147 research outputs found
a comparison of morphological and petrological methods
In planetary sciences, the emplacement of lava flows is commonly modelled
using a single rheological parameter (apparent viscosity or apparent yield
strength) calculated from morphological dimensions using Jeffreysʼ and Hulmeʼs
equations. The rheological parameter is then typically further interpreted in
terms of the nature and chemical composition of the lava (e.g., mafic or
felsic). Without the possibility of direct sampling of the erupted material,
the validity of this approach has remained largely untested. In modern
volcanology, the complex rheological behaviour of lavas is measured and
modelled as a function of chemical composition of the liquid phase, fractions
of crystals and bubbles, temperature and strain rate. Here, we test the
planetary approach using a terrestrial basaltic lava flow from the Western
Volcanic Zone in Iceland. The geometric parameters required to employ
Jeffreysʼ and Hulmeʼs equations are accurately estimated from high-resolution
HRSC-AX Digital Elevation Models. Samples collected along the lava flow are
used to constrain a detailed model of the transient rheology as a function of
cooling, crystallisation, and compositional evolution of the residual melt
during emplacement. We observe that the viscosity derived from the morphology
corresponds to the value estimated when significant crystallisation inhibits
viscous deformation, causing the flow to halt. As a consequence, the inferred
viscosity is highly dependent on the details of the crystallisation sequence
and crystal shapes, and as such, is neither uniquely nor simply related to the
bulk chemical composition of the erupted material. This conclusion, drawn for
a mafic lava flow where crystallisation is the primary process responsible for
the increase of the viscosity during emplacement, should apply to most of
martian, lunar, or mercurian volcanic landforms, which are dominated by
basaltic compositions. However, it may not apply to felsic lavas where
vitrification resulting from degassing and cooling may ultimately cause lava
flows to halt
Enhanced Electron Pairing in a Lattice of Berry Phase Molecules
We show that electron hopping in a lattice of molecules possessing a Berry
phase naturally leads to pairing. Our building block is a simple molecular site
model inspired by C, but realized in closer similarity with Na. In
the resulting model electron hopping must be accompanied by orbital operators,
whose function is to switch on and off the Berry phase as the electron number
changes. The effective hamiltonians (electron-rotor and electron-pseudospin)
obtained in this way are then shown to exhibit a strong pairing phenomenon, by
means of 1D linear chain case studies. This emerges naturally from numerical
studies of small -site rings, as well as from a BCS-like mean-field theory
formulation. The pairing may be explained as resulting from the exchange of
singlet pairs of orbital excitations, and is intimately connected with the
extra degeneracy implied by the Berry phase when the electron number is odd.
The relevance of this model to fullerides, to other molecular superconductors,
as well as to present and future experiments, is discussed.Comment: 30 pages, RevTe
Rattling-Induced Superconductiviy in the Beta-Pyrochlore Oxides AOs2O6
The superconducting properties of two beta-pyrochlore oxides, CsOs2O6 and
RbOs2O6, are studied by thermodynamic and transport measurements using
high-quality single crystals. It is shown that the character of
superconductivity changes systematically from weak coupling for CsOs2O6 to
moderately strong coupling for RbOs2O6, and finally to extremely strong
coupling with BCS-type superconductivity for KOs2O6, with increasing Tc.
Strong-coupling correction analyses of the superconducting properties reveal
that a low-energy rattling mode of the alkali metal ions is responsible for the
mechanism of the superconductivity in each compound. The large enhancement of
Tc from Cs to K is attributed to the increase in the electron-rattler coupling
with decreasing characteristic energy of the rattling and with increasing
anharmonicity. The existence of weak anisotropy in the superconducting gap or
in the electron-rattler interactions is found for the Cs and Rb compounds
The Changing Face of the Epidemiology of Tuberculosis due to Molecular Strain Typing: A Review
Lava flow rheology: A comparison of morphological and petrological methods
In planetary sciences, the emplacement of lava flows is commonly modelled using a single rheological
parameter (apparent viscosity or apparent yield strength) calculated from morphological dimensions
using Jeffreys’ and Hulme’s equations. The rheological parameter is then typically further interpreted in
terms of the nature and chemical composition of the lava (e.g., mafic or felsic). Without the possibility of
direct sampling of the erupted material, the validity of this approach has remained largely untested.
In modern volcanology, the complex rheological behaviour of lavas is measured and modelled as a
function of chemical composition of the liquid phase, fractions of crystals and bubbles, temperature
and strain rate. Here, we test the planetary approach using a terrestrial basaltic lava flow from the
Western Volcanic Zone in Iceland. The geometric parameters required to employ Jeffreys’ and Hulme’s
equations are accurately estimated from high-resolution HRSC-AX Digital Elevation Models. Samples
collected along the lava flow are used to constrain a detailed model of the transient rheology as a
function of cooling, crystallisation, and compositional evolution of the residual melt during emplacement.
We observe that the viscosity derived from the morphology corresponds to the value estimated when
significant crystallisation inhibits viscous deformation, causing the flow to halt. As a consequence, the
inferred viscosity is highly dependent on the details of the crystallisation sequence and crystal shapes,
and as such, is neither uniquely nor simply related to the bulk chemical composition of the erupted
material. This conclusion, drawn for a mafic lava flow where crystallisation is the primary process
responsible for the increase of the viscosity during emplacement, should apply to most of martian, lunar,
or mercurian volcanic landforms, which are dominated by basaltic compositions. However, it may not
apply to felsic lavas where vitrification resulting from degassing and cooling may ultimately cause lava
flows to halt
Designing Low Parametric Sensitivity FWL Realizations of LTI Controllers/Filters within the Implicit State-Space Framework
International audienceno abstrac
Forme rho-modale : pour une implementation simple et efficace de filtres/regulateurs LTI
GT MOSAR, 4-5 jun 2009no abstrac
OLIVINE COMPOSITION AND REFLECTANCE SPECTROSCOPY RELATIONSHIP REVISITED
International audienc
- …