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Titel From dilatancy to contraction: Stress-dependent failure mode progression in two porous sandstones subjected to true triaxial testing
VerfasserIn Xiaodong Ma, Bezalel Haimson
Konferenz EGU General Assembly 2013
Medientyp Artikel
Sprache Englisch
Digitales Dokument PDF
Erschienen In: GRA - Volume 15 (2013)
Datensatznummer 250077869
 
Zusammenfassung
Porous sedimentary rocks such as sandstones are typical oil-bearing formations in which failure due to high stress concentration is likely to occur during wellbore drilling and subsequent operations. The objective of this research was to investigate the effect of Ïă2 on strength, failure-plane angle, and failure mode under realistically simulated field conditions (Ïă1 -‰¥Ïă2 -‰¥Ïă3). A series of true triaxial compression tests were conducted on two representative porous sandstones: Coconino (17.5% porosity, 99% quartz, with rounded and well-sorted 0.1 mm grains that are bonded by suturing and some quartz overgrowth), and Bentheim (24% porosity, 95% quartz, with sub-rounded 0.3 mm grains that are bonded exclusively by suturing). Square cuboidal specimens (19 x 19 x 38mm) were subjected to independent loads in three principal directions, using the University of Wisconsin testing apparatus, creating a true triaxial state of stress (Ïă1 -‰¥Ïă2 -‰¥Ïă3). In all tests, Ïă3 and Ïă2 were maintained constant at predetermined levels, while Ïă1 was raised monotonically until failure occurred. The magnitude of Ïă3 varied between 0 and 150 MPa, covering the range of brittle behavior, brittle-ductile transition, and the threshold to the ductile zone in the weaker Bentheim sandstone. It was found that in both rocks the compressive strength (Ïă1,peak) for a given Ïă3 increases as the preset Ïă2 is raised between tests, and reaches a peak (15% over Ïă1,peak when Ïă2 = Ïă3 in the Coconino, and less than 10% in the Bentheim), beyond which it gradually drops, such that when Ïă2 -‰ˆ Ïă1,peak, the strength is approximately the same as when Ïă2 = Ïă3. This strengthening effect is considerably lower than that in previously tested crystalline rocks, such as Westerly granite and KTB amphibolite (more than 50%, Haimson, 2006). Plotting the test data in the τoct vs. Ïăoct domain, where the two stress invariants τoct, the octahedral shear stress, and Ïăoct,the mean normal stress, are both taken at failure), Coconino shows a monotonically rising τoct with increasing Ïăoct. In the Bentheim, on the other hand, the initially rising τoct forms a ‘cap’ at about Ïăoct = 200 MPa, an indication of localized compaction, followed by a sharp decrease for larger magnitudes of Ïăoct. Failure characteristics in Coconino sandstone subjected to Ïă3= Ïă2evolve from a dilatant mode, expressed by a single shear band, or fault, dipping steeply from 80˚ at Ïă3= 0 MPa, to 60˚ at Ïă3= 100 MPa; to a diminishing dilatant mode, signaled by multiple parallel and conjugate shear bands (a characteristic of brittle-ductile transition) dipping at nearly 50˚ , at Ïă3 = 120-150 MPa. At low preset Ïă3, failure plane dip increases by as much as 15˚ as Ïă2 is raised, but the increase gradually drops at higher Ïă3. The role of Ïă2in retarding the progression of the failure mode is noted, for example, at Ïă3 = 100 MPa, where characteristics of brittle-ductile transition are gradually reversed as Ïă2is raised. The more porous Bentheim sandstone is generally weaker. When subjected to Ïă3= Ïă2 between 0 to 60 MPa, its failure mode is dilatant, leading to a single fault dipping 80˚ at Ïă3 = 0 MPa, to 50˚ at Ïă3 = 60 MPa. For a constant Ïă3, failure-plane angle rises with Ïă2, but the increase is typically under 10˚ , somewhat less than in the Coconino. In the range of 60