OxMOS Workshop/Meeting/Lecture
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Mon, 14/01/2008 15:00 |
Professor Qiang Du (Penn State University) |
OxMOS Workshop/Meeting/Lecture |
DH 3rd floor SR |
| Professor Qiang Du will go over some work on modelling interface/microstructures with curvature dependent energies and also the effect of elasticity on critical nuclei morphology. | |||
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Mon, 21/01/2008 11:00 |
Mariano Vazquez (Barcelona) |
OxMOS Workshop/Meeting/Lecture |
DH 3rd floor SR |
| Computational Mechanics (CM) has become a scientific discipline in itself, being High Perfomance Computational Mechanics (HPCM) a key sub-discipline. The effort for the most efficient use of distributed memory machines provides a different perspective to CM scientists relative to a wide range of topics, from the very physics of the problem to solve to the numerical method used. Marenostrum supercomputer is the largest facility in Europe and the 5th in the world (top500.org - Spring 2007). This talk describes the research lines in the CASE Dpt. of the BSC applied to Aerospace, Bio-mechanics, Geophysics or Environment, through the development of Alya, the in-house HPCM code for complex coupled problems capable of running efficiently in large distributed memory facilities. | |||
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Thu, 24/01/2008 11:00 |
Bernhard Langwallner and Konstantinos Koumatos (Oxford) |
OxMOS Workshop/Meeting/Lecture |
DH 3rd floor SR |
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Tue, 19/02/2008 10:00 |
Timothy Squires and Pras Pathmanathan (Oxford) |
OxMOS Workshop/Meeting/Lecture |
Gibson 1st Floor SR |
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Thu, 28/02/2008 10:00 |
Patrizo Neff (University of Essen & T.U. Darmstadt) |
OxMOS Workshop/Meeting/Lecture |
Gibson 1st Floor SR |
We are concerned with the derivation of the -limit to a three-dimensional geometrically exact
Cosserat model as the relative thickness of a flat domain tends to zero. The Cosserat bulk model involves
already exact rotations as a second independent field and this model is meant to describe defective elastic crystals liable to fracture under shear.
It is shown that the -limit based on a natural scaling assumption
consists of a membrane like energy contribution and a homogenized transverse shear energy both scaling with ,
augmented by an additional curvature stiffness due to the underlying Cosserat bulk formulation, also scaling with .
No specific bending term appears in the dimensional homogenization process. The formulation
exhibits an internal length scale which survives the homogenization process.
A major technical difficulty, which we encounter in applying the -convergence arguments,
is to establish equi-coercivity of the sequence of
functionals as the relative thickness tends to zero. Usually, equi-coercivity follows from a local coerciveness assumption.
While the three-dimensional problem is well-posed for the Cosserat couple modulus , equi-coercivity forces us
to assume a strictly positive Cosserat couple modulus . The -limit model determines the
midsurface deformation . For the case of zero Cosserat couple modulus
we obtain an estimate of the and , without equi-coercivity which is then strenghtened to a -convergence result for zero Cosserat couple modulus. The classical linear
Reissner-Mindlin model is "almost" the linearization of the -limit for
apart from a stabilizing shear energy term. |
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-limit of a finite-strain Cosserat model for asymptotically thin domains versus a formal dimensional reduction
of a flat domain tends to zero. The Cosserat bulk model involves
already exact rotations as a second independent field and this model is meant to describe defective elastic crystals liable to fracture under shear.
It is shown that the
,
augmented by an additional curvature stiffness due to the underlying Cosserat bulk formulation, also scaling with
which survives the homogenization process.
A major technical difficulty, which we encounter in applying the
, equi-coercivity forces us
to assume a strictly positive Cosserat couple modulus
. The
. For the case of zero Cosserat couple modulus
we obtain an estimate of the
and
, without equi-coercivity which is then strenghtened to a