|
98 | 98 | "\n", |
99 | 99 | "\n" |
100 | 100 | ] |
| 101 | + }, |
| 102 | + { |
| 103 | + "cell_type": "markdown", |
| 104 | + "id": "fe021d63-9952-4a7e-8ebb-e5ff94b04a3b", |
| 105 | + "metadata": {}, |
| 106 | + "source": [ |
| 107 | + "## Example\n", |
| 108 | + "\n", |
| 109 | + "This section demonstrates the use of rotated gradients on a semi-realistic synthetic example. \n", |
| 110 | + "\n", |
| 111 | + "### Setup \n", |
| 112 | + "\n", |
| 113 | + "The model has been generated with the help of [Gempy](https://app.readthedocs.com/projects/mirageoscience-gempy-drivers/builds/?version__slug=stable). The model comprises a folded and faulted magnetic layer (0.5 SI) dipping 20 degrees towards East. The geometry is meant to mimic a banded-iron formation.\n", |
| 114 | + "\n", |
| 115 | + "```{figure} ./images/fold_model.png\n", |
| 116 | + "---\n", |
| 117 | + "scale: 30%\n", |
| 118 | + "---\n", |
| 119 | + "```\n", |
| 120 | + "\n", |
| 121 | + "From this model, we simulate residual magnetic field data along an East-West survey, 200 m line spacing and a mean terrain clearance of 150 m. For simplicity, we use a vertical inducing field with a magnitude of 50,000 nT.\n", |
| 122 | + "\n", |
| 123 | + "```{figure} ./images/fold_model.png\n", |
| 124 | + "---\n", |
| 125 | + "scale: 30%\n", |
| 126 | + "---\n", |
| 127 | + "```\n", |
| 128 | + "\n", |
| 129 | + "The basic components (data, model and topography) to reproduce this example can be [downloaded here]()." |
| 130 | + ] |
| 131 | + }, |
| 132 | + { |
| 133 | + "cell_type": "markdown", |
| 134 | + "id": "6bdbf088-2983-4975-99f5-cb1fba3d2741", |
| 135 | + "metadata": {}, |
| 136 | + "source": [ |
| 137 | + "### Standard unconstrained inversion\n", |
| 138 | + "\n", |
| 139 | + "As a starting point, we invert the magnetic data with standard constraints (lower bounds and reference value of 0 SI). \n", |
| 140 | + "The resulting smooth model shows clear breaks between the survey lines and poorly resolves the dip of the magnetic layer. The subsequent compact model further exacerbates these issues. \n", |
| 141 | + "\n", |
| 142 | + "\n", |
| 143 | + "### Directional constraints\n", |
| 144 | + "\n", |
| 145 | + "To improve the continuity of the magnetic layer across lines and down-dip, we can provide trend information to the inversion from our structural control points.\n", |
| 146 | + "\n", |
| 147 | + "We interpolate the dip and dip direction data from the `structural markers` to the inversion mesh. We use the Radial Basis Function (RBF) application, but users may want to experiment with different interpolation algorithms.\n", |
| 148 | + "\n", |
| 149 | + "```{figure} ./images/fold_model.png\n", |
| 150 | + "---\n", |
| 151 | + "scale: 30%\n", |
| 152 | + "---\n", |
| 153 | + "```\n", |
| 154 | + "\n", |
| 155 | + "Following the instructions presented in the [previous section](rotated-gradients), we group the interpolated data as type `Dip Direction & Dip`. Users can validate the constraint by displaying the vectors onto sections of the mesh. Once created, the orientation information is provided to the inversion. \n", |
| 156 | + "\n", |
| 157 | + "```{figure} ./images/invert_fault_equal.png\n", |
| 158 | + "---\n", |
| 159 | + "scale: 30%\n", |
| 160 | + "---\n", |
| 161 | + "```\n", |
| 162 | + "\n", |
| 163 | + "The resulting model shows an improved \n", |
| 164 | + "\n", |
| 165 | + "\n", |
| 166 | + "We can further improve this result by decreasing the relative weight applied to the gradient penalty perpendicular (z) to the rotated plane.\n", |
| 167 | + "\n", |
| 168 | + "```{figure} ./images/invert_fault_wz0p5.png\n", |
| 169 | + "---\n", |
| 170 | + "scale: 30%\n", |
| 171 | + "---\n", |
| 172 | + "```\n", |
| 173 | + "\n" |
| 174 | + ] |
101 | 175 | } |
102 | 176 | ], |
103 | 177 | "metadata": { |
|
116 | 190 | "name": "python", |
117 | 191 | "nbconvert_exporter": "python", |
118 | 192 | "pygments_lexer": "ipython3", |
119 | | - "version": "3.10.17" |
| 193 | + "version": "3.10.19" |
120 | 194 | } |
121 | 195 | }, |
122 | 196 | "nbformat": 4, |
|
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