature difference (Δ) between the poor and rich solute zones. The concentration difference of C on both sides of the α/γ phase interface increases from 0.350 mass% to 0.431 mass%, and the diffusion distance of C decreases from 34.38 to 7.57 μm. When the diffusion distance of C is less than half of the width of the solute‐rich banding (12.5 μm), the ferrite banded structure disappears.

show abstract