Erratum to: Cracks coalescence mechanism and cracks propagation paths in rock-like specimens containing pre-existing random cracks under compression

The mechanism of cracks propagation and cracks coalescence due to compressive loading of the brittle substances containing pre-existing cracks (flaws) was modeled experimentally using specially made rock-like specimens from Portland Pozzolana Cement (PPC). The breakage process of the specimens was studied by inserting single and double flaws with different inclination angles at the center and applying uniaxial compressive stress at both ends of the specimen. The first crack was oriented at 50° from the horizontal direction and kept constant throughout the analysis while the orientation of the second crack was changed. It is experimentally observed that the wing cracks are produced at the first stage of loading and start their propagation toward the direction of uniaxial compressive loading. The secondary cracks may also be produced in form of quasi-coplanar and/or oblique cracks in a stable manner. The secondary cracks may eventually continue their propagation in the direction of maximum principle stress. These experimental works were also simulated numerically by a modified higher order displacement discontinuity method and the cracks propagation and cracks coalescence were studied based on Mode I and Mode II stress intensity factors (SIFs). It is concluded that the wing cracks initiation stresses for the specimens change from 11.3 to 14.1 MPa in the case of numerical simulations and from 7.3 to 13.8 MPa in the case of experimental works. It is observed that cracks coalescence stresses change from 21.8 to 25.3 MPa and from 19.5 to 21.8 MPa in the numerical and experimental analyses, respectively. Comparing some of the numerical and experimental results with those recently cited in the literature validates the results obtained by the proposed study. Finally, a numerical simulation was accomplished to study the effect of confining pressure on the crack propagation process, showing that the SIFs increase and the crack initiation angles change in this case.

[1]  D. Rooke,et al.  Numerical Fracture Mechanics , 1990 .

[2]  L. C. Schmidt,et al.  Linear elastic crack tip modelling by the displacement discontinuity method , 1990 .

[3]  Sheng-Qi Yang,et al.  Experimental study on mechanical behavior of brittle marble samples containing different flaws under uniaxial compression , 2009 .

[4]  Kourosh Shahriar,et al.  Modeling the propagation mechanism of two random micro cracks in rock Samples under uniform tensile loading , 2013 .

[5]  Ove Stephansson,et al.  Modification of the G-criterion for crack propagation subjected to compression , 1994 .

[6]  H. H. Einstein,et al.  Crack Coalescence Tests on Granite , 2008 .

[7]  Peng Lin,et al.  Splitting failure in brittle rocks containing pre-existing flaws under uniaxial compression , 2002 .

[8]  A. Dyskin,et al.  Crack growth under biaxial compression , 2002 .

[9]  Sheng-Qi Yang,et al.  Crack coalescence behavior of brittle sandstone samples containing two coplanar fissures in the process of deformation failure , 2011 .

[10]  A. Bobet,et al.  The initiation of slip on frictional fractures , 2006 .

[11]  Louis Ngai Yuen Wong,et al.  Influence of flaw inclination angle and loading condition on crack initiation and propagation , 2012 .

[12]  H. H. Einstein,et al.  Crack Coalescence in Molded Gypsum and Carrara Marble: Part 2—Microscopic Observations and Interpretation , 2008 .

[13]  H. Einstein,et al.  Experimental study of the cracking behavior of specimens containing inclusions (under uniaxial compression) , 2010 .

[14]  Hussain,et al.  Strain Energy Release Rate for a Crack Under Combined Mode I and Mode II , 1974 .

[15]  Steven L. Crouch,et al.  A higher order displacement discontinuity method for analysis of crack problems , 1995 .

[16]  S. L. Crouch,et al.  Boundary element methods in solid mechanics , 1983 .

[17]  B. Mohanty,et al.  Explosion generated fractures in rock and rock-like materials , 1990 .

[18]  K. Shahriar,et al.  On the crack propagation analysis of rock like Brazilian disc specimens containing cracks under compressive line loading , 2014 .

[19]  G. Sih Strain-energy-density factor applied to mixed mode crack problems , 1974 .

[20]  Ping Cao,et al.  Failure characteristics and its influencing factors of rock-like material with multi-fissures under uniaxial compression , 2012 .

[21]  Louis Ngai Yuen Wong,et al.  Systematic evaluation of cracking behavior in specimens containing single flaws under uniaxial compression , 2009 .

[22]  Claudio Scavia,et al.  Fracture mechanics approach to stability analysis of rock slopes , 1990 .

[23]  A. Bobet The initiation of secondary cracks in compression , 2000 .

[24]  Hasan Hosseini Nasab,et al.  On the uses of special crack tip elements in numerical rock fracture mechanics , 2006 .

[25]  M. F. Marji,et al.  Numerical simulation of crack propagation in layered formations , 2014, Arabian Journal of Geosciences.

[26]  Kourosh Shahriar,et al.  A coupled numerical–experimental study of the breakage process of brittle substances , 2015, Arabian Journal of Geosciences.

[27]  M. F. Marji,et al.  On the crack propagation modeling of hydraulic fracturing by a hybridized displacement discontinuity/boundary collocation method , 2012 .

[28]  Antonio Bobet,et al.  Crack coalescence in specimens with open and closed flaws: A comparison , 2009 .

[29]  Y. Yang,et al.  Crack branching mechanism of rock-like quasi-brittle materials under dynamic stress , 2012 .

[30]  K. T. Chau,et al.  Analysis of crack coalescence in rock-like materials containing three flaws—Part I: experimental approach , 2001 .

[31]  Vahab Sarfarazi,et al.  Mixed mode crack propagation in low brittle rock-like materials , 2013, Arabian Journal of Geosciences.

[32]  L. Wong,et al.  Crack Coalescence in Molded Gypsum and Carrara Marble: Part 1. Macroscopic Observations and Interpretation , 2009 .

[33]  Ping Cao,et al.  Wing crack model subjected to high hydraulic pressure and far field stresses and its numerical simulation , 2012 .

[34]  Guk-Rwang Won American Society for Testing and Materials , 1987 .

[35]  M. F. Marji,et al.  Kinked crack analysis by a hybridized boundary element/boundary collocation method , 2010 .

[36]  Chao-Shi Chen,et al.  Determination of Fracture Toughness of Anisotropic Rocks by Boundary Element Method , 2008 .

[37]  Yin-Ping Li,et al.  Experimental research on pre-cracked marble under compression , 2005 .

[38]  M. F. Marji On the use of power series solution method in the crack analysis of brittle materials by indirect boundary element method , 2013 .

[39]  Seokwon Jeon,et al.  An experimental and numerical study of fracture coalescence in pre-cracked specimens under uniaxial compression , 2011 .

[40]  E. G. Bombolakis Photoelastic study of initial stages of brittle fracture in compression , 1968 .

[41]  M. F. Marji,et al.  Numerical analysis of confinement effect on crack propagation mechanism from a flaw in a pre-cracked rock under compression , 2012 .

[42]  Huang Jiefan,et al.  An experimental study of the strain field development prior to failure of a marble plate under compression , 1990 .

[43]  Antonio Bobet,et al.  Crack initiation, propagation and coalescence from frictional flaws in uniaxial compression , 2010 .

[44]  F. Erdogan,et al.  On the Crack Extension in Plates Under Plane Loading and Transverse Shear , 1963 .