[CIG-ALL] PyLith 0.8.2 beta release
Charles Williams
willic3 at rpi.edu
Mon May 7 11:18:00 PDT 2007
Greetings,
I am pleased to announce the beta version 0.8.2 release of PyLith, a
finite element code designed to solve quasi-static viscoelastic
problems in lithospheric dynamics. The latest release offers the use
of traction boundary conditions, load histories for split nodes, a
number of new
material models, including power-law Maxwell and generalized Maxwell
(3 Maxwell models in parallel), the use of .cfg files for setting
simulation parameters, much simpler top-level code structure, and
several bug fixes.
You can download the source code from
http://geodynamics.org/cig/software/packages/short/pylith
Installation instructions are in the bundled README and INSTALL files.
Release Notes:
1. The code now makes use of time histories for split node fault
displacements, allowing users to slip different faults (or sections
of a fault) according to a given history. The format of split node
input files has not changed, since time histories were still present
in the input files (they were just ignored).
2. Traction boundary conditions were broken in the previous version
of PyLith, and they are now functioning for both tetrahedral
(triangular faces) and hexahedral (quadrilateral faces) elements.
3. There are now 6 different material models in PyLith:
IsotropicLinearElastic: Standard elastic model that was available
previously
IsotropicLinearMaxwellViscoelastic: New formulation for the Maxwell
viscoelastic model
IsotropicLinearGenMaxwellViscoelastic: New material model consisting
of a spring in parallel with 3 linear Maxwell models
IsotropicPowerLawMaxwellViscoelastic: New power-law Maxwell model
using the Effective Stress Function approach
IsotropicLinearMaxwellViscoelasticESF: Previous formulation of the
linear Maxwell model using the Effective Stress Function approach
IsotropicPowerLawMaxwellViscoelasticZT: New formulation for the
power-law Maxwell model using a formulation based on that of
Zienkiewicz & Taylor
4. The ability to use .cfg files means that this is now the
preferred method for setting parameters in PyLith, rather than the
command line or using .pml files. These files have a very simple
format, and setting up simulations should now be much simpler.
5. The top-level code structure has been much simplified. The
primary benefit of this to users (in addition to more efficient
code), is that there are no longer separate pylith3d.scanner
options. Instead, there are now just pylith3d options. Also, PETSc
options may now be set as 'petsc.xxx=yyy' in a .cfg file.
While this release should be useful to many researchers, we are
presently focusing our efforts on PyLith 1.0, which will be the first
version of the code to include both quasi-static and dynamic
capabilities. We will make an announcement on this list when the
initial version of PyLith 1.0 is released.
Charles A. Williams
Dept. of Earth & Environmental Sciences
Science Center, 2C01B
Rensselaer Polytechnic Institute
Troy, NY 12180
Phone: (518) 276-3369
FAX: (518) 276-2012
e-mail: willic3 at rpi.edu
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