P. Schmoldt, PhD - MTNet - DIAS
P. Schmoldt, PhD - MTNet - DIAS P. Schmoldt, PhD - MTNet - DIAS
10. Data inversion WinGLink software [WinGLink, 2005], also based on the algorithm by Rodi and Mackie [2001]. The ai1D code by Pek and Santos [2006] is used for anisotropic 1D inversion, and isotropic 3D inversion is carried out using the program WSINV3DMT [Siripunvaraporn et al., 2005a]. First, optimal smoothing parameters and enhanced a priori models are determined for inversion of crust and mantle ranges. Inversion models for the two modes of MT in 2D (TE and TM) are derived separately to gain better insight about the nature of the subsurface; particularly, in order to infer the extent of 3D effects in each of the modes. In addition, hypotheses from previous studies regarding the Tajo Basin subsurface (see Sec. 7) are tested and an enhanced subsurface model is presented. Furthermore, results of anisotropic 1D, isotropic 2D, anisotropic 2D, and isotropic 3D inversion are contrasted and their applicability for the Tajo Basin subsurface case is evaluated. 10.1. Inversion for crustal structures 10.1.1. Determining smoothing parameters for inversion As illustrated in Section 6.3, inversion of MT data is non-unique and additional constraints have to be applied to limit the range of acceptable models. The choice of smoothing parameters, reducing spatial variation of electric resistivity in the inversion model, can have significant impacts on the derived inversion model. Therefore, a deliberate parameter study is carried out prior to the final inversion for crustal structures. The 2D inversion program implemented in WinGLink [WinGLink, 2005], based on the algorithm by Rodi and Mackie [2001], includes three smoothing parameters, controlling different aspects of model constraints (cf. Sec. 6.3), namely • α: multiplication factor of the horizontal derivatives in the objective function; higher values of alpha drive horizontal smoothness of the inversion model; • β: exponential factor in the weighting function for uniform grid Laplacian regularisation; higher values increase the penalty on horizontal roughness; • τ: “global” weighting function, determines the trade-off between data-misfit and model-roughness (cf. Eq. 6.31); higher values are in favour of smoother models. An increased global model smoothing (i.e. an increased τ) is usually preferable, as it reduces the number of features within a model for most cases; thus, yielding a minimum structure model (cf. Sec. 6.3.3). An increased horizontal smoothing (i.e. an increased α) is reasoned for the Tajo Basin subsurface model by results of crustal seismic studies in the region (Sec. 7.3.2), indicating relatively homogeneous intermediate and lower crustal layers with small variations in depth. β is kept at a value of 1, following recommendations by Mackie [2002] for the case of isotropic 2D inversion using uniform grids with Laplacian regularisation (∆(m) 2 ). 226
Parameter Value 10.1. Inversion for crustal structures Invert modes: TM and TE min./max. resistivities: 0.1 – 10 5 Ωm period range: 10 −3 – 10 s and 10 −3 – 100 s interpolate data: 5 Freq./decade (use smooth curve if existing) solving for: the smoothest model regularisation operator: uniform grid Laplacian regularisation order: minimising integral of ∆(m) 2 smoothing parameters (α): [1.0, 1.1, 1.3, 1.6, 2.0, 3.0, 5.0] smoothing parameters (β): 1 smoothing parameters (τ): [0.01, 0.1, 1.0, 3.0, 6.0, 10.0] static shift correction: yes (variance: 20 %, damping: 10000) fixed parameters: no data errors: ρa = 10 %, φ = 5 % (use data if existing) error floor: ρa = 10 %, φ = 5 % (use data if existing) Tab. 10.1.: Settings used to determine the optimal smoothing parameter combination in the inversion for Tajo Basin crustal structures. A range of α and τ values is sampled in order to identify an optimal parameter combination for inversion of the Tajo Basin subsurface. To assure that all crustal structures are sensed while the influence of mantle structures kept at a minimum, the optimal smoothing parameter combination is determined for two different period ranges, i.e. 10 −3 – 10 s and 10 −3 – 100 s. For both period ranges, global RMS misfits of 42 models are determined, wherein each model is generated through inversion with different combinations of smoothing parameters and the same set of auxiliary inversion parameters (summarised in Table 10.1). RMS misfits for intermediate smoothing parameter combinations are derived through linear interpolation. Resulting plots for the two frequency ranges exhibit similar L-curve-like behaviour (cf. Sec. 6.3), i.e. curves possessing low RMS misfit values for low values of τ and α (Fig. 10.1). Hence, the chosen parameter combination has to be a trade-off between increased values of τ and α, and a low RMS misfit. An RMS misfit of 2, i.e. 95% of the data are fit to within their error bounds, is chosen as the acceptable upper limit and α,τ - combinations of three models are selected, which represent distinct situations for the range of smoothing parameters used in this study, i.e. • model a3b1t6 (α = 3, β = 1, τ = 6): possessing intermediate values for both variables in the parameter space under consideration; • model a5b1t3 (α = 5, β = 1, τ = 3): representing the horizontally smooth endmember; and • model a2b1t10 (α = 2, β = 1, τ = 10): representing the (relatively) horizontally rough end-member. 227
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10. Data inversion<br />
WinGLink software [WinGLink, 2005], also based on the algorithm by Rodi and Mackie<br />
[2001]. The ai1D code by Pek and Santos [2006] is used for anisotropic 1D inversion,<br />
and isotropic 3D inversion is carried out using the program WSINV3DMT [Siripunvaraporn<br />
et al., 2005a].<br />
First, optimal smoothing parameters and enhanced a priori models are determined for<br />
inversion of crust and mantle ranges. Inversion models for the two modes of MT in<br />
2D (TE and TM) are derived separately to gain better insight about the nature of the<br />
subsurface; particularly, in order to infer the extent of 3D effects in each of the modes.<br />
In addition, hypotheses from previous studies regarding the Tajo Basin subsurface (see<br />
Sec. 7) are tested and an enhanced subsurface model is presented. Furthermore, results<br />
of anisotropic 1D, isotropic 2D, anisotropic 2D, and isotropic 3D inversion are contrasted<br />
and their applicability for the Tajo Basin subsurface case is evaluated.<br />
10.1. Inversion for crustal structures<br />
10.1.1. Determining smoothing parameters for inversion<br />
As illustrated in Section 6.3, inversion of MT data is non-unique and additional constraints<br />
have to be applied to limit the range of acceptable models. The choice of smoothing<br />
parameters, reducing spatial variation of electric resistivity in the inversion model, can<br />
have significant impacts on the derived inversion model. Therefore, a deliberate parameter<br />
study is carried out prior to the final inversion for crustal structures. The 2D inversion<br />
program implemented in WinGLink [WinGLink, 2005], based on the algorithm by Rodi<br />
and Mackie [2001], includes three smoothing parameters, controlling different aspects of<br />
model constraints (cf. Sec. 6.3), namely<br />
• α: multiplication factor of the horizontal derivatives in the objective function; higher<br />
values of alpha drive horizontal smoothness of the inversion model;<br />
• β: exponential factor in the weighting function for uniform grid Laplacian regularisation;<br />
higher values increase the penalty on horizontal roughness;<br />
• τ: “global” weighting function, determines the trade-off between data-misfit and<br />
model-roughness (cf. Eq. 6.31); higher values are in favour of smoother models.<br />
An increased global model smoothing (i.e. an increased τ) is usually preferable, as it<br />
reduces the number of features within a model for most cases; thus, yielding a minimum<br />
structure model (cf. Sec. 6.3.3). An increased horizontal smoothing (i.e. an increased α)<br />
is reasoned for the Tajo Basin subsurface model by results of crustal seismic studies in<br />
the region (Sec. 7.3.2), indicating relatively homogeneous intermediate and lower crustal<br />
layers with small variations in depth. β is kept at a value of 1, following recommendations<br />
by Mackie [2002] for the case of isotropic 2D inversion using uniform grids with<br />
Laplacian regularisation (∆(m) 2 ).<br />
226