On nonlinearity parameters describing elastic wave interactions

W. Domański
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引用次数: 2

Abstract

Elastic wave interaction coefficients were defined in the case of arbitrary n-th order nonlinearity and calculated explicitly in cases of quadratically and cubically nonlinear interactions. In the first case the isotropic Murnaghan material, and the cubic crystal of class m3m were analyzed. The calculated coefficients were displayed graphically in the form of tables which reveal the difference in behavior of shear elastic waves for isotropic and anisotropic materials. In the isotropic case there is no quadratically nonlinear coupling between propagating collinearly shear waves and the appropriate coefficients disappear. In the anisotropic case there are special directions along which such a coupling takes place and the coefficients responsible for this coupling are not equal to zero. Moreover, choosing a particular direction of propagation, namely a three-fold symmetry acoustic axis, (e.g. [111] direction in a cubic crystal) results in a a very special symmetry among these coefficients. Besides, the cubically nonlinear interaction coefficients were calculated for a model of a soft solid.Elastic wave interaction coefficients were defined in the case of arbitrary n-th order nonlinearity and calculated explicitly in cases of quadratically and cubically nonlinear interactions. In the first case the isotropic Murnaghan material, and the cubic crystal of class m3m were analyzed. The calculated coefficients were displayed graphically in the form of tables which reveal the difference in behavior of shear elastic waves for isotropic and anisotropic materials. In the isotropic case there is no quadratically nonlinear coupling between propagating collinearly shear waves and the appropriate coefficients disappear. In the anisotropic case there are special directions along which such a coupling takes place and the coefficients responsible for this coupling are not equal to zero. Moreover, choosing a particular direction of propagation, namely a three-fold symmetry acoustic axis, (e.g. [111] direction in a cubic crystal) results in a a very special symmetry among these coefficients. Besides, the cubic...
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描述弹性波相互作用的非线性参数
弹性波相互作用系数在任意n阶非线性情况下定义,在二次和三次非线性相互作用情况下显式计算。在第一种情况下,分析了各向同性的Murnaghan材料和m3m类立方晶体。计算出的系数以图表的形式显示,显示了各向同性和各向异性材料的剪切弹性波行为的差异。在各向同性情况下,共线横波传播之间没有二次非线性耦合,相应系数消失。在各向异性的情况下,有一些特殊的方向发生这种耦合,导致这种耦合的系数不等于零。此外,选择特定的传播方向,即三重对称声轴(例如[111]在立方晶体中的方向)会导致这些系数之间具有非常特殊的对称性。此外,还计算了软固体模型的三次非线性相互作用系数。弹性波相互作用系数在任意n阶非线性情况下定义,在二次和三次非线性相互作用情况下显式计算。在第一种情况下,分析了各向同性的Murnaghan材料和m3m类立方晶体。计算出的系数以图表的形式显示,显示了各向同性和各向异性材料的剪切弹性波行为的差异。在各向同性情况下,共线横波传播之间没有二次非线性耦合,相应系数消失。在各向异性的情况下,有一些特殊的方向发生这种耦合,导致这种耦合的系数不等于零。此外,选择特定的传播方向,即三重对称声轴(例如[111]在立方晶体中的方向)会导致这些系数之间具有非常特殊的对称性。此外,立方…
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