Gallardo-Basile Francisco-José, Naunheim Yannick, Roters Franz, Diehl Martin
Max-Planck-Institut für Eisenforschung, Max-Planck-Straße 1, 40237 Düsseldorf, Germany.
Department of Materials Science and Engineering, Massachusetts Institute of Technology (MIT), 77 Massachusetts Avenue, Cambridge, MA 02139, USA.
Materials (Basel). 2021 Feb 2;14(3):691. doi: 10.3390/ma14030691.
Lath martensite is a complex hierarchical compound structure that forms during rapid cooling of carbon steels from the austenitic phase. At the smallest, i.e., 'single crystal' scale, individual, elongated domains, form the elemental microstructural building blocks: the name-giving laths. Several laths of nearly identical crystallographic orientation are grouped together to blocks, in which-depending on the exact material characteristics-clearly distinguishable subblocks might be observed. Several blocks with the same habit plane together form a packet of which typically three to four together finally make up the former parent austenitic grain. Here, a fully parametrized approach is presented which converts an austenitic polycrystal representation into martensitic microstructures incorporating all these details. Two-dimensional (2D) and three-dimensional (3D) Representative Volume Elements (RVEs) are generated based on prior austenite microstructure reconstructed from a 2D experimental martensitic microstructure. The RVEs are used for high-resolution crystal plasticity simulations with a fast spectral method-based solver and a phenomenological constitutive description. The comparison of the results obtained from the 2D experimental microstructure and the 2D RVEs reveals a high quantitative agreement. The stress and strain distributions and their characteristics change significantly if 3D microstructures are used. Further simulations are conducted to systematically investigate the influence of microstructural parameters, such as lath aspect ratio, lath volume, subblock thickness, orientation scatter, and prior austenitic grain shape on the global and local mechanical behavior. These microstructural features happen to change the local mechanical behavior, whereas the average stress-strain response is not significantly altered. Correlations between the microstructure and the plastic behavior are established.
板条马氏体是一种复杂的分层复合结构,在碳钢从奥氏体相快速冷却过程中形成。在最小尺度,即“单晶”尺度下,单个细长的区域构成了基本的微观结构单元:即赋予名称的板条。几个具有几乎相同晶体取向的板条聚集在一起形成块,根据具体材料特性,在这些块中可能会观察到明显可区分的子块。几个具有相同惯习面的块共同形成一个束,通常三到四个束最终共同构成原来的母奥氏体晶粒。在此,提出了一种完全参数化的方法,该方法将奥氏体多晶体表示转换为包含所有这些细节的马氏体微观结构。基于从二维实验马氏体微观结构重建的先前奥氏体微观结构生成二维(2D)和三维(3D)代表性体积单元(RVE)。这些RVE用于基于快速谱方法的求解器和唯象本构描述的高分辨率晶体塑性模拟。从二维实验微观结构和二维RVE获得的结果比较显示出高度的定量一致性。如果使用三维微观结构,应力和应变分布及其特征会发生显著变化。进行了进一步的模拟,以系统地研究微观结构参数,如板条长宽比、板条体积、子块厚度、取向散射和先前奥氏体晶粒形状对整体和局部力学行为的影响。这些微观结构特征恰好改变了局部力学行为,而平均应力-应变响应没有明显改变。建立了微观结构与塑性行为之间的相关性。