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dc.contributor.authorZ. Zheng
dc.contributor.authorL. R. Myer
dc.contributor.authorJ. M. Kemeny
dc.contributor.authorR. Suarez
dc.contributor.authorR. T. Ewy
dc.contributor.authorN. G. W. Cook
dc.date.accessioned2017-05-08T23:37:15Z
dc.date.available2017-05-08T23:37:15Z
dc.date.copyrightAugust, 1992
dc.date.issued1992
dc.identifier.issn0003-6900
dc.identifier.otherAMREAD-25630#263_1.pdf
dc.identifier.urihttp://yetl.yabesh.ir/yetl/handle/yetl/109554
dc.description.abstractUnder differential compressive stress rocks exhibit nonlinear deformation that includes initial compaction, near-linear elastic behavior, and strain-hardening followed by strain-softening and dilation (or compaction in clastic rocks) and localization. This behavior derives largely from changes in the microstructure of the rocks. Much of it has been attributed to the growth of extensile microcracks. The stress-induced microstructural changes brought about by successively more complicated states of stress produced by uniaxial and triaxial compression of circular cylinders, axisymmetric stresses in hollow cylinders, and indentation by hemispheres in Indiana limestone and Berea sandstone have been preserved using Wood’s metal porosimetry. In this technique molten Wood’s metal at about 100°C is used as a pore fluid at a pressure of about 10 MPa, and the experiments are conducted using the concepts of effective stress. At the deformation state of interest, the temperature is lowered to solidify the metal, thereby preserving the microstructure as it exists under load and facilitating subsequent preparation of the specimen for microscopic study. Mode I microcrack growth is observed to occur by a variety of mechanisms such as bending, point loading and sliding cracks. The effects of this are analyzed using an elastic continuum within which Mode II displacement across microcracks and Mode I microcrack growth results from heterogeneous stress concentrations that produce local tensile stresses. While the continuum model replicates many of the observations, it fails to account for localization by en echelon arrays of extensile microcracks that precede macroscopic shear faulting. Using a “zero order” continuum approximation, the spatially stochastic distribution of grains in clastic rocks is shown to be important in the formation of the en echelon arrays of microcracks that form shear bands.
dc.publisherThe American Society of Mechanical Engineers (ASME)
dc.titleExtensile Cracking in Porous Rock Under Differential Compressive Stress
dc.typeJournal Paper
dc.journal.volume45
dc.journal.issue8
dc.journal.titleApplied Mechanics Reviews
dc.identifier.doi10.1115/1.3119758
dc.journal.fristpage263
dc.journal.lastpage280
dc.identifier.eissn0003-6900
dc.keywordsFracture (Process)
dc.keywordsCompressive stress
dc.keywordsRocks
dc.keywordsMicrocracks
dc.keywordsStress
dc.keywordsMetals
dc.keywordsCompacting
dc.keywordsShear (Mechanics)
dc.keywordsDeformation
dc.keywordsTemperature
dc.keywordsFluids
dc.keywordsPressure
dc.keywordsElasticity
dc.keywordsFracture (Materials)
dc.keywordsCylinders
dc.keywordsDisplacement
dc.keywordsApproximation
dc.keywordsCircular cylinders
dc.keywordsCompression
dc.keywordsTension
dc.keywordsWork hardening AND Mechanisms
dc.treeApplied Mechanics Reviews:;1992:;volume( 045 ):;issue: 008
dc.contenttypeFulltext


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