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A modified Lekhnitskii formalism a la Stroh for anisotropic elasticity and classifications of the 6 * 6 matrix N

机译:修正的Lekhnitskii形式主义a la Stroh用于各向异性弹性和6 * 6矩阵N的分类

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The Stroh formalism for two-dimensional deformations of anisotropic elastic materials computes the eigenvalue p and the eigenvector a from an eigenrelation. The vector b is then determined from a. Depending on the number of repeated eigenvalues p and the number of independent eigenvectors (a,b) the system has, it can be classified into six groups. The Lekhnitskii formalism has no eigenrelation to speak of. We present a modified Lekhnitskii formalism that computes the eigenvalue p and the eigenvector b from an eigenrelation. The vector a is then determined from b. Thus the modified Lekhnitskii formalism is a dual to the Stroh formalism. Not only does the modified formalism enable us to do the classifications, it is much simpler than using the Stroh formalism. The six groups are the SP, SS, D1, D2, ED and ES groups. The ES group does not exist for a real material. The SS group (that has p_1 = p_2 not= p_3) and the D2 group (that has p_1 = p_2 = p_3) can be identified without computing the eigenvalues p and the eigenvectors (a,b). We show that the repeated eigenvalue p_1 = p_2 in the SS and D2 groups is simply a root of the quadratic equation l_2 = 0. We present an explicit expression of p_3 for the SS group. The ED group that has three identical p can also be identified without computing p and (a,b); however, we do present an explicit expression of p. We show that monoclinic materials with the symmetry plane at x_3 = 0 cannot belong to the ED group. The identification of the SP and D1 groups is the only one that requires computation of p but not (a,b). For special classes of materials, however, they can be identified without computing p. In all cases, the eigenvectors and the generalized eigenvectors are obtained explicitly.
机译:各向异性弹性材料的二维变形的Stroh形式主义根据特征关系计算特征值p和特征向量a。然后从a确定向量b。根据系统具有的重复特征值p的数量和独立特征向量(a,b)的数量,可以将其分为六组。 Lekhnitskii形式主义没有本征关系可言。我们提出了一种改进的Lekhnitskii形式主义,可以从特征关系计算特征值p和特征向量b。然后从b确定向量a。因此,修改后的列赫尼茨基形式主义是斯特罗形式主义的对偶。修改后的形式主义不仅使我们能够进行分类,而且比使用Stroh形式主义要简单得多。这六个组是SP,SS,D1,D2,ED和ES组。对于真实材料,ES组不存在。无需计算特征值p和特征向量(a,b)即可识别SS组(具有p_1 = p_2 not = p_3)和D2组(具有p_1 = p_2 = p_3)。我们表明,SS和D2组中重复的特征值p_1 = p_2只是二次方程l_2 = 0的根。我们为SS组给出了p_3的显式表达式。无需计算p和(a,b),也可以识别出具有三个相同p的ED组。但是,我们确实给出了p的显式表达式。我们表明,具有x_3 = 0的对称平面的单斜晶材料不能属于ED组。 SP和D1组的标识是唯一需要计算p而不需要(a,b)的标识。但是,对于特殊类别的材料,无需计算p即可识别它们。在所有情况下,特征向量和广义特征向量都是明确获得的。

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