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151 changes: 151 additions & 0 deletions src/pages/models/cenki-2022-uht-granulitic-terranes/index.md
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---
templateKey: model
slug: test-2022-sunda-subduction
title: 'Subduction dynamics and plate coupling along seismically active margin: the
role of slab steps'
date: '2024-10-24T02:18:49.000Z'
featuredpost:
for_codes:
- 370401
status:
- completed
doi: https://doi.org/10.25914/aaen-nc33
url: https://mate.science//models/gollapalli-2022-sunda-subduction
creditText: 'Cenki-Tok or Cenki, B., Rey, Patrice F.., Arcay, D., & Giordani, J. (2024).
Timing of partial melting and granulite formation during the genesis of high to
ultra‐high temperature terranes: Insight from numerical experiments [Data set].
AuScope, National Computational Infrastructure. https://doi.org/aaen-nc33'
software:
name: 'Underworld2: Python Geodynamics Modelling for Desktop, HPC and Cloud'
doi: https://doi.org/10.5281/zenodo.3975252
url_source: ''
licence:
licence_url: https://creativecommons.org/licenses/by/4.0/legalcode
licence_image: ../../../img/licence/by.png
description: Creative Commons Attribution 4.0 International
licence_file: license.txt
submitter:
name: Thyagarajulu
family_name: Gollapalli
ORCID: https://orcid.org/0000-0001-9394-4104
creators:
- name: Thyagarajulu
family_name: Gollapalli
ORCID: 0000-0001-9394-4104
associated_publication:
title: Unravelling tectonic coupling and loading along the Sunda margin through
3-D regional numerical modelling
doi: https://doi.org/10.26180/21664034.v1
date: 2022-12
authors:
- name: Thyagarajulu
family_name: Gollapalli
compute_info:
name: Gadi Supercomputer
organisation: National Computational Infrastructure
url: https://pid.nci.org.au/doi/f5966_0057_9267_4579
doi: https://doi.org/10.25914/608bfd1838db2
research_tags:
- Subduction
- Plate boundary
compute_tags:
- Python
- Finite element
- Particle-in-cell
funder:
name: National Computational Infrastructure
doi: https://ror.org/04yx6dh41
abstract: The negative buoyancy of the slab primarily controls the subducting plate
and trench motions, and tectonic stresses around the convergent margins. Lateral
variations in negative buoyancy associated with varying slab depth along strike
must affect plate and margin motions, and, most importantly, have an impact on the
stress acting across the margin, thereby setting the context for plate coupling,
tectonics and present-day seismicity. Here, we investigated these interactions in
3-D subduction numerical models, focusing on along-trench variations in the subduction
depth and the resulting perturbations to the force balance. While we focus on the
steps in the slab depth, we additionally test the role of subducting plate, i.e.,
cohesion and viscosity, and upper plate properties, i.e., thickness, viscosity,
and cohesion. The results show that the magnitude of convergence velocity only depends
on the integrated slab mass and rheology of the subducting plate when the upper
plate is thin. Instead, the trench retreat/advance is sensitive to the heterogeneity
in the slab depth, and a complex pattern arises atop the slab step, with a characteristic
length of ~500 km from the slab depth perturbation. The remaining parameters of
the subducting and upper plate mainly affect the magnitude of the trench velocities
with minor influence on the pattern. The highest deformation/stress in the upper
plate is observed around the slab step due to the rigidity of the plate, causing
mutual perturbation between the deep and shallow slab portions, and the lateral
flow around the step. These results are compared with the observations along the
Sunda margin, where similar slab depth variations are found. The upper plate deformation
in the model shows remarkable compatibility with the observed distributions of compression
and extension of the Andaman- Sumatra-Java segments. Our study indicates that trench-parallel
forces, arising from the natural variations of slab depth, exert a first-order control
on the plate coupling and deformation along convergent margins and should not be
neglected.
description: The negative buoyancy of the slab drives subducting plate and trench
motions, influencing tectonic stresses at convergent margins. Variations in slab
depth along the trench affect plate coupling and seismicity. We investigated these
effects using 3-D subduction models, focusing on slab depth variations and their
impact on force balance. Results show convergence velocity is primarily controlled
by slab mass and subducting plate rheology, while trench movement is sensitive to
slab depth heterogeneity. The highest stress occurs around slab steps, aligning
with deformation patterns observed along the Sunda margin. This study highlights
the crucial role of trench-parallel forces in plate dynamics.
images:
landing_image:
src: ./graphics/vel_sr_inv_landing_page.png
caption: "\nMantle flow and upper plate deformation due to slab step"
graphic_abstract:
src: ./graphics/sketch.png
caption: "\nSketch of the tectonic forces acting at the Sunda margin and interface
stress along Andaman (DD’), Sumatra (FF’), and Java (MM’). At the Sumatra margin,
an additional transferred force ($F^*_{SP}$) from Java is acting that contributes
to crustal thickening/compression in the upper plate. The blue stars represent
the interplate earthquakes, and black dots are intraplate seismicity. The sketch
neglects the curvature of the trench and the obliquity of convergence."
model_setup:
src: ./graphics/model_matvar_edit_model_setup.png
caption: "\nNumerical model setup. The parameter `d` denotes the depth of the
long slab (i.e., 660 km, green plane), and `Δ𝑑` represents step length (i.e.,
the difference between the long and short slab). The long and short slabs extend
from 0-2000 and 2000-4000 km in the Y-direction. The trench is located at X
= 2000 km."
animation:
src: ./graphics/
caption: ''
model_setup_info:
url: ''
summary: The model setup consists of the subducting plate with attached slab and
upper plate inserted in the 660 km upper mantle lying over 340 km lower mantle.
The model extends 4000 km in each x, y, and 1000 km in the z-axis with a numerical
resolution of 512×512×128, respectively. This resolution results in an element
size of 7.8 km in all three directions. Each element is populated with 20 Lagrangian
particles to store material properties. All boundaries in the model are under
free slip conditions. All models include a 100 km thick subducting plate and slab.
The rheology in the top 30 km (crust) is viscoplastic, and the rest (70 km lithospheric
mantle) is viscous. Oceanic lithosphere has a density contrast of 50 $kg/m^3$
with respect to the underlying sublithospheric mantle. The entire slab has a uniform
initial dip angle of 45°. The upper plate consists of crust 30 km thick, and its
lithospheric mantle thickness is varied between 20 km, 40 km, and 60 km. The trailing
end of the subducting plate is free and upper plate end is fixed. The density
contrast between the upper plate and mantle is set to zero. This avoids lithostatic
pressure gradients, and the stress distribution in the upper plate is only influenced
by the dynamics driven by lateral slab buoyancy variations. Therefore, the stress
distribution in the upper plate can be used as a proxy for tectonic coupling at
the interface.
model_files:
url: ''
notes: Underworld2 input files of Sunda Subduction Zone (3D cartesian models).
file_tree: ''
existing_identifier: https://doi.org/10.5281/zenodo.7022845
nci_file_path:
https://thredds.nci.org.au/thredds/catalog/nm08/MATE/gollapalli-2022-sunda-subduction/catalog.html
include: true
dataset:
url: ''
notes: Output data mainly contains *.h5 and *.xdmf files.
existing_identifier: ''
nci_file_path:
https://thredds.nci.org.au/thredds/catalog/nm08/MATE/gollapalli-2022-sunda-subduction/catalog.html
include: true
metadataFile: ro-crate-metadata.json
---
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