Fall 2004
Place: Loyola University -
Monroe Hall, Room 222
Day: Wednesday
Time: 4:00pm - 5:00pm
October 6
Prof. Feride Tiglay
Department of Mathematics, University of New Orleans
Well-posedness for an evolution
equation in Sobolev spaces
October 13
No Seminar
October 20
Prof. Dongming Wei
Department of Mathematics, University of New Orleans
Modeling of Nonlinear Waves in Strain
Hardening Structures
October 27
Prof. Ralph Saxton
Department of Mathematics, University of New Orleans
Flow in an Infinite Channel
November 3
Prof. Katarzyna Saxton
Department of Mathematics and Computer Science, Loyola University
Phase Transitions in Heat Propagation
at Temperatures Close to Absolute Zero
November 10
Dr. Alexei Medovikov
Department of Mathematics, Tulane University
Increasing Asymptotic Stability of the Crank-Nicolson Method
Abstract:
We study the optimization of the Crank-Nicolson method for stiff
ordinary
differential equations. The Crank-Nicolson method for numerical
integration of first order ordinary differential equations is
absolutely stable, but the stability function |R(z)| tends to 1
rather than zero as Re z approaches infinity. This causes unexpected
oscillatory behavior of the numerical solution of stiff differential
equations. In order to avoid this problem, we optimize the stability
property of the stability function. Variable steps within the
sequence of steps by the Crank-Nicolson method allows us to obtain
different
stability functions and formulate an optimization problem for roots and
poles of the stability function. The optimal solution of this problem
is the classical rational Zolotarev function. An appropriate selection
of the sequence of step-sizes eliminates oscillatory behavior of the
numerical solution.
The talk is based on a joint work
with Vyacheslav I. Lebedev (Institute of Numerical Mathematics of The
Russian Academy of Science 117334 Russia, Moscow, Gubkina Street 8.)
November 17
Dr. Samer Al-Ashhab
Department of Mathematics, University of New Orleans
Canonical Transformations of
Local Functionals
Abstract:
When a Lie group acts on some fiber bundle of a manifold it induces
what is called a prolonged action on the jet bundle of the manifold.
This in turn induces an action (transformation) on local functions and
local functionals which are defined on the jet bundle. The
transformations that leave the Poisson bracket of two functionals
unchanged are called canonical transformations. We find the necessary
and sufficient conditions for a transformation to be canonical.
November 24
No Seminar
December 1
No Seminar
Questions or comments please e-mail Ralph Saxton.