Properties of singular points in a special case of orthorhombic media

IF 0.6 Q4 GEOCHEMISTRY & GEOPHYSICS
Y. Roganov, A. Stovas, V. Roganov
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引用次数: 1

Abstract

The position of singular lines for orthorhombic (ORT) media with fixed diagonal elements of the elasticity matrix cij, i=1…6 is studied under the condition that c11, c22, c33>c66>c44>c55. In this case, the off-diagonal coefficients of the elasticity matrix c12, c13, c23 are chosen so that some of the values of d12=c12+c66, d13=c13+c55, d23=c23+c44 are zero. For orthorhombic medium, where the only one of d12, d13, d23 is zero, contains only singular points in the planes of symmetry. If two or all three dij are zero, then the ORT medium contains singular lines and discrete singular points. We call such media pathological. A degenerate ORT medium with positive d12, d13, d23 has at most two singular lines, which are the intersection of a quadratic cone with a sphere. The pathological media may have up to 6 singular lines on the surface of the slowness. Singular lines for pathological media are described by more complex equations than conventional degenerate ORT models. The article proposes to using squares x, y, z of the components of the slowness vector in the equations. In a new coordinate system, equations defining singular lines for pathological media become linear or quadratic. Intersecting with the plane x+y+z =1, they define the straight lines, ellipses, or hyperbolas. If non-zero values d12, d13, d23 increase, the singular lines pass through four fixed points on the plane x+y+z =1, which makes it possible to describe the evolution of their change. Conditions are derived under which the singular curves of pathological ORT models are limiting the singular curves for degenerate ORT models with positive values of d12, d13, d23. Formulas are derived for transforming surfaces of slowness and singular lines of pathological media into the region of group velocities. The results are demonstrated with examples of pathological models obtained from the standard model of the ORT medium by changing the elasticity coefficients c12, c13, c23 so that some of the values d12, d13, d23 are zero
正交介质特殊情况下奇异点的性质
在c11, c22, c33>c66>c44>c55条件下,研究了弹性矩阵cij, i=1…6的对角线单元固定的正交介质奇异线的位置。在这种情况下,选择弹性矩阵c12, c13, c23的非对角线系数,使得d12=c12+c66, d13=c13+c55, d23=c23+c44的一些值为零。对于正交介质,其中d12, d13, d23中只有一个为零,在对称平面上只包含奇异点。如果两个或全部三个dij为零,则ORT介质包含奇异线和离散奇异点。我们称这种媒体为病态。对于d12, d13, d23为正的简并ORT介质,其奇异线最多有两条,即二次锥与球的交点。病理介质可能在缓慢的表面上有多达6条奇异线。病理介质的奇异线用比传统的退化ORT模型更复杂的方程来描述。本文建议在方程中使用慢度矢量分量的x、y、z的平方。在新的坐标系中,病态介质的奇异线方程变成了线性或二次的。它们与平面x+y+z =1相交,定义直线、椭圆或双曲线。如果非零值d12, d13, d23增加,奇异线经过x+y+z =1平面上的四个固定点,可以描述它们的变化演变。推导了病态ORT模型奇异曲线限制d12、d13、d23为正值的退化ORT模型奇异曲线的条件。导出了将病理介质的慢速面和奇异线转化为群速度区的公式。通过改变弹性系数c12、c13、c23,使d12、d13、d23的某些值为零,从ORT介质的标准模型得到病理模型的例子证明了这一结果
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来源期刊
Geofizicheskiy Zhurnal-Geophysical Journal
Geofizicheskiy Zhurnal-Geophysical Journal GEOCHEMISTRY & GEOPHYSICS-
自引率
60.00%
发文量
50
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