脉冲直流粉末包硼法在 AISI 316 L 钢上生长的 FeB-Fe2B 层的微观结构和动力学分析

I. Campos-Silva, J. Cedeño-Velázquez, A. D. Contla-Pacheco, I. Arzate-Vázquez, L. E. Castillo-Vela, M. Olivares-Luna, J. L. Rosales-Lopez, F. P. Espino-Cortes
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引用次数: 0

摘要

本研究就脉冲直流粉末包硼化过程中 10 A 电流强度对 FeB-Fe2B 层生长的影响获得了新的发现。在 1123-1223 K 的 AISI 316 L 钢上形成了硼化物层,每个温度下的暴露时间不同,极性反转周期为 10 秒。通过 X 射线衍射和高速 Berkovich 纳米压痕法对硼化物层进行了表征,后者用于确定硼化物层-基底系统沿深度方向的硬度和还原杨氏模量映射。此外,还使用热平衡积分法(HBIM)对钢表面的 FeB-Fe2B 层的生长动力学进行了建模。这包括将菲克第二定律转化为随时间变化的常微分方程,假设空间中的硼浓度曲线为二次曲线,以分别确定铁硼和铁二硼中的硼扩散系数。根据阿伦尼乌斯关系,考虑到电迁移效应的贡献,对硼化物层中的硼活化能进行了估算;结果表明,与 AISI 316 L 钢的传统粉末包硼化物相比,硼活化能降低了约 30%。最后,HBIM 得出的理论硼化物层厚度与实验得出的 FeB 和 FeB + Fe2B 层厚度值相比,误差不超过 5%。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Microstructural and kinetics analysis of FeB–Fe2B layer grown by pulsed-DC powder-pack boriding on AISI 316 L steel
In this study, novel findings were obtained regarding the influence of a 10 A current intensity on the growth of an FeB–Fe2B layer during pulsed-DC powder-pack boriding. Boride layer formation was carried out on AISI 316 L steel at 1123–1223 K for different exposure times at each temperature, considering 10 s polarity inversion cycles. The boride layer was characterized by x-ray diffraction and high-speed Berkovich nanoindentation, the latter being used to determine the hardness and reduced Young’s modulus mappings along the depth of the layer-substrate system. Moreover, the growth kinetics of the FeB–Fe2B layer on the steel’s surface was modeled using the heat balance integral method (HBIM). This involved transforming Fick’s second law into ordinary differential equations over time, assuming a quadratic boron concentration profile in space to determine the B diffusion coefficients in FeB and Fe2B, respectively. From the Arrhenius relationship, the B activation energies in the boride layer were estimated considering the contribution of the electromigration effect; the results showed an approximately 30% reduction compared to the values obtained in the conventional powder-pack boriding for AISI 316 L steel. Finally, the theoretical layer thickness obtained by the HBIM demonstrated an error of no more than 5% against the experimental FeB and FeB + Fe2B layer thickness values.
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