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Quartic moveout coefficient: 3D description and application to tilted TI media

机译:四级时差系数:倾斜的TI媒体的3D描述和应用

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摘要

Nonhyperbolic (long-spread) moveout provides essential information for a number of seismic inversion/ processing applications, particularly for parameter estimation in anisotropic media. Here, we present an analytic expression for the quartic moveout coefficient A_4 that controls the magnitude of nonhyperbolic moveout of pure (nonconverted) modes. Our result takes into account reflection-point dispersal on irregular interfaces and is valid for arbitrarily anisotropic, heterogeneous media. All quantities needed to compute A_4 can be evaluated during the tracing of the zero-offset ray, so long-spread moveout can be modeled without time-consuming multioffset, multiazimuth ray tracing. The general equation for the quartic coefficient is then used to study azimuthally varying nonhyperbolic moveout of P-waves in a dipping transversely isotropic (TI) layer with an arbitrary tilt v of the symmetry axis. Assuming that the symmetry axis is confined to the dip plane, we employed the weak-anisotropy approximation to analyze the dependence of A_4 on the anisotropic parameters. The linearized expression for A_4 is proportional to the anellipticity coefficient η≈ε―δ and does not depend on the individual values of the Thomsen parameters. Typically, the magnitude of nonhyperbolic moveout in tilted TI media above a dipping reflector is highest near the reflector strike, whereas deviations from hyperbolic moveout on the dip line are substantial only for mild dips. The azimuthal variation of the quartic coefficient is governed by the tilt v and reflector dip φ and has a much more complicated character than the NMO-velocity ellipse. For example, if the symmetry axis is vertical (VTI media, v = 0) and the dip φ > 30°, A_4 goes to zero on two lines with different azimuths where it changes sign. If the symmetry axis is orthogonal to the reflector (this model is typical for thrust-and-fold belts), the strike-line quartic coefficient is defined by the well-known expression for a horizontal VTI layer (i.e., it is independent of dip), while the dip-line A_4 is proportional to cos~4 φ and rapidly decreases with dip. The high sensitivity of the quartic moveout coefficient to the parameter η and the tilt of the symmetry axis can be exploited in the inversion of wide-azimuth, long-spread P-wave data for the parameters of TI media.
机译:非双曲线(长展宽)时差为许多地震反演/处理应用程序(尤其是各向异性介质中的参数估计)提供了重要信息。在这里,我们为四次运动系数A_4给出了一个解析表达式,该表达式控制纯(非转换)模式的非双曲线运动量的大小。我们的结果考虑了在不规则界面上的反射点分散,对于任意各向异性的非均质介质都是有效的。可以在追踪零偏移射线的过程中评估计算A_4所需的所有量,因此可以对长距离偏移进行建模,而无需耗时的多偏移,多方位射线跟踪。然后,使用四次系数的一般方程式来研究在对称轴具有任意倾斜v的浸入横向各向同性(TI)层中P波的方位角变化的非双曲运动。假设对称轴限制在倾角平面内,我们使用弱各向异性近似分析A_4对各向异性参数的依赖性。 A_4的线性化表达式与椭圆系数η≈ε-δ成比例,并且不依赖于Thomsen参数的各个值。通常,在浸入反射器上方的倾斜TI介质中非双曲线偏移的幅度在反射器走向附近最高,而在浸入线上与双曲线偏移的偏差仅在轻度浸入时才大。四次系数的方位角变化由倾斜度v和反射器倾角φ决定,并且比NMO速度椭圆形复杂得多。例如,如果对称轴为垂直轴(VTI介质,v = 0),并且倾角φ> 30°,则A_4在两条具有不同方位角的直线上会变为零,从而改变符号。如果对称轴正交于反射器(此模型是推力和褶皱带的典型模型),则直线的四次系数由水平VTI层的众所周知的表达式定义(即,与倾角无关) ),而垂线A_4与cos〜4φ成比例,并且随着垂线而迅速减小。对于TI介质的参数,在宽方位角,长传播的P波数据的反演中,可以利用四次时空偏移系数对参数η的高灵敏度和对称轴的倾斜。

著录项

  • 来源
    《Geophysics》 |2003年第5期|p.1600-1610|共11页
  • 作者单位

    Colorado School of Mines, Center for Wave Phenomena, Department of Geophysics, Green Center, Golden, Colorado 80401;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 地球物理学;
  • 关键词

  • 入库时间 2022-08-18 00:19:50

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