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P. Schmoldt, PhD - MTNet - DIAS

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Layer Density Thermal conductivity<br />

7.3. Tajo Basin and central Spain<br />

Thickness Heat production<br />

North South North South<br />

(kg m −3 ) (W m −1 K −1 ) (km) (µW m −3 )<br />

Sediment layer 2400 2.5 2 1 2.5 2.5<br />

Upper crust 2700 2.5 12 13 3.3 2.5<br />

Middle crust 2850 2.5 9<br />

Lower crust 2900 2.1 8 0.8<br />

Tab. 7.4.: Parameters of the thermal model for the Tajo Basin, assuming the thermal conductivity of the lithospheric-mantle to be<br />

3.4 Wm −1 K −1 ; after Tejero and Ruiz [2002].<br />

Fig. 7.27.: Geotherms of the Tajo Basin calculated for the parameters given in Table 7.4; modified from Tejero and Ruiz [2002].<br />

the lower crust acting as an incompetent layer (Fig. 7.28). The concept of a weak<br />

lower crust, as proposed by Tejero and Ruiz [2002], is in agreement with the observed<br />

seismicity in this region, exhibiting no events in the lower crust of central Spain [Instituto<br />

Geografico Nacional, 2010] (cf. earthquake locations depict in Figure 7.22). The<br />

seismic–aseismic boundary is accordingly related to the brittle–ductile boundary of the<br />

crust; observed events are assumed to be transmitted through inherit fault zones and flexural<br />

bounding stresses from regional compression [Tejero and Ruiz, 2002]. However, the<br />

assumption of an exponential decay of heat production with depth used by the authors<br />

for the calculation of their model is questionable (cf. Vilà et al. [2010]), and the obtained<br />

thermal structure could be significantly different for the case of a constant heat production<br />

within each layer.<br />

Recently European scale models of the lithosphere’s thermal and rheological proper-<br />

163

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