SEG Technical Program Expanded Abstracts 2006 2006
DOI: 10.1190/1.2370279
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Tube‐wave monitoring of oil fields

Abstract: Tube-wave monitoring is a fit-for-purpose downhole imaging and monitoring technique. It aims to detect and characterize time-lapse changes in a cross-well space. In contrast to conventional cross-well seismic it does not require production interruption or reduces it to a minimum. Monitoring relies on tube waves in a well fluid column to carry the seismic signals to and from the reservoir. We present a simple modeling to support the concept and validate experimental data acquired at Stratton and Mallik fields.

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Cited by 7 publications
(4 citation statements)
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“…We may also interpret decrease of A s /A p in a porous media with higher mobility as redistribution of elastic energy from shear to fast compressional wave. Finally, different radiation in elastic and poroelastic media can shed some light on why tubewave conversion to body and guided waves is larger on permeable as opposed to impermeable layers (Korneev et al, 2006).…”
Section: Radiation Patternmentioning
confidence: 99%
See 1 more Smart Citation
“…We may also interpret decrease of A s /A p in a porous media with higher mobility as redistribution of elastic energy from shear to fast compressional wave. Finally, different radiation in elastic and poroelastic media can shed some light on why tubewave conversion to body and guided waves is larger on permeable as opposed to impermeable layers (Korneev et al, 2006).…”
Section: Radiation Patternmentioning
confidence: 99%
“…In this study we focus on a task of cylindrical borehole surrounded by homogeneous poroelastic Biot media. This task is important for cross-well tube-wave monitoring which relies on increased conversion of tube waves into body and guided waves on poroelastic layers compared to elastic impermeable beds (Korneev et al, 2006). Such conversion can be thought as a secondary point source in the borehole and we aim to understand how presence of permeable porous formation modifies the radiation.…”
Section: Introductionmentioning
confidence: 99%
“…; Henry ), as well as in subsurface‐feature resonance calculations (Chouet ; Ferrazini and Aki ). In addition, measuring a trapped‐mode phase speed and attenuation via subsurface seismic stations proximate to a fault may be an input for the validation of fault properties, including its aperture and the surrounding medium permeability (Nagano and Niitsuma ; Korneev, Parra, and Bakulin ; Korneev, Bakulin, and Ziatdinov ). In reality, no subsurface feature is a perfect slot of a constant aperture; one can reasonably assume, however, that our formulae are applicable asymptotically as long as wavelength is much larger than the asperity and inflection lengthscale.…”
Section: Introductionmentioning
confidence: 99%
“…Knowing that the highly dispersive trapped wave properties may turn out to be important in various studies involving seismic propagation in the presence of subsurface fractures and faults, e.g., fracture width monitoring via borehole tube wave reflections Kostek et al 1989) or fracture length assessment from tip reflections (Paige et al 1992;Henry 2005), as well as in subsurface-feature resonance calculations (Chouet 1981;Ferrazini and Aki 1987). In addition, measuring a trapped-mode phase speed and attenuation via subsurface seismic stations proximate to a fault may be an input for the validation of fault properties, including its aperture and the surrounding medium permeability (Nagano and Niitsuma 1996;Korneev, Parra, and Bakulin 2005;Korneev, Bakulin, and Ziatdinov 2006). In reality, no subsurface feature is a perfect slot of a constant aperture; one can reasonably assume, however, that our formulae are applicable asymptotically as long as wavelength is much larger than the asperity and inflection lengthscale.…”
Section: Introductionmentioning
confidence: 99%