横向各向同性介质中优化的声波场建模

Y. Nikonenko, M. Charara, M. Spasennykh
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引用次数: 0

摘要

关于各向异性介质中声波场建模的研究已经发表了大量的论文。所有这些都是基于选择合适的波动方程进行数值实现。然而,这些波动方程通常是繁琐的,具有不明确的物理性质,计算要求高,并产生人为的伪剪切模式,这被认为是地震成像过程中的伪影。Duveneck和Bakker(2011)仅基于胡克定律和运动方程推导了耦合微分波动方程系统。尽管有这些优点,但这些方程在某些各向异性参数配置下是不稳定的,并且会产生s波伪影。另一方面,Liu et al.(2009)推导了一个无条件稳定的单波方程,结果证明该方程很难建模。此外,它只负责p波模式。Nikonenko和Charara(2020)已经证明,该单波方程只是Duveneck耦合方程的一个模态,并提出了其解的可能的全显式格式。我们继续使用这种方法,使解决方案最优,并将其扩展到其他各向异性的情况。数值算例表明该方法不存在伪影,具有较高的精度。
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Optimized acoustic wavefield modelling in transversely isotropic media
Summary A large number of studies have been published on the topic of acoustic wavefield modeling in anisotropic media. All of them are based on the choice of the suitable wave equation for numerical implementation. However, these wave equations are usually cumbersome, have an unclear physical nature, are computationally demanding, and generate artificial pseudo shear modes, which are considered as artifacts in the seismic imaging process. Duveneck and Bakker (2011) derived a system of coupled differential wave equations based on Hooke’s law and equation of motion only. Despite all the advantages, these equations are unstable for a certain configuration of anisotropic parameters and generate S-wave artifacts. Liu et al. (2009) , on the other hand, derived an unconditionally stable single wave equation that turned out to be difficult to model. Moreover, it is responsible only for the P-wave mode. Nikonenko and Charara (2020) have shown that this single wave equation is just one mode for the Duveneck coupled equations and proposed a possible fully explicit scheme for its solution. We continue this approach making the solution optimal and extending it to other cases of anisotropy. Numerical examples illustrate the absence of artifacts and the accuracy of the proposed method.
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