182 REFERENCES Bourbié, T., Coussy, O., and Zinszner, B., 1987, Acoustics of porous media: Editions Technip. Harjes, H.-P., Bram, K., Dürbaum, H.-J., Gebrande, H., Hirschmann, G., Janik, M., Klöckner, M., Lüschen, E., Rabbel, W., Simon, M., Thomas, R., Tormann, J., and Wenzel, F., 1997, Origin and nature of crustal reflections: results from integrated seismic measurements at the KTB superdeep drill hole: Journal of Geophysical Research, 102, 18267–18288. Holliger, K., 1996, Upper-crustal seismic velocity heterogeneity as derived from a variety of p-wave logs: Geophys J. Int., 125, 813–829. Holliger, K., 1997, Seismic scattering in the upper crystalline crust based on the evidence from sonic logs: Geophys J. Int., 128, 65–72. Jia, Y., and Harjes, H.-P., 1997, Seismische q-werte als ausdruck von intrinsischer dämpfung und streudämpfung der kristallinen kruste um die ktb-lokation: ICDP- Kolloquium, Bochum. Jones, A. G., and Holliger, K., 1997, Spectral analyses of the ktb sonic an density logs using robust nonparametric methods: Journal of Geophysical Research, 102, 18,391–18,403. Kneib, G., 1995, The statistical nature of the upper continental crystalline crust derived from in situ seismic measurements: Geophys J. Int., 122, 594–616. Li, X.-P., and Richwalski, S., 1996, Seismic attenuation and velocities of p- and s- waves in the german ktb area: J. Appl. Geophys., 36, 67–76. Müller, T. M., Shapiro, S. A., and Sick, C., <strong>2000</strong>, A weak fluctuation approximation of primary waves in random media: Waves Random Media, submitted. Pujol, J., Lüschen, E., and Hu, Y., 1998, Seismic wave attenuation in methamorphic rocks from vsp data recorded in germany's continental super-deep borehole: Geophysics, 63, 354–365. Sato, H., and Fehler, M., 1998, Wave propagation and scattering in the heterogenous earth: AIP-press. Shapiro, S. A., and Hubral, P., 1999, Elastic waves in random media: Springer. Shapiro, S. A., Schwarz, R., and Gold, N., 1996, The effect of random isotropic inhomogeneities on the phase velocity of seismic waves: Geophys. J. Int., 127, 783–794. Wu, R.-S., Xu, Z., and Li, X.-P., 1994, Heterogeneity spectrum and scale-anisotropy in the upper crust revealed by the german continental deep-drilling (ktb) holes: Geophysical Research Letters, 21, 911–914.
Wave Inversion Technology, <strong>Report</strong> No. 4, pages 183-191 Effective velocities in fractured media: Intersecting and parallel cracks E.H. Saenger and S.A. Shapiro 1 keywords: finite differences, effective velocities, fractured media ABSTRACT This paper is concerned with a numerical study of effective velocities in two types of fractured media. We apply the so-called rotated staggered finite difference grid technique. Using this modified grid it is possible to simulate the propagation of elastic waves in a 2D or 3D medium containing cracks, pores or free surfaces without hardcoded boundary conditions. Therefore it allows an efficient and precise numerical study of effective velocities in fractured structures. We model the propagation of plane waves through a set of different randomly cracked media. In these numerical experiments we vary the crack density. The synthetic results are compared with several theories that predict the effective P- and S-wave velocities in fractured materials. For randomly distributed and randomly oriented rectilinear intersecting thin dry cracks the numerical simulations of velocities of P-, SV- and SH-waves are in excellent agreement with the results of a new critical crack density (CCD) formulation. On the other hand for randomly distributed rectilinear parallel thin dry cracks three different classical theories are compared with our numerical results. INTRODUCTION The problem of effective elastic properties of fractured solids is of considerable interest for geophysics, for material science, and for solid mechanics. In this paper we consider the problem of a fractured medium in two dimensions. With this work some broad generalizations can be elucidated that will help solving problems with more complicated geometries. Strong scattering caused by many dry cracks can be treated only by numerical techniques because an analytical solution of the wave equation is not available. So-called boundary integral methods are well suited to handle such discrete scatterers in a homogeneous embedding. They allow the study of SV-waves (Davis and Knopoff, 1995; Murai et al., 1995), SH-waves (Dahm and Becker, 1998) and P-waves (Kelner et al., 1 email: saenger@geophysik.fu-berlin.de, shapiro@geophysik.fu-berlin.de 183
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14 Trace no. 1000 1500 2000 0.5 1.0
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16 CDP number 3100 3000 2900 2800 2
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18 REFERENCES Höcht, G., de Bazela
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20 INVERSION BY MEANS OF CRS ATTRIB
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22 For synthetic data, it is easy t
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31 Dürbaum, H., 1954, Zur Bestimmu
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0 0 ˜ ” Z ˜ ” Z 4 4
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39 strategy by combining global and
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41 elled data is presented in Figur
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43 0.2 Distance [m] 1000 1500 2000
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45 In Figure 10 we have the optimiz
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47 Gelchinsky, B., 1989, Homeomorph
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54 As stated in Hubral and Krey, 19
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§ ó § 56 sequence. We made tes
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58 precision of the modeled input d
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60 Cohen, J., Hagin, F., and Bleist
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£ 65 The details of the theory inv
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67 of the figure. On both sides, a
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69 (a) (b) Depth (m) 600 800 Depth
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71 Langenberg, K., 1986, Applied in
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g ý g [ ^ â g [ g g g g g â h [
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g § » ¹ [ƒŽ g 79 We now subst
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ê 81 ing was realized by an implem
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85 on a second-order approximation.
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88 kinematic (related to traveltime
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94 1 taper value ksi1 0 ksi2 Figure
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96 0 1 2 3 4 5 Depth [km] CMP [km]
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98 CONCLUSION As a generalization o
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100 weight during the stacking proc
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102 are not illuminated for every o
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104 obtained from Zoeppritz' equati
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106 PreSDM of Porous layer 0.358 re
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108 REFERENCES Gassmann, F., 1951,
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110 et al., 1992), Hanitzsch (1997)
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112 consecutive wavefronts). Howeve
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114 Numerical example We test the W
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116 Versteeg, R., and Grau, G., 199
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118 indicator. To extract elastic p
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€ b b 120 S where is the position
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É É É É 122 The À constant (da
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124 0 Distance [ m ] 1000 2000 3000
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126 Kosloff, D., Sherwood, J., Kore
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128
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130 penetration distances and a pot
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- Page 156 and 157: 144 Shapiro, S. A., and Müller, T.
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- Page 160 and 161: 148 RESULTS Soultz-sous-Forêts Inv
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232 Figure 3: The evolution of a WF
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236 CONCLUSIONS We have presented a
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238
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Ž Ž Ã Ž 242 Other two approxima
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248 Ettrich, N., 1998, FD eikonal s
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‹ 256 transport equation. Neverth
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268 NUMERICAL RESULTS We constructe
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£ -š' - 272 Ô- —- Figure 6: C
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274 REFERENCES Aldridge, D. F. (199
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276
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278 3. 4. True-amplitude imaging, m
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280 Research Group Hamburg (Gajewsk
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282 Stefan Lüth Robert Patzig Refr
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284 Landmark Graphics Corp. 7409 S.
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286 TotalFinaElf Exploration UK plc
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288 as research assistant at Geoeco
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290 Ingo Koglin is a diploma studen
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292 Matthias Riede received his M.S
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294 Svetlana Soukina received her d
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296 Yonghai Zhang received the Mast