- A - Physics of the Earth's Interior
- B - Seismology
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C - Geomagnetism
C-118, C-117, C-116, C-115, C-114, C-113, C-112, C-111, C-110, C-109, C-108, C-107, C-106, C-105, C-104, C-103, C-102, C-101, C-100, C-99, C-98, C-97, C-96, C-95, C-94, C-93, C-92, C-91, C-90, C-89, C-88, C-87, C-86, C-85, C-84, C-83, C-82, C-81, C-80, C-79, C-78, C-77, C-76, C-75, C-74, C-73, C-72, C-71, C-70, C-69, C-68, C-67, C-66, C-65, C-64, C-63, C-62, C-61, C-60, C-59, C-58, C-57, C-56, C-55, C-54, C-53, C-52, C-51, C-50, C-49, C-48, C-47, C-46, C-45, C-44, C-43, C-42, C-41, C-40, C-39, C-38, C-37, C-36, C-35, C-33, C-32, C-31, C-30, C-29, C-28, C-27, C-26, C-25, C-24, C-23, C-22, C-21, C-20, C-19, C-18, C-17, C-16, C-15, C-14, C-13, C-12, C-11, C-10, C-9, C-8, C-7, C-6, C-5, C-4, C-3, C-2, C-1
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D - Physics of the Atmosphere
D-79, D-78, D-77, D-76, D-75, D-74, D-73, D-72, D-71, D-70, D-69, D-68, D-67, D-66, D-65, D-64, D-63, D-62, D-61, D-60, D-59, D-58, D-57, D-56, D-55, D-54, D-53, D-52, D-51, D-50, D-49, D-48, D-47, D-46, D-44, D-45, D-43, D-42, D-41, D-40, D-39, D-38, D-37, D-35, D-34, D-33, D-32, D-31, D-30, D-28, D-27, D-26, D-25, D-24, D-23, D-22, D-21, D-20, D-19, D-18, D-17, D-16, D-15, D-14, D-13, D-12, D-11, D-10, D-9, D-8, D-7, D-6, D-5, D-4, D-3, D-2, D-1
- E - Hydrology
- P - Polar Research
- M - Miscellanea
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Online First
Anisotropy Estimation of Lower Paleozoic Shales from Northern Poland using Microseismic Data
Volume: 432
Series: B-43
DOI: 10.25171/InstGeoph_PAS_Publs-2021-001
Downhole microseismic monitoring is a widely used tool for the assessment of hydraulic fracturing job effectiveness. During the process of fluid injection into the reservoir, new fractures develop due to the induced pressure, which gives rise to microseismic events. Therefore, the knowledge of an accurate velocity model is necessary in order to locate the induced micro-seismic events. Subsurface complexity is often raised by a horizontal layering, an intrinsic anisotropy of shales, and aligned fracture sets. That introduces anisotropic effects into the velocity field. In such a case, the anisotropy should be taken into account during the velocity model building. Otherwise, some errors will be introduced into the microseismic event locations, and hence, the interpretation of treatment effects will be biased. Therefore, this thesis is devoted to the anisotropy estimation using downhole microseismic data. It examines possible location errors caused when the anisotropy effect is not considered and proposes a technique of anisotropic velocity model inversion. It also presents field data examples of anisotropic model building and fractures characterization.
In this thesis, I introduce a new technique for anisotropic (VTI) velocity model inversion based on traveltimes of the P-, SH-, and SV-waves onsets and probabilistic event location algorithm. This is followed by synthetic studies showcasing errors expected in microseismic event locations when anisotropy is neglected. In addition, a feasibility study of performing quasi-real-time anisotropic velocity model inversion during an ongoing hydraulic fracturing job is included.
Then, I present two different applications of the developed methodologies to the field data from a downhole microseismic survey that was carried out to monitor hydraulic fracturing in the Lower Paleozoic gas-bearing shales in Lubocino well, Northern Poland. In the first application, the VTI anisotropic velocity model inversion using the traveltimes of perforation shots is applied. The accuracy of the model provides high-quality locations of microseismic events induced during the hydraulic treatment. Then, the locations become a basis for a detailed stage-by-stage evaluation of the stimulation performance and provide information about geological units that were successfully fractured.
In the second application, I utilize shear-wave splitting (SWS) measurements to reveal weak azimuthal (HTI) anisotropy caused by aligned fractures. The HTI is dominated by stronger VTI fabric produced by the alignment of anisotropic platy clay minerals and by thin horizontal layering. I perform the rock-physics model inversion based on SWS measurements to finally obtain an orthorhombic stiffness tensor, which links the dominant VTI fabric with HTI anisotropy produced by the presence of aligned vertical natural fracture sets in the shale-gas reservoir.
Finally, based on both synthetic and real data examples, it is concluded that taking the anisotropy into account during the velocity model building in downhole applications always enhances the accuracy of microseismic event locations, and hence, raises the quality of the final assessment of hydraulic fracturing operation. It is also demonstrated that the proposed VTI anisotropic velocity model inversion can be implemented on-site during an ongoing industry operation.
MONOGRAPHIC VOLUME
C O N T E N T S
Editorial note, ...4
Acknowledgements, ...4
List of symbols, ...8
List of abbreviations, ...9
Abstract, ...5
Streszczenie, ...6
1. Introduction, ...10
1.1 Microseismic monitoring – what is it?, ...10
1.2 The aims of this thesis, ...11
1.3 Summary of the following chapters, ...12
1.4 Geological setting, ...13
1.5 Data used in this research, ...14
2. Theory, ...15
2.1 Seismic wave propagation in anisotropic media, ...16
2.2 Problem of earthquake location using a downhole monitoring array, ...21
2.2.1 Traveltime calculation, ...22
2.2.2 Traveltime-based velocity model inversion, ...23
2.3 Shear-wave splitting, ...24
2.3.1 Measuring the shear-wave splitting, ...26
2.3.2 Inversion of SWS measurements for rock-physics parameters, ...27
3. Developed methodology and synthetic examples, ...28
3.1 Probabilistic event location, ...29
3.1.1 Station-event back-azimuth estimation, ...33
3.2 VTI velocity model inversion scheme, ...34
3.2.1 Synthetic tests, ...36
I. Proximate single-stage isotropic, ...38
II. Proximate isotropic, ...40
III. Proximate anisotropic, ...42
IV. Distant anisotropic, ...45
V. Thinning layer accuracy test, ...47
VI. Effective anisotropy, ...8
3.2.2 Feasibility of real-time inversion, ...49
3.3 Conclusions from this chapter, ...50
4. Building an anisotropic velocity model for microseismic events location, ...51
4.1 Data and initial data processing, ...51
4.1.1 Perforation shots, ...51
4.1.2 Determining the orientation of geophones, ...53
4.1.3 Microseismic events detection, ...55
4.1.4 Arrivals picking, ...55
4.2 Anisotropic velocity model building, ...56
4.2.1 Inverting for VP0 and VS0 of top four layers and Thomsen’s ε, ...58
4.2.2 Inverting for Thomsen’s γ using extra traveltimes of microseismic events, ...59
4.2.3 Estimating VP0 and VS0 of the bottom layer, ...60
4.2.4 The final model, ...61
4.2.5 Locating the perforation shots in horizontal plane, ...63
4.3 Locating the microseismic events, ...65
4.4 Evaluation of the stimulation performance, ...68
4.5 Conclusions from this chapter, ...70
5. Estimating fracture parameters based on shear-wave splitting, ...71
5.1 Data and SWS measurements, ...71
5.2 Inversion of SWS measurements for rock-physics parameters, ...75
5.2.1 Inversion results, ...77
5.2.2 Discussion, ...77
5.3 Conclusions from this chapter, ...81
6. Summary and conclusions, ...82
References, ...83