Friday, 26 May, 11:00 - EARTH SYSTEM PHYSICS SEMINAR
Earth System Physics Section
esp at ictp.it
Wed May 24 10:04:56 CEST 2017
EARTH SYSTEM PHYSICS SEMINAR
Friday, 26 May - 11:00 hrs
Leonardo Building, Luigi Stasi Seminar Room
LITHOSPHERIC STRUCTURE OF THE NORTH AMERICAN MODEL
Magdala Tesauro
University of Trieste
Lithospheric structure of the North American continent
Seismic data on the North American continent are unevenly distributed
and in some cases discrepancies exist between published models. In order
to construct a consistent 3D crustal model with three layers in the
crystalline crust, the following sequence of steps have been
implemented: 1. Definition of the geometry of the main tectonic
provinces of North America; 2. Selection and evaluation of the
reliability of seismic crustal models in the database; 3. Estimation of
the P-wave seismic velocity and thickness of the upper, middle and lower
crust for each tectonic province; 4. Estimation of the interpolated Pn
velocity distribution. In comparison with the global crustal model CRUST
1.0, the new crustal model, NACr14, is more heterogeneous, showing a
larger spatial variability of the thickness and average velocities of
the crustal layers. The largest velocities of the crystalline crust
(>6.6 km/s) reflect the presence of a 7.x layer (>7.0 km/s) in the
lowermost part of the crust.
Using NACr2014, a regional (NA07) and a global (SL201sv) seismic
tomography model, and gravity data, an iterative technique, which
jointly interprets seismic tomography and gravity data, to estimate
temperature and compositional variations in the NA upper mantle has been
applied. The results obtained demonstrate that temperature of the
cratonic mantle is up to 150°C higher than when using a uniform
compositional model. The differences between the two tomography models
influence the results more strongly than possible changes of the depth
distribution of compositional variations. Strong negative compositional
density anomalies, corresponding to Mg # >92, characterize the upper
mantle of the northwestern part of the Superior craton and the central
part of the Slave and Churchill craton. The Proterozoic upper mantle of
the western and more deformed part of the NA cratons, appears weakly
depleted (Mg# ~ 91) when NA07 is used, in agreement with the results
based on the interpretation of xenolith data. When SL2013sv is used, the
same areas are locally characterized by high density bodies, which might
be interpreted as the effect due to fragments of subducted slabs, as
those close to the suture of the Appalachians and Grenville province.
The two thermal models have been used to estimate the integrated
strength and effective elastic thickness (Te) of the lithosphere. In the
peripheral parts of the cratons, as the Proterozoic Canadian Platform
and Grenville, the integrated strength for model NA07 is ten times
larger than in model SL2013sv, due to a model-dependent temperature
difference of >200°C in the uppermost mantle. In both models,
Proterozoic regions reactivated by Meso- Cenozoic tectonics (e.g., Rocky
Mountains and the Mississippi Embayment) show a weak lithosphere due to
the absence of the mechanically strong part of the mantle lithospheric
layer. Intraplate earthquakes are distributed along the edges of the
cratons, characterized by a weak lithosphere or pronounced variations in
integrated lithospheric strength and Te. In addition, the sum of the
seismic moments shows that most of the energy is released by the weak
lithosphere. These results suggest that the edges of the cratons are
more prone to accumulation of tectonic stress and subsequent release by
earthquakes, in comparison with the stable cratonic regions which resist
deformation.**
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