Anomalous Refraction of Transversely Isotropic Media with Strong Anisotropy

Sedimentary rocks in the interior of the earth are usually considered in a sequence of thin layers. The physical properties, such as acoustic impedance, are commonly treated as invariant within a layer but can vary from layer to layer. Therefore, the layered rocks are preserved as transversely isotropic with respect to its vertical axis of symmetry but macroscopically anisotropic [1-4]. Reflection and refraction of acoustic waves between adjacent rocks have profound implications in geophysics, e.g., in earthquake seismology, seismic image and analysis, and underwater acoustics [5-11]. The physical properties of the transversely isotropic media with a vertical axis of symmetry (VTI media), as shown in Figure 1(a), can be described by an elastic stiffness tensor [2, 7, 12-16],


Introduction
Sedimentary rocks in the interior of the earth are usually considered in a sequence of thin layers. The physical properties, such as acoustic impedance, are commonly treated as invariant within a layer but can vary from layer to layer. Therefore, the layered rocks are preserved as transversely isotropic with respect to its vertical axis of symmetry but macroscopically anisotropic [1][2][3][4]. Reflection and refraction of acoustic waves between adjacent rocks have profound implications in geophysics, e.g., in earthquake seismology, seismic image and analysis, and underwater acoustics [5][6][7][8][9][10][11]. The physical properties of the transversely isotropic media with a vertical axis of symmetry (VTI media), as shown in Figure 1(a), can be described by an elastic stiffness tensor [2,7,[12][13][14][15][16] where the matrix elements are functions of stress and strain in the medium and c =c -2c .
The reflection and refraction coefficients are influenced by several factors, including the acousticimpedance, the anisotropy of the media at two sides of the interface, and the incident angle of the acoustic signal. The critical incident angles are also affected by the anisotropy. At the interface between two VTI media, as shown in Figure 2, Snell's law can be used to establish a fourthorder polynomial for the angles of the reflection and refraction [13]. Most recently, an eighth-order polynomial has also been established for the transversely isotropic medium with a tilt axis of symmetry (TTI medium), as shown in Figure 1(b) [22]. The solution reveals a possible anomalous incident angle that occurs for strongly anisotropic media.

Anomalous Incident Angle
The angles of reflection and refraction are defined in Figure 2. The anomalous incident angle is usually in the post-critical incidence region. The phase velocities are given as . The reflection and refraction are defined such that R is the reflection coefficient of P-wave to P-wave, R is the refraction coefficient of Pwave to P-wave, R is the reflection coefficient of P-wave to SV-wave, and R is the refraction coefficient of P-wave to SV-wave. Finally, is a phase shift for an induced wave relative to the incident P-wave.
The physical origin of the anomalous reflection is the strong anisotropy of the media, embedded in Snell's law. For any given incident angle regime, all waves involved in the reflection and refraction must satisfy Snell's law (see Figure 2), .
For some specific incident angle, the required root of the phase velocities of the refracted P-wave must be adjusted in order to satisfy Snell's law, , where (i = 1, 2) are the two phasevelocity solutions.
Encyclopedia 2020 doi: 10.32545/encyclopedia202001.0005.v1 As an example, let's consider the interface between two sedimentary rocks, specifically, anisotropic shale (A-shale) as the incidence medium and oil shale (O-shale) as the refraction medium. The physical properties of these sedimentary rocks have been reported in the literature [17][18][19], from which the angles of reflection and refraction may be calculated based on a fourth-order polynomial [13,[17][18][19]. Figure 3 shows the angle of the refracted P-wave as a function of the incident angle. Figure 4 presents the velocity of the refracted P-wave as a function of the incident angle.

Anomalous Refraction
For the calculated results at the incident angle of 62.04 as shown in Figure 4, the phase velocity solution of the refracted P-wave is different before and after this incident angle, switching from to . The switching of the phase velocity solutions at this incident angle avoids a step variation of the calculated reflection and refraction coefficients that must abide by the law of energy conservation. This justification of the phase velocity from to is anomalous for the P-wave to P-wave refraction.
As an example, consider the P-wave to P-wave refraction coefficient R . For the interface of O-shale and Ashale, the refraction coefficient, as a function of incident angle, is presented in Figure 5. Similar results have been found for the reflection and refraction of P-wave to SV-waves. It is noted that in the case of an anisotropic interface, the incident critical angle of the refracted P-wave is at 40.45°, e.g., in the weak anisotropic interface of A-shale and T-sandstone. In a strong anisotropic interface such as the interface of A-shale and O-shale, an anomalous incident angle is at 62.04° in the post-incident angle region. This corresponds to a critical angle of 33.63° for the refracted P-wave. At this critical angle of incidence, discontinuities in the reflection and refraction coefficients occur, as shown in Figure 5.
In such an abnormal angle of incidence, the solution of the phase velocity of the refracted P-wave must be adjusted, so that the solution of the phase velocity satisfies Snell's law. This guarantees that the calculated reflection and refraction coefficients are continuous at this anomalous incident-angle.
For the interface between A-shale and O-shale, the calculated reflection and refraction coefficients as functions of media anisotropy and incident-angle are given in Figure 6.

Final Remarks
For the interface between two VTI media, it should be noted that the anomalous incident angle and the anomalous reflection are not universal for all interfaces of VTI media. The anomalous angle is most likely to occur only when there is strong anisotropy across the interface, e.g., at the interface of O-shale and Ashale, but not at the interface of O-shale and T-sandstone.
Intuitively, the anomalous incident angle and the anomalous reflection could also occur at the interface between two different sedimentary rock layers with strong anisotropy, e.g., at the interface either between VTI and TTI media or between TTI and TTI media. However, up to this moment, there is no published work Encyclopedia 2020 doi: 10.32545/encyclopedia202001.0005.v1 to show this phenomenon at such an interface.
Finally, we consider the usefulness of these findings in the real world. While the existence and determination of anomalous reflections are theoretically substantial, their significance can be more fully realized if they are confirmed from experimental observations and applied to practical applications such as in geophysics and seismic exploration. Similar to many other cases of optical and acoustic phenomena [23][24], additional work needs to be done to fully understand their practical significance, which may further lead to productive industrial applications.