Continental plate collision: Unstable vs. stable slab dynamics

We study possible scenarios for the evolution of continental collision zones by using a dynamic thermomechanical model that includes brittle-elastic-ductile rheology, surface erosion, and explicit metamorphic changes. This paper focuses primarily on the influence of four key parameters: (1) geotherm or thermotectonic age (which controls the rheological profile), (2) lower-crustal composition (weak or strong rheology), (3) convergence rate, and (4) metamorphic changes in the downgoing crust. The experiments suggest that, de- pending on these parameters, plate convergence is accommodated by four distinct mech- anisms: stable subduction, shortening by pure-shear thickening or folding, and Rayleigh- Taylor instabilities. It appears that stable, oceanic-type subduction can only occur in the case of cold lithospheres (Moho temperature, TMoho , 550 8C), and basically needs high convergence rates (.4-5 cm/yr). Depending on the lower-crustal rheology (strong or weak), either the whole (upper and lower) crust or only the lower crust can be involved in subduction. It appears that in the case of weak metamorphic rheologies, phase changes only slightly improve chances for stable subduction. Lithospheric shortening becomes a dominant mechanism when TMoho . 550 8C or convergence rates are ,4-5 cm/yr. Pure- shear thickening becomes important in all cases of hot lithospheres (TMoho . 650 8C). Large-scale folding is favored in the case of TMoho 5 500-650 8C and is more effective in the case of mechanical coupling between crust and mantle (e.g., strong lower crust). Grav- itational (Rayleigh-Taylor) instabilities overcome other mechanisms for very high values of TMoho (.800 8C) and may lead to development of subvertical cold spots.

[1]  C. Prodehl,et al.  Seismic experiments target earthquake-prone region in Romania , 2002 .

[2]  J. Arkani‐Hamed,et al.  Thermo-mechanical modeling of subduction of continental lithosphere , 2002 .

[3]  M. Doin,et al.  Subduction initiation and continental crust recycling: the roles of rheology and eclogitization $ , 2001 .

[4]  L. Jolivet,et al.  A thermomechanical model of exhumation of high pressure (HP) and ultra-high pressure (UHP) metamorphic rocks in Alpine-type collision belts , 2001 .

[5]  C. Beaumont,et al.  Modeling the behavior of the continental mantle lithosphere during plate convergence , 2000 .

[6]  A. Poliakov,et al.  Lithosphere folding: Primary response to compression? (from central Asia to Paris basin) , 1999 .

[7]  C. Beaumont,et al.  The continental collision zone, South Island, New Zealand: Comparison of geodynamical models and observations , 1996 .

[8]  C. Federico,et al.  Crustal shortening and duplication of the Moho in the Northern Apennines: a view from seismic refraction data , 1995 .

[9]  J. Malavieille,et al.  A mechanism for syn-collisional rock exhumation and associated normal faulting: Results from physical modelling , 1995 .

[10]  A. Poliakov,et al.  Initiation of salt diapirs with frictional overburdens: numerical experiments , 1993 .

[11]  Mark Cloos,et al.  Lithospheric buoyancy and collisional orogenesis: Subduction of oceanic plateaus, continental margins, island arcs, spreading ridges, and seamounts , 1993 .

[12]  L. Jolivet,et al.  Kinematics, topography, shortening, and extrusion in the India‐Eurasia collision , 1992 .

[13]  H. Austrheim Eclogite formation and dynamics of crustal roots under continental collision zones , 1991 .

[14]  P. Cundall Numerical experiments on localization in frictional materials , 1989 .

[15]  J. Achache,et al.  India–Eurasia collision chronology has implications for crustal shortening and driving mechanism of plates , 1984, Nature.

[16]  C. Chopin Coesite and pure pyrope in high-grade blueschists of the Western Alps: a first record and some consequences , 1984 .

[17]  Y. Podladchikov,et al.  From buckling to asymmetric folding of the continental lithosphere: numerical modelling and application to the Himalayan syntaxes , 2000, Geological Society, London, Special Publications.

[18]  P. Molnar,et al.  Gravitational (Rayleigh–Taylor) instability of a layer with non-linear viscosity and convective thinning of continental lithosphere , 1997 .

[19]  M. Cloos Lithospheric buoyancy and collisional orogenesis , 1993 .

[20]  Donald L. Turcotte,et al.  Geodynamics : applications of continuum physics to geological problems , 1982 .