Improving subduction interface implementation in dynamic numerical models

<p>Numerical subduction models often implement an entrained weak layer (WL) to facilitate decoupling of the slab and upper plate. This approach is attractive in its simplicity, and can provide stable, asymmetric subduction systems that persist for many tens of millions of years. In this study...

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Main Authors: D. Sandiford, L. Moresi
Format: Article
Language:English
Published: Copernicus Publications 2019-06-01
Series:Solid Earth
Online Access:https://www.solid-earth.net/10/969/2019/se-10-969-2019.pdf
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spelling doaj-444548cabd1642ff9e3e6b2c1128ebda2020-11-25T01:16:34ZengCopernicus PublicationsSolid Earth1869-95101869-95292019-06-011096998510.5194/se-10-969-2019Improving subduction interface implementation in dynamic numerical modelsD. Sandiford0D. Sandiford1L. Moresi2School of Earth Sciences, University of Melbourne, Melbourne, VIC, 3010, AustraliaInstitute of Marine and Antarctic Studies, University of Tasmania, Hobart, TAS, 7004, AustraliaSchool of Earth Sciences, University of Melbourne, Melbourne, VIC, 3010, Australia<p>Numerical subduction models often implement an entrained weak layer (WL) to facilitate decoupling of the slab and upper plate. This approach is attractive in its simplicity, and can provide stable, asymmetric subduction systems that persist for many tens of millions of years. In this study we undertake a methodological analysis of the WL approach, and use these insights to guide improvements to the implementation. The issue that primarily motivates the study is the emergence of significant spatial and temporal thickness variations within the WL. We show that these variations are mainly the response to volumetric flux gradients, caused by the change in boundary conditions as the WL material enters and exits the zone of decoupling. The time taken to reach a quasi-equilibrium thickness profile will depend on the total plate convergence, and is around 7&thinsp;Myr for the models presented here. During the transient stage, width variations along the WL can exceed 4<span class="inline-formula">×</span>, which may impact the effective strength of the interface, through physical effects if the rheology is linear, or simply if the interface becomes inadequately numerically resolved. The transient stage also induces strong sensitivity to model resolution. By prescribing a variable-thickness WL at the outset of the model, and by controlling the limits of the layer thickness during the model evolution, we find improved stability and resolution convergence of the models.</p>https://www.solid-earth.net/10/969/2019/se-10-969-2019.pdf
collection DOAJ
language English
format Article
sources DOAJ
author D. Sandiford
D. Sandiford
L. Moresi
spellingShingle D. Sandiford
D. Sandiford
L. Moresi
Improving subduction interface implementation in dynamic numerical models
Solid Earth
author_facet D. Sandiford
D. Sandiford
L. Moresi
author_sort D. Sandiford
title Improving subduction interface implementation in dynamic numerical models
title_short Improving subduction interface implementation in dynamic numerical models
title_full Improving subduction interface implementation in dynamic numerical models
title_fullStr Improving subduction interface implementation in dynamic numerical models
title_full_unstemmed Improving subduction interface implementation in dynamic numerical models
title_sort improving subduction interface implementation in dynamic numerical models
publisher Copernicus Publications
series Solid Earth
issn 1869-9510
1869-9529
publishDate 2019-06-01
description <p>Numerical subduction models often implement an entrained weak layer (WL) to facilitate decoupling of the slab and upper plate. This approach is attractive in its simplicity, and can provide stable, asymmetric subduction systems that persist for many tens of millions of years. In this study we undertake a methodological analysis of the WL approach, and use these insights to guide improvements to the implementation. The issue that primarily motivates the study is the emergence of significant spatial and temporal thickness variations within the WL. We show that these variations are mainly the response to volumetric flux gradients, caused by the change in boundary conditions as the WL material enters and exits the zone of decoupling. The time taken to reach a quasi-equilibrium thickness profile will depend on the total plate convergence, and is around 7&thinsp;Myr for the models presented here. During the transient stage, width variations along the WL can exceed 4<span class="inline-formula">×</span>, which may impact the effective strength of the interface, through physical effects if the rheology is linear, or simply if the interface becomes inadequately numerically resolved. The transient stage also induces strong sensitivity to model resolution. By prescribing a variable-thickness WL at the outset of the model, and by controlling the limits of the layer thickness during the model evolution, we find improved stability and resolution convergence of the models.</p>
url https://www.solid-earth.net/10/969/2019/se-10-969-2019.pdf
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