Available Models

 Fast modeling results (1.8 cm.y-1 extension speed) at an average strain rate of 3e-15 s-1 and 25 % extension. Colors are the same as in Fig 2. Model a. Only partial melting is allowed (garnet-pyroxene isograde and retrogression into amphibolite are removed). Model b. Partial melting, crystallization of garnet-pyroxene assemblages and retrogression are allowed. The temperature for the transformation of the continental crust into garnet-pyroxene rich rocks is 777 °C (see text for explanation). The reference temperatures for the solidus of the continental crust and the garnet-pyroxene rich crust are 650 °C and 790 °C, respectively. Model c. Same as model b but the temperature for the continental crust solidus is increased to 720 °C. Model d.  Zoom on model b illustrating the velocity field (black arrows) when the boundary condition mimicking extension is removed (after 2 Myr of gravity forces operating) showing that the partially molten crust flows while garnet-pyroxene rich rocks do not.

Strain and retrogression partitioning explain long-term stability of crustal roots in stable continents

Uploaded by: Bénédicte Cenki-Tok or Cenki

Uploaded: October 28, 2024

Software: Underworld 2

Tags:

crustal rootsretrogressionstability

Finite ElementPython


Mantle flow and upper plate deformation due to slab step

Subduction dynamics and plate coupling along seismically active margin: the role of slab steps

Uploaded by: Thyagarajulu Gollapalli

Uploaded: October 24, 2024

Software: Underworld2: Python Geodynamics Modelling for Desktop, HPC and Cloud

Tags:

Plate boundarySubduction

Finite elementParticle-in-cellPython

Marker lines prior to (a) and after 750 years of flow of (b) isotropic and (c) anisotropic ice. The axial plane of the resulting shear fold in isotropic ice mimics the bedrock topography, while it is controlled by shearing along a horizontal shear zone in the case of anisotropic ice. Green: bedrock, flow to the right.

ISMIP-HOM benchmark experiments using Underworld

Uploaded by: Dan Sandiford

Uploaded: August 19, 2024

Software: Underworld2: Python Geodynamics Modelling for Desktop, HPC and Cloud

Tags:

Stokesanisotropybenchmarkice-sheetmechanical

Finite-ElementParticle-in-cellPython

Figure 5. Evolution of the stress at the reference point (0, 0, −10 km) (a), maximum slip rate along the entire fault zone (b)
and the adaptive time step used in simulation (c) for the reference model.

Numerical Modeling of Earthquake Cycles Based On Navier-Stokes Equations With Viscoelastic-Plasticity Rheology

Uploaded by: Haibin Yang

Uploaded: August 16, 2024

Software: Underworld

Tags:

Cratonic EarthquakesEarthquake CyclesNavier-StokesViscoelastic-Plasticity

Finite elementParticle-in-cellPython

Downdip component of strain rate tensor and resolved stress difference from the numerical model, focusing on features within the plate/slab. The resolved stress difference is defined as ($\sigma_{s} - \sigma_{z}$), where $\hat{s}$, and $\hat{z}$ are unit vectors in the downdip and slab normal directions. The fields show, for example, shortening/extension in the downdip direction. Stress profiles at four locations are shown. The blue line ($x_0$) is the first zero crossing based on analysis of the flexural component of the topography. The black line is the location of maximum bending moment.

Plate bending earthquakes and the strength distribution of the lithosphere

Uploaded by: Dan Sandiford

Uploaded: May 28, 2024

Software: ASPECT v2.4.0

Tags:

Dynamics of lithosphereEarthquakesLithospheric flexureSubduction

C++adaptive-mesh-refinementfinite-elementparticles

Stress evolution of more buoyant arc-continent collision. This style of collision results in slab break-off

The Role of Lithospheric-Deep Mantle Interactions on the Style and Stress Evolution of Arc-Continent Collision

Uploaded by: Andres Felipe Rodriguez Corcho

Uploaded: May 24, 2024

Software: Underworld2

Tags:

arc-collisionbuoyancy contrastgravitational collapseslab-anchoringslab-folding

Finite ElementMPIParticle-in-cellPython

Our simulations produce catchment areas, river lengths, and volumes of deposited sediment that are consistent with the ranges observed in continental-scale deltas such as the Mississippi and Amazon rivers. (a) Example showing the outputs from the numerical simulation showing the elevation and bathymetry (top) and cumulative flexure (bottom). Model dimensions are 4500 km x 2000 km, with a vertical exaggeration of 100x. (b) Scatter plot of river length (top) and 405 shelf width (bottom) versus catchment area from river systems. Data is from Somme et al. (2009), Nyberg et al. (2018), Blum et al. (2013, 2017) and simulations presented in this study. Pal= Paleocene, Oli=Oligocene, PM= Paleo-Mississippi. (c) Example of synthetic stratigraphy from a simulation without (left) and with flexural compensation (right).

Flexural isostatic response of continental-scale deltas to climatically driven sea level changes

Uploaded by: Sara Polanco

Uploaded: May 24, 2024

Software: Badlands

Tags:

Deltaic depocentersFlexural isostasyGlacial isostatic adjustment (GIA)Stratigraphic record

Constraining the response of continental-scale groundwater flow to climate change

Constraining the response of continental-scale groundwater flow to climate change

Uploaded by: Dan Sandiford

Uploaded: May 20, 2024

Software: Underworld2: Python Geodynamics Modelling for Desktop, HPC and Cloud

Tags:

BayesianPythongroundwaterthermal-hydraulicwater-management

CPythonadvection-diffusionfinite elementheat equation

Deviatoric stresses and vorticity in reference model.

Kinematics of Footwall Exhumation at Oceanic Detachment faults: Solid‐Block Rotation and Apparent Unbending

Uploaded by: Dan Sandiford

Uploaded: May 17, 2024

Software: geodynamics/aspect: ASPECT 2.5.0

Tags:

detachment faultsfaultingtectonics

C++finite-elementmesh-refinement