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dc.contributor.authorSzewczyk, Dawid
dc.contributor.authorHolt, Rune Martin
dc.contributor.authorBauer, Andreas
dc.date.accessioned2019-01-16T07:07:20Z
dc.date.available2019-01-16T07:07:20Z
dc.date.created2018-05-22T09:47:15Z
dc.date.issued2018
dc.identifier.citationGeophysical Prospecting. 2018, 66 99-115.nb_NO
dc.identifier.issn0016-8025
dc.identifier.urihttp://hdl.handle.net/11250/2580770
dc.description.abstractSeismic monitoring of reservoir and overburden performance during subsurface CO2 storage plays a key role in ensuring efficiency and safety. Proper interpretation of monitoring data requires knowledge about the rock physical phenomena occurring in the subsurface formations. This work focuses on rock stiffness and elastic velocity changes of a shale overburden formation caused by both reservoir inflation induced stress changes and leakage of CO2 into the overburden. In laboratory experiments, Pierre shale I core plugs were loaded along the stress path representative for the in situ stress changes experienced by caprock during reservoir inflation. Tests were carried out in a triaxial compaction cell combining three measurement techniques and permitting for determination of (i) ultrasonic velocities, (ii) quasistatic rock deformations, and (iii) dynamic elastic stiffness at seismic frequencies within a single test, which allowed to quantify effects of seismic dispersion. In addition, fluid substitution effects connected with possible CO2 leakage into the caprock formation were modelled by the modified anisotropic Gassmann model. Results of this work indicate that (i) stress sensitivity of Pierre shale I is frequency dependent; (ii) reservoir inflation leads to the increase of the overburden Young's modulus and Poisson's ratio; (iii) in situ stress changes mostly affect the P‐wave velocities; (iv) small leakage of the CO2 into the overburden may lead to the velocity changes, which are comparable with one associated with geomechanical influence; (v) non‐elastic effects increase stress sensitivity of an acoustic waves; (iv) and both geomechanical and fluid substitution effects would create significant time shifts, which should be detectable by time‐lapse seismic.nb_NO
dc.language.isoengnb_NO
dc.publisherEuropean Association of Geoscientists and Engineers (EAGE)nb_NO
dc.titleInfluence of subsurface injection on time-lapse seismic: laboratory studies at seismic and ultrasonic frequenciesnb_NO
dc.typeJournal articlenb_NO
dc.typePeer reviewednb_NO
dc.description.versionacceptedVersionnb_NO
dc.source.pagenumber99-115nb_NO
dc.source.volume66nb_NO
dc.source.journalGeophysical Prospectingnb_NO
dc.identifier.doi10.1111/1365-2478.12606
dc.identifier.cristin1585831
dc.relation.projectNorges forskningsråd: 234074nb_NO
dc.description.localcodeThis is the peer reviewed version of an article, which has been published in final form at [https://doi.org/10.1111/1365-2478.12606]. This article may be used for non-commercial purposes in accordance with Wiley Terms and Conditions for Self-Archiving.nb_NO
cristin.unitcode194,64,90,0
cristin.unitnameInstitutt for geovitenskap og petroleum
cristin.ispublishedtrue
cristin.fulltextpostprint
cristin.qualitycode1


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