Topographic Correction
Contents
Topographic Correction¶
Computing the gravity disturbance is usually the first step towards generating a dataset that could provide insight of the structures and bodies that lie beneath Earth surface.
One of the strongest signals present in the gravity disturbances are the gravitational effect of the topography, i.e. every body located above the surface of the reference ellipsoid. Mainly because their proximity to the observation points but also because their density contrast could be considered the same as their own absolute density.
For this reason, geophysicists usually remove the gravitational effect of the topography from the gravity disturbance in a processes called topographic correction. The resulting field is often called Bouguer gravity disturbance or topography-free gravity disturbance.
The simpler way to apply the topographic correction is through the Bouguer correction. It consists in approximating the topographic masses that lay underneath each computation point as an infinite slab of constant density. It has been widely used on ground surveys because it’s easy to compute and because we don’t need any other data than the observation height (the height at which the gravity has been measured). It’s main drawback is it’s accuracy: the approximation might be too simple to accurately reproduce the gravitational effect of the topography present in our region of interest.
On the other hand, we can compute the topographic correction by forward modelling the topographic masses. To do so we will need a 2D grid of the topography, a.k.a. a DEM (digital elevation model). This method produces accurate corrections if the DEM has good resolutions, but its computation is much more expensive.
In the following sections we will explore how we can apply both methods using Harmonica.
Lets start by downloading some gravity data over the Bushveld Igneous Complex in Southern Africa.
import ensaio
import pandas as pd
fname = ensaio.fetch_bushveld_gravity(version=1)
data = pd.read_csv(fname)
data
longitude | latitude | height_sea_level_m | height_geometric_m | gravity_mgal | gravity_disturbance_mgal | gravity_bouguer_mgal | |
---|---|---|---|---|---|---|---|
0 | 25.01500 | -26.26334 | 1230.2 | 1257.474535 | 978681.38 | 25.081592 | -113.259165 |
1 | 25.01932 | -26.38713 | 1297.0 | 1324.574150 | 978669.02 | 24.538158 | -122.662101 |
2 | 25.02499 | -26.39667 | 1304.8 | 1332.401322 | 978669.28 | 26.526960 | -121.339321 |
3 | 25.04500 | -26.07668 | 1165.2 | 1192.107148 | 978681.08 | 17.954814 | -113.817543 |
4 | 25.07668 | -26.35001 | 1262.5 | 1289.971792 | 978665.19 | 12.700307 | -130.460126 |
... | ... | ... | ... | ... | ... | ... | ... |
3872 | 31.51500 | -23.86333 | 300.5 | 312.710241 | 978776.85 | -4.783965 | -39.543608 |
3873 | 31.52499 | -23.30000 | 280.7 | 292.686630 | 978798.55 | 48.012766 | 16.602026 |
3874 | 31.54832 | -23.19333 | 245.7 | 257.592670 | 978803.55 | 49.161771 | 22.456674 |
3875 | 31.57333 | -23.84833 | 226.8 | 239.199065 | 978808.44 | 5.116904 | -20.419870 |
3876 | 31.37500 | -23.00000 | 285.6 | 297.165672 | 978734.77 | 5.186926 | -25.922627 |
3877 rows × 7 columns
And plot it:
import cartopy.crs as ccrs
import matplotlib.pyplot as plt
import verde as vd
maxabs = vd.maxabs(data.gravity_disturbance_mgal)
fig = plt.figure(figsize=(10, 8), dpi=300)
ax = plt.axes(projection=ccrs.Mercator())
ax.set_title("Gravity disturbance", pad=25)
tmp = ax.scatter(
data.longitude,
data.latitude,
c=data.gravity_disturbance_mgal,
s=2,
vmin=-maxabs,
vmax=maxabs,
cmap="seismic",
transform=ccrs.PlateCarree(),
)
plt.colorbar(
tmp,
ax=ax,
orientation="horizontal",
label="mGal",
aspect=50,
pad=0.05,
shrink=0.7,
)
ax.set_extent(vd.get_region((data.longitude, data.latitude)))
ax.gridlines(draw_labels=True)
ax.coastlines()
plt.show()
Bouguer correction¶
We can compute the Bouguer correction through the
harmonica.bouguer_correction
function.
Because our gravity data has been obtained on the Earth surface, the
height_geometric_m
coordinate coincides with the topographic height at each
observation point (referenced above the ellipsoid), so we can pass it as the
topography
argument.
import harmonica as hm
bouguer_correction = hm.bouguer_correction(data.height_geometric_m)
Hint
The harmonica.bouguer_correction
assigns default values for the
density of the upper crust and the water.
Warning
In case the observations heights were referenced over the geoid (usually marked as above the mean sea level), it’s advisable to convert them to geometric heights by removing the geoid height.
We can now compute the Bouguer disturbance and plot it:
bouguer_disturbance = data.gravity_disturbance_mgal - bouguer_correction
bouguer_disturbance
0 -115.688843
1 -123.743874
2 -122.631301
3 -115.497942
4 -131.708097
...
3872 -39.790922
3873 15.247392
3874 20.325058
3875 -21.660701
3876 -28.079864
Length: 3877, dtype: float64
maxabs = vd.maxabs(bouguer_disturbance)
fig = plt.figure(figsize=(10, 8), dpi=300)
ax = plt.axes(projection=ccrs.Mercator())
ax.set_title("Bouguer disturbance (with simple Bouguer correction)", pad=25)
tmp = ax.scatter(
data.longitude,
data.latitude,
c=bouguer_disturbance,
s=2,
vmin=-maxabs,
vmax=maxabs,
cmap="seismic",
transform=ccrs.PlateCarree(),
)
plt.colorbar(
tmp,
ax=ax,
orientation="horizontal",
label="mGal",
aspect=50,
pad=0.05,
shrink=0.7,
)
ax.set_extent(vd.get_region((data.longitude, data.latitude)))
ax.gridlines(draw_labels=True)
ax.coastlines()
plt.show()
Forward modelling the topography¶
In order to forward model the topographic masses, we need to build a 3D model made out of simpler geometric bodies. In this case, we are going to use rectangular prisms. Then we will compute the gravitational effect of every prism on each computation point.
To do so, we need a regular grid of the topographic heights (or DEM as in Digital Elevation Model) around the Bushveld Igneous Complex. We can download a global topography grid:
import xarray as xr
fname = ensaio.fetch_southern_africa_topography(version=1)
topography = xr.load_dataarray(fname)
topography
<xarray.DataArray 'topography' (latitude: 1182, longitude: 1371)> array([[-5039., -5027., -5014., ..., -3846., -3867., -3873.], [-5036., -5021., -5007., ..., -3839., -3863., -3872.], [-5031., -5016., -5001., ..., -3835., -3860., -3870.], ..., [-2906., -2901., -2884., ..., 173., 134., 118.], [-2908., -2906., -2888., ..., 132., 119., 118.], [-2912., -2910., -2894., ..., 122., 120., 128.]], dtype=float32) Coordinates: * longitude (longitude) float64 10.92 10.93 10.95 10.97 ... 33.72 33.73 33.75 * latitude (latitude) float64 -36.0 -35.98 -35.97 ... -16.35 -16.33 -16.32 Attributes: Conventions: CF-1.8 title: Topographic and bathymetric height for Southern Africa ob... crs: WGS84 source: Downloaded from NOAA website (https://ngdc.noaa.gov/mgg/g... license: public domain references: https://doi.org/10.7289/V5C8276M long_name: topographic height above mean sea level standard_name: height_above_mean_sea_level description: height topography/bathymetry referenced to mean sea level units: m actual_range: [-5685. 3376.] noaa_metadata: Conventions: COARDS/CF-1.0\ntitle: ETOPO1_Ice_g_gmt4.grd\...
And then crop it to a slightly larger region than the gravity observations:
region = vd.get_region((data.longitude, data.latitude))
region_pad = vd.pad_region(region, pad=1)
topography = topography.sel(
longitude=slice(region_pad[0], region_pad[1]),
latitude=slice(region_pad[2], region_pad[3]),
)
topography
<xarray.DataArray 'topography' (latitude: 360, longitude: 539)> array([[ 1408., 1403., 1398., ..., -1300., -1316., -1336.], [ 1413., 1406., 1400., ..., -1292., -1305., -1319.], [ 1415., 1409., 1402., ..., -1284., -1295., -1306.], ..., [ 970., 972., 973., ..., 121., 120., 122.], [ 970., 973., 974., ..., 121., 120., 123.], [ 967., 970., 974., ..., 122., 122., 123.]], dtype=float32) Coordinates: * longitude (longitude) float64 24.02 24.03 24.05 24.07 ... 32.95 32.97 32.98 * latitude (latitude) float64 -28.0 -27.98 -27.97 ... -22.05 -22.03 -22.02 Attributes: Conventions: CF-1.8 title: Topographic and bathymetric height for Southern Africa ob... crs: WGS84 source: Downloaded from NOAA website (https://ngdc.noaa.gov/mgg/g... license: public domain references: https://doi.org/10.7289/V5C8276M long_name: topographic height above mean sea level standard_name: height_above_mean_sea_level description: height topography/bathymetry referenced to mean sea level units: m actual_range: [-5685. 3376.] noaa_metadata: Conventions: COARDS/CF-1.0\ntitle: ETOPO1_Ice_g_gmt4.grd\...
And project it to plain coordinates using pyproj
and verde
.
We start by defining a Mercator projection:
import pyproj
projection = pyproj.Proj(proj="merc", lat_ts=topography.latitude.values.mean())
And project the grid using verde.project_grid
:
topography_proj = vd.project_grid(topography, projection, method="nearest")
topography_proj
<xarray.DataArray 'topography' (northing: 360, easting: 539)> array([[ 1408. , 1403. , 1396.5, ..., -1300. , -1316. , -1336. ], [ 1409.5, 1409.5, 1399. , ..., -1292. , -1305. , -1319. ], [ 1412. , 1412. , 1399.5, ..., -1276. , -1295. , -1306. ], ..., [ 971. , 971. , 973. , ..., 122.5, 120. , 122. ], [ 970. , 970. , 974.5, ..., 122.5, 121. , 123. ], [ 970. , 970. , 974.5, ..., 122.5, 121. , 123. ]], dtype=float32) Coordinates: * easting (easting) float64 2.424e+06 2.426e+06 ... 3.328e+06 3.329e+06 * northing (northing) float64 -2.928e+06 -2.926e+06 ... -2.267e+06 -2.265e+06 Attributes: metadata: Generated by Chain(steps=[('mean',\n BlockReduce(...
Tip
Using the "nearest"
method makes the projection process faster than
using the "linear"
one.
Now we can create a 3D model of the topographic masses using a layer of
rectangular prisms. We can use the harmonica.prism_layer
function to
build it.
We also need to assign density values to each prism in the layer.
For every prism above the ellipsoid we will set the density of the upper crust
(2670 kg/m3), while for each prism below it we will assign the
density contrast equal to the density of the water (1040 kg/m3) minus
the density of the upper crust.
import numpy as np
density = np.where(topography_proj >= 0, 2670, 1040 - 2670)
prisms = hm.prism_layer(
(topography_proj.easting, topography_proj.northing),
surface=topography_proj,
reference=0,
properties={"density": density},
)
prisms
<xarray.Dataset> Dimensions: (northing: 360, easting: 539) Coordinates: * easting (easting) float64 2.424e+06 2.426e+06 ... 3.328e+06 3.329e+06 * northing (northing) float64 -2.928e+06 -2.926e+06 ... -2.267e+06 -2.265e+06 top (northing, easting) float32 1.408e+03 1.403e+03 ... 121.0 123.0 bottom (northing, easting) float64 0.0 0.0 0.0 0.0 ... 0.0 0.0 0.0 0.0 Data variables: density (northing, easting) int64 2670 2670 2670 2670 ... 2670 2670 2670 Attributes: coords_units: meters properties_units: SI
Now we need to compute the gravitational effect of these prisms on every
observation point. We can do it through the
harmonica.DatasetAccessorPrismLayer.gravity
method. But the coordinates
of the observation points must be also projected.
# Project the coordinates of the observation points
easting, northing = projection(data.longitude.values, data.latitude.values)
coordinates = (easting, northing, data.height_geometric_m)
# Compute the terrain effect
terrain_effect = prisms.prism_layer.gravity(coordinates, field="g_z")
Finally, we can compute the topography-free gravity disturbance:
topo_free_disturbance = data.gravity_disturbance_mgal - terrain_effect
And plot it:
maxabs = vd.maxabs(topo_free_disturbance)
fig = plt.figure(figsize=(10, 8), dpi=300)
ax = plt.axes(projection=ccrs.Mercator())
ax.set_title("Topography-free gravity disturbance", pad=25)
tmp = ax.scatter(
data.longitude,
data.latitude,
c=topo_free_disturbance,
s=2,
vmin=-maxabs,
vmax=maxabs,
cmap="seismic",
transform=ccrs.PlateCarree(),
)
plt.colorbar(
tmp,
ax=ax,
orientation="horizontal",
label="mGal",
aspect=50,
pad=0.05,
shrink=0.7,
)
ax.set_extent(vd.get_region((data.longitude, data.latitude)))
ax.gridlines(draw_labels=True)
ax.coastlines()
plt.show()