Abstract:[1] Two distinct modes of compressive brittle-like failure are observed in laboratory samples of rock and ice. Under low to moderate confinement, terminal failure follows microcrack growth and interaction when damage is localized along a fault oriented $30°t o the greatest compressive stress. Under higher confinement, frictional sliding is suppressed, and sudden, localized, brittle-like failure is not attended by a concentration of microcracks near the main fault. Also, faults that form under higher confinemen… Show more
“…3.9a). When yield stresses in better agreement with experimental results are used (e.g., Shimada 1993;Renshaw and Schulson 2004), the volume of detached oceanic crust decrease, but do not cease to occur in our models ( Fig. 3.9d).…”
Section: Detachment Of the Oceanic Crustmentioning
“…3.9a). When yield stresses in better agreement with experimental results are used (e.g., Shimada 1993;Renshaw and Schulson 2004), the volume of detached oceanic crust decrease, but do not cease to occur in our models ( Fig. 3.9d).…”
Section: Detachment Of the Oceanic Crustmentioning
“…It is conceivable that cavitation may contribute to an enhanced permeability and fluid flow localized in shear zones that is frequently observed [Rutter and Brodie, 1985]. Unstable ductile failure in mylonite shear zones at the base of the seismogenic upper crust has been suggested as a possible source mechanism for earthquakes [Hobbs and Ord, 1988] and pseudotachylytes at great depth [Austrheim and Boundy, 1994;Hobbs et al, 1986;White, 1996;Renshaw and Schulson, 2004]. Failure is often attributed to shear heating and/or dehydration reactions and possibly transient fluid pressure pulses.…”
[1] We performed high-strain torsion experiments on fine-grained (≈4 mm) anorthite aggregates in a Paterson-type gas deformation apparatus. The dense hydrous (≈0.1 wt% H 2 O) samples contain < 3 vol% Si-enriched residual glass located at triple junctions. Specimens were twisted at constant rate to a maximum shear strain of about 5 at experimental conditions of 100-400 MPa confining pressure, temperatures of 950°C-1200°C, and shear strain rates of ≈2 × 10 −5 , 5 × 10 −5 , and 2 × 10 −4 s −1 . Resulting maximum shear stresses at the sample periphery were in the range of ≈2-80 MPa. The samples showed strain hardening at slow deformation rate and strain weakening at fast strain rate, respectively. Fitting the stress strain rate data to a power law yields linear viscous behavior. Microstructural analysis shows locally enhanced dislocation density, suggesting diffusion-assisted and/or dislocation-assisted grain boundary sliding as the dominant deformation mechanism. Deformed samples exhibit abundant cavities, nucleated mostly at grain triple junctions and at grain boundaries in response to cooperative grain boundary sliding. At shear strains ≥ 2, growth and coalescence of the cavities form an anastomozing network of regularly spaced strings oriented at about 30°to the direction of maximum compressive stress and ∼15°to the shear plane. Strain is localized along these shear bands associated with a shape-preferred orientation of high-aspect ratio feldspar grains and with segregation of initial pore fluids (residual glass) into the bands. More than one third of the samples were deformed to terminal failure that occurred suddenly at shear strains of ≈3-5. The experiments indicate that cavitation damage may facilitate fluid flow and deep seismicity in highly strained shear zones.Citation: Rybacki, E., R. Wirth, and G. Dresen (2010), Superplasticity and ductile fracture of synthetic feldspar deformed to large strain,
“…Iliescu and Schulson (2004) describe this new process and present a physical model that is based upon the competition between wing crack growth and Euler buckling of deformation-produced thin plates. Under triaxial confinement greater than that required to suppress frictional sliding, plastic faults develop (Schulson 2002b), a failuremode transition that is again seen in rocks and minerals (Renshaw and Schulson 2004).…”
Section: Brittle Compressive Failure Under Multiaxial Loadingmentioning
Abstract-This paper presents a short overview of the fracture of water ice Ih. Topics include the ductile-to-brittle transition, tensile and compressive strength, compressive failure under multiaxial loading, compressive failure modes, and brittle failure on the geophysical scale (Arctic sea ice cover, Europa's icy crust). Emphasis is placed on the underlying physical mechanisms. Where appropriate, comment is made on the formation of high-latitude impact craters on Mars.
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