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Alexandrov Dmitriy, Saint-Petersburg State University Numerical modeling: Tube-wave reflections in cased borehole
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Outline Modeling approaches: 1D effective wavenumber approach finite-difference Wave field in cased borehole wave field in isotropic homogeneous fluid wave field in isotropic homogeneous elastic media Reflection from geological interfaces behind casing; Reflection from corroded section of the casing; Response of perforation in cased borehole: Idealized disk-shaped perforation Idealized zero-length disk-shaped perforation 1D approach limitations; Conclusions. Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Outline Limitations Model 1 Model 2 Model 3 Conclusions 1D effective wavenumber approach Modeling approaches
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Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Introduction Outline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches
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Finite-difference (FD) code flexible little analytical insight 1D effective wavenumber approach Attractive for analysis Approximate Validity for cased borehole is unknown Validate 1D approach using FD code Outline Limitations Model 1 Model 2 Model 3 Conclusions 1D effective wavenumber approach Modeling approaches Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia.
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1D effective wavenumber approach Helmholtz equations: Solution form: Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Outline Limitations Wavefield in cased borehole Results Conclusions Modeling approaches 1D effective wavenumber approach
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Boundary conditions: Boundary conditions: continuity of pressure: continuity of fluid flow: Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Outline Limitations Wavefield in cased borehole Results Conclusions Modeling approaches 1D effective wavenumber approach
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Multilayered model Boundary conditions: continuity of pressure: continuity of fluid flow: Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Outline Limitations Wavefield in cased borehole Results Conclusions Modeling approaches 1D effective wavenumber approach
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Motion equation: Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Wave field in isotropic homogeneous fluid Outline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches
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Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Outline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches Wave field in isotropic homogeneous fluid
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Wave field in isotropic homogeneous elastic media Motion equation: Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Outline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches
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Boundary conditions Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Outline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches
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Reflection from geological interfaces behind casing Reflection coefficient for tube wave Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Outline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches
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Reflection from corroded section of the casing Reflection of tube wave from three different types of corroded section. Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Outline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches
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Idealized perforation in cased borehole Considered models: Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Finite-length perforation (10 cm) Zero-length perforation (break in casing) Outline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches
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Reflection of the tube wave from perforation with 10 cm length. Reflection of the tube wave from zero-length perforation. Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Idealized perforation in cased borehole Outline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches
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Limitations Low frequency approximation for tube-wave slowness (White J.E. 1984): Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Outline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches
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Relative error defined as: Relative error of 1D approach Considered model: Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Limitations Outline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches
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Finite-difference code 1D approach Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Reflection coefficientsOutline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches
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Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Finite-difference code 1D approach Reflection coefficientsOutline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches
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Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Finite-difference code 1D approach Reflection coefficientsOutline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches
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Validated 1D approach for multi-layered media (cased boreholes) inhomogeneous borehole casing idealized perforations in cased borehole Defined the limitations for 1D approach Conclusions Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Outline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches
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Thank you for attention! Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. Outline Limitations Wavefield in cased borehole Results Conclusions 1D effective wavenumber approach Modeling approaches
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References Outline Limitations Model 1 Model 2 Model 3 Conclusions 1D effective wavenumber approach Modeling approaches Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia. References Bakulin, A., Gurevich, B., Ciz, R., and Ziatdinov S., 2005, Tube-wave reflection from a porous permeable layer with an idealized perforation: 75th Annual Meeting, Society of Exploration Geophysicists, Expanded Abstract, 332-335. Krauklis, P. V., and A. P. Krauklis, 2005, Tube Wave Reflection and Transmission on the Fracture: 67th Meeting, EAGE, Expanded Abstracts, P217. Medlin, W.L., Schmitt, D.P., 1994, Fracture diagnostics with tube-wave reflections logs: Journal of Petroleum Technology, March, 239-248. Paige, R.W., L.R. Murray, and J.D.M. Roberts, 1995, Field applications of hydraulic impedance testing for fracture measurements: SPE Production and Facilities, February, 7-12. Tang, X. M., and C. H. Cheng, 1993, Borehole Stoneley waves propagation across permeable structures: Geophysical Prospecting, 41, 165-187. Tezuka, K., C.H. Cheng, and X.M. Tang, 1997, Modeling of low-frequency Stoneley- wave propagation in an irregular borehole: Geophysics, 62, 1047-1058. White, J. E., 1983, Underground sound, Elsevier. Winkler, K. W., H. Liu, and D.L. Johnson, 1989, Permeability and borehole Stoneley waves: Comparison between experiment and theory: Geophysics, 54, 66–75.
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Formation parameters Longitudinal velocity (m/s) Shear velocity (m/s) Density (kg/m 3 ) Elastic half- spaces 350025003400 Fluid1500-1000 Casing 1 (steel) 600030007000 Casing 2 (plastic) 284014801200 Layer 1310018002600 Layer 2370024003000 Corroded section 1 12006001400 Corroded section 2 300015003500 Corroded section 3 420021004900 Outline Limitations Model 1 Model 2 Model 3 Conclusions 1D effective wavenumber approach Modeling approaches Tube-wave reflections in cased borehole AlexandrovDmitriy, StPSU, Saint-Petersburg, Russia.
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