diff --git a/myst.yml b/myst.yml index 9db9d49..8d4c4df 100644 --- a/myst.yml +++ b/myst.yml @@ -73,48 +73,48 @@ project: toc: - file: index.md - - file: notebooks/gravity_index.md + - file: notebooks/gravity/index.md children: - - file: notebooks/03-gravity/fwd_gravity_anomaly_3d.ipynb - - file: notebooks/03-gravity/fwd_gravity_gradiometry_3d.ipynb - - file: notebooks/03-gravity/inv_gravity_anomaly_3d.ipynb - - file: notebooks/03-gravity/weighting_strategies.ipynb - - file: notebooks/magnetics_index.md + - file: notebooks/gravity/fwd_gravity_anomaly_3d.ipynb + - file: notebooks/gravity/fwd_gravity_gradiometry_3d.ipynb + - file: notebooks/gravity/inv_gravity_anomaly_3d.ipynb + - file: notebooks/gravity/weighting_strategies.ipynb + - file: notebooks/magnetics/index.md children: - - file: notebooks/04-magnetics/fwd_magnetics_induced_3d.ipynb - - file: notebooks/04-magnetics/fwd_magnetics_mvi_3d.ipynb - - file: notebooks/04-magnetics/inv_magnetics_induced_3d.ipynb - - file: notebooks/dcr_index.md + - file: notebooks/magnetics/fwd_magnetics_induced_3d.ipynb + - file: notebooks/magnetics/fwd_magnetics_mvi_3d.ipynb + - file: notebooks/magnetics/inv_magnetics_induced_3d.ipynb + - file: notebooks/dc-resistivity/index.md children: - - file: notebooks/05-dcr/fwd_dcr_1d.ipynb - - file: notebooks/05-dcr/fwd_dcr_2d.ipynb - - file: notebooks/05-dcr/fwd_dcr_3d.ipynb - - file: notebooks/05-dcr/inv_dcr_1d.ipynb - - file: notebooks/05-dcr/inv_dcr_2d.ipynb - - file: notebooks/05-dcr/inv_dcr_3d.ipynb - - file: notebooks/ip_index.md + - file: notebooks/dc-resistivity/fwd_dcr_1d.ipynb + - file: notebooks/dc-resistivity/fwd_dcr_2d.ipynb + - file: notebooks/dc-resistivity/fwd_dcr_3d.ipynb + - file: notebooks/dc-resistivity/inv_dcr_1d.ipynb + - file: notebooks/dc-resistivity/inv_dcr_2d.ipynb + - file: notebooks/dc-resistivity/inv_dcr_3d.ipynb + - file: notebooks/induced-polarization/index.md children: - - file: notebooks/06-ip/fwd_ip_2d.ipynb - - file: notebooks/06-ip/fwd_ip_3d.ipynb - - file: notebooks/06-ip/inv_ip_2d.ipynb - - file: notebooks/06-ip/inv_ip_3d.ipynb - - file: notebooks/fdem_index.md + - file: notebooks/induced-polarization/fwd_ip_2d.ipynb + - file: notebooks/induced-polarization/fwd_ip_3d.ipynb + - file: notebooks/induced-polarization/inv_ip_2d.ipynb + - file: notebooks/induced-polarization/inv_ip_3d.ipynb + - file: notebooks/frequency-domain-em/index.md children: - - file: notebooks/07-fdem/fwd_fdem_1d.ipynb - - file: notebooks/07-fdem/inv_fdem_1d.ipynb - - file: notebooks/tdem_index.md + - file: notebooks/frequency-domain-em/fwd_fdem_1d.ipynb + - file: notebooks/frequency-domain-em/inv_fdem_1d.ipynb + - file: notebooks/time-domain-em/index.md children: - - file: notebooks/08-tdem/fwd_tdem_1d.ipynb - - file: notebooks/08-tdem/fwd_tdem_fundamentals.ipynb - - file: notebooks/08-tdem/fwd_utem_3d.ipynb - - file: notebooks/08-tdem/inv_tdem_1d.ipynb + - file: notebooks/time-domain-em/fwd_tdem_1d.ipynb + - file: notebooks/time-domain-em/fwd_tdem_fundamentals.ipynb + - file: notebooks/time-domain-em/fwd_utem_3d.ipynb + - file: notebooks/time-domain-em/inv_tdem_1d.ipynb - title: Joint Inversion children: - - file: notebooks/11-joint-inversion/plot_inv_3_cross_gradient_pf.ipynb + - file: notebooks/joint-inversion/plot_inv_3_cross_gradient_pf.ipynb - title: PGI Inversion children: - - file: notebooks/12-pgi-inversion/plot_inv_1_joint_pf_pgi_full_info_tutorial.ipynb - - file: notebooks/12-pgi-inversion/plot_inv_2_joint_pf_pgi_no_info_tutorial.ipynb + - file: notebooks/pgi/plot_inv_1_joint_pf_pgi_full_info_tutorial.ipynb + - file: notebooks/pgi/plot_inv_2_joint_pf_pgi_no_info_tutorial.ipynb site: template: book-theme diff --git a/notebooks/05-dcr/inv_dcr_3d_files/dc_data.xyz b/notebooks/05-dcr/inv_dcr_3d_files/dc_data.xyz deleted file mode 100755 index 88d8948..0000000 --- a/notebooks/05-dcr/inv_dcr_3d_files/dc_data.xyz +++ /dev/null @@ -1,697 +0,0 @@ -XA YA ZA XB YB ZB XM YM ZM XN YN ZN V/A UNCERT 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3.00000000e+02 3.95244766e+02 -6.00000000e+02 4.00000000e+02 3.97322571e+02 -6.00000000e+02 5.00000000e+02 3.98912707e+02 -5.25403218e-02 5.63404675e-03 2.00000000e+00 --6.00000000e+02 2.00000000e+02 3.92474965e+02 -6.00000000e+02 3.00000000e+02 3.95244766e+02 -6.00000000e+02 5.00000000e+02 3.98912707e+02 -6.00000000e+02 6.00000000e+02 4.00139729e+02 -1.27926443e-02 1.48528840e-03 2.00000000e+00 --6.00000000e+02 2.00000000e+02 3.92474965e+02 -6.00000000e+02 3.00000000e+02 3.95244766e+02 -6.00000000e+02 6.00000000e+02 4.00139729e+02 -6.00000000e+02 7.00000000e+02 4.01084774e+02 -5.92794633e-03 5.95114047e-04 2.00000000e+00 --6.00000000e+02 2.00000000e+02 3.92474965e+02 -6.00000000e+02 3.00000000e+02 3.95244766e+02 -6.00000000e+02 7.00000000e+02 4.01084774e+02 -6.00000000e+02 8.00000000e+02 4.01818963e+02 -2.94526650e-03 3.48943521e-04 2.00000000e+00 --6.00000000e+02 2.00000000e+02 3.92474965e+02 -6.00000000e+02 3.00000000e+02 3.95244766e+02 -6.00000000e+02 8.00000000e+02 4.01818963e+02 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--3.00000000e+02 -1.00000000e+03 3.15640211e+02 -3.00000000e+02 -9.00000000e+02 3.14162039e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -8.87423231e-04 9.89429859e-05 3.00000000e+00 --3.00000000e+02 -1.00000000e+03 3.15640211e+02 -3.00000000e+02 -9.00000000e+02 3.14162039e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -6.11792910e-04 5.92382859e-05 3.00000000e+00 --3.00000000e+02 -1.00000000e+03 3.15640211e+02 -3.00000000e+02 -9.00000000e+02 3.14162039e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -2.44814719e-04 2.59640737e-05 3.00000000e+00 --3.00000000e+02 -9.00000000e+02 3.14162039e+02 -3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 -6.00000000e+02 3.11348012e+02 -4.60072304e-02 5.73135980e-03 3.00000000e+00 --3.00000000e+02 -9.00000000e+02 3.14162039e+02 -3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 -5.00000000e+02 3.11538687e+02 -1.25210673e-02 1.35279621e-03 3.00000000e+00 --3.00000000e+02 -9.00000000e+02 3.14162039e+02 -3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 -4.00000000e+02 3.12589787e+02 -5.62018294e-03 5.34936199e-04 3.00000000e+00 --3.00000000e+02 -9.00000000e+02 3.14162039e+02 -3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -2.51407693e-03 2.69331191e-04 3.00000000e+00 --3.00000000e+02 -9.00000000e+02 3.14162039e+02 -3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -1.58234811e-03 1.59280108e-04 3.00000000e+00 --3.00000000e+02 -9.00000000e+02 3.14162039e+02 -3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -7.62022165e-04 9.00665063e-05 3.00000000e+00 --3.00000000e+02 -9.00000000e+02 3.14162039e+02 -3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.75715288e-04 3.80504576e-05 3.00000000e+00 --3.00000000e+02 -9.00000000e+02 3.14162039e+02 -3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -2.21743502e-04 2.13999589e-05 3.00000000e+00 --3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 -5.00000000e+02 3.11538687e+02 -6.24593096e-02 5.73899611e-03 3.00000000e+00 --3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 -4.00000000e+02 3.12589787e+02 -1.66700727e-02 1.36107502e-03 3.00000000e+00 --3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -4.82249098e-03 5.42519059e-04 3.00000000e+00 --3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -2.38050111e-03 2.79219900e-04 3.00000000e+00 --3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -1.41947823e-03 1.45667265e-04 3.00000000e+00 --3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -6.21748902e-04 5.86682426e-05 3.00000000e+00 --3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.12718473e-04 3.04740335e-05 3.00000000e+00 --3.00000000e+02 -8.00000000e+02 3.12837092e+02 -3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.19201590e-04 3.27754274e-05 3.00000000e+00 --3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 -4.00000000e+02 3.12589787e+02 -6.96302479e-02 5.74762159e-03 3.00000000e+00 --3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -1.36092477e-02 1.37056879e-03 3.00000000e+00 --3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -5.78858108e-03 5.56654684e-04 3.00000000e+00 --3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -2.84502066e-03 2.56409951e-04 3.00000000e+00 --3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -8.46294055e-04 9.67679749e-05 3.00000000e+00 --3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.75663603e-04 4.54277486e-05 3.00000000e+00 --3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -4.25283099e-04 4.55038730e-05 3.00000000e+00 --3.00000000e+02 -7.00000000e+02 3.11844034e+02 -3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -3.19877900e-04 3.91190180e-05 3.00000000e+00 --3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -5.59129188e-02 5.76733117e-03 3.00000000e+00 --3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -1.53779782e-02 1.39184883e-03 3.00000000e+00 --3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -4.87614071e-03 5.13341405e-04 3.00000000e+00 --3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -2.00201922e-03 1.75768306e-04 3.00000000e+00 --3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -7.09825173e-04 7.21724146e-05 3.00000000e+00 --3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -7.53288484e-04 6.53387176e-05 3.00000000e+00 --3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -5.18467047e-04 5.43990959e-05 3.00000000e+00 --3.00000000e+02 -6.00000000e+02 3.11348012e+02 -3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -3.00000000e+02 4.00000000e+02 3.73126500e+02 -4.35158910e-04 4.44542008e-05 3.00000000e+00 --3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -6.01503632e-02 5.80863838e-03 3.00000000e+00 --3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -1.21602761e-02 1.28585537e-03 3.00000000e+00 --3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.62990620e-03 3.71022531e-04 3.00000000e+00 --3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -1.20225959e-03 1.26406347e-04 3.00000000e+00 --3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -9.97787361e-04 9.79458974e-05 3.00000000e+00 --3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -9.33763501e-04 7.78481348e-05 3.00000000e+00 --3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -3.00000000e+02 4.00000000e+02 3.73126500e+02 -5.74207018e-04 6.18439320e-05 3.00000000e+00 --3.00000000e+02 -5.00000000e+02 3.11538687e+02 -3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 4.00000000e+02 3.73126500e+02 -3.00000000e+02 5.00000000e+02 3.79953392e+02 -4.57049885e-04 4.30551140e-05 3.00000000e+00 --3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -5.55945688e-02 5.34902940e-03 3.00000000e+00 --3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -9.52932770e-03 1.01994554e-03 3.00000000e+00 --3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -2.28426133e-03 2.63149846e-04 3.00000000e+00 --3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -1.67177807e-03 1.56198333e-04 3.00000000e+00 --3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -1.09400836e-03 1.14913664e-04 3.00000000e+00 --3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -3.00000000e+02 4.00000000e+02 3.73126500e+02 -9.42235609e-04 8.76476585e-05 3.00000000e+00 --3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 4.00000000e+02 3.73126500e+02 -3.00000000e+02 5.00000000e+02 3.79953392e+02 -6.17294435e-04 5.93530341e-05 3.00000000e+00 --3.00000000e+02 -4.00000000e+02 3.12589787e+02 -3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 5.00000000e+02 3.79953392e+02 -3.00000000e+02 6.00000000e+02 3.84967899e+02 -5.04675100e-04 4.59618750e-05 3.00000000e+00 --3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -6.00561398e-02 5.23497482e-03 3.00000000e+00 --3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -8.02754345e-03 8.21581473e-04 3.00000000e+00 --3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.22020240e-03 2.87155516e-04 3.00000000e+00 --3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -1.65181305e-03 1.78168452e-04 3.00000000e+00 --3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -3.00000000e+02 4.00000000e+02 3.73126500e+02 -1.25625808e-03 1.25842453e-04 3.00000000e+00 --3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 4.00000000e+02 3.73126500e+02 -3.00000000e+02 5.00000000e+02 3.79953392e+02 -9.11857985e-04 8.19826183e-05 3.00000000e+00 --3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 5.00000000e+02 3.79953392e+02 -3.00000000e+02 6.00000000e+02 3.84967899e+02 -6.09365007e-04 6.16654565e-05 3.00000000e+00 --3.00000000e+02 -3.00000000e+02 3.14745724e+02 -3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 6.00000000e+02 3.84967899e+02 -3.00000000e+02 7.00000000e+02 3.88588066e+02 -4.88064475e-04 4.60557726e-05 3.00000000e+00 --3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -5.30138171e-02 5.29217221e-03 3.00000000e+00 --3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -6.96020731e-03 7.29770517e-04 3.00000000e+00 --3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -3.02523401e-03 2.83527645e-04 3.00000000e+00 --3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -3.00000000e+02 4.00000000e+02 3.73126500e+02 -1.56186651e-03 1.62731857e-04 3.00000000e+00 --3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 4.00000000e+02 3.73126500e+02 -3.00000000e+02 5.00000000e+02 3.79953392e+02 -9.82491294e-04 9.68499145e-05 3.00000000e+00 --3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 5.00000000e+02 3.79953392e+02 -3.00000000e+02 6.00000000e+02 3.84967899e+02 -7.12427282e-04 6.87081265e-05 3.00000000e+00 --3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 6.00000000e+02 3.84967899e+02 -3.00000000e+02 7.00000000e+02 3.88588066e+02 -4.72810703e-04 4.92647189e-05 3.00000000e+00 --3.00000000e+02 -2.00000000e+02 3.18392787e+02 -3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 7.00000000e+02 3.88588066e+02 -3.00000000e+02 8.00000000e+02 3.91233522e+02 -3.79417513e-04 4.35281495e-05 3.00000000e+00 --3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.44658813e-02 3.93260013e-03 3.00000000e+00 --3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -7.87960403e-03 7.25557080e-04 3.00000000e+00 --3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -3.00000000e+02 4.00000000e+02 3.73126500e+02 -3.09020153e-03 2.66117892e-04 3.00000000e+00 --3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 4.00000000e+02 3.73126500e+02 -3.00000000e+02 5.00000000e+02 3.79953392e+02 -9.25016051e-04 1.25031328e-04 3.00000000e+00 --3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 5.00000000e+02 3.79953392e+02 -3.00000000e+02 6.00000000e+02 3.84967899e+02 -6.75743194e-04 7.60939990e-05 3.00000000e+00 --3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 6.00000000e+02 3.84967899e+02 -3.00000000e+02 7.00000000e+02 3.88588066e+02 -5.02100018e-04 4.89835306e-05 3.00000000e+00 --3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 7.00000000e+02 3.88588066e+02 -3.00000000e+02 8.00000000e+02 3.91233522e+02 -4.00965145e-04 3.97407969e-05 3.00000000e+00 --3.00000000e+02 -1.00000000e+02 3.23924204e+02 -3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 8.00000000e+02 3.91233522e+02 -3.00000000e+02 9.00000000e+02 3.93167437e+02 -1.74880714e-04 1.68295683e-05 3.00000000e+00 --3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -4.87576472e-02 5.16191440e-03 3.00000000e+00 --3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -3.00000000e+02 4.00000000e+02 3.73126500e+02 -1.18917825e-02 1.16470323e-03 3.00000000e+00 --3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 4.00000000e+02 3.73126500e+02 -3.00000000e+02 5.00000000e+02 3.79953392e+02 -4.75138756e-03 4.24924109e-04 3.00000000e+00 --3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 5.00000000e+02 3.79953392e+02 -3.00000000e+02 6.00000000e+02 3.84967899e+02 -1.82058082e-03 2.16665709e-04 3.00000000e+00 --3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 6.00000000e+02 3.84967899e+02 -3.00000000e+02 7.00000000e+02 3.88588066e+02 -1.25365513e-03 1.21911062e-04 3.00000000e+00 --3.00000000e+02 0.00000000e+00 3.31740268e+02 -3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 7.00000000e+02 3.88588066e+02 -3.00000000e+02 8.00000000e+02 3.91233522e+02 -7.71861413e-04 8.82092309e-05 3.00000000e+00 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2.00000000e+02 3.53272678e+02 -3.00000000e+02 5.00000000e+02 3.79953392e+02 -3.00000000e+02 6.00000000e+02 3.84967899e+02 -7.25730843e-03 6.21506628e-04 3.00000000e+00 --3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.00000000e+02 6.00000000e+02 3.84967899e+02 -3.00000000e+02 7.00000000e+02 3.88588066e+02 -3.03077046e-03 3.15719278e-04 3.00000000e+00 --3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.00000000e+02 7.00000000e+02 3.88588066e+02 -3.00000000e+02 8.00000000e+02 3.91233522e+02 -2.36293014e-03 2.11836681e-04 3.00000000e+00 --3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.00000000e+02 8.00000000e+02 3.91233522e+02 -3.00000000e+02 9.00000000e+02 3.93167437e+02 -8.24236009e-04 7.81872969e-05 3.00000000e+00 --3.00000000e+02 1.00000000e+02 3.41884509e+02 -3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.00000000e+02 9.00000000e+02 3.93167437e+02 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3.00000000e+00 --3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -3.00000000e+02 8.00000000e+02 3.91233522e+02 -3.00000000e+02 9.00000000e+02 3.93167437e+02 -1.24980055e-03 1.18274411e-04 3.00000000e+00 --3.00000000e+02 2.00000000e+02 3.53272678e+02 -3.00000000e+02 3.00000000e+02 3.64155509e+02 -3.00000000e+02 9.00000000e+02 3.93167437e+02 -3.00000000e+02 1.00000000e+03 3.94557840e+02 -1.10676649e-03 1.04972350e-04 3.00000000e+00 --3.00000000e+02 3.00000000e+02 3.64155509e+02 -3.00000000e+02 4.00000000e+02 3.73126500e+02 -3.00000000e+02 5.00000000e+02 3.79953392e+02 -3.00000000e+02 6.00000000e+02 3.84967899e+02 -7.95393601e-02 7.15657046e-03 3.00000000e+00 --3.00000000e+02 3.00000000e+02 3.64155509e+02 -3.00000000e+02 4.00000000e+02 3.73126500e+02 -3.00000000e+02 6.00000000e+02 3.84967899e+02 -3.00000000e+02 7.00000000e+02 3.88588066e+02 -1.52307187e-02 1.63308214e-03 3.00000000e+00 --3.00000000e+02 3.00000000e+02 3.64155509e+02 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3.88588066e+02 -3.00000000e+02 8.00000000e+02 3.91233522e+02 -1.26898469e-02 1.57097199e-03 3.00000000e+00 --3.00000000e+02 4.00000000e+02 3.73126500e+02 -3.00000000e+02 5.00000000e+02 3.79953392e+02 -3.00000000e+02 8.00000000e+02 3.91233522e+02 -3.00000000e+02 9.00000000e+02 3.93167437e+02 -3.21161064e-03 3.64248348e-04 3.00000000e+00 --3.00000000e+02 4.00000000e+02 3.73126500e+02 -3.00000000e+02 5.00000000e+02 3.79953392e+02 -3.00000000e+02 9.00000000e+02 3.93167437e+02 -3.00000000e+02 1.00000000e+03 3.94557840e+02 -2.28392227e-03 2.66688888e-04 3.00000000e+00 --3.00000000e+02 5.00000000e+02 3.79953392e+02 -3.00000000e+02 6.00000000e+02 3.84967899e+02 -3.00000000e+02 7.00000000e+02 3.88588066e+02 -3.00000000e+02 8.00000000e+02 3.91233522e+02 -5.32912628e-02 6.21620006e-03 3.00000000e+00 --3.00000000e+02 5.00000000e+02 3.79953392e+02 -3.00000000e+02 6.00000000e+02 3.84967899e+02 -3.00000000e+02 8.00000000e+02 3.91233522e+02 -3.00000000e+02 9.00000000e+02 3.93167437e+02 -9.20618685e-03 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5.00000000e+02 3.37667798e+02 6.00000000e+02 6.00000000e+02 3.29896799e+02 6.00000000e+02 9.00000000e+02 3.17421099e+02 6.00000000e+02 1.00000000e+03 3.15588071e+02 -4.62307062e-03 5.08408859e-04 6.00000000e+00 -6.00000000e+02 6.00000000e+02 3.29896799e+02 6.00000000e+02 7.00000000e+02 3.24208682e+02 6.00000000e+02 8.00000000e+02 3.20186714e+02 6.00000000e+02 9.00000000e+02 3.17421099e+02 -5.13188029e-02 5.27663333e-03 6.00000000e+00 -6.00000000e+02 6.00000000e+02 3.29896799e+02 6.00000000e+02 7.00000000e+02 3.24208682e+02 6.00000000e+02 9.00000000e+02 3.17421099e+02 6.00000000e+02 1.00000000e+03 3.15588071e+02 -1.25326958e-02 1.22059014e-03 6.00000000e+00 -6.00000000e+02 7.00000000e+02 3.24208682e+02 6.00000000e+02 8.00000000e+02 3.20186714e+02 6.00000000e+02 9.00000000e+02 3.17421099e+02 6.00000000e+02 1.00000000e+03 3.15588071e+02 -4.89061210e-02 5.05536867e-03 6.00000000e+00 diff --git a/notebooks/05-dcr/fwd_dcr_1d.ipynb b/notebooks/dc-resistivity/fwd_dcr_1d.ipynb similarity index 100% rename from notebooks/05-dcr/fwd_dcr_1d.ipynb rename to notebooks/dc-resistivity/fwd_dcr_1d.ipynb diff --git a/notebooks/05-dcr/fwd_dcr_2d.ipynb b/notebooks/dc-resistivity/fwd_dcr_2d.ipynb similarity index 100% rename from notebooks/05-dcr/fwd_dcr_2d.ipynb rename to notebooks/dc-resistivity/fwd_dcr_2d.ipynb diff --git a/notebooks/05-dcr/fwd_dcr_3d.ipynb b/notebooks/dc-resistivity/fwd_dcr_3d.ipynb similarity index 100% rename from notebooks/05-dcr/fwd_dcr_3d.ipynb rename to notebooks/dc-resistivity/fwd_dcr_3d.ipynb diff --git a/notebooks/dc-resistivity/index.md b/notebooks/dc-resistivity/index.md new file mode 100644 index 0000000..0448b61 --- /dev/null +++ b/notebooks/dc-resistivity/index.md @@ -0,0 +1,33 @@ +Direct Current Resistivity +====================== + +Direct current resistivity data are simulated using functionality within the ``SimPEG.electromagnetics.static.resistivity`` module. Here, we provide a multitude of introductory and indermediate level tutorials for forward simulation and inversion of direct current resistivity data. Links to each tutorial can be accessed below or from the left-side menu. + +```{figure} ../../assets/website_images/dcip_physics.png +:width: 800px +:align: center + +Schematic illustrating the physics of the DC/IP method ([image source](https://em.geosci.xyz/content/geophysical_surveys/ip/physics.html)) +``` + +## Tutorial Notebooks + + +[1D Forward Simulation for a Single Sounding](dc-resistivity/fwd_dcr_1d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$ +
+ +[2.5D Forward Simulation](dc-resistivity/fwd_dcr_2d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$ +
+ +[3D Forward Simulation](dc-resistivity/fwd_dcr_3d) $({\color{orange}Intermediate}$, ${\color{orange}Moderate})$ +
+ +[1D Inversion for a Single Sounding](dc-resistivity/inv_dcr_1d) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$ +
+ +[2.5D DC Resistivity Inversion](dc-resistivity/inv_dcr_2d) $({\color{orange}Intermediate}$, ${\color{orange}Moderate})$ +
+ +[3D DC Resistivity Inversion](dc-resistivity/inv_dcr_3d) $({\color{orange}Intermediate}$, ${\color{orange}Moderate})$ +
+ diff --git a/notebooks/05-dcr/inv_dcr_1d.ipynb b/notebooks/dc-resistivity/inv_dcr_1d.ipynb similarity index 99% rename from notebooks/05-dcr/inv_dcr_1d.ipynb rename to notebooks/dc-resistivity/inv_dcr_1d.ipynb index c8d0b19..ad9ab3f 100644 --- a/notebooks/05-dcr/inv_dcr_1d.ipynb +++ b/notebooks/dc-resistivity/inv_dcr_1d.ipynb @@ -135,22 +135,22 @@ "name": "stdout", "output_type": "stream", "text": [ - "overwriting /home/ssoler/git/user-tutorials/notebooks/05-dcr/inv_dcr_1d_files.tar.gz\n", - "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/05-dcr/inv_dcr_1d_files.tar.gz\n" + "overwriting /home/ssoler/git/user-tutorials/notebooks/dc-resistivity/inv_dcr_1d_files.tar.gz\n", + "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/dc-resistivity/inv_dcr_1d_files.tar.gz\n" ] }, { "name": "stdout", "output_type": "stream", "text": [ - " saved to: /home/ssoler/git/user-tutorials/notebooks/05-dcr/inv_dcr_1d_files.tar.gz\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/dc-resistivity/inv_dcr_1d_files.tar.gz\n", "Download completed!\n" ] } ], "source": [ "# URL to download from repository assets\n", - "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/05-dcr/inv_dcr_1d_files.tar.gz\"\n", + "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/dc-resistivity/inv_dcr_1d_files.tar.gz\"\n", "\n", "# download the data\n", "downloaded_data = download(data_source, overwrite=True)\n", diff --git a/notebooks/05-dcr/inv_dcr_1d_files/app_res_1d_data.dobs b/notebooks/dc-resistivity/inv_dcr_1d_files/app_res_1d_data.dobs similarity index 100% rename from notebooks/05-dcr/inv_dcr_1d_files/app_res_1d_data.dobs rename to notebooks/dc-resistivity/inv_dcr_1d_files/app_res_1d_data.dobs diff --git a/notebooks/05-dcr/inv_dcr_2d.ipynb b/notebooks/dc-resistivity/inv_dcr_2d.ipynb similarity index 99% rename from notebooks/05-dcr/inv_dcr_2d.ipynb rename to notebooks/dc-resistivity/inv_dcr_2d.ipynb index 36a0930..d78a071 100644 --- a/notebooks/05-dcr/inv_dcr_2d.ipynb +++ b/notebooks/dc-resistivity/inv_dcr_2d.ipynb @@ -146,22 +146,22 @@ "name": "stdout", "output_type": "stream", "text": [ - "overwriting /home/ssoler/git/user-tutorials/notebooks/05-dcr/inv_dcr_2d_files.tar.gz\n", - "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/05-dcr/inv_dcr_2d_files.tar.gz\n" + "overwriting /home/ssoler/git/user-tutorials/notebooks/dc-resistivity/inv_dcr_2d_files.tar.gz\n", + "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/dc-resistivity/inv_dcr_2d_files.tar.gz\n" ] }, { "name": "stdout", "output_type": "stream", "text": [ - " saved to: /home/ssoler/git/user-tutorials/notebooks/05-dcr/inv_dcr_2d_files.tar.gz\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/dc-resistivity/inv_dcr_2d_files.tar.gz\n", "Download completed!\n" ] } ], "source": [ "# URL to download from repository assets\n", - "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/05-dcr/inv_dcr_2d_files.tar.gz\"\n", + "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/dc-resistivity/inv_dcr_2d_files.tar.gz\"\n", "\n", "# download the data\n", "downloaded_data = download(data_source, overwrite=True)\n", diff --git a/notebooks/05-dcr/inv_dcr_3d.ipynb b/notebooks/dc-resistivity/inv_dcr_3d.ipynb similarity index 99% rename from notebooks/05-dcr/inv_dcr_3d.ipynb rename to notebooks/dc-resistivity/inv_dcr_3d.ipynb index ab619bd..890eab3 100644 --- a/notebooks/05-dcr/inv_dcr_3d.ipynb +++ b/notebooks/dc-resistivity/inv_dcr_3d.ipynb @@ -143,22 +143,22 @@ "name": "stdout", "output_type": "stream", "text": [ - "overwriting /home/ssoler/git/user-tutorials/notebooks/05-dcr/inv_dcr_3d_files.tar.gz\n", - "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/05-dcr/inv_dcr_3d_files.tar.gz\n" + "overwriting /home/ssoler/git/user-tutorials/notebooks/dc-resistivity/inv_dcr_3d_files.tar.gz\n", + "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/dc-resistivity/inv_dcr_3d_files.tar.gz\n" ] }, { "name": "stdout", "output_type": "stream", "text": [ - " saved to: /home/ssoler/git/user-tutorials/notebooks/05-dcr/inv_dcr_3d_files.tar.gz\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/dc-resistivity/inv_dcr_3d_files.tar.gz\n", "Download completed!\n" ] } ], "source": [ "# URL to download from repository assets\n", - "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/05-dcr/inv_dcr_3d_files.tar.gz\"\n", + "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/dc-resistivity/inv_dcr_3d_files.tar.gz\"\n", "\n", "# download the data\n", "downloaded_data = download(data_source, overwrite=True)\n", diff --git a/notebooks/dcr_index.md b/notebooks/dcr_index.md deleted file mode 100644 index 4af9b1d..0000000 --- a/notebooks/dcr_index.md +++ /dev/null @@ -1,33 +0,0 @@ -Direct Current Resistivity -====================== - -Direct current resistivity data are simulated using functionality within the ``SimPEG.electromagnetics.static.resistivity`` module. Here, we provide a multitude of introductory and indermediate level tutorials for forward simulation and inversion of direct current resistivity data. Links to each tutorial can be accessed below or from the left-side menu. - -```{figure} ../assets/website_images/dcip_physics.png -:width: 800px -:align: center - -Schematic illustrating the physics of the DC/IP method ([image source](https://em.geosci.xyz/content/geophysical_surveys/ip/physics.html)) -``` - -## Tutorial Notebooks - - -[1D Forward Simulation for a Single Sounding](05-dcr/fwd_dcr_1d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$ -
- -[2.5D Forward Simulation](05-dcr/fwd_dcr_2d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$ -
- -[3D Forward Simulation](05-dcr/fwd_dcr_3d) $({\color{orange}Intermediate}$, ${\color{orange}Moderate})$ -
- -[1D Inversion for a Single Sounding](05-dcr/inv_dcr_1d) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$ -
- -[2.5D DC Resistivity Inversion](05-dcr/inv_dcr_2d) $({\color{orange}Intermediate}$, ${\color{orange}Moderate})$ -
- -[3D DC Resistivity Inversion](05-dcr/inv_dcr_3d) $({\color{orange}Intermediate}$, ${\color{orange}Moderate})$ -
- diff --git a/notebooks/07-fdem/fwd_fdem_1d.ipynb b/notebooks/frequency-domain-em/fwd_fdem_1d.ipynb similarity index 100% rename from notebooks/07-fdem/fwd_fdem_1d.ipynb rename to notebooks/frequency-domain-em/fwd_fdem_1d.ipynb diff --git a/notebooks/07-fdem/fwd_fdem_3d.ipynb b/notebooks/frequency-domain-em/fwd_fdem_3d.ipynb similarity index 100% rename from notebooks/07-fdem/fwd_fdem_3d.ipynb rename to notebooks/frequency-domain-em/fwd_fdem_3d.ipynb diff --git a/notebooks/07-fdem/fwd_fdem_cyl.ipynb b/notebooks/frequency-domain-em/fwd_fdem_cyl.ipynb similarity index 100% rename from notebooks/07-fdem/fwd_fdem_cyl.ipynb rename to notebooks/frequency-domain-em/fwd_fdem_cyl.ipynb diff --git a/notebooks/fdem_index.md b/notebooks/frequency-domain-em/index.md similarity index 57% rename from notebooks/fdem_index.md rename to notebooks/frequency-domain-em/index.md index 71e7000..5eaf5ac 100644 --- a/notebooks/fdem_index.md +++ b/notebooks/frequency-domain-em/index.md @@ -4,7 +4,7 @@ Frequency-Domain Electromagnetics In this chapter, we publish code comparisons and validations for frequency-domain electromagnetic modeling packages. In SimPEG, the *SimPEG.electromagnetics.frequency_domain* module is used for modeling frequency-domain data. -```{figure} ../assets/website_images/fem_physics.png +```{figure} ../../assets/website_images/fem_physics.png :width: 800px :align: center @@ -13,8 +13,8 @@ Schematic illustrating the physics of the FEM method for an inductive source. ## Tutorial Notebooks -[1D Forward Simulation for a Single Sounding](07-fdem/fwd_fdem_1d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$ +[1D Forward Simulation for a Single Sounding](frequency-domain-em/fwd_fdem_1d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$
-[1D Inversion for a Single Sounding](07-fdem/inv_fdem_1d) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$ +[1D Inversion for a Single Sounding](frequency-domain-em/inv_fdem_1d) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$
diff --git a/notebooks/07-fdem/inv_fdem_1d.ipynb b/notebooks/frequency-domain-em/inv_fdem_1d.ipynb similarity index 99% rename from notebooks/07-fdem/inv_fdem_1d.ipynb rename to notebooks/frequency-domain-em/inv_fdem_1d.ipynb index e2158e6..4e4b911 100644 --- a/notebooks/07-fdem/inv_fdem_1d.ipynb +++ b/notebooks/frequency-domain-em/inv_fdem_1d.ipynb @@ -132,22 +132,22 @@ "name": "stdout", "output_type": "stream", "text": [ - "overwriting /home/ssoler/git/user-tutorials/notebooks/07-fdem/inv_fdem_1d_files.tar.gz\n", - "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/07-fdem/inv_fdem_1d_files.tar.gz\n" + "overwriting /home/ssoler/git/user-tutorials/notebooks/frequency-domain-em/inv_fdem_1d_files.tar.gz\n", + "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/frequency-domain-em/inv_fdem_1d_files.tar.gz\n" ] }, { "name": "stdout", "output_type": "stream", "text": [ - " saved to: /home/ssoler/git/user-tutorials/notebooks/07-fdem/inv_fdem_1d_files.tar.gz\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/frequency-domain-em/inv_fdem_1d_files.tar.gz\n", "Download completed!\n" ] } ], "source": [ "# URL to assets\n", - "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/07-fdem/inv_fdem_1d_files.tar.gz\"\n", + "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/frequency-domain-em/inv_fdem_1d_files.tar.gz\"\n", "\n", "# download the data\n", "downloaded_data = download(data_source, overwrite=True)\n", diff --git a/notebooks/03-gravity/fwd_gravity_anomaly_3d.ipynb b/notebooks/gravity/fwd_gravity_anomaly_3d.ipynb similarity index 100% rename from notebooks/03-gravity/fwd_gravity_anomaly_3d.ipynb rename to notebooks/gravity/fwd_gravity_anomaly_3d.ipynb diff --git a/notebooks/03-gravity/fwd_gravity_gradiometry_3d.ipynb b/notebooks/gravity/fwd_gravity_gradiometry_3d.ipynb similarity index 100% rename from notebooks/03-gravity/fwd_gravity_gradiometry_3d.ipynb rename to notebooks/gravity/fwd_gravity_gradiometry_3d.ipynb diff --git a/notebooks/gravity_index.md b/notebooks/gravity/index.md similarity index 58% rename from notebooks/gravity_index.md rename to notebooks/gravity/index.md index 2e58383..9eaaf74 100644 --- a/notebooks/gravity_index.md +++ b/notebooks/gravity/index.md @@ -12,14 +12,14 @@ Earth's gravity anomalies ([image source](https://upload.wikimedia.org/wikipedia ## Tutorial Notebooks -[3D Forward Simulation of Gravity Anomaly Data](03-gravity/fwd_gravity_anomaly_3d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$ +[3D Forward Simulation of Gravity Anomaly Data](gravity/fwd_gravity_anomaly_3d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$
-[3D Forward Simulation of Gravity Gradiometry Data](03-gravity/fwd_gravity_gradiometry_3d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$ +[3D Forward Simulation of Gravity Gradiometry Data](gravity/fwd_gravity_gradiometry_3d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$
-[3D Inversion of Gravity Anomaly Data](03-gravity/inv_gravity_anomaly_3d) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$ +[3D Inversion of Gravity Anomaly Data](gravity/inv_gravity_anomaly_3d) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$
-[Compare weighting strategy with Inversion of surface Gravity Anomaly Data](03-gravity/weighting_strategies) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$ +[Compare weighting strategy with Inversion of surface Gravity Anomaly Data](gravity/weighting_strategies) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$
diff --git a/notebooks/03-gravity/inv_gravity_anomaly_3d.ipynb b/notebooks/gravity/inv_gravity_anomaly_3d.ipynb similarity index 99% rename from notebooks/03-gravity/inv_gravity_anomaly_3d.ipynb rename to notebooks/gravity/inv_gravity_anomaly_3d.ipynb index e439f02..546741e 100644 --- a/notebooks/03-gravity/inv_gravity_anomaly_3d.ipynb +++ b/notebooks/gravity/inv_gravity_anomaly_3d.ipynb @@ -139,22 +139,22 @@ "name": "stdout", "output_type": "stream", "text": [ - "overwriting /home/ssoler/git/user-tutorials/notebooks/03-gravity/inv_gravity_anomaly_3d_files.tar.gz\n", - "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/03-gravity/inv_gravity_anomaly_3d_files.tar.gz\n" + "overwriting /home/ssoler/git/user-tutorials/notebooks/gravity/inv_gravity_anomaly_3d_files.tar.gz\n", + "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/gravity/inv_gravity_anomaly_3d_files.tar.gz\n" ] }, { "name": "stdout", "output_type": "stream", "text": [ - " saved to: /home/ssoler/git/user-tutorials/notebooks/03-gravity/inv_gravity_anomaly_3d_files.tar.gz\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/gravity/inv_gravity_anomaly_3d_files.tar.gz\n", "Download completed!\n" ] } ], "source": [ "# URL to download from repository assets\n", - "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/03-gravity/inv_gravity_anomaly_3d_files.tar.gz\"\n", + "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/gravity/inv_gravity_anomaly_3d_files.tar.gz\"\n", "\n", "# download the data\n", "downloaded_data = download(data_source, overwrite=True)\n", diff --git a/notebooks/03-gravity/weighting_strategies.ipynb b/notebooks/gravity/weighting_strategies.ipynb similarity index 99% rename from notebooks/03-gravity/weighting_strategies.ipynb rename to notebooks/gravity/weighting_strategies.ipynb index c5f5fac..2896efc 100644 --- a/notebooks/03-gravity/weighting_strategies.ipynb +++ b/notebooks/gravity/weighting_strategies.ipynb @@ -141,9 +141,9 @@ "name": "stdout", "output_type": "stream", "text": [ - "overwriting /home/ssoler/git/user-tutorials/notebooks/03-gravity/gravity.tar.gz\n", + "overwriting /home/ssoler/git/user-tutorials/notebooks/gravity/gravity.tar.gz\n", "Downloading https://storage.googleapis.com/simpeg/doc-assets/gravity.tar.gz\n", - " saved to: /home/ssoler/git/user-tutorials/notebooks/03-gravity/gravity.tar.gz\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/gravity/gravity.tar.gz\n", "Download completed!\n" ] } diff --git a/notebooks/06-ip/fwd_ip_2d.ipynb b/notebooks/induced-polarization/fwd_ip_2d.ipynb similarity index 99% rename from notebooks/06-ip/fwd_ip_2d.ipynb rename to notebooks/induced-polarization/fwd_ip_2d.ipynb index d3e042d..5f60d16 100644 --- a/notebooks/06-ip/fwd_ip_2d.ipynb +++ b/notebooks/induced-polarization/fwd_ip_2d.ipynb @@ -41,7 +41,7 @@ "\n", "**Summary:** Here, we use the [simpeg.electromagnetics.static.induced_polarization](xref:simpeg#simpeg.electromagnetics.static.induced_polarization) module to simulate 2.5D DC induced polarization (IP) data on a tree mesh. This approach is ideal when the local geology doesn't change along the strike direction, as we can leverage the symmetry of the problem to reduce computational cost.\n", "\n", - "Because the same survey geometry, mesh and topography that are used to simulate DC resistivity data are used simulate IP data, almost all of the fundamental functionality used in this tutorial is described in detail in the [2.5D Forward Simulation of DC Resistivity Data](../05-dcr/fwd_dcr_2d.ipynb) tutorial. In this tutorial, we focus primarily on functionality related to the simulation of IP data. More specifically, we discuss:\n", + "Because the same survey geometry, mesh and topography that are used to simulate DC resistivity data are used simulate IP data, almost all of the fundamental functionality used in this tutorial is described in detail in the [2.5D Forward Simulation of DC Resistivity Data](../dc-resistivity/fwd_dcr_2d.ipynb) tutorial. In this tutorial, we focus primarily on functionality related to the simulation of IP data. More specifically, we discuss:\n", "\n", "- Defining the chargeability model\n", "- How to simulate IP data\n", @@ -178,7 +178,7 @@ "source": [ "## Define the IP Survey\n", "\n", - "A full description of elements required to define DC and IP surveys was presented in the [2.5D Forward Simulation of DC Resistivity Data](../05-dcr/fwd_dcr_2d.ipynb) tutorial. Here, we take the same approach. The only difference is that our receivers are defined to measure apparent chargeabilities. Because SimPEG uses a linearized formulation for simulating IP data; see [Simulation2DCellCentered](xref:simpeg#simpeg.electromagnetics.static.induced_polarization.Simulation2DCellCentered) or [Simulation2DNodal](xref:simpeg#simpeg.electromagnetics.static.induced_polarization.Simulation2DNodal), the units of the apparent chargeability data are the same as the units chosen to represent the subsurface chargeabilities.\n", + "A full description of elements required to define DC and IP surveys was presented in the [2.5D Forward Simulation of DC Resistivity Data](../dc-resistivity/fwd_dcr_2d.ipynb) tutorial. Here, we take the same approach. The only difference is that our receivers are defined to measure apparent chargeabilities. Because SimPEG uses a linearized formulation for simulating IP data; see [Simulation2DCellCentered](xref:simpeg#simpeg.electromagnetics.static.induced_polarization.Simulation2DCellCentered) or [Simulation2DNodal](xref:simpeg#simpeg.electromagnetics.static.induced_polarization.Simulation2DNodal), the units of the apparent chargeability data are the same as the units chosen to represent the subsurface chargeabilities.\n", "\n", "The survey line is an 800 m long EW dipole-dipole line with an electrode spacing of 40 m. There is a maximum of 10 potential electrodes per current electrode." ] @@ -271,7 +271,7 @@ "source": [ "## Design a (Tree) Mesh\n", "\n", - "Here, we generate a tree mesh based on the survey geometry. The best-practice approach for generating meshes for DC/IP simulations is provided in the [2.5D Forward Simulation of DC Resistivity Data](../05-dcr/fwd_dcr_2d.ipynb) tutorial." + "Here, we generate a tree mesh based on the survey geometry. The best-practice approach for generating meshes for DC/IP simulations is provided in the [2.5D Forward Simulation of DC Resistivity Data](../dc-resistivity/fwd_dcr_2d.ipynb) tutorial." ] }, { @@ -356,7 +356,7 @@ "\n", "In order to simulate IP data, we require the background conductivity/resistivity defined on the entire mesh. You can generate this directly, or apply the appropriate mapping to a different parameterization of the conductivity/resistivity. \n", "\n", - "For the tutorial, we generate the conductivity model that was used for the [2.5D Forward Simulation of DC Resistivity Data](../05-dcr/fwd_dcr_2d.ipynb) tutorial; i.e. the electrical conductivities of all active cells. And so we must use the [simpeg.maps.InjectActiveCells](xref:simpeg#simpeg.maps.InjectActiveCells) mapping to map from the model space to the conductivities on the entire mesh." + "For the tutorial, we generate the conductivity model that was used for the [2.5D Forward Simulation of DC Resistivity Data](../dc-resistivity/fwd_dcr_2d.ipynb) tutorial; i.e. the electrical conductivities of all active cells. And so we must use the [simpeg.maps.InjectActiveCells](xref:simpeg#simpeg.maps.InjectActiveCells) mapping to map from the model space to the conductivities on the entire mesh." ] }, { @@ -617,7 +617,7 @@ "source": [ "## Project Electrodes to Discretized Topography\n", "\n", - "As explained in the [2.5D Forward Simulation of DC Resistivity Data](../05-dcr/fwd_dcr_2d.ipynb) tutorial, we use the [drape_electrodes_on_topography](xref:simpeg#simpeg.electromagnetics.static.resistivity.Survey.drape_electrodes_on_topography) method to project the electrodes to the discrete surface topography." + "As explained in the [2.5D Forward Simulation of DC Resistivity Data](../dc-resistivity/fwd_dcr_2d.ipynb) tutorial, we use the [drape_electrodes_on_topography](xref:simpeg#simpeg.electromagnetics.static.resistivity.Survey.drape_electrodes_on_topography) method to project the electrodes to the discrete surface topography." ] }, { diff --git a/notebooks/06-ip/fwd_ip_3d.ipynb b/notebooks/induced-polarization/fwd_ip_3d.ipynb similarity index 99% rename from notebooks/06-ip/fwd_ip_3d.ipynb rename to notebooks/induced-polarization/fwd_ip_3d.ipynb index 7b7d392..7c6807d 100644 --- a/notebooks/06-ip/fwd_ip_3d.ipynb +++ b/notebooks/induced-polarization/fwd_ip_3d.ipynb @@ -41,7 +41,7 @@ "\n", "**Summary:** Here, we use the [simpeg.electromagnetics.static.induced_polarization](xref:simpeg#simpeg.electromagnetics.static.induced_polarization) module to simulate 3D DC induced polarization (IP) data on a tree mesh. This approach is ideal when the local geology doesn't change along the strike direction, as we can leverage the symmetry of the problem to reduce computational cost.\n", "\n", - "Because the same survey geometry, mesh and topography that are used to simulate DC resistivity data are used simulate IP data, almost all of the fundamental functionality used in this tutorial is described in detail in the [3D Forward Simulation of DC Resistivity Data](../05-dcr/fwd_dcr_3d.ipynb) tutorial. In this tutorial, we focus primarily on functionality related to the simulation of IP data. More specifically, we discuss:\n", + "Because the same survey geometry, mesh and topography that are used to simulate DC resistivity data are used simulate IP data, almost all of the fundamental functionality used in this tutorial is described in detail in the [3D Forward Simulation of DC Resistivity Data](../dc-resistivity/fwd_dcr_3d.ipynb) tutorial. In this tutorial, we focus primarily on functionality related to the simulation of IP data. More specifically, we discuss:\n", "\n", "- Defining the chargeability model\n", "- How to simulate IP data\n", @@ -205,7 +205,7 @@ "source": [ "## Define the IP Survey\n", "\n", - "A full description of elements required to define DC and IP surveys was presented in the [3D Forward Simulation of DC Resistivity Data](../05-dcr/fwd_dcr_3d.ipynb) tutorial. Here, we take the same approach. The only difference is that our receivers are defined to measure apparent chargeabilities. Because SimPEG uses a linearized formulation for simulating IP data; see [Simulation3DCellCentered](xref:simpeg#simpeg.electromagnetics.static.induced_polarization.Simulation3DCellCentered) or [Simulation3DNodal](xref:simpeg#simpeg.electromagnetics.static.induced_polarization.Simulation3DNodal), the units of the apparent chargeability data are the same as the units chosen to represent the subsurface chargeabilities..\n", + "A full description of elements required to define DC and IP surveys was presented in the [3D Forward Simulation of DC Resistivity Data](../dc-resistivity/fwd_dcr_3d.ipynb) tutorial. Here, we take the same approach. The only difference is that our receivers are defined to measure apparent chargeabilities. Because SimPEG uses a linearized formulation for simulating IP data; see [Simulation3DCellCentered](xref:simpeg#simpeg.electromagnetics.static.induced_polarization.Simulation3DCellCentered) or [Simulation3DNodal](xref:simpeg#simpeg.electromagnetics.static.induced_polarization.Simulation3DNodal), the units of the apparent chargeability data are the same as the units chosen to represent the subsurface chargeabilities..\n", "\n", "Here, the survey consists of 5 IP lines that use a dipole-dipole electrode configuration; 1 line along the East-West direction and 2 lines along the North-South direction. Each line is 2000 m in length and has an electrode spacing of 100 m." ] @@ -316,7 +316,7 @@ "source": [ "## Design a (Tree) Mesh\n", "\n", - "Here, we generate a tree mesh based on the survey geometry. We use the same mesh that was generated for the [3D Forward Simulation of DC Resistivity Data](../05-dcr/fwd_dcr_3d.ipynb) tutorial. The best-practices for generating meshes for DC/IP simulations is presented in the [2.5D Forward Simulation of DC Resistivity Data](../05-dcr/fwd_dcr_2d.ipynb) tutorial." + "Here, we generate a tree mesh based on the survey geometry. We use the same mesh that was generated for the [3D Forward Simulation of DC Resistivity Data](../dc-resistivity/fwd_dcr_3d.ipynb) tutorial. The best-practices for generating meshes for DC/IP simulations is presented in the [2.5D Forward Simulation of DC Resistivity Data](../dc-resistivity/fwd_dcr_2d.ipynb) tutorial." ] }, { @@ -398,7 +398,7 @@ "source": [ "## Define the Background Conductivity/Resistivity\n", "\n", - "In order to simulate IP data, we require the background conductivity/resistivity defined on the entire mesh. You can generate this directly, or apply the appropriate mapping to different parameterization of the conductivity/resistivity. Here, we generate the same conuductivity model that was used for the [3D Forward Simulation of DC Resistivity Data](../05-dcr/fwd_dcr_3d.ipynb) tutorial." + "In order to simulate IP data, we require the background conductivity/resistivity defined on the entire mesh. You can generate this directly, or apply the appropriate mapping to different parameterization of the conductivity/resistivity. Here, we generate the same conuductivity model that was used for the [3D Forward Simulation of DC Resistivity Data](../dc-resistivity/fwd_dcr_3d.ipynb) tutorial." ] }, { @@ -669,7 +669,7 @@ "source": [ "## Project Electrodes to Discretized Topography\n", "\n", - "As explained in the [3D Forward Simulation of DC Resistivity Data](../05-dcr/fwd_dcr_3d.ipynb) tutorial, we use the [drape_electrodes_on_topography](xref:simpeg#simpeg.electromagnetics.static.resistivity.Survey.drape_electrodes_on_topography) method to project the electrodes to the discrete surface topography." + "As explained in the [3D Forward Simulation of DC Resistivity Data](../dc-resistivity/fwd_dcr_3d.ipynb) tutorial, we use the [drape_electrodes_on_topography](xref:simpeg#simpeg.electromagnetics.static.resistivity.Survey.drape_electrodes_on_topography) method to project the electrodes to the discrete surface topography." ] }, { @@ -875,7 +875,7 @@ "source": [ "### Plot Individual Lines in 2D Pseudosection\n", "\n", - "For conventional DC resistivity surveys, the electrodes are located along a set of survey lines. If we know which the survey line associated with each datum, we can parse the 3D survey into a set of 2D survey lines. Then we can plot individual pseudosections for each survey line. This was detailed in the [3D Forward Simulation of DC Resistivity Data](../05-dcr/fwd_dcr_3d.ipynb) tutorial. Here, we have 6 survey lines, each of which has the same number of data. So assigning a line ID to each datum is easy. You may need to do something more sophisticated in other cases." + "For conventional DC resistivity surveys, the electrodes are located along a set of survey lines. If we know which the survey line associated with each datum, we can parse the 3D survey into a set of 2D survey lines. Then we can plot individual pseudosections for each survey line. This was detailed in the [3D Forward Simulation of DC Resistivity Data](../dc-resistivity/fwd_dcr_3d.ipynb) tutorial. Here, we have 6 survey lines, each of which has the same number of data. So assigning a line ID to each datum is easy. You may need to do something more sophisticated in other cases." ] }, { diff --git a/notebooks/ip_index.md b/notebooks/induced-polarization/index.md similarity index 54% rename from notebooks/ip_index.md rename to notebooks/induced-polarization/index.md index c905e21..6e0292e 100644 --- a/notebooks/ip_index.md +++ b/notebooks/induced-polarization/index.md @@ -3,7 +3,7 @@ Induced Polarization Induced polarization data are simulated using functionality within the ``SimPEG.electromagnetics.static.induced_polarization`` module. Here, we provide a multitude of introductory and indermediate level tutorials for forward simulation and inversion of induced polarization data. Links to each tutorial can be accessed below or from the left-side menu. -```{figure} ../assets/website_images/dcip_physics.png +```{figure} ../../assets/website_images/dcip_physics.png :width: 800px :align: center @@ -12,14 +12,14 @@ Schematic illustrating the physics of the DC/IP method ([image source](https://e ## Tutorial Notebooks -[2.5D Forward Simulation](06-ip/fwd_ip_2d) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$ +[2.5D Forward Simulation](induced-polarization/fwd_ip_2d) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$
-[3D Forward Simulation](06-ip/fwd_ip_3d) $({\color{orange}Intermediate}$, ${\color{orange}Moderate})$ +[3D Forward Simulation](induced-polarization/fwd_ip_3d) $({\color{orange}Intermediate}$, ${\color{orange}Moderate})$
-[2.5D Inversion](06-ip/inv_ip_2d) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$ +[2.5D Inversion](induced-polarization/inv_ip_2d) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$
-[3D Inversion](06-ip/inv_ip_3d) $({\color{orange}Intermediate}$, ${\color{orange}Moderate})$ -
\ No newline at end of file +[3D Inversion](induced-polarization/inv_ip_3d) $({\color{orange}Intermediate}$, ${\color{orange}Moderate})$ +
diff --git a/notebooks/06-ip/inv_ip_2d.ipynb b/notebooks/induced-polarization/inv_ip_2d.ipynb similarity index 99% rename from notebooks/06-ip/inv_ip_2d.ipynb rename to notebooks/induced-polarization/inv_ip_2d.ipynb index f0c6855..65c6c01 100644 --- a/notebooks/06-ip/inv_ip_2d.ipynb +++ b/notebooks/induced-polarization/inv_ip_2d.ipynb @@ -138,22 +138,22 @@ "name": "stdout", "output_type": "stream", "text": [ - "overwriting /home/ssoler/git/user-tutorials/notebooks/06-ip/inv_ip_2d_files.tar.gz\n", - "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/06-ip/inv_ip_2d_files.tar.gz\n" + "overwriting /home/ssoler/git/user-tutorials/notebooks/induced-polarization/inv_ip_2d_files.tar.gz\n", + "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/induced-polarization/inv_ip_2d_files.tar.gz\n" ] }, { "name": "stdout", "output_type": "stream", "text": [ - " saved to: /home/ssoler/git/user-tutorials/notebooks/06-ip/inv_ip_2d_files.tar.gz\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/induced-polarization/inv_ip_2d_files.tar.gz\n", "Download completed!\n" ] } ], "source": [ "# URL to download from repository assets\n", - "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/06-ip/inv_ip_2d_files.tar.gz\"\n", + "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/induced-polarization/inv_ip_2d_files.tar.gz\"\n", "\n", "# download the data\n", "downloaded_data = download(data_source, overwrite=True)\n", @@ -393,7 +393,7 @@ "source": [ "## Design a (Tree) Mesh\n", "\n", - "IP inversion is carried out on the same mesh that is used for DC resistivity inversion. Here, we reproduce the survey-based meshing approach that was used in the [2.5D Inversion of DC Resistivity Data](../05-dcr/inv_dcr_2d.ipynb) tutorial. The best-practices for meshes design for DC/IP problems is provided in the [2.5D Forward Simulation of DC Resistivity Data](../05-dcr/fwd_dcr_2d.ipynb) tutorial.\n", + "IP inversion is carried out on the same mesh that is used for DC resistivity inversion. Here, we reproduce the survey-based meshing approach that was used in the [2.5D Inversion of DC Resistivity Data](../dc-resistivity/inv_dcr_2d.ipynb) tutorial. The best-practices for meshes design for DC/IP problems is provided in the [2.5D Forward Simulation of DC Resistivity Data](../dc-resistivity/fwd_dcr_2d.ipynb) tutorial.\n", "\n", "**Tutorial mesh:** Here, a minimum cell width of 4 m (or 1/10 the minimum electrode spacing) is used within our survey region. The largest electrode spacing was 400 m, so a the padding was extended at least 1200 m from the survey region. Using the [refine_surface](xref:discretize#discretize.TreeMesh.refine_surface) method, we refine the tree mesh where there is significant topography. And using the [refine_points](xref:discretize#discretize.TreeMesh.refine_points) methods, we refine based on electrodes locations. Visit the [tree mesh](xref:discretize#discretize.TreeMesh) API to see additional refinement methods." ] @@ -503,7 +503,7 @@ "source": [ "## Define the Background Conductivity/Resistivity\n", "\n", - "In order to invert IP data, we require the background conductivity/resistivity model. **In practice,** a conductivity/resistivity model is recovered by inverting DC resistivity data; see the [2.5D Inversion of DC Resistivity Data](../05-dcr/inv_dcr_2d.ipynb) tutorial. Since the conductivity/resistivity model greatly impacts the sensitivities for the IP problem, IP inversion is most successful when the recovered conductivity/resistivity model accurately characterizes the true subsurface distribution of electrical properties.\n", + "In order to invert IP data, we require the background conductivity/resistivity model. **In practice,** a conductivity/resistivity model is recovered by inverting DC resistivity data; see the [2.5D Inversion of DC Resistivity Data](../dc-resistivity/inv_dcr_2d.ipynb) tutorial. Since the conductivity/resistivity model greatly impacts the sensitivities for the IP problem, IP inversion is most successful when the recovered conductivity/resistivity model accurately characterizes the true subsurface distribution of electrical properties.\n", "\n", "**For the tutorial,** we will demonstrate the importance of using an appropriate background conductivity model for IP inversion. For our weighted least-squares inversion approach, we use a halfspace as the background conductivity model. For the iteratively re-weighted least-squares inversion approach, we use the true subsurface conductivity model. In both cases, the model is defined on the active mesh cells, and we must use the [simpeg.maps.InjectActiveCells](xref:simpeg#simpeg.maps.InjectActiveCells) mapping to map from the model space to the conductivities on the entire mesh." ] diff --git a/notebooks/06-ip/inv_ip_3d.ipynb b/notebooks/induced-polarization/inv_ip_3d.ipynb similarity index 99% rename from notebooks/06-ip/inv_ip_3d.ipynb rename to notebooks/induced-polarization/inv_ip_3d.ipynb index e280f8a..9d2c7a5 100644 --- a/notebooks/06-ip/inv_ip_3d.ipynb +++ b/notebooks/induced-polarization/inv_ip_3d.ipynb @@ -148,22 +148,22 @@ "name": "stdout", "output_type": "stream", "text": [ - "overwriting /home/ssoler/git/user-tutorials/notebooks/06-ip/inv_ip_3d_files.tar.gz\n", - "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/06-ip/inv_ip_3d_files.tar.gz\n" + "overwriting /home/ssoler/git/user-tutorials/notebooks/induced-polarization/inv_ip_3d_files.tar.gz\n", + "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/induced-polarization/inv_ip_3d_files.tar.gz\n" ] }, { "name": "stdout", "output_type": "stream", "text": [ - " saved to: /home/ssoler/git/user-tutorials/notebooks/06-ip/inv_ip_3d_files.tar.gz\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/induced-polarization/inv_ip_3d_files.tar.gz\n", "Download completed!\n" ] } ], "source": [ "# URL to download from repository assets\n", - "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/06-ip/inv_ip_3d_files.tar.gz\"\n", + "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/induced-polarization/inv_ip_3d_files.tar.gz\"\n", "\n", "# download the data\n", "downloaded_data = download(data_source, overwrite=True)\n", @@ -490,7 +490,7 @@ "source": [ "## Design a (Tree) Mesh\n", "\n", - "IP inversion is carried out on the same mesh that is used for DC resistivity inversion. Here, we reproduce the survey-based meshing approach that was used in the [3D Inversion of DC Resistivity Data](../05-dcr/inv_dcr_3d.ipynb) tutorial. The best-practices for meshes design for DC/IP problems is provided in the [2.5D Forward Simulation of DC Resistivity Data](../05-dcr/fwd_dcr_2d.ipynb) tutorial. The same rules for defining appropriate meshes for 2.5D simulations and inversion apply to 3D simulations and inversion.\n", + "IP inversion is carried out on the same mesh that is used for DC resistivity inversion. Here, we reproduce the survey-based meshing approach that was used in the [3D Inversion of DC Resistivity Data](../dc-resistivity/inv_dcr_3d.ipynb) tutorial. The best-practices for meshes design for DC/IP problems is provided in the [2.5D Forward Simulation of DC Resistivity Data](../dc-resistivity/fwd_dcr_2d.ipynb) tutorial. The same rules for defining appropriate meshes for 2.5D simulations and inversion apply to 3D simulations and inversion.\n", "\n", "**Tutorial mesh:** Here, a minimum cell width of 25 m (or 1/4 the minimum electrode spacing) is used within our survey region. The largest electrode spacing was 1000 m, so a the padding was extended at least 3000 m from the survey region. Using the [refine_surface](xref:discretize#discretize.TreeMesh.refine_surface) method, we refine the tree mesh where there is significant topography. And using the [refine_points](xref:discretize#discretize.TreeMesh.refine_points) methods, we refine based on electrodes locations. Visit the [tree mesh](xref:discretize#discretize.TreeMesh) API to see additional refinement methods." ] @@ -602,7 +602,7 @@ "source": [ "## Define the Background Conductivity/Resistivity\n", "\n", - "In order to invert IP data, we require the background conductivity/resistivity defined on the entire mesh. **In practice,** a conductivity/resistivity model is recovered via inverting DC resistivity data; see the [3D Inversion of DC Resistivity Data](../05-dcr/inv_dcr_3d.ipynb) tutorial. Since the conductivity/resistivity model greatly impacts the sensitivities for the IP problem, IP inversion is most successful when the recovered conductivity/resistivity model accurately characterizes the true subsurface distribution of electrical properties. **For the tutorial,** the true subsurface conductivity is used as the background conductivity for the IP inversion." + "In order to invert IP data, we require the background conductivity/resistivity defined on the entire mesh. **In practice,** a conductivity/resistivity model is recovered via inverting DC resistivity data; see the [3D Inversion of DC Resistivity Data](../dc-resistivity/inv_dcr_3d.ipynb) tutorial. Since the conductivity/resistivity model greatly impacts the sensitivities for the IP problem, IP inversion is most successful when the recovered conductivity/resistivity model accurately characterizes the true subsurface distribution of electrical properties. **For the tutorial,** the true subsurface conductivity is used as the background conductivity for the IP inversion." ] }, { diff --git a/notebooks/11-joint-inversion/plot_inv_3_cross_gradient_pf.ipynb b/notebooks/joint-inversion/plot_inv_3_cross_gradient_pf.ipynb similarity index 99% rename from notebooks/11-joint-inversion/plot_inv_3_cross_gradient_pf.ipynb rename to notebooks/joint-inversion/plot_inv_3_cross_gradient_pf.ipynb index ea9d8f1..8aa9c09 100644 --- a/notebooks/11-joint-inversion/plot_inv_3_cross_gradient_pf.ipynb +++ b/notebooks/joint-inversion/plot_inv_3_cross_gradient_pf.ipynb @@ -135,9 +135,9 @@ "name": "stdout", "output_type": "stream", "text": [ - "overwriting /home/ssoler/git/user-tutorials/notebooks/11-joint-inversion/cross_gradient_data.tar.gz\n", + "overwriting /home/ssoler/git/user-tutorials/notebooks/joint-inversion/cross_gradient_data.tar.gz\n", "Downloading https://storage.googleapis.com/simpeg/doc-assets/cross_gradient_data.tar.gz\n", - " saved to: /home/ssoler/git/user-tutorials/notebooks/11-joint-inversion/cross_gradient_data.tar.gz\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/joint-inversion/cross_gradient_data.tar.gz\n", "Download completed!\n" ] } diff --git a/notebooks/04-magnetics/fwd_magnetics_induced_3d.ipynb b/notebooks/magnetics/fwd_magnetics_induced_3d.ipynb similarity index 100% rename from notebooks/04-magnetics/fwd_magnetics_induced_3d.ipynb rename to notebooks/magnetics/fwd_magnetics_induced_3d.ipynb diff --git a/notebooks/04-magnetics/fwd_magnetics_mvi_3d.ipynb b/notebooks/magnetics/fwd_magnetics_mvi_3d.ipynb similarity index 100% rename from notebooks/04-magnetics/fwd_magnetics_mvi_3d.ipynb rename to notebooks/magnetics/fwd_magnetics_mvi_3d.ipynb diff --git a/notebooks/magnetics_index.md b/notebooks/magnetics/index.md similarity index 53% rename from notebooks/magnetics_index.md rename to notebooks/magnetics/index.md index 8525a3e..e9f9f7f 100644 --- a/notebooks/magnetics_index.md +++ b/notebooks/magnetics/index.md @@ -13,11 +13,11 @@ Global scale magnetic anomalies over Africa ([image source](https://upload.wikim ## Tutorial Notebooks -[3D Forward Simulation of Total Magnetic Intensity Data](04-magnetics/fwd_magnetics_induced_3d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$ +[3D Forward Simulation of Total Magnetic Intensity Data](magnetics/fwd_magnetics_induced_3d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$
-[3D Forward Simulation of Magnetic Gradiometry Data](04-magnetics/fwd_magnetics_mvi_3d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$ +[3D Forward Simulation of Magnetic Gradiometry Data](magnetics/fwd_magnetics_mvi_3d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$
-[3D Inversion of TMI Data to Recover a Susceptibility Model](04-magnetics/inv_magnetics_induced_3d) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$ -
\ No newline at end of file +[3D Inversion of TMI Data to Recover a Susceptibility Model](magnetics/inv_magnetics_induced_3d) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$ +
diff --git a/notebooks/04-magnetics/inv_magnetics_induced_3d.ipynb b/notebooks/magnetics/inv_magnetics_induced_3d.ipynb similarity index 99% rename from notebooks/04-magnetics/inv_magnetics_induced_3d.ipynb rename to notebooks/magnetics/inv_magnetics_induced_3d.ipynb index 350cea0..20c8654 100644 --- a/notebooks/04-magnetics/inv_magnetics_induced_3d.ipynb +++ b/notebooks/magnetics/inv_magnetics_induced_3d.ipynb @@ -139,22 +139,22 @@ "name": "stdout", "output_type": "stream", "text": [ - "overwriting /home/ssoler/git/user-tutorials/notebooks/04-magnetics/inv_magnetics_induced_3d_files.tar.gz\n", - "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/04-magnetics/inv_magnetics_induced_3d_files.tar.gz\n" + "overwriting /home/ssoler/git/user-tutorials/notebooks/magnetics/inv_magnetics_induced_3d_files.tar.gz\n", + "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/magnetics/inv_magnetics_induced_3d_files.tar.gz\n" ] }, { "name": "stdout", "output_type": "stream", "text": [ - " saved to: /home/ssoler/git/user-tutorials/notebooks/04-magnetics/inv_magnetics_induced_3d_files.tar.gz\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/magnetics/inv_magnetics_induced_3d_files.tar.gz\n", "Download completed!\n" ] } ], "source": [ "# URL to download from repository assets\n", - "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/04-magnetics/inv_magnetics_induced_3d_files.tar.gz\"\n", + "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/magnetics/inv_magnetics_induced_3d_files.tar.gz\"\n", "\n", "# download the data\n", "downloaded_data = download(data_source, overwrite=True)\n", diff --git a/notebooks/12-pgi-inversion/plot_inv_1_joint_pf_pgi_full_info_tutorial.ipynb b/notebooks/pgi/plot_inv_1_joint_pf_pgi_full_info_tutorial.ipynb similarity index 99% rename from notebooks/12-pgi-inversion/plot_inv_1_joint_pf_pgi_full_info_tutorial.ipynb rename to notebooks/pgi/plot_inv_1_joint_pf_pgi_full_info_tutorial.ipynb index 2f1cc80..ed2b351 100644 --- a/notebooks/12-pgi-inversion/plot_inv_1_joint_pf_pgi_full_info_tutorial.ipynb +++ b/notebooks/pgi/plot_inv_1_joint_pf_pgi_full_info_tutorial.ipynb @@ -134,7 +134,7 @@ "name": "stdout", "output_type": "stream", "text": [ - " saved to: /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/mesh_tutorial.ubc\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/pgi/mesh_tutorial.ubc\n", "Download completed!\n" ] }, @@ -151,7 +151,7 @@ "output_type": "stream", "text": [ "Downloading https://storage.googleapis.com/simpeg/pgi_tutorial_assets/geology_true.mod\n", - " saved to: /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/geology_true.mod\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/pgi/geology_true.mod\n", "Download completed!\n" ] }, @@ -177,11 +177,11 @@ "name": "stdout", "output_type": "stream", "text": [ - "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/gravity_data.obs\n", + "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/pgi/gravity_data.obs\n", "Downloading https://storage.googleapis.com/simpeg/pgi_tutorial_assets/gravity_data.obs\n", - " saved to: /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/gravity_data.obs\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/pgi/gravity_data.obs\n", "Download completed!\n", - "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/magnetic_data.obs\n", + "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/pgi/magnetic_data.obs\n", "Downloading https://storage.googleapis.com/simpeg/pgi_tutorial_assets/magnetic_data.obs\n" ] }, @@ -189,7 +189,7 @@ "name": "stdout", "output_type": "stream", "text": [ - " saved to: /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/magnetic_data.obs\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/pgi/magnetic_data.obs\n", "Download completed!\n" ] }, @@ -215,7 +215,7 @@ "name": "stdout", "output_type": "stream", "text": [ - "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/CDED_Lake_warp.xyz\n", + "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/pgi/CDED_Lake_warp.xyz\n", "Downloading https://storage.googleapis.com/simpeg/pgi_tutorial_assets/CDED_Lake_warp.xyz\n" ] }, @@ -223,7 +223,7 @@ "name": "stdout", "output_type": "stream", "text": [ - " saved to: /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/CDED_Lake_warp.xyz\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/pgi/CDED_Lake_warp.xyz\n", "Download completed!\n" ] } diff --git a/notebooks/12-pgi-inversion/plot_inv_2_joint_pf_pgi_no_info_tutorial.ipynb b/notebooks/pgi/plot_inv_2_joint_pf_pgi_no_info_tutorial.ipynb similarity index 99% rename from notebooks/12-pgi-inversion/plot_inv_2_joint_pf_pgi_no_info_tutorial.ipynb rename to notebooks/pgi/plot_inv_2_joint_pf_pgi_no_info_tutorial.ipynb index 85ed38d..f5bf107 100644 --- a/notebooks/12-pgi-inversion/plot_inv_2_joint_pf_pgi_no_info_tutorial.ipynb +++ b/notebooks/pgi/plot_inv_2_joint_pf_pgi_no_info_tutorial.ipynb @@ -128,9 +128,9 @@ "name": "stdout", "output_type": "stream", "text": [ - "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/mesh_tutorial.ubc\n", + "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/pgi/mesh_tutorial.ubc\n", "Downloading https://storage.googleapis.com/simpeg/pgi_tutorial_assets/mesh_tutorial.ubc\n", - " saved to: /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/mesh_tutorial.ubc\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/pgi/mesh_tutorial.ubc\n", "Download completed!\n" ] }, @@ -146,9 +146,9 @@ "name": "stdout", "output_type": "stream", "text": [ - "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/geology_true.mod\n", + "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/pgi/geology_true.mod\n", "Downloading https://storage.googleapis.com/simpeg/pgi_tutorial_assets/geology_true.mod\n", - " saved to: /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/geology_true.mod\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/pgi/geology_true.mod\n", "Download completed!\n" ] }, @@ -174,13 +174,13 @@ "name": "stdout", "output_type": "stream", "text": [ - "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/gravity_data.obs\n", + "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/pgi/gravity_data.obs\n", "Downloading https://storage.googleapis.com/simpeg/pgi_tutorial_assets/gravity_data.obs\n", - " saved to: /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/gravity_data.obs\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/pgi/gravity_data.obs\n", "Download completed!\n", - "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/magnetic_data.obs\n", + "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/pgi/magnetic_data.obs\n", "Downloading https://storage.googleapis.com/simpeg/pgi_tutorial_assets/magnetic_data.obs\n", - " saved to: /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/magnetic_data.obs\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/pgi/magnetic_data.obs\n", "Download completed!\n" ] }, @@ -206,7 +206,7 @@ "name": "stdout", "output_type": "stream", "text": [ - "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/CDED_Lake_warp.xyz\n", + "file already exists, new file is called /home/ssoler/git/user-tutorials/notebooks/pgi/CDED_Lake_warp.xyz\n", "Downloading https://storage.googleapis.com/simpeg/pgi_tutorial_assets/CDED_Lake_warp.xyz\n" ] }, @@ -214,7 +214,7 @@ "name": "stdout", "output_type": "stream", "text": [ - " saved to: /home/ssoler/git/user-tutorials/notebooks/12-pgi-inversion/CDED_Lake_warp.xyz\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/pgi/CDED_Lake_warp.xyz\n", "Download completed!\n" ] } diff --git a/notebooks/tdem_index.md b/notebooks/tdem_index.md deleted file mode 100644 index 95068ce..0000000 --- a/notebooks/tdem_index.md +++ /dev/null @@ -1,28 +0,0 @@ -Time-Domain Electromagnetics -============================ - -In this chapter, we publish code comparisons and validations for time-domain electromagnetic modeling packages. -In SimPEG, the -[`simpeg.electromagnetics.time_domain`](xref:simpeg#simpeg.electromagnetics.time_domain) -module is used for modeling time-domain data. - -```{figure} ../assets/website_images/tem_physics.png -:width: 800px -:align: center - -Schematic illustrating the physics of the TEM method for an inductive source. -``` - -## Tutorial Notebooks - -[1D Forward Simulation for a Single Sounding](08-tdem/fwd_tdem_1d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$ -
- -[Fundamentals of Finite Volume for TDEM Simulations](08-tdem/fwd_tdem_fundamentals) $({\color{green}Introductory}$, ${\color{green}Lightweight})$ -
- -[3D Forward Simulation for On-Time Large-Loop Data](08-tdem/fwd_utem_3d) $({\color{orange}Intermediate}$, ${\color{orange}Moderate})$ -
- -[1D Inversion for a Single Sounding](08-tdem/inv_tdem_1d) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$ -
diff --git a/notebooks/08-tdem/fwd_tdem_1d.ipynb b/notebooks/time-domain-em/fwd_tdem_1d.ipynb similarity index 99% rename from notebooks/08-tdem/fwd_tdem_1d.ipynb rename to notebooks/time-domain-em/fwd_tdem_1d.ipynb index 36cad32..01cbc3c 100644 --- a/notebooks/08-tdem/fwd_tdem_1d.ipynb +++ b/notebooks/time-domain-em/fwd_tdem_1d.ipynb @@ -471,7 +471,7 @@ "source": [ "### Case 1: the conductive layer is also magnetically permeable\n", "\n", - "In this case, the middle layer is magnetically permeable in addition to being more conductive than the host. For TDEM simulation classes within SimPEG, the Earth's magnetic properties are defined as magnetic permeabilities (not susceptibilities). Here, the layer magnetic permeabilities are set as a static property of the simulation using the ``mu`` keyword argument. However, one could define a model whose parameters contain the layer magnetic permeabilities; see the [1D Forward Simulation of Frequency Domain EM Data for a Single Sounding](../07-fdem/fwd_fdem_1d.ipynb) tutorial. This would require the user set ``muMap``." + "In this case, the middle layer is magnetically permeable in addition to being more conductive than the host. For TDEM simulation classes within SimPEG, the Earth's magnetic properties are defined as magnetic permeabilities (not susceptibilities). Here, the layer magnetic permeabilities are set as a static property of the simulation using the ``mu`` keyword argument. However, one could define a model whose parameters contain the layer magnetic permeabilities; see the [1D Forward Simulation of Frequency Domain EM Data for a Single Sounding](../frequency-domain-em/fwd_fdem_1d.ipynb) tutorial. This would require the user set ``muMap``." ] }, { diff --git a/notebooks/08-tdem/fwd_tdem_3d.ipynb b/notebooks/time-domain-em/fwd_tdem_3d.ipynb similarity index 100% rename from notebooks/08-tdem/fwd_tdem_3d.ipynb rename to notebooks/time-domain-em/fwd_tdem_3d.ipynb diff --git a/notebooks/08-tdem/fwd_tdem_fundamentals.ipynb b/notebooks/time-domain-em/fwd_tdem_fundamentals.ipynb similarity index 100% rename from notebooks/08-tdem/fwd_tdem_fundamentals.ipynb rename to notebooks/time-domain-em/fwd_tdem_fundamentals.ipynb diff --git a/notebooks/08-tdem/fwd_utem_3d.ipynb b/notebooks/time-domain-em/fwd_utem_3d.ipynb similarity index 100% rename from notebooks/08-tdem/fwd_utem_3d.ipynb rename to notebooks/time-domain-em/fwd_utem_3d.ipynb diff --git a/notebooks/time-domain-em/index.md b/notebooks/time-domain-em/index.md new file mode 100644 index 0000000..a361a69 --- /dev/null +++ b/notebooks/time-domain-em/index.md @@ -0,0 +1,28 @@ +Time-Domain Electromagnetics +============================ + +In this chapter, we publish code comparisons and validations for time-domain electromagnetic modeling packages. +In SimPEG, the +[`simpeg.electromagnetics.time_domain`](xref:simpeg#simpeg.electromagnetics.time_domain) +module is used for modeling time-domain data. + +```{figure} ../../assets/website_images/tem_physics.png +:width: 800px +:align: center + +Schematic illustrating the physics of the TEM method for an inductive source. +``` + +## Tutorial Notebooks + +[1D Forward Simulation for a Single Sounding](time-domain-em/fwd_tdem_1d) $({\color{green}Introductory}$, ${\color{green}Lightweight})$ +
+ +[Fundamentals of Finite Volume for TDEM Simulations](time-domain-em/fwd_tdem_fundamentals) $({\color{green}Introductory}$, ${\color{green}Lightweight})$ +
+ +[3D Forward Simulation for On-Time Large-Loop Data](time-domain-em/fwd_utem_3d) $({\color{orange}Intermediate}$, ${\color{orange}Moderate})$ +
+ +[1D Inversion for a Single Sounding](time-domain-em/inv_tdem_1d) $({\color{orange}Intermediate}$, ${\color{green}Lightweight})$ +
diff --git a/notebooks/08-tdem/inv_tdem_1d.ipynb b/notebooks/time-domain-em/inv_tdem_1d.ipynb similarity index 99% rename from notebooks/08-tdem/inv_tdem_1d.ipynb rename to notebooks/time-domain-em/inv_tdem_1d.ipynb index 63b6b63..94ef518 100644 --- a/notebooks/08-tdem/inv_tdem_1d.ipynb +++ b/notebooks/time-domain-em/inv_tdem_1d.ipynb @@ -131,22 +131,22 @@ "name": "stdout", "output_type": "stream", "text": [ - "overwriting /home/ssoler/git/user-tutorials/notebooks/08-tdem/inv_tdem_1d_files.tar.gz\n", - "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/08-tdem/inv_tdem_1d_files.tar.gz\n" + "overwriting /home/ssoler/git/user-tutorials/notebooks/time-domain-em/inv_tdem_1d_files.tar.gz\n", + "Downloading https://github.com/simpeg/user-tutorials/raw/main/assets/time-domain-em/inv_tdem_1d_files.tar.gz\n" ] }, { "name": "stdout", "output_type": "stream", "text": [ - " saved to: /home/ssoler/git/user-tutorials/notebooks/08-tdem/inv_tdem_1d_files.tar.gz\n", + " saved to: /home/ssoler/git/user-tutorials/notebooks/time-domain-em/inv_tdem_1d_files.tar.gz\n", "Download completed!\n" ] } ], "source": [ "# URL to assets folder\n", - "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/08-tdem/inv_tdem_1d_files.tar.gz\"\n", + "data_source = \"https://github.com/simpeg/user-tutorials/raw/main/assets/time-domain-em/inv_tdem_1d_files.tar.gz\"\n", "\n", "# download the data\n", "downloaded_data = download(data_source, overwrite=True)\n",