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Novel surface modification of steel using high-density infrared heating.

机译:使用高密度红外加热对钢进行新颖的表面改性。

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摘要

High-density infrared heating is a surface heating technique capable of producing wear-resistant coatings over a considerably larger processing area than currently available techniques (e.g. lasers). High-density infrared heating from a plasma arc-lamp is typically used for thermal annealing of silicon wafers, but this project expands the use of the plasma arc-lamp to produce carbon-enriched wear-resistant coatings on steel substrates. The focus of this study was to establish plasma arc-lamp processing parameters for the production of such coatings on a 1018 steel. The phase transformations involved were found to be in accordance with what occur in a fast-cooled hypoeutectic Fe-C system. The resulting structures contained a significant amount of Fe 3C near the surface present as discrete plates and with the ledeburite (i.e., eutectic microconstituent). A large fraction of carbide and the fine scale of the structures resulted in high hardnesses, reaching 750 HV 0.1 and 980 HV 0.1 for the graphite-only and Fe-Mo-C surface-modified regions, respectively. The high hardness and carbide fraction resulted in a significant improvement in two-body sliding wear-resistance over a standard carburized-and-hardened microstructure.
机译:高密度红外加热是一种表面加热技术,它能够在比目前可用的技术(例如激光)大得多的处理区域上产生耐磨涂层。来自等离子弧灯的高密度红外加热通常用于硅晶片的热退火,但是该项目扩大了等离子弧灯的使用范围,以在钢基板上生产富碳的耐磨涂层。这项研究的重点是确定在1018钢上生产此类涂层的等离子弧光灯加工参数。发现所涉及的相变与在快速冷却的亚共晶Fe-C系统中发生的相变一致。所得结构在作为离散板存在的表面附近具有大量的Fe 3C,并具有方晶石(即共晶微成分)。大量的碳化物和精细的结构导致高硬度,仅石墨表面和Fe-Mo-C表面改性区域的硬度分别达到750 HV 0.1和980 HV 0.1。与标准的渗碳和淬火显微组织相比,高硬度和碳化物分数导致两体滑动耐磨性显着改善。

著录项

  • 作者

    Haase, Ryan Jeffrey.;

  • 作者单位

    Iowa State University.$bMaterials Science and Engineering.;

  • 授予单位 Iowa State University.$bMaterials Science and Engineering.;
  • 学科 Engineering Metallurgy.; Engineering Materials Science.
  • 学位 M.S.
  • 年度 2007
  • 页码 115 p.
  • 总页数 115
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 冶金工业;工程材料学;
  • 关键词

  • 入库时间 2022-08-17 11:40:28

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