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首页> 外文期刊>Steel Research International >Control of Microstructure during the Eutectoid Transformation in the As-cast Spheroidal Graphite Cast Iron with 》in-situ《 Dilatation Analysis and Quenching Experiments
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Control of Microstructure during the Eutectoid Transformation in the As-cast Spheroidal Graphite Cast Iron with 》in-situ《 Dilatation Analysis and Quenching Experiments

机译:《原位》膨胀分析和淬火实验控制球墨铸铁共析转变过程中的组织

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Transformation of austenite can proceed into ferrite and graphite (gamma_(Fe)- >alpha_(Fe)+G) and/or in pearlite (gamma_(Fe)- >alpha_(Fe)+Fe_3C). Investigation of the eu-tectoid transformation has been undertaken by evaluation of the "in-situ" dilatation curves in connection with metallographic examinations, DTA and dilatation analyses of the solid state. On a basis of numerous quantitative relations, such as the relation between ferrite and pearlite fractions in as-cast spheroidal graphite cast iron (SGI), the ratio between ferrite and pearlite in the microstructure is determined in a very short time. Thus the melt composition was corrected using the "in situ" dilatation analyses by addition of Cu and/or Mn or Si respectively. From the kinetics of austenite transformation and temperature dependence of the ferrite or pearlite growth, the following characteristic temperatures of the eutectoid transformation have been established: the ferrite nucleation T_(alpha)~0, the beginning of the ferrite growth T_(alpha), and pearlite growth T_p, respectively. Both temperatures T_(alpha)~0 and T_p are determined from the differential inflection point of the dilatometric curves. For mainly ferrite and pearlite SGI, the kinetic curves, which show the fraction of the single microstructure constituents in the microstructure in dependence of the transformation time, are well represented by the physical sigmoidal Boltzmann model. In case of the kinetics temperature dependence, however, pearlite growth does not follow the sigmoidal transformation course, which results from the recalescence of the pearlite reaction. The time of transformation is a more suitable criterion for the description of the transformation.
机译:奥氏体的转变可以进行成铁素体和石墨(γ_(Fe)->α_(Fe)+ G)和/或珠光体(γ_(Fe)->α_(Fe)+ Fe_3C)。通过评价“原位”膨胀曲线并结合金相检查,DTA和固态膨胀分析,对共-共析转变进行了研究。基于许多定量关系,例如球墨铸铁(SGI)中的铁素体和珠光体组分之间的关​​系,可以在很短的时间内确定铁素体与珠光体之间的比例。因此,使用“原位”膨胀分析通过分别添加Cu和/或Mn或Si来校正熔体组成。根据奥氏体转变的动力学和铁素体或珠光体生长的温度依赖性,建立了共析相变的以下特征温度:铁素体成核T_α〜0,铁素体生长的开始T_α,以及珠光体的生长T_p分别。温度T_α〜0和T_p均由膨胀曲线的微分拐点确定。对于主要的铁素体和珠光体SGI,动力学曲线可以很好地表示为物理S型Boltzmann模型,该动力学曲线显示了微观组织中单个微观结构成分随转化时间的变化比例。然而,在动力学温度依赖性的情况下,珠光体的生长不遵循S形曲线的转变过程,后者是由珠光体反应的重新发光引起的。转换时间是描述转换的更合适标准。

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