Note
Go to the end to download the full example code
3D gravity modelling and inversion#
Based on the synthetic model of Li & Oldenburg (1998), we demonstrate 3D inversion of magnetic data. The forward operator bases on the formula given by Holstein et al. (2007).
In the following, we will build the model, create synthetic data, and do inversion using a depth-weighting function as outlined in the paper.
import numpy as np
import matplotlib.pyplot as plt
import pygimli as pg
from pygimli.viewer import pv
from pygimli.physics.gravimetry import GravityModelling
Synthetic model and data generation#
The grid is 1x1x0.5 km with a spacing of 50 m.
Mesh: Nodes: 4851 Cells: 4000 Boundaries: 12800
We create a 3D matrix that is later filled as vector into the grid. The model consists of zeros and patches of 5x6 cells per depth slice that are shifted by one cell for subsequent cells.
We show the model making use of the pyvista package that can be called by
pygimli.show(). The mesh itself is shown as a wireframe, the anomaly
is plotted as a surface plot using a threshold filter. After the first call
with hold=True, the plotter is used to draw any subsequent plots that can
also be slices or clips. Moreover, the camera position is set so that the
vertical axis is going downwards (x is Northing and y is Easting as common in
magnetics).
pl, _ = pg.show(grid, style="wireframe", hold=True)
pv.drawMesh(pl, grid, label="synth", style="surface", cMap="Spectral_r",
filter={"threshold": dict(value=0.05, scalars="synth")})
pl.camera_position = "yz"
pl.camera.roll = 90
pl.camera.azimuth = 180 - 15
pl.camera.elevation = 10
pl.camera.zoom(1.2)
_ = pl.show()
We simulate the synthetic model and display the model response.
xx, yy = np.meshgrid(x, y)
points = np.column_stack((xx.ravel(), yy.ravel(), -np.ones(np.prod(xx.shape))))
fop = GravityModelling(grid, points)
data = fop.response(grid["synth"])
noise_level = 1
data += np.random.randn(len(data)) * noise_level
plt.contourf(yy, xx, np.reshape(data, xx.shape))
plt.colorbar();
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<matplotlib.colorbar.Colorbar object at 0x7ff74f11b5b0>
Depth weighting#
In the paper of Li & Oldenburg (1996), they propose a depth weighting of the constraints with the formula
\[w_z = \frac{1}{(z+z_0)^{\beta/2}}\]
Inversion#
The inversion is rather straightforward using the standard inversion
framework pygimli.Inversion.
inv = pg.Inversion(fop=fop, verbose=True) # , debug=True)
inv.modelTrans = pg.trans.TransCotLU(-2, 2)
# inv.setRegularization(correlationLengths=[500, 500, 100])
inv.setConstraintWeights(wz)
invmodel = inv.run(data, absoluteError=noise_level, lam=1e4, # zWeight=0.3,
startModel=0.1, verbose=True)
grid["inv"] = invmodel
fop: <pygimli.physics.gravimetry.GravityModelling.GravityModelling object at 0x7ff754825e90>
Data transformation: <pygimli.core._pygimli_.RTransLin object at 0x7ff754826110>
Model transformation: <pygimli.core._pygimli_.RTransCotLU object at 0x7ff754827920>
min/max (data): -464/-14.33
min/max (error): 0.22%/6.98%
min/max (start model): 0.1/0.1
--------------------------------------------------------------------------------
inv.iter 0 ... chi² = 9000.83
--------------------------------------------------------------------------------
inv.iter 1 ... chi² = 16.01 (dPhi = 99.63%) lam: 10000.0
--------------------------------------------------------------------------------
inv.iter 2 ... chi² = 1.30 (dPhi = 40.76%) lam: 10000.0
--------------------------------------------------------------------------------
inv.iter 3 ... chi² = 1.29 (dPhi = 0.02%) lam: 10000.0
################################################################################
# Abort criterion reached: dPhi = 0.02 (< 2.0%) #
################################################################################
Model response
misfit = np.reshape(data-inv.response, xx.shape) / noise_level
plt.pcolor(yy, xx, misfit, cmap="bwr", vmin=-3, vmax=3)
plt.colorbar();
<matplotlib.colorbar.Colorbar object at 0x7ff746ad0820>
Visualization#
For showing the model, we again use the threshold filter with a value of 0.02. For comparison with the synthetic model, we plot the latter as a wireframe.
ftr = dict(value=0.5, scalars="synth")
pl, _ = pg.show(grid, label="synth", style="wireframe",
filter={"threshold": ftr}, hold=True)
ftr = dict(value=0.4, scalars="inv")
pv.drawMesh(pl, grid, label="inv", style="surface", filter={"threshold": ftr},
cMin=0, cMax=1)
pl.camera_position = "yz"
pl.camera.roll = 90
pl.camera.azimuth = 180
pl.camera.zoom(1.2)
_ = pl.show()
The model can outline the top part of the anomalous body and its lateral extent, but not its depth extent due to the ambiguity of gravity. We use a vertical slice to illustrate that.
(500.0, 0.0)
References#
Li, Y. & Oldenburg, D. (1998): 3-D inversion of gravity data. Geophysics 63(1), 109-119.
Holstein, H., Sherratt, E.M., Reid, A.B. (2007): Gravimagnetic field tensor gradiometry formulas for uniform polyhedra, SEG Ext. Abstr.
Total running time of the script: (0 minutes 13.636 seconds)