Modeling the behavior of the continental mantle lithosphere during plate convergence

In studying orogenic processes, the mechanism of viscous Rayleigh-Taylor–type removal of gravitationally unstable lithosphere is often invoked to explain the behavior of the mantle lithosphere. Using numerical models, we consider this mechanism and explore alternate styles of deep lithospheric deformation during tectonic convergence. The numerical experiments incorporate a mix of viscous and plastic rheologies to model the mechanical evolution of the lithosphere-asthenosphere system. Our results suggest that there are a number of deformational modes of the model mantle lithosphere: (1) a dripping or Rayleigh-Taylor–type instability; (2) an asymmetric underthrusting or subduction; (3) symmetric, ablative plate consumption; (4) slab breakoff, the failure and detachment of the strong lithosphere; and (5) mixed modes with combinations of these processes. The development of the modes is controlled by the rate of convergence associated with the background tectonic regime, the density field, and the rheology of the mantle lithosphere. It is important to determine whether these modes occur in the Earth beneath collisional orogens.

[1]  J. Chéry,et al.  A simple parameterization of strain localization in the ductile regime due to grain size reduction: A case study for olivine , 1999 .

[2]  Anderson,et al.  Continuous deformation versus faulting through the continental lithosphere of new zealand , 1999, Science.

[3]  G. Houseman,et al.  Rayleigh–Taylor instability of the upper mantle and its role in intraplate orogeny , 1999 .

[4]  Peter Molnar,et al.  Rayleigh–Taylor instability and convective thinning of mechanically thickened lithosphere: effects of non‐linear viscosity decreasing exponentially with depth and of horizontal shortening of the layer , 1998 .

[5]  Marie-Pierre Doin,et al.  A comparison of methods for the modeling of thermochemical convection , 1997 .

[6]  P. Molnar,et al.  The growth of Rayleigh-Taylor-type instabilities in the lithosphere for various rheological and dens , 1997 .

[7]  W. M. Kaula,et al.  More thoughts on convergent crustal plateau formation and mantle dynamics with regard to Tibet , 1995 .

[8]  R. O’Connell,et al.  Ablative subduction: A two‐sided alternative to the conventional subduction model , 1992 .

[9]  Philip England,et al.  Extension during continental convergence, with application to the Tibetan Plateau , 1989 .

[10]  M. Toksöz,et al.  Thermal effects of continental collisions: Thickening a variable viscosity lithosphere , 1983 .

[11]  P. Molnar,et al.  Convective instability of a thickened boundary layer and its relevance for the thermal evolution of , 1981 .

[12]  P. Bird Continental delamination and the Colorado Plateau , 1979 .

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

[14]  P. Fullsack An arbitrary Lagrangian-Eulerian formulation for creeping flows and its application in tectonic models , 1995 .

[15]  J. Poirier Shear localization and shear instability in materials in the ductile field , 1980 .