Extensile Cracking in Porous Rock Under Differential Compressive Stress

[+] Author and Article Information
L. R. Myer, J. M. Kemeny

Earth Sciences Division, Lawrence Berkeley Laboratory, University of California, Berkeley CA

Z. Zheng, R. Suarez, R. T. Ewy, N. G. W. Cook

Earth Sciences Division, Lawrence Berkeley Laboratory, University of California, Berkeley CA and Department of Material Sciences & Mineral Engineering, University of California, Berkeley CA

Appl. Mech. Rev 45(8), 263-280 (Aug 01, 1992) (18 pages) doi:10.1115/1.3119758 History: Online April 30, 2009


Under 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.

Copyright © 1992 by American Society of Mechanical Engineers
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