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Crystallographic Peculiarities of Shear α-γ Transformation in Austenitic Stainless Steel in the High Temperature Area

机译:高温区奥氏体不锈钢剪切α-γ相变的晶体学特性

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Structure-texture states in 18Cr-9Ni austenitic stainless steel after long-term operation of the tube at high temperatures and neutron irradiation have been investigated with orientation microscopy (EBSD). In the examined samples, cut out at the external surface, a significant concentration of α-phase with the lattice close to bcc has been detected. Phase transformation shows prominent crystallographic direction, caused by initial orientation of austenite grains and tensile stress effect, normally directed at a tangent to its external surface. High-angle boundary spectrum with the most prominent coincidence site lattice (CSL) boundaries, ∑3, ∑11, ∑25b, ∑33c ∑41c, is typical for α-phase. Thus, it can be claimed that austenite transformation was carried out by shear (bainite, taking into account high temperature) mechanism, according to orientation relationships (OR), intermediate between Kurdjumov-Sachs (K-S) and Nishiyama-Wassermann (N-W). Shear γ-a transformation began in austenite on twin boundaries (CSL Σ3), and was carried out in the range determined by initial orientation of γ-phase crystals and effective stress value. Based on high density of CSL boundaries Σ3 in α-phase it has been suggested that its nuclei are represented not by single crystallites, but crystallite couples in twin misorientation.
机译:用取向显微镜(EBSD)研究了18Cr-9Ni奥氏体不锈钢在高温和中子辐照下长期运行后的组织结构状态。在检查的样品中,在外表面切出的样品中,已检测到明显的α相浓度,且晶格接近bcc。相变显示出明显的晶体学方向,这是由于奥氏体晶粒的初始取向和拉伸应力效应(通常指向其外表面的切线)引起的。高相边界晶格(CSL)边界最突出的高角度边界光谱∑3,∑11,∑25b,∑33c,∑41c是α相的典型特征。因此,可以说奥氏体转变是通过剪切(贝氏体,考虑到高温)机制,根据Kurdjumov-Sachs(K-S)和Nishiyama-Wassermann(N-W)之间的取向关系(OR)进行的。剪切γ-a转变在双边界(CSLΣ3)的奥氏体中开始,并且在由γ相晶体的初始取向和有效应力值确定的范围内进行。基于α相中CSL边界Σ3的高密度,已提出其核不以单微晶表示,而是以孪晶取向失调表示微晶对。

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