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首页> 外文期刊>Bulletin of the Seismological Society of America >Energy partitions among elastic waves for dynamic surface loads in a semi-infinite solid
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Energy partitions among elastic waves for dynamic surface loads in a semi-infinite solid

机译:半无限固体中动态表面载荷在弹性波之间的能量分配

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摘要

We examine the energy partitions among elastic waves due to dynamic normal and tangential surface loads in a semi-infinite elastic solid. While the results for a dynamic normal load on the surface of a half-space with Poisson ratio of 1=4 is a well-known result by Miller and Pursey (1955), the corresponding results for a dynamic tangential load are almost unknown. The partitions for the normal and tangential loads were computed independently by Weaver (1985) versus Poisson ratio (0 ≤ ν ≤ 1=2), using diffuse-field concepts within the context of ultrasonic measurements. The connection with the surface load point was not explicit, which partially explains why these results did not reach the seismological and engineering literature. The characteristics of the elastic radiation of these two cases are quite different. For a normal load, about 2=3 of the energy leaves the loaded point as Rayleigh surface waves. On the other hand, the tangential load induces a similar amount in the form of body shear waves. It is established that the energies injected into the elastic half space by concentrated normal and tangential harmonic surface loads are proportional to the imaginary part of the corresponding components of the Green's tensor when both source and receiver coincide. The relationship between the Green's function and average correlations of motions within a diffuse field is clearly established.
机译:我们研究了半无限弹性固体中由于动态法向和切向表面载荷而在弹性波之间的能量分配。虽然泊松比为1 = 4的半空间表面上的动态法向载荷的结果是Miller和Pursey(1955)众所周知的结果,但动态切向载荷的相应结果几乎是未知的。法线和切向载荷的分配是由Weaver(1985)对泊松比(0≤v≤1 = 2)进行独立计算的,其中使用了超声测量范围内的扩散场概念。与表面载荷点的联系并不明确,这在一定程度上解释了为什么这些结果未达到地震和工程文献的原因。这两种情况的弹性辐射的特征完全不同。对于正常负载,大约2 = 3的能量作为瑞利表面波离开负载点。另一方面,切向载荷以人体剪切波的形式感应出类似的量。可以确定,当源和接收器重合时,由集中的法向和切向谐波表面载荷注入弹性半空间的能量与格林张量的相应分量的虚部成比例。格林函数与弥散场中运动的平均相关性之间的关系已明确建立。

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