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Surface Relief of Phase Transformation Products of Supercooled Austenite

机译:过冷奥氏体相变产物的表面浮雕

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摘要

It is very important to investigate surface relief of phase transformation products of supercooled austenite. Recently, many works have been carried out on the observation of surface relief of bainite, martensite, pearlite by means of AFM, STM, and SEM. In this paper, the surface relief of transformation products of super-cooling austenite was studied. The results show the surface relief of bainite, martensite and pearlite are all tented(∧) or N(N) type, the height of surface relief is commonly about ten nanometer, and with flat slope. The surface reliefs of martensite haven't the special character of N (N) type. The relief patterns correspond to their own microstructure, respectively. The formation mechanism of surface relief is complex as aberrance of heat treatment. The phase transformation of supercooled austenite is all first order phase transformation, namely, bulk expansion occur when supercooled austenite transforms to pearlite, bainite, or martensite. Surface reliefs indicate the super-cooling austenite transform on the surface of specimen, the formation condition and transformation resistance for new phase is different on surface and in interior of specimen. The free limit of bulk expansion is larger in the direction perpendicularly to specimen surface, and ferrite, cementite, bainite ferrite, martensite are all expanse outward. Accordingly, the surface relief results from the heterogeneous bulk expansion of specimen surface during phase transformation, which is a commonly phenomenon during supercooed austenite transformation on surface of specimen, not belong to a special phase transformation yet.
机译:研究过冷奥氏体的相变产物的表面起伏非常重要。近来,已经通过AFM,STM和SEM对贝氏体,马氏体,珠光体的表面起伏进行了许多研究。本文研究了过冷奥氏体相变产物的表面浮雕。结果表明,贝氏体,马氏体和珠光体的表面起伏均为帐篷型(∧)或N(N)型,表面起伏高度通常为十纳米左右,且坡度平坦。马氏体的表面浮雕没有N(N)型的特征。浮雕图案分别对应于它们自己的微观结构。表面凹凸的形成机理由于热处理的异常而复杂。过冷奥氏体的相变均为一阶相变,即,当过冷奥氏体转变为珠光体,贝氏体或马氏体时,发生体积膨胀。表面浮雕表明试样表面过冷奥氏体相变,试样表面和内部新相的形成条件和相变阻力不同。体膨胀的自由极限在垂直于试样表面的方向上更大,并且铁素体,渗碳体,贝氏体铁素体,马氏体都向外扩展。因此,表面起伏是由于相变过程中试样表面的不均匀膨胀引起的,这是试样表面超冷奥氏体转变时的普遍现象,尚不属于特殊的相变。

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