Establishment and application of an anisotropic shale rock physical model in the observation coordinate system
No shale-rock physical model has been established in the observation coordinate system. To this end, this paper carried out anisotropic wave velocity tests on shale rock and compared the Thomsen, Daley, and Berryman solutions to characterize anisotropic acoustic wave velocity. Finally, the Daley sol...
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description | No shale-rock physical model has been established in the observation coordinate system. To this end, this paper carried out anisotropic wave velocity tests on shale rock and compared the Thomsen, Daley, and Berryman solutions to characterize anisotropic acoustic wave velocity. Finally, the Daley solution was selected. Based on basic rock physical models, such as SCA and DEM methods, and combined with the Daley solution, an anisotropic shalerock physical model was established in the observation coordinate system and applied in Well B1 in the Luzhou area, Sichuan Basin. Our research conclusions were as follows: 1. for the samples from the same core, the P-wave velocities in three directions were in the order
V
P11
>
V
P45
>
V
P33
, shear-wave velocity
V
S11
was the largest, but
V
S33
and
V
S45
did not follow the law of
V
s33
>
V
s45
for some samples; 2. the Daley solution, which not only considers the accuracy requirements but also has a complete expression of P-, SV-, and SH-waves, is most suitable for characterization of anisotropic wave velocity in this study area; 3. the rock physical model constructed in the observation coordinate system has high accuracy, in which the absolute value of the relative error of the P-wave slowness was between 0% and 5.05% (0.55% on average), and that of shear-wave slowness was between 0% and 6.05% (0.59% on average); 4. the acoustic waves recorded in Well B1 in the observation coordinate system were very different from those in the constitutive coordinate system. The relative difference of the P-wave was between 6.76% and 30.84% (14.68% on average), and that of the S-wave was between 7.00% and 23.44% (13.99% on average). The acoustic slowness measured in the observation coordinate system, such as in a deviated well or a horizontal well section, must be converted to the constitutive coordinate system before it can be used in subsequent engineering applications; 5. the anisotropic shale-rock physical model built in the observation coordinate system proposed in this paper can provide basic data and guidance for subsequent pore pressure prediction, geomechanical modeling, and fracturing stimulation design for deviated and horizontal wells. |
doi_str_mv | 10.1007/s11770-022-0998-3 |
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fullrecord | <record><control><sourceid>wanfang_jour_proqu</sourceid><recordid>TN_cdi_wanfang_journals_yydqwl202203002</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><wanfj_id>yydqwl202203002</wanfj_id><sourcerecordid>yydqwl202203002</sourcerecordid><originalsourceid>FETCH-LOGICAL-a323t-c3efae003bb0c7d86f4c99f36e9d130784df232a2e1be99b1f34684127a7bfa3</originalsourceid><addsrcrecordid>eNp10E1rwyAYB_AwNlj38gF2E3bYKdujpjEeR-leoLBL72ISbexSTdWu5NvPkkFPA0GR3_954J9lDxieMQB7CRgzBjkQkgPnVU4vshnmnOZQzqvL9C4ZyRln8-vsJoQtQElJWcwyuwxR1r0J3U7ZiKRtkRyG3jQyGmeR0-krHRNc9G4wDQqd7BXyrvlGQzeGBHu0c63qkbEodgq5Oij_M8Ub53xrrIwKhTFEtbvLrrTsg7r_u2-z9dtyvfjIV1_vn4vXVS4poTFvqNJSAdC6hoa1VamLhnNNS8VbTIFVRasJJZIoXCvOa6xpUVYFJkyyWkt6mz1NY4_Samk3YusO3qaFYhzb_bEnqSegACTJx0kO3u0PKsQzJRWpCkjopPCkGu9C8EqLwZud9KPAIE79i6l_kbA49S9oypApE5K1G-XPk_8P_QJYYIoH</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2828400022</pqid></control><display><type>article</type><title>Establishment and application of an anisotropic shale rock physical model in the observation coordinate system</title><source>SpringerNature Journals</source><source>Alma/SFX Local Collection</source><creator>Gui, Jun-Chuan ; Sang, Yu ; Guo, Jian-Chun ; Zeng, Bo ; Song, Yi ; Huang, Hao-Yong ; Xu, Er-si ; Chen, Ya-xi</creator><creatorcontrib>Gui, Jun-Chuan ; Sang, Yu ; Guo, Jian-Chun ; Zeng, Bo ; Song, Yi ; Huang, Hao-Yong ; Xu, Er-si ; Chen, Ya-xi</creatorcontrib><description>No shale-rock physical model has been established in the observation coordinate system. To this end, this paper carried out anisotropic wave velocity tests on shale rock and compared the Thomsen, Daley, and Berryman solutions to characterize anisotropic acoustic wave velocity. Finally, the Daley solution was selected. Based on basic rock physical models, such as SCA and DEM methods, and combined with the Daley solution, an anisotropic shalerock physical model was established in the observation coordinate system and applied in Well B1 in the Luzhou area, Sichuan Basin. Our research conclusions were as follows: 1. for the samples from the same core, the P-wave velocities in three directions were in the order
V
P11
>
V
P45
>
V
P33
, shear-wave velocity
V
S11
was the largest, but
V
S33
and
V
S45
did not follow the law of
V
s33
>
V
s45
for some samples; 2. the Daley solution, which not only considers the accuracy requirements but also has a complete expression of P-, SV-, and SH-waves, is most suitable for characterization of anisotropic wave velocity in this study area; 3. the rock physical model constructed in the observation coordinate system has high accuracy, in which the absolute value of the relative error of the P-wave slowness was between 0% and 5.05% (0.55% on average), and that of shear-wave slowness was between 0% and 6.05% (0.59% on average); 4. the acoustic waves recorded in Well B1 in the observation coordinate system were very different from those in the constitutive coordinate system. The relative difference of the P-wave was between 6.76% and 30.84% (14.68% on average), and that of the S-wave was between 7.00% and 23.44% (13.99% on average). The acoustic slowness measured in the observation coordinate system, such as in a deviated well or a horizontal well section, must be converted to the constitutive coordinate system before it can be used in subsequent engineering applications; 5. the anisotropic shale-rock physical model built in the observation coordinate system proposed in this paper can provide basic data and guidance for subsequent pore pressure prediction, geomechanical modeling, and fracturing stimulation design for deviated and horizontal wells.</description><identifier>ISSN: 1672-7975</identifier><identifier>EISSN: 1993-0658</identifier><identifier>DOI: 10.1007/s11770-022-0998-3</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer Berlin Heidelberg</publisher><subject>Accuracy ; Acoustic waves ; Acoustics ; Anisotropy ; Borehole Geophysics and Rock Properties ; Coordinate systems ; Coordinates ; Earth and Environmental Science ; Earth Sciences ; Geomechanics ; Geophysics/Geodesy ; Geotechnical Engineering & Applied Earth Sciences ; Horizontal wells ; Modelling ; P waves ; Pore pressure ; Pore water pressure ; Rocks ; S waves ; Sedimentary rocks ; Seismic wave velocities ; Shale ; Shales ; Shear ; Sound waves ; Velocity ; Wave velocity</subject><ispartof>Applied geophysics, 2022-09, Vol.19 (3), p.325-342</ispartof><rights>The Editorial Department of APPLIED GEOPHYSICS 2022</rights><rights>The Editorial Department of APPLIED GEOPHYSICS 2022.</rights><rights>Copyright © Wanfang Data Co. Ltd. All Rights Reserved.</rights><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-a323t-c3efae003bb0c7d86f4c99f36e9d130784df232a2e1be99b1f34684127a7bfa3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Uhttp://www.wanfangdata.com.cn/images/PeriodicalImages/yydqwl/yydqwl.jpg</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/s11770-022-0998-3$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1007/s11770-022-0998-3$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>315,781,785,27926,27927,41490,42559,51321</link.rule.ids></links><search><creatorcontrib>Gui, Jun-Chuan</creatorcontrib><creatorcontrib>Sang, Yu</creatorcontrib><creatorcontrib>Guo, Jian-Chun</creatorcontrib><creatorcontrib>Zeng, Bo</creatorcontrib><creatorcontrib>Song, Yi</creatorcontrib><creatorcontrib>Huang, Hao-Yong</creatorcontrib><creatorcontrib>Xu, Er-si</creatorcontrib><creatorcontrib>Chen, Ya-xi</creatorcontrib><title>Establishment and application of an anisotropic shale rock physical model in the observation coordinate system</title><title>Applied geophysics</title><addtitle>Appl. Geophys</addtitle><description>No shale-rock physical model has been established in the observation coordinate system. To this end, this paper carried out anisotropic wave velocity tests on shale rock and compared the Thomsen, Daley, and Berryman solutions to characterize anisotropic acoustic wave velocity. Finally, the Daley solution was selected. Based on basic rock physical models, such as SCA and DEM methods, and combined with the Daley solution, an anisotropic shalerock physical model was established in the observation coordinate system and applied in Well B1 in the Luzhou area, Sichuan Basin. Our research conclusions were as follows: 1. for the samples from the same core, the P-wave velocities in three directions were in the order
V
P11
>
V
P45
>
V
P33
, shear-wave velocity
V
S11
was the largest, but
V
S33
and
V
S45
did not follow the law of
V
s33
>
V
s45
for some samples; 2. the Daley solution, which not only considers the accuracy requirements but also has a complete expression of P-, SV-, and SH-waves, is most suitable for characterization of anisotropic wave velocity in this study area; 3. the rock physical model constructed in the observation coordinate system has high accuracy, in which the absolute value of the relative error of the P-wave slowness was between 0% and 5.05% (0.55% on average), and that of shear-wave slowness was between 0% and 6.05% (0.59% on average); 4. the acoustic waves recorded in Well B1 in the observation coordinate system were very different from those in the constitutive coordinate system. The relative difference of the P-wave was between 6.76% and 30.84% (14.68% on average), and that of the S-wave was between 7.00% and 23.44% (13.99% on average). The acoustic slowness measured in the observation coordinate system, such as in a deviated well or a horizontal well section, must be converted to the constitutive coordinate system before it can be used in subsequent engineering applications; 5. the anisotropic shale-rock physical model built in the observation coordinate system proposed in this paper can provide basic data and guidance for subsequent pore pressure prediction, geomechanical modeling, and fracturing stimulation design for deviated and horizontal wells.</description><subject>Accuracy</subject><subject>Acoustic waves</subject><subject>Acoustics</subject><subject>Anisotropy</subject><subject>Borehole Geophysics and Rock Properties</subject><subject>Coordinate systems</subject><subject>Coordinates</subject><subject>Earth and Environmental Science</subject><subject>Earth Sciences</subject><subject>Geomechanics</subject><subject>Geophysics/Geodesy</subject><subject>Geotechnical Engineering & Applied Earth Sciences</subject><subject>Horizontal wells</subject><subject>Modelling</subject><subject>P waves</subject><subject>Pore pressure</subject><subject>Pore water pressure</subject><subject>Rocks</subject><subject>S waves</subject><subject>Sedimentary rocks</subject><subject>Seismic wave velocities</subject><subject>Shale</subject><subject>Shales</subject><subject>Shear</subject><subject>Sound waves</subject><subject>Velocity</subject><subject>Wave velocity</subject><issn>1672-7975</issn><issn>1993-0658</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNp10E1rwyAYB_AwNlj38gF2E3bYKdujpjEeR-leoLBL72ISbexSTdWu5NvPkkFPA0GR3_954J9lDxieMQB7CRgzBjkQkgPnVU4vshnmnOZQzqvL9C4ZyRln8-vsJoQtQElJWcwyuwxR1r0J3U7ZiKRtkRyG3jQyGmeR0-krHRNc9G4wDQqd7BXyrvlGQzeGBHu0c63qkbEodgq5Oij_M8Ub53xrrIwKhTFEtbvLrrTsg7r_u2-z9dtyvfjIV1_vn4vXVS4poTFvqNJSAdC6hoa1VamLhnNNS8VbTIFVRasJJZIoXCvOa6xpUVYFJkyyWkt6mz1NY4_Samk3YusO3qaFYhzb_bEnqSegACTJx0kO3u0PKsQzJRWpCkjopPCkGu9C8EqLwZud9KPAIE79i6l_kbA49S9oypApE5K1G-XPk_8P_QJYYIoH</recordid><startdate>20220901</startdate><enddate>20220901</enddate><creator>Gui, Jun-Chuan</creator><creator>Sang, Yu</creator><creator>Guo, Jian-Chun</creator><creator>Zeng, Bo</creator><creator>Song, Yi</creator><creator>Huang, Hao-Yong</creator><creator>Xu, Er-si</creator><creator>Chen, Ya-xi</creator><general>Springer Berlin Heidelberg</general><general>Springer Nature B.V</general><general>Shale Gas Research Institute,PetroChina Southwest Oil and Gas Field Company,Chengdu 610051,China%PetroChina Southwest Oil and Gas Field Company,Chengdu 610051,China%Southwest Petroleum University,State Key Laboratory of Oil and Gas Reservoir Geology and Development Engineering,Chengdu 610500,China%Chuanqing Drilling Engineering Co.,Ltd.Downhole Operation Company,Chengdu 610051,China</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>7UA</scope><scope>8FD</scope><scope>C1K</scope><scope>F1W</scope><scope>H8D</scope><scope>H96</scope><scope>KL.</scope><scope>L.G</scope><scope>L7M</scope><scope>2B.</scope><scope>4A8</scope><scope>92I</scope><scope>93N</scope><scope>PSX</scope><scope>TCJ</scope></search><sort><creationdate>20220901</creationdate><title>Establishment and application of an anisotropic shale rock physical model in the observation coordinate system</title><author>Gui, Jun-Chuan ; Sang, Yu ; Guo, Jian-Chun ; Zeng, Bo ; Song, Yi ; Huang, Hao-Yong ; Xu, Er-si ; Chen, Ya-xi</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a323t-c3efae003bb0c7d86f4c99f36e9d130784df232a2e1be99b1f34684127a7bfa3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Accuracy</topic><topic>Acoustic waves</topic><topic>Acoustics</topic><topic>Anisotropy</topic><topic>Borehole Geophysics and Rock Properties</topic><topic>Coordinate systems</topic><topic>Coordinates</topic><topic>Earth and Environmental Science</topic><topic>Earth Sciences</topic><topic>Geomechanics</topic><topic>Geophysics/Geodesy</topic><topic>Geotechnical Engineering & Applied Earth Sciences</topic><topic>Horizontal wells</topic><topic>Modelling</topic><topic>P waves</topic><topic>Pore pressure</topic><topic>Pore water pressure</topic><topic>Rocks</topic><topic>S waves</topic><topic>Sedimentary rocks</topic><topic>Seismic wave velocities</topic><topic>Shale</topic><topic>Shales</topic><topic>Shear</topic><topic>Sound waves</topic><topic>Velocity</topic><topic>Wave velocity</topic><toplevel>online_resources</toplevel><creatorcontrib>Gui, Jun-Chuan</creatorcontrib><creatorcontrib>Sang, Yu</creatorcontrib><creatorcontrib>Guo, Jian-Chun</creatorcontrib><creatorcontrib>Zeng, Bo</creatorcontrib><creatorcontrib>Song, Yi</creatorcontrib><creatorcontrib>Huang, Hao-Yong</creatorcontrib><creatorcontrib>Xu, Er-si</creatorcontrib><creatorcontrib>Chen, Ya-xi</creatorcontrib><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Water Resources Abstracts</collection><collection>Technology Research Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>Aerospace Database</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Wanfang Data Journals - Hong Kong</collection><collection>WANFANG Data Centre</collection><collection>Wanfang Data Journals</collection><collection>万方数据期刊 - 香港版</collection><collection>China Online Journals (COJ)</collection><collection>China Online Journals (COJ)</collection><jtitle>Applied geophysics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Gui, Jun-Chuan</au><au>Sang, Yu</au><au>Guo, Jian-Chun</au><au>Zeng, Bo</au><au>Song, Yi</au><au>Huang, Hao-Yong</au><au>Xu, Er-si</au><au>Chen, Ya-xi</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Establishment and application of an anisotropic shale rock physical model in the observation coordinate system</atitle><jtitle>Applied geophysics</jtitle><stitle>Appl. Geophys</stitle><date>2022-09-01</date><risdate>2022</risdate><volume>19</volume><issue>3</issue><spage>325</spage><epage>342</epage><pages>325-342</pages><issn>1672-7975</issn><eissn>1993-0658</eissn><abstract>No shale-rock physical model has been established in the observation coordinate system. To this end, this paper carried out anisotropic wave velocity tests on shale rock and compared the Thomsen, Daley, and Berryman solutions to characterize anisotropic acoustic wave velocity. Finally, the Daley solution was selected. Based on basic rock physical models, such as SCA and DEM methods, and combined with the Daley solution, an anisotropic shalerock physical model was established in the observation coordinate system and applied in Well B1 in the Luzhou area, Sichuan Basin. Our research conclusions were as follows: 1. for the samples from the same core, the P-wave velocities in three directions were in the order
V
P11
>
V
P45
>
V
P33
, shear-wave velocity
V
S11
was the largest, but
V
S33
and
V
S45
did not follow the law of
V
s33
>
V
s45
for some samples; 2. the Daley solution, which not only considers the accuracy requirements but also has a complete expression of P-, SV-, and SH-waves, is most suitable for characterization of anisotropic wave velocity in this study area; 3. the rock physical model constructed in the observation coordinate system has high accuracy, in which the absolute value of the relative error of the P-wave slowness was between 0% and 5.05% (0.55% on average), and that of shear-wave slowness was between 0% and 6.05% (0.59% on average); 4. the acoustic waves recorded in Well B1 in the observation coordinate system were very different from those in the constitutive coordinate system. The relative difference of the P-wave was between 6.76% and 30.84% (14.68% on average), and that of the S-wave was between 7.00% and 23.44% (13.99% on average). The acoustic slowness measured in the observation coordinate system, such as in a deviated well or a horizontal well section, must be converted to the constitutive coordinate system before it can be used in subsequent engineering applications; 5. the anisotropic shale-rock physical model built in the observation coordinate system proposed in this paper can provide basic data and guidance for subsequent pore pressure prediction, geomechanical modeling, and fracturing stimulation design for deviated and horizontal wells.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer Berlin Heidelberg</pub><doi>10.1007/s11770-022-0998-3</doi><tpages>18</tpages></addata></record> |
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subjects | Accuracy Acoustic waves Acoustics Anisotropy Borehole Geophysics and Rock Properties Coordinate systems Coordinates Earth and Environmental Science Earth Sciences Geomechanics Geophysics/Geodesy Geotechnical Engineering & Applied Earth Sciences Horizontal wells Modelling P waves Pore pressure Pore water pressure Rocks S waves Sedimentary rocks Seismic wave velocities Shale Shales Shear Sound waves Velocity Wave velocity |
title | Establishment and application of an anisotropic shale rock physical model in the observation coordinate system |
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