Inductive Source Simulation: 1D Layered Earth (Conductive)#
Geoscientific Problem#
For this code comparison, we simulated secondary magnetic fields over a layered Earth. From the top layer down we defined 3 layers with electrical conductivities \(\sigma_1\) = 0.05 S/m, \(\sigma_2\) = 0.5 S/m and \(\sigma_3\) = 0.05 S/m. The thicknesses of the top two layers were both 64 m.
Secondary magnetic fields were simulated for x, y and z oriented magnetic dipole sources at (0,0,5). For each source, the x, y and z components of the response were simulated at (10,0,5). We plot only the horizontal coaxial, horizontal coplanar and vertical coplanar data.
A figure illustrating the conductivity model and survey geometry is shown further down
Codes/Formulations Being Compared#
SimPEG 1D Formulation:
SimPEG 3D OcTree Formulation (H-formulation):
UBC E3DRH v1: E3DRH v1 is a voxel cell FDEM forward modeling and inversion package developed by the UBC Geophysical Inversion Facility. This software is proprietary and can ONLY be acquired through appropriate commerical license. The numerical approach of the forward simulation is described in the online manual’s theory section. If you have a valid license, there are instructions for reproducing the results (add link).
UBC E3DRH v2: E3DRH v2 is a voxel cell FDEM forward modeling and inversion package developed by the UBC Geophysical Inversion Facility. This software is proprietary and can ONLY be acquired through appropriate commerical license. The numerical approach of the forward simulation is described in the online manual’s theory section. If you have a valid license, there are instructions for reproducing the results (add link).
Loading Assets Into the SimPEG Framework#
We start by importing any necessary packages for running the notebook.
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import numpy as np
import matplotlib as mpl
import matplotlib.pyplot as plt
from discretize import TreeMesh
from SimPEG import maps
mpl.rcParams.update({"font.size": 10})
frequencies = np.logspace(2, 5, 10)
plot_simpeg_1d = True
plot_simpeg_octree = True
plot_ubc_e3drh_v1 = True
plot_ubc_e3drh_v2 = True
Next we download the mesh, model and simulated data for each code.
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# For each package, download .tar files
The mesh, model and predicted data for each code are then loaded into the SimPEG framework for plotting.
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rootdir = './../../../assets/fdem/layered_earth_conductive_fwd'
mesh_simpeg = TreeMesh.read_UBC(rootdir+'_simpeg/octree_mesh.txt')
model_simpeg = TreeMesh.read_model_UBC(mesh_simpeg, rootdir+'_simpeg/model.con')
data_list = []
legend_str = []
style_list_real = ['k-o', 'b-o', 'r-o', 'g-o', 'c-o']
style_list_imag = ['k--s', 'b--s', 'r--s', 'g--s', 'c--s']
if plot_simpeg_1d:
fname = '_simpeg/dpred_1d.txt'
data_array = np.loadtxt(rootdir+fname, skiprows=1)[:, 1:]
data_array = np.reshape(data_array, (3, len(frequencies), 6))
data_list.append(data_array)
legend_str += ['1D (real)', '1D (imag)']
if plot_simpeg_octree:
fname = '_simpeg/dpred_octree.txt'
data_array = np.loadtxt(rootdir+fname, skiprows=1)[:, 1:]
data_array = np.reshape(data_array, (3, len(frequencies), 6))
data_list.append(data_array)
legend_str += ['OcTree (real)', 'OcTree (imag)']
if plot_ubc_e3drh_v1:
fname = '_ubc_octree/fwd_v1/dpred_fwd.txt'
d_e3dv1 = np.loadtxt(rootdir+fname, comments='%')
d_e3dv1 = d_e3dv1[:, 9:15] # extract Hx, Hy and Hz columns
# Convert -iwt to +iwt
d_e3dv1 = np.c_[
d_e3dv1[:, 0], -d_e3dv1[:, 1],
d_e3dv1[:, 2], -d_e3dv1[:, 3],
d_e3dv1[:, 4], -d_e3dv1[:, 5]
]
d_e3dv1 = np.reshape(d_e3dv1, (3, len(frequencies), 6))
data_list.append(d_e3dv1)
legend_str += ['E3DRH v1 (real)', 'E3DRH v1 (imag)']
if plot_ubc_e3drh_v2:
fname = '_ubc_octree/fwd_v2/dpredFWD.txt'
d_e3dv2 = np.loadtxt(rootdir+fname)
# Extract Hx, Hy and Hz, and convert -iwt to +iwt
d_e3dv2 = np.c_[
d_e3dv2[0::3, 0], -d_e3dv2[0::3, 1],
d_e3dv2[1::3, 0], -d_e3dv2[1::3, 1],
d_e3dv2[2::3, 0], -d_e3dv2[2::3, 1]
]
d_e3dv2 = np.reshape(d_e3dv2, (3, len(frequencies), 6))
data_list.append(d_e3dv2)
legend_str += ['E3DRH v2 (real)', 'E3DRH v2 (imag)']
Geophysical Scenario#
Here, we plot the conductivity model used in the forward simulation.
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fig = plt.figure(figsize=(12,4))
ind_active = mesh_simpeg.cell_centers[:, 2] < 0
plotting_map = maps.InjectActiveCells(mesh_simpeg, ind_active, np.nan)
log_model = np.log10(model_simpeg[ind_active])
ax1 = fig.add_axes([0.14, 0.1, 0.6, 0.85])
mesh_simpeg.plot_slice(
plotting_map * log_model,
normal="Y", ax=ax1, ind=int(mesh_simpeg.h[1].size / 2),
clim=(np.min(log_model), np.max(log_model)), grid=True
)
ax1.set_xlim([-300, 300])
ax1.set_ylim([-250, 50])
ax1.set_title("OcTree Conductivity Model: {} Cells".format(mesh_simpeg.nC))
ax2 = fig.add_axes([0.76, 0.1, 0.05, 0.85])
norm = mpl.colors.Normalize(
vmin=np.min(log_model), vmax=np.max(log_model)
)
cbar = mpl.colorbar.ColorbarBase(
ax2, norm=norm, orientation="vertical", format="$10^{%.1f}$"
)
cbar.set_label("Conductivity [S/m]", rotation=270, labelpad=15, size=12)
Simulated Data Comparison#
Here we plot the simulated data for all codes/formulations.
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fig = plt.figure(figsize=(16, 7))
lw = 2
ms = [7, 6, 5, 4, 3]
ax = 3*[None]
for ii, comp in enumerate(['X','Y','Z']):
ax[ii] = fig.add_axes([0.05 + 0.3*ii, 0.1, 0.25, 0.8])
for jj in range(0, len(data_list)):
ax[ii].semilogx(
frequencies, data_list[jj][ii, :, 2*ii], style_list_real[jj], lw=lw, markersize=ms[jj]
)
ax[ii].semilogx(
frequencies, data_list[jj][ii, :, 2*ii+1], style_list_imag[jj], lw=lw, markersize=ms[jj]
)
ax[ii].grid()
ax[ii].set_xlabel('Frequency (Hz)')
ax[ii].set_ylabel('Secondary field (A/m)')
ax[ii].set_title(comp + ' dipole, ' + comp + ' component')
ax[ii].legend(legend_str)
