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Crystallographic analysis of cubic to orthorhombic martensitic transformation for the formation of the oxide plates in tantalum

机译:立方晶向正交晶马氏体相变的晶体学分析,用于钽中氧化物板的形成

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摘要

In the theory of martensitic transformations described by Wechsler et al. [1], the total transformation distortion is factorized into a pure distortion, which produces the essential change in crystal structure, and a lattice invariant or inhomogeneous shear. The magnitude of this shear is determined by the condition that a plane of zero distortion exist and this plane is identified as the habit plane separating the two phases. In this manner the crystallographic features of the transformation, viz. the habit plane, the orientation relation-ship between crystal axes, and the macroscopic change in shape, are determined as a function of the lattice parameters of the two phases. In the theory of Bowles and Mackenzie [2], a different factorization of the total distortion and mathematical formulation are used. This theory includes a dilatation parameter, δ, which in effect slightly relaxes the requirements that the habit plane be undistorted. But the two theories yield almost identical results [3].
机译:在Wechsler等人描述的马氏体转变理论中。 [1],总的变形畸变被分解成一个纯畸变,它产生晶体结构的本质变化,以及晶格不变或不均匀的剪切。该剪切的大小由存在零变形的平面并且该平面被识别为将两相分开的惯性平面的条件确定。以这种方式,转变的晶体学特征即。根据两相的晶格参数确定惯性平面,晶轴之间的取向关系以及形状的宏观变化。在Bowles和Mackenzie [2]的理论中,使用了总失真的不同因式分解和数学公式。该理论包括膨胀参数δ,该参数实际上稍微放宽了习惯平面不失真的要求。但是,这两种理论产生的结果几乎相同[3]。

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