knitr::opts_chunk$set( collapse = TRUE, comment = "#>" )
This vignette teaches you how to spatially interpolate stress fields and display the lateral patterns of stress anomalies.
library(tectonicr) library(ggplot2) # load ggplot library
data("san_andreas") data("cpm_models") por <- cpm_models |> subset(model == "NNR-MORVEL56") |> equivalent_rotation("na", "pa")
Spatial interpolation of stress data is based on the aforementioned metrics:
mean_SH <- stress2grid(san_andreas, gridsize = 1, R_range = seq(50, 350, 100))
The default settings apply quality and inverse distance weighting of the mean, as well as a 25% cut-off for the standard deviation.
The
tectonicr
algorithm is a modified version of the MATLAB algorithm 'stress2grid' by Ziegler and Heidbach (2017) but it is faster and provides additional features. Seehelp(stress2grid)
for more details and settings, such as different statistics for calculating the orientation average, adjustments of the weighting power of the distance, quality or method.
The data can now be visualized:
trajectories <- eulerpole_loxodromes(x = por, n = 40, cw = FALSE) ggplot(mean_SH) + geom_sf(data = trajectories, lty = 2) + geom_spoke(data = san_andreas, aes(lon, lat, angle = deg2rad(90 - azi)), radius = .5, color = "grey30", position = "center_spoke") + geom_spoke(aes(lon, lat, angle = deg2rad(90 - azi), alpha = sd, color = mdr), radius = 1, position = "center_spoke", lwd = 1) + coord_sf(xlim = range(san_andreas$lon), ylim = range(san_andreas$lat)) + scale_alpha(name = "Standard deviation", range = c(1, .25)) + scale_color_viridis_c( "Wavelength\n(R-normalized mean distance)", limits = c(0, 1), breaks = seq(0, 1, .25) ) + facet_wrap(~R)
The interpolated direction of far apart data points will suffer from distortions due to the underlying projection. In order to prevent such effects, the interpolation can be done in the PoR reference frame where the direction stays constant no matter the distance between the data points. Assuming that the stress field is sourced by the plate boundary force, the model-based interpolation allows more reliable results for areas close to plate boundaries.
mean_SH_PoR <- PoR_stress2grid(san_andreas, PoR = por, gridsize = 1, R_range = seq(50, 350, 100))
ggplot(mean_SH_PoR) + geom_sf(data = trajectories, lty = 2) + geom_spoke(data = san_andreas, aes(lon, lat, angle = deg2rad(90 - azi)), radius = .5, color = "grey30", position = "center_spoke") + geom_spoke(aes(lon, lat, angle = deg2rad(90 - azi), alpha = sd, color = mdr), radius = 1, position = "center_spoke", lwd = 1) + coord_sf(xlim = range(san_andreas$lon), ylim = range(san_andreas$lat)) + scale_alpha(name = "Standard deviation", range = c(1, .25)) + scale_color_viridis_c( "Wavelength\n(R-normalized mean distance)", limits = c(0, 1), breaks = seq(0, 1, .25) ) + facet_wrap(~R)
The function compact_grid()
selects only data with the minimum search radius
from interpolated layers with different search radii. Since the interpolation
was performed in the PoR CRS, the interpolated azimuths are additionally given
in the transformed azimuths. This allows to easily calculate misfits from
predicted directions:
mean_SH_PoR_reduced <- mean_SH_PoR |> compact_grid() |> dplyr::mutate(cdist = circular_distance(azi.PoR, 135))
Using circular_distance()
in the example above, we can display the spatial
patterns of the misfits of the stress direction from the predicted direction of
the plate boundary force. Since the interpolation was performed in the PoR CRS,
the grid is not composed of equally spaced grid cells in the geographic CRS. To
rasterize such grids, we can, e.g., use Voronoi cells from the ggforce
package.
ggplot(mean_SH_PoR_reduced) + ggforce::geom_voronoi_tile( aes(lon, lat, fill = cdist), max.radius = .7, normalize = FALSE ) + scale_fill_viridis_c("Angular distance", limits = c(0, 1)) + geom_sf(data = trajectories, lty = 2) + geom_spoke( aes(lon, lat, angle = deg2rad(90 - azi), alpha = sd), radius = .5, position = "center_spoke", lwd = .2, colour = "white" ) + scale_alpha("Standard deviation", range = c(1, .25)) + coord_sf(xlim = range(san_andreas$lon), ylim = range(san_andreas$lat))
The map highlights stress anomalies which show misfits to the direction of tested plate boundary force.
Another way to analyse spatial misfits is the kernel dispersion, i.e. the
local dispersion within a user-defined window (kernel). The kernel´s half width
can be a single number (km) or a range of widths. The latter requires to compact
the grid result (x
) to find the smallest kernel size containing the the least
dispersion (compact_grid(x, 'dispersion')
).
It is recommended to calculate the kernel dispersion on PoR transformed data to avoid angle distortions due to projections.
san_andreas_por <- san_andreas san_andreas_por$azi <- PoR_shmax(san_andreas, por, "right")$azi.PoR # transform to PoR azimuth san_andreas_por$prd <- 135 # test direction san_andreas_kdisp <- kernel_dispersion(san_andreas_por, gridsize = 1, R_range = seq(50, 350, 100)) san_andreas_kdisp <- compact_grid(san_andreas_kdisp, "dispersion") ggplot(san_andreas_kdisp) + ggforce::geom_voronoi_tile( aes(lon, lat, fill = stat), max.radius = .7, normalize = FALSE ) + scale_fill_viridis_c("Dispersion", limits = c(0, 1)) + geom_sf(data = trajectories, lty = 2) + geom_spoke( data = san_andreas, aes(lon, lat, angle = deg2rad(90 - azi), alpha = unc), radius = .5, position = "center_spoke", lwd = .2, colour = "white" ) + scale_alpha("Standard deviation", range = c(1, .25)) + coord_sf(xlim = range(san_andreas$lon), ylim = range(san_andreas$lat))
Mardia, K. V., and Jupp, P. E. (Eds.). (1999). "Directional Statistics" Hoboken, NJ, USA: John Wiley & Sons, Inc. doi: 10.1002/9780470316979.
Ziegler, Moritz O., and Oliver Heidbach. 2017. “Manual of the Matlab Script Stress2Grid” GFZ German Research Centre for Geosciences; World Stress Map Technical Report 17-02. doi: 10.5880/wsm.2017.002.
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