Crack tip fields in soft elastic solids subjected to large quasi-static deformation — A review

Abstract We review analytical solutions for the asymptotic deformation and stress fields near the tip of a crack in soft elastic solids. These solutions are based on finite strain elastostatics and hyperelastic material models, and exhibit significantly different characteristics than the classical crack tip field solutions in linear elastic fracture mechanics. Specifically, we summarize some available finite strain crack tip solutions for two dimensional cracks, namely that plane strain, plane stress, and anti-plane shear cracks in a certain class of homogeneous materials. Interface cracks between soft elastic solids and a rigid substrate are also discussed. We focus on incompressible material models with various degrees of strain stiffening effect such as generalized neo-Hookean model, exponentially hardening model and Gent model. We also explored the physical implications of the crack tip fields, and highlighted pitfalls in the applications of these solutions, particularly the J-integral and the distribution of true stress in the deformed configuration which have not been discussed in the literature.

[1]  Finite plane and anti-plane elastostatic fields with discontinuous deformation gradients near the tip of a crack , 1982 .

[2]  J. Fineberg,et al.  The 1/r singularity in weakly nonlinear fracture mechanics , 2009, 0902.2121.

[3]  D. Mooney,et al.  Hydrogels for tissue engineering. , 2001, Chemical Reviews.

[4]  J. Fineberg,et al.  Breakdown of linear elastic fracture mechanics near the tip of a rapid crack. , 2008, Physical review letters.

[5]  M. Williams,et al.  On the Stress Distribution at the Base of a Stationary Crack , 1956 .

[6]  P. Calvert Hydrogels for Soft Machines , 2009 .

[7]  T. Kurokawa,et al.  Double‐Network Hydrogels with Extremely High Mechanical Strength , 2003 .

[8]  M. Marder Supersonic rupture of rubber , 2005, cond-mat/0504613.

[9]  B. Newby,et al.  Macroscopic Evidence of the Effect of Interfacial Slippage on Adhesion , 1995, Science.

[10]  J. P. Zhang,et al.  ANALYSIS OF DEFORMATIONS NEAR A CRACK TIP IN A COMPRESSIBLE NONLINEAR ELASTIC MATERIAL , 1993 .

[11]  Y. Fung,et al.  Biomechanics: Mechanical Properties of Living Tissues , 1981 .

[12]  T. Hao Near field behavior of in-plane crack extension in nonlinear incompressible material , 1990 .

[13]  Y. Gao,et al.  Large Strain Field Near a Crack Tip in a Rubber Sheet , 2001 .

[14]  H. Swinney,et al.  Oscillating fracture paths in rubber. , 2001, Physical review letters.

[15]  Guansuo Dui,et al.  Stresses, Singularities, and a Complementary Energy Principle for Large Strain Elasticity , 2008 .

[16]  Andy Ruina,et al.  Why K? High order singularities and small scale yielding , 1995 .

[17]  Xuanhe Zhao,et al.  Multi-scale multi-mechanism design of tough hydrogels: building dissipation into stretchy networks. , 2014, Soft matter.

[18]  A. Jagota,et al.  Crack blunting and the strength of soft elastic solids , 2003, Proceedings of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences.

[19]  A. Gent Adhesion and Strength of Viscoelastic Solids. Is There a Relationship between Adhesion and Bulk Properties , 1996 .

[20]  T. Baumberger,et al.  A convective instability mechanism for quasistatic crack branching in a hydrogel , 2009, The European physical journal. E, Soft matter.

[21]  D. Parks,et al.  The finite deformation field surrounding a mode I plane strain crack in a hyperelastic incompressible material under small-scale nonlinearity , 1994 .

[22]  A. Thomas,et al.  Rupture of rubber , 1960 .

[23]  R. Westmann,et al.  Finite element analysis of hyperelastic large deformation crack tip fields , 1990 .

[24]  M. Boyce,et al.  Constitutive models of rubber elasticity: A review , 2000 .

[25]  A finite elastostatic analysis of bimaterial interface cracks , 1989 .

[26]  C. Ru Finite Strain Singular Field Near the Tip of a Crack Terminating at a Material Interface , 1997 .

[27]  James K. Knowles,et al.  The finite anti-plane shear field near the tip of a crack for a class of incompressible elastic solids , 1977 .

[28]  Angelo Marcello Tarantino Thin Hyperelastic sheets of compressible material: Field equations, airy stress function and an application in fracture mechanics , 1996 .

[29]  Rodney Alan Stephenson,et al.  The equilibrium field near the tip of a crack for finite plane strain of incompressible elastic materials , 1982 .

[30]  James K. Knowles,et al.  Finite-deformation analysis of the elastostatic field near the tip of a crack: Reconsideration and higher-order results , 1974 .

[31]  D. Durban,et al.  The crack tip field in a rubber sheet , 1995 .

[32]  N. Peppas,et al.  Hydrogels as mucoadhesive and bioadhesive materials: a review. , 1996, Biomaterials.

[33]  James K. Knowles,et al.  Large deformations near a tip of an interface-crack between two Neo-Hookean sheets , 1983 .

[34]  J. M. Herrmann An asymptotic analysis of finite deformations near the tip of an interface-crack , 1989 .

[35]  W. Hong,et al.  Delayed fracture in gels , 2012 .

[36]  Chung-Yuen Hui,et al.  Finite strain analysis of crack tip fields in incompressible hyperelastic solids loaded in plane stress , 2011 .

[37]  C. Q. Ru,et al.  On complex-variable formulation for finite plane elastostatics of harmonic materials , 2002 .

[38]  H. Stumpf,et al.  The singular elastostatic field due to a crack in rubberlike materials , 1993 .

[39]  A. Thomas,et al.  The strength of highly elastic materials , 1967, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[40]  A. Thomas,et al.  Rupture of Rubber. III. Determination of Tear Properties , 1955 .

[41]  Alan N. Gent,et al.  Internal rupture of bonded rubber cylinders in tension , 1961, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[42]  Oscillatory instability in two-dimensional dynamic fracture. , 2006, Physical review letters.

[43]  David Martina,et al.  Solvent control of crack dynamics in a reversible hydrogel , 2006, Nature materials.

[44]  C. Hui,et al.  Fracture and large strain behavior of self-assembled triblock copolymer gels , 2009 .

[45]  J. Fineberg,et al.  Weakly nonlinear fracture mechanics: experiments and theory , 2010 .

[46]  Localized shear discontinuities near the tip of a mode I crack , 1987 .

[47]  William L. Ko,et al.  Application of Finite Elastic Theory to the Deformation of Rubbery Materials , 1962 .

[48]  Cracks in Rubber under Tension Exceed the Shear Wave Speed , 2003, cond-mat/0311422.

[49]  C. Hui,et al.  Finite strain crack tip fields in soft incompressible elastic solids. , 2008, Langmuir : the ACS journal of surfaces and colloids.

[50]  P. Albouy,et al.  Stress-Induced Crystallization around a Crack Tip in Natural Rubber , 2002 .

[51]  Y. C. Gao,et al.  Large deformation field near a crack tip in rubber-like material , 1997 .

[52]  On the Finite Motions Generated by a Mode I Propagating Crack , 1999 .

[53]  C. H. Chen,et al.  Scaling of crack propagation in rubber sheets , 2011 .

[54]  John R. Rice,et al.  Stresses Due to a Sharp Notch in a Work-Hardening Elastic-Plastic Material Loaded by Longitudinal Shear , 1967 .

[55]  C. Hui,et al.  Finite strain stress fields near the tip of an interface crack between a soft incompressible elastic material and a rigid substrate , 2009, The European physical journal. E, Soft matter.

[56]  E. Bouchaud,et al.  Mode I fracture of a biopolymer gel: rate-dependent dissipation and large deformations disentangled , 2014, 1501.01322.

[57]  C. Hui,et al.  An experimental investigation of fracture by cavitation of model elastomeric networks , 2010 .

[58]  E. Verron,et al.  Stress analysis around crack tips in finite strain problems using the eXtended finite element method , 2005 .

[59]  James K. Knowles,et al.  An asymptotic finite-deformation analysis of the elastostatic field near the tip of a crack , 1973 .

[60]  Gerhard A. Holzapfel,et al.  Nonlinear Solid Mechanics: A Continuum Approach for Engineering Science , 2000 .

[61]  Jian Ping Gong,et al.  Physical hydrogels composed of polyampholytes demonstrate high toughness and viscoelasticity. , 2013, Nature materials.

[62]  K. Shull,et al.  Ionically Cross-Linked Triblock Copolymer Hydrogels with High Strength , 2010 .

[63]  J. Fineberg,et al.  Weakly nonlinear theory of dynamic fracture. , 2008, Physical review letters.

[64]  A. Gent A New Constitutive Relation for Rubber , 1996 .

[65]  J. Fineberg,et al.  The Near-Tip Fields of Fast Cracks , 2010, Science.

[66]  L. Mahadevan,et al.  Crack-front instability in a confined elastic film , 2006, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[67]  S. Mohammadi,et al.  Finite strain fracture analysis using the extended finite element method with new set of enrichment functions , 2015 .

[68]  J. Rice A path-independent integral and the approximate analysis of strain , 1968 .

[69]  M. Chaudhury,et al.  Adhesion-Induced Instability Patterns in Thin Confined Elastic Film , 2003 .

[70]  Alan N. Gent,et al.  Fracture mechanics and cavitation in rubber-like solids , 1991 .

[71]  J. Fineberg,et al.  Failing softly: a fracture theory of highly-deformable materials. , 2015, Soft matter.

[72]  Z. Suo,et al.  Highly stretchable and tough hydrogels , 2012, Nature.

[73]  E. Bouchbinder,et al.  A nonlinear symmetry breaking effect in shear cracks , 2011, 1111.2452.

[74]  Y. Osada,et al.  Biomechanical properties of high-toughness double network hydrogels. , 2005, Biomaterials.

[75]  Costantino Creton,et al.  Toughening Elastomers with Sacrificial Bonds and Watching Them Break , 2014, Science.

[76]  A. Thomas,et al.  Rupture of rubber. II. The strain concentration at an incision , 1955 .

[77]  C. Caroli,et al.  Crack front échelon instability in mixed mode fracture of a strongly nonlinear elastic solid , 2013, 1310.0235.

[78]  Crack Propagation in Finite Elastodynamics , 2005 .

[79]  Tetsuo Yamaguchi,et al.  Measurement of the receding contact angle at the interface between a viscoelastic material and a rigid surface , 2010 .

[80]  C. Hui,et al.  Stress Relaxation Near the Tip of a Stationary Mode I Crack in a Poroelastic Solid , 2013 .

[81]  C. Hui,et al.  Effects of finite chain extensibility on the stress fields near the tip of a mode III crack , 2011, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[82]  P. Schiavone,et al.  Effect of interfacial slippage on the near-tip fields of an interface crack between a soft elastomer and a rigid substrate , 2014, Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[83]  Magic angles and cross-hatching instability in hydrogel fracture. , 2008, Physical review letters.

[84]  Philippe H. Geubelle,et al.  Finite strains at the tip of a crack in a sheet of hyperelastic material: I. Homogeneous case , 1994 .

[85]  J. Duszczyk,et al.  A study on an atomized Al-Fe-Mo-Zr powder to be processed for high temperature applications , 1991 .

[86]  F. S. Wong,et al.  Large plane deformations of thin elastic sheets of neo-Hookean material , 1969 .

[87]  H. Neuber Theory of Stress Concentration for Shear-Strained Prismatical Bodies With Arbitrary Nonlinear Stress-Strain Law , 1961 .

[88]  R. Rivlin,et al.  Rupture of rubber. I. Characteristic energy for tearing , 1953 .

[89]  M. Boyce,et al.  A three-dimensional constitutive model for the large stretch behavior of rubber elastic materials , 1993 .

[90]  Y. C. Gao,et al.  Elastostatic crack tip behavior for a rubber-like material , 1990 .

[91]  W. Knauss,et al.  Finite strains at the tip of a crack in a sheet of hyperelastic material: III. General bimaterial case , 1994 .