Authors: Samantha Ross1, Simon Williams1, Mike Gurnis2, Ting Yang2
1EarthByte Research Group, School of Geosciences, The University of Sydney, Australia
2Division of Geological and Planetary Sciences, California Institute of Technology
Updated for GPlates 2.2 and the reconstruction of Müller et al. (2019) by Christopher Alfonso and Behnam Sadeghi
EarthByte Research Group, School of Geosciences, The University of Sydney, Australia
Deforming Plate Models and Crustal Thickness
Exercise 1 - Cretaceous Rift Basins in Africa
Part 1: Understanding the deformation inherent within existing reconstruction models
Part 2: Deciding where the deformation should be distributed
Part 3: Build the Topological Boundaries and Network Topology
Exercise 2 - Tracking Crustal Thickness Changes
This tutorial is designed to introduce the user to deforming plate models and visualising crustal thickness.
Click here to download the data bundle for this tutorial.
The tutorial dataset includes the following files:
NOTE: This tutorial requires functionalities that are only available in GPlates 2.0 or newer versions.
Firstly, we will load the files from the Muller et al. (2019) plate motion model, and look at how deformation is represented within a rigid, topological plate model. Within this global model, the poles of rotation that describe South Atlantic rifting are taken from the studies of Nürnberg and Müller (1991) and Torsvik et al (2009).
Note the overlap between the static polygons that represent NW Africa, NE Africa, Southern Africa, South America, and the two subplates in Southern South America (labelled Colorado and Parana subplates) (Figure 1). The overlap represents the fact that these plates will move away from each other at some point between this reconstruction time and present day (you can compare what you are looking at with Figure 10 of Torsvik et al., 2009).
Figure 1: Overlap between static polygons in Africa and South America at 132 Ma.
Figure 2: Extensional boundaries within Africa and South America at 132 Ma (Step 5)
Within the Muller et al (2019) topologies, the extensional boundaries within Africa and South America are represented as lines. Our aim will be to modify these boundaries to be more analogous to more diffuse zones of continental rifting. Note that in this tutorial we will only deal with the intracontinental rifts.
Before we modify the topologies to include deforming regions, we first need some basis for where the deformation is distributed. For the purposes of this tutorial we will focus on one such example, sediment thickness. We will use the global, 1 degree resolution sediment thickness included in the CRUST1.0 model of global crustal structure.
A global grid file (and associated .gpml file) has been included in the tutorial data (resampled to 15 minute resolution).
Figure 3: Adding the connection to the static polygons layer for the sediment thickness raster (Step 2).
As you reconstruct back through time, you should now notice that the raster layer moves with the static polygons.
Figure 4: Sediment thickness reconstructed to 84 Ma (the raster layer is connected to the Static Polygons layer).
The rationale for using a map of sediment thickness to guide our definition of deforming regions is fairly simple - if the deforming regions are extensional basins, then we might expect the zones of high extension and crustal thinning to correlate with thick sediment accumulations. The sediment thickness map alone provides no indication of the timing that these sediments accumulated, or whether the accumulations correspond to rift basins or some other mechanism. For the thick sediments along the boundaries separating NW, NE and Southern Africa, we can check against the locations of rift basins defined in different literature (Figures 5 & 6).
Figure 5: Development of major rift basins at 108 Ma (Genik et al, 1992).
Figure 6: Rift configuration at 30 Ma (Genik et al, 1992).
If we compare the distribution of Cretaceous basins in this interpretation (Figure 5) to the sediment thickness grid and the plate boundaries in the topological model (Figure 4), we can see that there is a pretty good correlation between all three for the basins of the Central African Rift System. The sediment thickness grid also includes additional significant accumulations in other areas (e.g., the Congo Basin within southern Africa, or the Taoudeni Basin within NW Africa), which are not thought to be related to South Atlantic rifting, and are therefore not represented in the topological plate boundaries.
It is also worth considering the timing of the motion between the different blocks. The three plate polygons in question have plates IDs of 714 (NW Africa), 715 (NE Africa) and 701 (Southern Africa).
701 moves relative to the absolute reference frame, and the relative motion between the different African blocks is described by the relative motions of 714 and 715 (as the moving plates, column 1) relative to 701 (as the fixed plate, column 6).
Figure 7: Rotation data for different African blocks (Step 4).
We can determine that NW Africa (714) moves relative to Southern Africa (701) from 131.7 Ma to 120.4 Ma in this model, while NE Africa (715) moves relative to Southern Africa from 120.4 Ma to 83.5 Ma (Figure 7). Note that, by implication, there is also relative motion between NW Africa and NE Africa during the 131.7 to 83.5 Ma time period.
The first step to building a deforming network over the deformation regions is to define line geometries that will define the boundaries of the deformation zone.
When constructing these lines, keep in mind the following:
Figure 8: Example of the three new boundaries (black lines) which encompass the regions of the Central African Rift System Basins. The appropriate Plate IDs that they should be assigned are also shown. Coastlines are shown in silver.
Note: Using this one dataset alone is somewhat approximate. In this case, we have no choice but to define boundaries that to some extent correspond to the rigid geometries in Torsvik et al (2009) model, even if the location of the implied deformation may not be immediately apparent from the sediment thickness. An example is the northern part of the boundary between NW and NE Africa. In practical cases, it is recommended to use as many alternative lines of available geological and geophysical data to refine these boundaries.
Figure 9: Building the network topology with line segments (Step 3).
Figure 10: Layer options when Resolved Topological Networks Layer is expanded.
Notice that now the African rift basin appears like a network (Figure 11) (raster turned off for clarity).
Figure 11: African Rift Basin network topologies.
(Note that red = extension and blue = compression)
Another way to visualise the strain rate in a topological network is by filling the triangulations
Don’t forget to save both the new line topologies and the topological network layer!
GPlates has the functionality that allows points to be generated within a deforming region which then allow crustal thickness to be tracked.
The outline of the network should be highlighted in white once it has been selected.
Figure 12: Features → Generate Deforming Mesh Points.
A new window will open where we specify properties of the points we will generate (Figure 13).
Figure 13: Generating Crustal Thickness Points Window (Step 5).
Figure 14: Generating Crustal Thickness Points Window (Step 6).
We are generating points at 132 Ma, so all changes to crustal thickness will be calculated relative to this time (hence it is very important to think about what time you generate your points at - check your reconstruction time now!).
You will now notice that there are lots of green points within the deforming region (Figure 15), and that two new layers have been generated: a green Reconstructed Geometries layer and a dark grey Reconstructed Scalar Coverages layer.
Figure 15: The newly generated crustal thickness points.
Figure 16: Layer options for the new Reconstructed Geometries layer.
Figure 17: Redefining the colour palette range (Step 10).
Notice how the scalar points have changed colour, reflecting changes in crustal thickness (Figure 18).
Figure 18: Stretching factor (beta factor) at 84 Ma relative to 132 Ma.
Since we are modelling a rift basin, it makes sense that the crust has thinned from 132-84 Ma due to rifting.
There are other options available to visualise changes to crustal thickness if you do not like the current colour palette.
A new window will open where you can choose from a range of colour palettes, choose the number of classes, whether the palette is discrete or whether you’d like to invert the palette (Figure 19).
Figure 19: Choose colour palette from a range of built-in options.
Figure 20: African Rift Basin at 84 Ma, visualised using the spectral colour palette (inverted and discrete).
For more detailed information about tracking crustal thickness changes, see Tutorial 8.4.
Genik, G. J. (1992). Regional framework, structural and petroleum aspects of rift basins in Niger, Chad and the Central African Republic (CAR).Tectonophysics, 213(1), 169-185.
Müller, R.D., Zahirovic, S., Williams, S.E., Cannon, J., Seton, M., Bower, D.J., Tetley, M.G., Heine, C., Le Breton, E., Liu, S., Russell, S.H.J., Yang, T., Leonard, J., & Gurnis, M. (2019). A Global Plate Model Including Lithospheric Deformation Along Major Rifts and Orogens Since the Triassic. Tectonics, 38(6), 169-185. doi: 10.1029/2018tc005462
Nürnberg, D., & Müller, R. D. (1991). The tectonic evolution of the South Atlantic from Late Jurassic to present. Tectonophysics, 191(1), 27-53.
Torsvik, T. H., Rousse, S., Labails, C., & Smethurst, M. A. (2009). A new scheme for the opening of the South Atlantic Ocean and the dissection of an Aptian salt basin. Geophysical Journal International, 177(3), 1315–1333. doi:10.1111/j.1365-246X.2009.04137.x
Müller, R. D., Zahirovic, S., Williams, S. E., Cannon, J., Seton, M., Bower, D. J., Tetley, M. G., Heine, C., Le Breton, E., Liu, S., Russell, S. H. J., Yang, T., Leonard, J., and Gurnis, M., 2019, A Global Plate Model Including Lithospheric Deformation Along Major Rifts and Orogens Since the Triassic: Tectonics, v. 38, no. 6, p. 1884-1907. doi: 10.1029/2018tc005462.