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Carburizing Behavior of AISI 4115 Steel According to the Flow Rates of Acetylene in Vacuum Carburizing

机译:AISI 4115钢的渗碳行为根据乙炔的流动率在真空渗碳中

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摘要

The vacuum carburizing behavior of AISI 4115 steel according to acetylene flow rates (1, 5, 10, 20, 30, 40, and 50 sccm) and temperatures (900, 950, and 1000 °C) was quantitatively investigated through microstructure, carbon concentration and hardness analyses. As the acetylene flow rate increased, the penetration rate of carbon into the surface of the samples (surface-carbon flux) increased, resulting in an increase in the solute carbon concentration at the surface up to the solubility of carbon in austenite. At the same time, the amount of carbon diffusion into the interior of the specimen and overall carburizing depth increased. When the carbon concentration in the surface of the carburized specimen exceeded the solubility of carbon in the austenite above a certain flow rate, cementite precipitated in the austenite grain boundaries. Accordingly, the surface hardness decreased and the amount of carbon diffusion into the specimen became constant as the solute carbon concentration in the austenite matrix at the surface of the specimen became constant. As a result, the overall solute carbon concentration and the effective case depth no longer increased. Meanwhile, the tendency of vacuum carburizing behavior according to temperature was the same, but as temperature increased, the surface-carbon flux and rate of carbon diffusion into the interior of the sample increased, resulting in increased carburizing depth. The appropriate flow rates (10, 20, and 30 sccm) and the corresponding surface-carbon fluxes (62.3, 135.7, and 216.7 g/m~2h) were derived according to carburizing temperatures (900, 950, and 1000 °C), respectively.
机译:通过显微组织、碳浓度和硬度分析,定量研究了AISI 4115钢在乙炔流量(1、5、10、20、30、40和50 sccm)和温度(900、950和1000°C)下的真空渗碳行为。随着乙炔流速的增加,碳在样品表面的渗透速率(表面碳通量)增加,导致表面的溶质碳浓度增加,直至碳在奥氏体中的溶解度。同时,碳向试样内部的扩散量和整体渗碳深度增加。当渗碳试样表面的碳浓度超过一定流速时,渗碳体在奥氏体晶界析出。因此,随着试样表面奥氏体基体中的溶质碳浓度变得恒定,表面硬度降低,碳扩散到试样中的量变得恒定。因此,总溶质碳浓度和有效保护层深度不再增加。同时,真空渗碳行为随温度的变化趋势是相同的,但随着温度的升高,表面碳通量和碳向试样内部扩散的速率增加,导致渗碳深度增加。根据渗碳温度(900、950和1000°C),分别得出了合适的流速(10、20和30 sccm)和相应的表面碳通量(62.3、135.7和216.7 g/m~2h)。

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