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SH-and SV-reflection waves after minimizing cross-component energy. Residual crosscomponents XY and YX after minimization are also shown. The E curve indicates the effectiveness of the minimization. High values of the SH-to SVwave energy ratio SH/SV indicate that the SH-reflection has been determined unambiguously. The dashed line in the SH-wave panel represents the S-wave reflection traveltime.

SH-and SV-reflection waves after minimizing cross-component energy. Residual crosscomponents XY and YX after minimization are also shown. The E curve indicates the effectiveness of the minimization. High values of the SH-to SVwave energy ratio SH/SV indicate that the SH-reflection has been determined unambiguously. The dashed line in the SH-wave panel represents the S-wave reflection traveltime.

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Single-well S-wave imaging has several attractive features because of its directional sensitivity and usefulness for fracture characterization. To provide a method for single-well acoustic imaging, we analyzed the effects of wave radiation, reflection, and borehole acoustic response on S-wave reflection measurements from a multicomponent dipole aco...

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Context 1
... reflection data, after correction for tool rotation according to equation 9, are used in equation 13 to determine the strike of the reflector. The 4-C data following this procedure are shown in Figure 8 with the maximum-versus-minimum cross-energy relative difference E calculated from equation 15 and the SH-SV-wave energy ratio calculated from equation 17. The SH-and SV-reflection data computed from equations 16 are also displayed. ...
Context 2
... SH-wave reflection data in contrast to the alternating amplitudes of its xx and yy counterparts; see Figure 7 now shows continuous reflection events. After minimization according to equation 11, the XY and YX residuals Figure 8 show greatly reduced amplitudes compared to their counterparts before minimization Figure 7. Correspondingly, the E relative energy difference curve shows large values, indicating the minimization was effective. Figure 9 shows the final reflector image derived from the SHwave reflection data. ...
Context 3
... angle of the intersection of the reflectors with the borehole is less than 10° dip angle 80°, which means the wavepaths to and from the reflector are almost normal to the borehole. The near-normal radiation and reception direction correspond with the zones of near-zero amplitudes of the SV-wave radiation Figure 3 and reception Figure 2 patterns, which explains the lack of SV-reflections in the data Figure 8. ...
Context 4
... event intersects the borehole at an angle of about 6°, which agrees with observations from core samples Tang et al., 2009. Using this angle of intersection and the S-wave slowness profile of Figure 6, we computed the S-wave reflection traveltime and overlaid it on the processed SH-wave reflection data of Figure 8 see Tang et al. 2008 for the traveltime calculation. The S-wave traveltime tracks the reflection event from that depth very well and confirms that the reflection events of Figure 8 are reflected S-waves. ...
Context 5
... this angle of intersection and the S-wave slowness profile of Figure 6, we computed the S-wave reflection traveltime and overlaid it on the processed SH-wave reflection data of Figure 8 see Tang et al. 2008 for the traveltime calculation. The S-wave traveltime tracks the reflection event from that depth very well and confirms that the reflection events of Figure 8 are reflected S-waves. ...

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... Single-well reflection imaging can be classified as monopole reflected P-wave imaging and dipole reflected S-wave imaging (Hornby, 1989;Tang and Patterson, 2009). The reflected P-wave imaging logging technology using a monopole source was proposed by Hornby (1989). ...
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... Following the monopole P-wave technology, Tang (2004) is the first to develop the theory and method of S-wave reflection imaging using the low-frequency dipole source, enabling azimuthal sensitivity and enhancing penetration depth for the imaging application. With many years of development and practice, dipole Swave reflection imaging is now a maturing technology in field applications (Tang and Patterson, 2009, Tang et al., 2014Lee et al., 2019;Xu et al., 2019). Nevertheless, it should be noted that a drawback of dipole S-wave imaging is the 180°ambiguity. ...
... For reflection imaging away from the borehole, the virtual source distance r 0 2 is many wavelengths away from the borehole, such that jη F v r 0 2 j ≫ 1. This allows us to accurately calculate the wavenumber integration of equation 17 using the steepest descent method (Tang and Patterson, 2009) as follows: ...
... For the dipole modeling in Figure 3c and 3d, the radial displacement is calculated by differentiating fluid pressure along the receiving direction for WL (for ALWD, the pressure difference of two receivers at the opposite sides of the collar is taken). The WL amplitude variation for the SH-wave incidence shows symmetric patterns at 90°and 270°, showing the typical 180°ambiguity of dipole measurement (Tang and Patterson, 2009). In contrast, the ALWD pattern shows strong azimuthal asymmetry. ...
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... One is to use the P-P waves radiated from a monopole source and reflected back at the impedance interface outside of the borehole (Hornby, 1989;Wang et al., 2015;Hirabayashi et al., 2017;Bennett, 2019). The other is to use the S-S waves excited by a directional dipole source (Tang, 2004;Tang and Patterson, 2009). In recent years, both methods, especially the dipole S-wave method, have been applied in oil & gas exploration successfully. ...
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In view of most wells are completed by casing pipe in oil & gas exploration and development process, it is imperative to extend the application of borehole acoustic reflection imaging (BARI) from open to cased boreholes. To understand the characteristics of signals in borehole acoustic imaging, we study the radiated and reflected elastic waves in an open and cased borehole through numerical simulations. The results show that, for a broadband dipole source, the radiated SH-waves have the highest amplitudes and broadest radiation angles in the cased borehole, which is similar to the observation in an open borehole. It is believed that the cement and casing pipe would prevent to a certain extent the energy excited by the inner borehole sources from propagating into the outside formation. However, our modeling results clearly show the existence of the cement and casing will not influence the amplitude of the radiated SH-waves significantly. In fact, the decrease of the borehole radius, which is caused by cased borehole completion here, will increase the amplitude of the radiated SH-waves. As a result, the signal-to-noise ratio (SNR) of reflected waves relative to direct waves in the cased borehole is higher than that in the open borehole. Meanwhile, the cement bond quality does not heavily affect the SNR of the reflected waves and the SNR increases with the decrease of source frequency. Interestingly, as the cutoff frequency of the dipole flexural-wave mode in the cased borehole increases rapidly with the decrease of the formation S-wave velocity, the amplitude of the direct wave also decreases significantly. This results in an increase of SNR of the reflected waves, which is beneficial for extracting the reflected waves. The field data example certifies our theoretical analysis. Our results provide a theoretical foundation for the through-casing BARI with a dipole source.