Boudinage and folding as an energy instability in ductile deformation

We present a theory for the onset of localization in layered rate- and temperature-sensitive rocks, in which energy-related mechanical bifurcations lead to localized dissipation patterns in the transient deformation regime. The implementation of the coupled thermomechanical 2-D finite element model comprises an elastic and rate-dependent von Mises plastic rheology. The underlying system of equations is solved in a three-layer pure shear box, for constant velocity and isothermal boundary conditions. To examine the transition from stable to localized creep, we study how material instabilities are related to energy bifurcations, which arise independently of the sign of the stress conditions imposed on opposite boundaries, whether in compression or extension. The onset of localization is controlled by a critical amount of dissipation, termed Gruntfest number, when dissipative work by temperature-sensitive creep translated into heat overcomes the diffusive capacity of the layer. Through an additional mathematical bifurcation analysis using constant stress boundary conditions, we verify that boudinage and folding develop at the same critical Gruntfest number. Since the critical material parameters and boundary conditions for both structures to develop are found to coincide, the initiation of localized deformation in strong layered media within a weaker matrix can be captured by a unified theory for localization in ductile materials. In this energy framework, neither intrinsic nor extrinsic material weaknesses are required, because the nucleation process of strain localization arises out of steady state conditions. This finding allows us to describe boudinage and folding structures as the same energy attractor of ductile deformation.

[1]  M. Liebeck,et al.  Primitive Permutation Groups Containing an Element of Large Prime Order , 1985 .

[2]  John J. Cannon,et al.  The Magma Algebra System I: The User Language , 1997, J. Symb. Comput..

[3]  Peter J. Hudleston,et al.  Information from folds: A review , 2010 .

[4]  Bertrand Wattrisse,et al.  Fields of stored energy associated with localized necking of steel , 2009 .

[5]  Pablo Spiga,et al.  On the maximum orders of elements of finite almost simple groups and primitive permutation groups , 2013, 1301.5166.

[6]  C. Passchier,et al.  Boudinage classification: end-member boudin types and modified boudin structures , 2004 .

[7]  N. Mancktelow Single-layer folds developed from initial random perturbations: The effects of probability distribution, fractal dimension, phase, and amplitude , 2001 .

[8]  Alison Ord,et al.  Thermodynamics of folding in the middle to lower crust , 2007 .

[9]  D. Yuen,et al.  Physics‐controlled thickness of shear zones caused by viscous heating: Implications for crustal shear localization , 2014 .

[10]  David A. Yuen,et al.  Rapid conversion of elastic energy into plastic shear heating during incipient necking of the lithosphere , 1998 .

[11]  A. Needleman Material rate dependence and mesh sensitivity in localization problems , 1988 .

[12]  P. Cameron Transitivity of permutation groups on unordered sets , 1976 .

[13]  J. Rice,et al.  CONDITIONS FOR THE LOCALIZATION OF DEFORMATION IN PRESSURE-SENSITIVE DILATANT MATERIALS , 1975 .

[14]  H. Ramberg Natural and Experimental Boudinage and Pinch-and-Swell Structures , 1955, The Journal of Geology.

[15]  P. Steif On the Initiation of Necking Modes in Layered Plastic Solids , 1987 .

[16]  R. C. Fletcher Instability of an anisotropic power-law fluid in a basic state of plane flow , 2005 .

[17]  G. Hirth,et al.  Rheology of the Upper Mantle and the Mantle Wedge: A View from the Experimentalists , 2013 .

[18]  S. Schmalholz,et al.  Evolution of pinch-and-swell structures in a power-law layer , 2008 .

[19]  T. Shawki An Energy Criterion for the Onset of Shear Localization in Thermal Viscoplastic Materials, Part I: Necessary and Sufficient Initiation Conditions , 1994 .

[20]  Yuri Y. Podladchikov,et al.  Initiation of localized shear zones in viscoelastoplastic rocks , 2006 .

[21]  T. Shawki,et al.  An energy-based localization theory: II. Effects of the diffusion, inertia, and dissipation numbers , 1995 .

[22]  Ares J. Rosakis,et al.  Intersonic shear crack growth along weak planes , 2000 .

[23]  Georg Dresen,et al.  Rheology of the Lower Crust and Upper Mantle: Evidence from Rock Mechanics, Geodesy, and Field Observations , 2008 .

[24]  S. Schmalholz,et al.  Folding in power-law viscous multi-layers , 2012, Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[25]  Ioannis Vardoulakis,et al.  Catastrophic landslides due to frictional heating of the failure plane , 2000 .

[26]  D. Gorenstein,et al.  The Classification of the Finite Simple Groups , 1983 .

[27]  B. Hobbs,et al.  Localised folding in general deformations , 2013 .

[28]  G. Lancioni,et al.  Energy-based Modeling of Localization and Necking in Plasticity☆ , 2014 .

[29]  Ali Karrech,et al.  Frame indifferent elastoplasticity of frictional materials at finite strain , 2011 .

[30]  C. Praeger On elements of prime order in primitive permutation groups , 1979 .

[31]  Spontaneous thermal runaway as an ultimate failure mechanism of materials. , 2006, Physical review letters.

[32]  M. Abbassi,et al.  Single layer buckle folding in non-linear materials—II. Comparison between theory and experiment , 1992 .

[33]  L. Strayer,et al.  Numerical modeling of fold initiation at thrust ramps , 1997 .

[34]  J. Urai,et al.  Discrete element modeling of boudinage: Insights on rock rheology, matrix flow, and evolution of geometry , 2012 .

[35]  Y. Podladchikov,et al.  Spontaneous dissipation of elastic energy by self-localizing thermal runaway. , 2008, Physical review. E, Statistical, nonlinear, and soft matter physics.

[36]  G. Zulauf,et al.  Coeval folding and boudinage in four dimensions , 2005 .

[37]  Y. Podladchikov,et al.  A two-phase composite in simple shear: Effective mechanical anisotropy development and localization potential , 2012 .

[38]  D. Yuen,et al.  The Initiation of Subduction: Criticality by Addition of Water? , 2001, Science.

[39]  M. Paterson Localization in rate-dependent shearing deformation, with application to torsion testing , 2004 .

[40]  I. Gruntfest,et al.  Thermal Feedback in Liquid Flow; Plane Shear at Constant Stress , 1963 .

[41]  B. Hobbs,et al.  The interaction of deformation and metamorphic reactions , 2010 .

[42]  B. Hobbs,et al.  Deformation with coupled chemical diffusion , 2009 .

[43]  U. Zannier,et al.  Composite rational functions expressible with few terms , 2012 .

[44]  Unified theory of the onset of folding, boudinage, and mullion structure , 1975 .

[45]  G. Lloyd,et al.  Boudinage structure: some new interpretations based on elastic-plastic finite element simulations , 1981 .

[46]  Thomas Poulet,et al.  Multi-Physics Modelling of Fault Mechanics Using REDBACK: A Parallel Open-Source Simulator for Tightly Coupled Problems , 2017, Rock Mechanics and Rock Engineering.

[47]  B. Kennett,et al.  Boudinage of a stretching slablet implicated in earthquakes beneath the Hindu Kush , 2008 .

[48]  J. Sulem,et al.  Modeling of fault gouges with Cosserat Continuum Mechanics: Influence of thermal pressurization and chemical decomposition as coseismic weakening mechanisms , 2012 .

[49]  Marco Herwegh,et al.  Boudinage as a material instability of elasto-visco-plastic rocks , 2015 .

[50]  M. Rashid Incremental kinematics for finite element applications , 1993 .

[51]  G. Schubert,et al.  Asthenospheric shear flow: Thermally stable or unstable? , 1977 .

[52]  S. Schmalholz,et al.  Pinch-and-swell structure and shear zones in viscoplastic layers , 2012 .

[53]  Daniel Rittel,et al.  On the conversion of plastic work to heat during high strain rate deformation of glassy polymers , 1999 .

[54]  D. Yuen,et al.  Modeling shear zones in geological and planetary sciences: solid- and fluid-thermal-mechanical approaches , 2003 .

[55]  R. C. Fletcher,et al.  Wavelength selection in the folding of a single layer with power-law rheology , 1974 .

[56]  J. Rodríguez-Martínez,et al.  On the Taylor–Quinney coefficient in dynamically phase transforming materials. Application to 304 stainless steel , 2013 .

[57]  Gareth A. Jones,et al.  Cyclic regular subgroups of primitive permutation groups , 2002 .

[58]  Alain Molinari,et al.  Stability of steady states in shear zones , 1992 .

[59]  R. B. Smith,et al.  The effect of material properties on growth rates of folding and boudinage: Experiments with wax models , 1982 .

[60]  B. Hobbs,et al.  Localized and chaotic folding: the role of axial plane structures , 2012, Philosophical Transactions of the Royal Society A: Mathematical, Physical and Engineering Sciences.

[61]  M. Thielmann,et al.  Intermediate-depth earthquake generation and shear zone formation caused by grain size reduction and shear heating , 2015 .

[62]  J. Rice,et al.  A note on some features of the theory of localization of deformation , 1980 .

[63]  C. Froidevaux,et al.  Thermal and mechanical evolution of shear zones , 1980 .

[64]  Maurice A. Biot,et al.  Theory of Folding of Stratified Viscoelastic Media and its Implications in Tectonics and Orogenesis , 1998 .

[65]  Geoffrey Ingram Taylor,et al.  The Latent Energy Remaining in a Metal after Cold Working , 1934 .

[66]  C. Teyssier,et al.  An evaluation of quartzite flow laws based on comparisons between experimentally and naturally deformed rocks , 2001 .

[67]  Y. Podladchikov,et al.  Folding of a finite length power law layer , 2004 .

[68]  Derek Gaston,et al.  MOOSE: A parallel computational framework for coupled systems of nonlinear equations , 2009 .

[69]  T. Poulet,et al.  Thermo‐poro‐mechanics of chemically active creeping faults. 1: Theory and steady state considerations , 2014 .

[70]  B. Hobbs,et al.  Folding with thermal–mechanical feedback , 2008 .

[71]  B. Hobbs,et al.  Folding with thermal-mechanical feedback: A reply , 2009 .

[72]  Michael T. Bland,et al.  The formation of Ganymede's grooved terrain: Numerical modeling of extensional necking instabilities , 2007 .

[73]  Thomas Poulet,et al.  A viscoplastic approach for pore collapse in saturated soft rocks using REDBACK: An open-source parallel simulator for Rock mEchanics with Dissipative feedBACKs , 2016 .

[74]  P. Müller Permutation Groups with a Cyclic Two-Orbits Subgroup and Monodromy Groups of Laurent Polynomials , 2011 .

[75]  K. Regenauer‐Lieb,et al.  Review of extremum postulates , 2015 .

[76]  Ronald B. Smith Formation of folds, boudinage, and mullions in non-Newtonian materials , 1977 .

[77]  J. Burg,et al.  Boudinage in nature and experiment , 2012 .

[78]  Ioannis Vardoulakis,et al.  Steady shear and thermal run-away in clayey gouges , 2002 .

[79]  Mark F. Horstemeyer,et al.  Using a micromechanical finite element parametric study to motivate a phenomenological macroscale model for void/crack nucleation in aluminum with a hard second phase , 2003 .

[80]  Ioannis Vardoulakis,et al.  Thermoporomechanics of creeping landslides: The 1963 Vaiont slide, northern Italy , 2007 .

[81]  G. Dresen,et al.  Influence of water fugacity and activation volume on the flow properties of fine‐grained anorthite aggregates , 2006 .

[82]  David A. Yuen,et al.  Effects of temperature-dependent thermal diffusivity on shear instability in a viscoelastic zone: implications for faster ductile faulting and earthquakes in the spinel stability field , 2000 .

[83]  T. Shawki An Energy Criterion for the Onset of Shear Localization in Thermal Viscoplastic Materials, Part II: Applications and Implications , 1994 .

[84]  Marco Herwegh,et al.  Modeling episodic fluid‐release events in the ductile carbonates of the Glarus thrust , 2014 .

[85]  I. F. Collins,et al.  The algebraic-geometry of slip line fields with applications to boundary value problems , 1968, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[86]  B. Hobbs,et al.  Earthquakes in the ductile regime? , 1986 .

[87]  K. Regenauer‐Lieb,et al.  Conditions for the localisation of plastic deformation in temperature sensitive viscoplastic materials , 2016 .

[88]  D. Berend,et al.  Polynomials with roots modulo every integer , 1996 .

[89]  T. Shawki,et al.  An energy-based localization theory. I: Basic framework , 1995 .

[90]  John P. McSorley Cyclic permutations in doubly-transitive groups , 1997 .

[91]  J. T. Heege,et al.  Combining natural microstructures with composite flow laws: an improved approach for the extrapolation of lab data to nature , 2005 .

[92]  M. Handy,et al.  Frictional–viscous flow in mylonite with varied bimineralic composition and its effect on lithospheric strength , 1999 .

[93]  S. Piazolo,et al.  Pinch and swell structures: evidence for strain localisation by brittle–viscous behaviour in the middle crust , 2015 .

[94]  Ioannis Vardoulakis,et al.  Chemical reaction capping of thermal instabilities during shear of frictional faults , 2010 .

[95]  Klaus Regenauer-Lieb,et al.  Positive feedback of interacting ductile faults from coupling of equation of state, rheology and thermal-mechanics , 2004 .

[96]  Younan Xia,et al.  Discrete plasticity in sub-10-nm-sized gold crystals , 2010, Nature communications.