采用热喷涂工艺对低碳钢1.0060纯氧化铝陶瓷涂层接触温度进行建模

R. Younes, Y. Mouadji, H. Touati, M. A. Bradai
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摘要

在以往的研究中,问题的陈述出现在运动过程中达到表面间热通量的硬度上。采用热火焰喷涂技术研究了在1.0060型低碳钢表面涂覆Al2O3 (AL-99)陶瓷的热行为。采用的关键方法是微观结构表征和实验数据记录与数值程序的比较。SEM结果表明,Al2O3涂层具有致密的微观组织、层状结构和多相复合结构。喷涂后涂层的XRD分析表明,涂层主体相为α -Al2O3菱形体结构,次相为γ-Al2O3正交体结构。实验记录的磨损数据分为两个阶段,第一个阶段对应于表面(样品/盘)之间的容纳阶段,两对接触温度逐渐升高到75℃,第二阶段,我们可以从实验和数值模拟中看到,实验测试达到95℃,数值模型达到85℃。摩擦学结果的重要发现表明,接触处的温度与热流增加所产生的剪切应力有关。从这些结果可以看出,测量温度随电荷的增加而升高,随接触时间的增加而收敛。实验结果与数值结果的温度差距可能与微观结构参数有关,其中实验孔隙度改善了区域内的对流,而数值材料没有增加这一现象。
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Modeling Temperature of Contact Generated in Coatings of Pure Alumina Ceramic onto Low Carbon Steel Type 1.0060 Obtained by the Thermal Spraying Process
In previous research problem statement occur in hardness to reach the thermal flux between surfaces during movement. The aim of the present investigation has been conducted to study the thermal behavior of ceramic Al2O3 (AL-99) coated on a low carbon steel type 1.0060 by using a thermal flame spray technique. The key methods used is microstructural characterization and comparing between experimental data record and numerical program.SEM showed that the Al2O3 coatings have a dense microstructure, lamellar morphology and complex of several phases. The XRD analysis of the coating after the spray showed a majority phase of α -Al2O3 rhombohedral structure and secondary phase of γ-Al2O3 orthorhombic structure. The experimental data recorded From wear indicate two step, first one corresponds to the phase of accommodation between surfaces (samples/ disc), the contact temperature gradually increases to a value Of 75 °C for both pairs, the second step , we could remark from experimental and numerical simulation, it reach 95°C for experimental test and 85 for numerical model.The important findings in tribological results showed that the temperature at the contact is related to the shear stress that will result from the increase of the heat flux. From these results it can be said that the measured temperature increases with the increase of the charge and converges with the contact time. The gap of temperature between experimental and numerical results is probably due to the parameter of microstructure, where in experimental porosities improve convection in the area, in contrast the numerical materials don't add this phenomena.
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