Helical crack-front instability in mixed-mode fracture

被引:165
作者
Pons, Antonio J. [1 ,2 ]
Karma, Alain [1 ,2 ]
机构
[1] Northeastern Univ, Dept Phys, Boston, MA 02115 USA
[2] Northeastern Univ, Ctr Interdisciplinary Res Complex Syst, Boston, MA 02115 USA
关键词
PATTERN-FORMATION; GROWTH;
D O I
10.1038/nature08862
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
Planar crack propagation under pure tension loading (mode I) is generally stable. However, it becomes universally unstable with the superposition of a shear stress parallel to the crack front (mode III). Under this mixed-mode (I + III) loading configuration, an initially flat parent crack segments into an array of daughter cracks that rotate towards a direction of maximum tensile stress(1). This segmentation produces stepped fracture surfaces with characteristic 'lance-shaped' markings observed in a wide range of engineering(2-7) and geological materials(1,8). The origin of this instability remains poorly understood and a theory with which to predict the surface roughness scale is lacking. Here we perform large-scale simulations of mixed-mode I + III brittle fracture using a continuum phase-field method(9-11) that describes the complete three-dimensional crack-front evolution. The simulations reveal that planar crack propagation is linearly unstable against helical deformations of the crack front, which evolve nonlinearly into a segmented array of finger-shaped daughter cracks. Furthermore, during their evolution, facets gradually coarsen owing to the growth competition of daughter cracks in striking analogy with the coarsening of finger patterns observed in nonequilibrium growth phenomena(12-14). We show that the dynamically preferred unstable wavelength is governed by the balance of the destabilizing effect of far-field stresses and the stabilizing effect of cohesive forces on the process zone scale, and we derive a theoretical estimate for this scale using a new propagation law for curved cracks in three dimensions. The rotation angles of coarsened facets are also compared to theoretical predictions and available experimental data.
引用
收藏
页码:85 / 89
页数:5
相关论文
共 31 条
[1]   THE FORMATION OF PATTERNS IN NONEQUILIBRIUM GROWTH [J].
BENJACOB, E ;
GARIK, P .
NATURE, 1990, 343 (6258) :523-530
[2]   Weakly Nonlinear Theory of Dynamic Fracture [J].
Bouchbinder, Eran ;
Livne, Ariel ;
Fineberg, Jay .
PHYSICAL REVIEW LETTERS, 2008, 101 (26)
[3]   Dynamical fracture instabilities due to local hyperelasticity at crack tips [J].
Buehler, MJ ;
Gao, HJ .
NATURE, 2006, 439 (7074) :307-310
[4]   Fracture propagation paths under mixed mode loading within rectangular blocks of polymethyl methacrylate [J].
Cooke, ML ;
Pollard, DD .
JOURNAL OF GEOPHYSICAL RESEARCH-SOLID EARTH, 1996, 101 (B2) :3387-3400
[5]  
DEGRAFF JM, 1987, GEOL SOC AM BULL, V99, P605, DOI 10.1130/0016-7606(1987)99<605:SMOCJA>2.0.CO
[6]  
2
[7]   ELASTIC ENERGY-MOMENTUM TENSOR [J].
ESHELBY, JD .
JOURNAL OF ELASTICITY, 1975, 5 (3-4) :321-335
[8]   Instability in dynamic fracture [J].
Fineberg, J ;
Marder, M .
PHYSICS REPORTS-REVIEW SECTION OF PHYSICS LETTERS, 1999, 313 (1-2) :1-108
[9]   INSTABILITY IN DYNAMIC FRACTURE [J].
FINEBERG, J ;
GROSS, SP ;
MARDER, M ;
SWINNEY, HL .
PHYSICAL REVIEW LETTERS, 1991, 67 (04) :457-460
[10]  
Freund LB., 1998, DYNAMIC FRACTURE MEC