2012
DOI: 10.5194/se-3-313-2012
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Using open sidewalls for modelling self-consistent lithosphere subduction dynamics

Abstract: Abstract. Subduction modelling in regional model domains, in 2-D or 3-D, is commonly performed using closed (impermeable) vertical boundaries. Here we investigate the merits of using open boundaries for 2-D modelling of lithosphere subduction. Our experiments are focused on using open and closed (free slip) sidewalls while comparing results for two model aspect ratios of 3:1 and 6:1. Slab buoyancy driven subduction with open boundaries and free plates immediately develops into strong rollback with high trench … Show more

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Cited by 43 publications
(55 citation statements)
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“…Due to the confined boundaries, continued convergence after detachment [Capitanio and Replumaz, 2013] is limited and dynamic effects such as plate eduction [Duretz et al, 2012b] are minimized. Further studies would benefit from the implementation of dynamic boundary conditions [e.g., Chertova et al, 2012] to circumvent that aspect.…”
Section: Discussionmentioning
confidence: 99%
“…Due to the confined boundaries, continued convergence after detachment [Capitanio and Replumaz, 2013] is limited and dynamic effects such as plate eduction [Duretz et al, 2012b] are minimized. Further studies would benefit from the implementation of dynamic boundary conditions [e.g., Chertova et al, 2012] to circumvent that aspect.…”
Section: Discussionmentioning
confidence: 99%
“…The top boundary is free slip and the bottom is no slip. To allow for slab decoupling from the top surface, a weak crustal layer is emplaced on top of the oceanic lithosphere following Chertova et al [2012]. The side boundaries are open for lateral inflow and outflow [Chertova et al, 2012], except for the top 150 km of the southern and northern parts of the domain at which kinematic boundary conditions of plate motion will be implemented.…”
Section: Model Geometry and Boundary Conditionsmentioning
confidence: 99%
“…The equations of mass, momentum and energy conservation and the transport equation for advection of nondiffusive material properties are solved in the extended Boussinesq approximation [Christensen and Yuen, 1984; van Hunen, 2001;Chert14]. Our models include two major phase transitions at 410 km and at 660 km in the unperturbed mantle [Cizkova et al, 2007;Chertova et al, 2012;Garel et al, 2014]. For the detailed description of these equations, we refer to Christensen and Yuen [1984].…”
Section: Initial Numerical Setupmentioning
confidence: 99%