2019
DOI: 10.5194/se-10-969-2019
|View full text |Cite
|
Sign up to set email alerts
|

Improving subduction interface implementation in dynamic numerical models

Abstract: Abstract. 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 an… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

1
21
0

Year Published

2019
2019
2023
2023

Publication Types

Select...
6
3
1

Relationship

1
9

Authors

Journals

citations
Cited by 22 publications
(22 citation statements)
references
References 70 publications
1
21
0
Order By: Relevance
“…The initially uniformly thick (10 km) crust gradually thickens to ≈15 km as it descends into the trench. This is because slab rollback induces horizontal extension in the crust at upper plate depths which, in turn, thickens it locally within this region (cf., Beall et al, 2021;Sandiford and Moresi, 2019). The final, "mature" phase begins as the slab impinges on the lower mantle at a depth of 660 km.…”
Section: Geodynamic Evolutionmentioning
confidence: 99%
“…The initially uniformly thick (10 km) crust gradually thickens to ≈15 km as it descends into the trench. This is because slab rollback induces horizontal extension in the crust at upper plate depths which, in turn, thickens it locally within this region (cf., Beall et al, 2021;Sandiford and Moresi, 2019). The final, "mature" phase begins as the slab impinges on the lower mantle at a depth of 660 km.…”
Section: Geodynamic Evolutionmentioning
confidence: 99%
“…The setup is comparable to recent studies, where flow is driven entirely by the thermal density contrast of the plate slab, which develops as a naturally evolving thermal boundary layer at the surface (Agrusta et al., 2017; Garel et al., 2014). The model setup is described in detail in the supporting information S1 (see also Sandiford & Moresi, 2019). Mantle rheology (including oceanic lithosphere) is prescribed by a composite flow law including linear high‐temperature creep and a scalar viscoplasticity designed to capture both psuedo‐brittle as well as distributed plastic deformation within the slab.…”
Section: Insights From Numerical Modelingmentioning
confidence: 99%
“…Using these scaling factors and Equations 4 and 5, we can thus substitute the scaled parameters for their dimensionless counterparts in Equation 2, which after rearranging leads us to write the following dimensionless momentum conservation equation, similar to Sandiford and Moresi (2019):…”
Section: Scalingmentioning
confidence: 99%