Influence of the composition of the cumulative lattice during thermal diffusion chromiing on the depth of the diffusion layer

N. Shaburova
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Abstract

Presents the results of experiments on improving the technology of thermal diffusion chromium plating of structural steels through the use of an internal emission field created in the technological backfill during heating. To create a field in the separating part of the technological backfill, aluminum oxide was completely replaced by mixtures of two compositions: a mixture of scheelite (CaWO4) and serpentine (Mg3Si2O7); a mixture of scheelite (CaWO4), serpentine (Mg3Si2O7), MgO, dicalcium silicate (γ-2•CaO•SiO2). The choice of these materials was based on the results of preliminary experiments on measuring the thermionic current in them. Saturation of samples of steel 35CrNi2-3 with chromium was carried out at a temperature of 1000°C for 24 hours. For both variants of technological fillings, the ab-sence of sintering and good knockout of parts were noted. The chemical composition of the diffusion layer on metal samples was controlled using a JEOL JSM-6460LV universal scanning (scanning) electron microscope. The micro-hardness of the coatings was measured using an FM-800 microhardness tester. The results show that the additional use of cumulative lattices of nickel and nichrome for thermal diffusion chromium plating provides an increase in the depth of chromium diffusion by 1.5 times when saturated in the backfill of the same composition. In this case, the lattice material has little effect on the depth of chromium diffusion, but it influences the intensity of surface microalloying with nickel. The electron yield work of nichrome X20H80, equal to 4.5 eV, has been determined. It was found that the hardness of the diffusion layers formed on the surface correlates with the content of chromium and nickel in them. The hardness of the chrome layer is 790±10 HV and 820±10 HV, using nickel and nichrome cumulative lattices, respective-ly. In the case of saturation without grids, the hardness is 50 and 20 HV respectively lower.
热扩散铬化过程中累积晶格的组成对扩散层深度的影响
介绍通过利用加热过程中在技术回填中产生的内部发射场来改进结构钢热扩散镀铬技术的实验结果。为了在技术回填的分离部分产生场,氧化铝被两种成分的混合物完全取代:白钨矿(CaWO4)和蛇纹石(Mg3Si2O7)的混合物;白钨矿(CaWO4)、蛇纹石(Mg3Si2O7)、氧化镁、硅酸二钙(γ-2-CaO-SiO2)的混合物。选择这些材料的依据是测量其中热离子电流的初步实验结果。35CrNi2-3 钢样品的铬饱和度在 1000°C 的温度下进行了 24 小时。对于这两种不同的技术填充物,都注意到了烧结的不存在和零件的良好敲除。使用 JEOL JSM-6460LV 通用扫描(扫描)电子显微镜控制了金属样品上扩散层的化学成分。使用 FM-800 显微硬度计测量了涂层的显微硬度。结果表明,在热扩散镀铬中额外使用镍和镍铬的累积晶格,在相同成分的回填中达到饱和时,铬的扩散深度可增加 1.5 倍。在这种情况下,晶格材料对铬的扩散深度影响不大,但会影响镍的表面微合金化强度。测定了镍铬 X20H80 的电子屈服功,等于 4.5 eV。研究发现,表面形成的扩散层的硬度与其中铬和镍的含量有关。使用镍和镍铬累积晶格,铬层的硬度分别为 790±10 HV 和 820±10 HV。在无网格饱和的情况下,硬度分别低 50 和 20 HV。
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