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P. Schmoldt, PhD - MTNet - DIAS

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10. Data inversion<br />

Depth (km)<br />

Depth (km)<br />

(a)<br />

(b)<br />

S N<br />

Campo de Montiel M.P.<br />

Loranca Basin<br />

0<br />

50<br />

100<br />

150<br />

200<br />

250<br />

300<br />

0<br />

50<br />

100<br />

150<br />

200<br />

250<br />

300<br />

pic020<br />

pic019<br />

pic011<br />

pic009<br />

pic007<br />

pic005<br />

pic004<br />

pic003<br />

pic002<br />

pic001<br />

0 16 32 48 64 80 96 112 128 144<br />

Distance (km)<br />

log 10<br />

(Wm)<br />

0 1.1 2.2 3.3<br />

Fig. 10.19.: Models of the Tajo Basin subsurface used as starting model for anisotropic 2D inversion. The models contain crustal<br />

structures derived by the isotropic 2D inversion for the Tajo Basin crust and either (a) a homogeneous 100 Ωm halfspace or (b) a<br />

100 Ωm lithospheric-mantle and a 10 Ωm asthenosphere to represent the mantle.<br />

6.3); thereby masking information in the dataset. In particular, data for the longest periods<br />

are not well constraint due to their higher uncertainty levels. Accordingly, sensitivity<br />

to the asthenospheric region is low and regularisations are chosen to fit the characteristics<br />

of this region; i.e. (a) increased horizontal smoothing (α = 3) since the eLAB can<br />

be assumed to exhibit relatively low vertical variation, (b) intermediate global smoothing<br />

(τ = 6) to avoid loosing the electric resistivity decrease at the LAB due to too high<br />

smoothing, and (c) electric resistivity gradient regularisation because the asthenosphere<br />

is commonly assumed as a region of relatively homogeneous electric resistivity.<br />

Corresponding to findings of the synthetic model study presented in Chapter 8, results<br />

of the anisotropic 2D inversion approach are shown using electric resistivity values of<br />

the direction orthogonal to the profile (ρXX). Electric resistivity models for the opposite<br />

direction (ρYY) exhibit implausible low values (cf. Fig. 10.21) and are not considered<br />

representative for the Tajo Basin mantle. Inversion models obtained using either a halfspace<br />

or two layers to represent the mantle region (top and bottom plot in Figure 10.19,<br />

respectively) are virtually identical (cf. Fig. 10.21), thereby indicating robustness of the<br />

inversion process. Moreover, both models exhibit electric resistivity values ≥ 100 Ωm for<br />

the region associated with the asthenosphere; thus, indicating that an electrically conduc-<br />

258

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