Computational and Applied Mathematics (CAM) Seminar
Fall, 2006
CAM seminar usually runs from 2:00-3:00PM, Wednesday.
(Link to CAM seminar talks in other years.)
(Link to Numerical Analysis Group Webpage)
|
Date |
Speaker/Institution |
Title |
|
|
|
|
|
Aug 23 |
Organizing meeting |
|
|
Aug 30 |
Prof. Volker Mehrmann
(Guest speaker), Technische Universitat,
Berlin |
Optimal control of
differential-algebraic equations (abstract) |
|
Sept 6 |
Ralph Byers |
Dirty
Secrets of the TI83 and TI84 (abstract) (more information) |
|
Sept 13 |
Erik Van Vleck |
The error in orthogonal
integration (abstract) |
|
Sept 20 |
Weishi Liu |
On a class
of singular perturbation problems with turning points (abstract) |
|
Sept 27 |
Chuan-Tau Lan (Guest
speaker), J. L. Constant Professor, KU |
Identification of a nonlinear dynamical model from noisy test
data
(abstract) |
|
Oct 4 |
Weizhang Huang |
A mathematical theory for
anisotropic mesh adaptation (abstract) |
|
Oct 18 |
Hongguo Xu |
Krylov
matrix and matrix functions (abstract) |
|
Oct 25 |
Myunghyun Oh |
A brief survey on nonlinear stability (abstract) |
|
Nov 1 |
Xianping Li |
Effect of regularization on numerical simulation of phase
change problems (abstract) |
|
Nov 8 |
Milenna Stanislavova |
Nonlinear stability and instability for Hamiltonian systems
with symmetries (abstract) |
|
Nov 29 |
Ventsislav Ivanov |
Chaotic Synchronization (abstract) |
|
Dec 13 |
Dr. Jingtang Ma (Guest
speaker), Simon Fraser University |
Convergence of Moving Mesh Methods for Time-Dependent PDEs (abstract) |
1. Volker Mehrmann, Optimal control of differential-algebraic equations.
It has been an open problem for quite some time
to extend the classical theory of optimal control (e.g. the optimality
conditions and the maximum principle) to differential-algebraic equations
(DAEs). Some applications where these problems arise will be presented. Then
the classical optimal control theory for ordinary differential equations will
be reviewed and it will be demonstrated by some simple examples that this
theory cannot be extended directly to DAEs of arbitrary index.
It is then shown that via a behavior
approach and a reformulation of the DAE one can derive the optimality
conditions and a maximum principle. The resulting optimality boundary value
problems can then be reinterpreteted in terms of the original systems.
The results and appropriate numerical
methods are illustrated by applying them to a motor controlled pendulum.
2. Ralph Byers, Dirty Secrets of
the TI83 and TI84
or
IF (E/D = 2) and (E-D = 0); THEN GROAN
IF (A-100 = 0) and (A-.99-.01 not= 0); THEN
CRY
IF (B <= 2) and (2B
> 4); THEN SCREAM
Disclaimers:
o This is primarily
*not* a talk about rounding errors.
o It is not a research
talk.
o It is accessible to
anyone with a sound background in
decimal
arithmetic.
o Frustrating experience
with a TI83 or TI84 calculator is
recommended
but not required background.
o It is a short talk of
no more than 30 minutes.
The TI83 and TI84 are among the most popular
calculators on campus. Hundreds of unsuspecting undergraduates succeed with
help from these calculators despite (or perhaps because of) some hidden
``features'' in the built in arithmetic.
Students, instructors, engineers, scientists and hobbyists write complex
TI83/TI84 programs. Nevertheless,
it is difficult to calculate differences A - B and remarkable difficult to
correctly distinguish A>B from A=B from A<B.
This non-judgmental talk tells some (but
probably not all) of the hidden secrets of the TI83 and TI84 arithmetic and
sets forth some TI83/TI84 issues and pitfalls.
1)
Dirty Secrets Writeup in PDF format (here).
2) ASCREAM TI83/TI84
calculator program .TXT file (here).
This
is the program I showed in the seminar demonstrating some oddities in TI83/TI84
arithmetic.
3) ASCREAM TI83/TI84
calculator program .83p file (here).
4) DIGIT14 TI83/TI84
calculator program .TXT file (here).
This
program stores all significant digits in variable X as a string in str0.
5) DIGIT15 TI83/TI84
calculator program .83p file (here).
There are
two ways to get the following programs into a calculator.
The easy, inexpensive way:
Copy
the programs from someone who has them on their calculator already, e.g., the
instructor.
Use
the link cable that came with the calculator and follow the instructions in
Chapter 19
of
the guidebook
The difficult, expensive way:
You may use a web browser to
download the programs to a PC, then use
linking
software
And special cables to copy the
programs into your calculator. Of course, TI sells link cables and
distributes
link software through many academic bookstores.
Alternatively,
you may download
``free'' software and/or make your own cables.
3. Erik Van Vleck, The error in orthogonal integration.
Consider
the matrix differential equation Q' = Q*S(Q,A), t>0, Q(0) orthogonal, where
S(Q,A) is a specific skew-symmetric matrix function that depends on the
dependent variable Q and a given bounded matrix function A(.). In this talk we
outline a forward error analysis for the numerical approximation of Q(.) that
is valid on infinite time intervals.
Key ingredients are the uniqueness of the QR factorization of a matrix,
a recently developed backward error analysis that takes advantage of the
orthogonal structure in the problem, and integral separation.
4. Weishi Liu, On a class of
singular perturbation problems with turning points.
Phase portrait is the ultimate goal for
understanding nonlinear dynamics. If we couldn't obtain phase portraits for ALL
nonlinear systems (this is a safe assumption), we try to do so for some SPECIAL
and IMPORTANT classes; if we couldn't get GLOBAL phase portraits (this is also
a safe assumption), we try to get LOCAL ones.
Singularly perturbed problems (with and
without turning points) are a class of special but important systems. We will
try to get a rough sketch of local phase portraits for an even more special
class of singularly perturbed systems with turning points.
5. C. Edward Lan, Identification of a nonlinear dynamical model from noisy
test data
A fighter
aircraft suffered uncommanded rolling motion, called wing drop, during flight
tests at transonic speeds. The instability was not identified during the design
phase through the conventional wind-tunnel testing. Therefore, a new dynamic
wind-tunnel test program with a free-to-roll test rig was initiated. The main
purpose of our project is to identify possible dynamic instabilities of the
full-scale aircraft by examining the roll dynamic characteristics of the models
in the tunnel. To improve the tunnel balance data caused by model vibration, a
model-based filtering method is developed and applied. The corrected rolling
moment coefficients are then modeled through a fuzzy logic algorithm as
functions of: angle of attack, sideslip, roll angle, etc. A wing drop theory is
proposed and verified based on the values of the relative nonlinear aerodynamic
stiffness in the rolling equation of motion, Wing drop is predicted if the
relative aerodynamic stiffness becomes zero, or changes sign. This is
equivalent to the vanishing of frequency in the vibration theory. It is found
that among those test runs examined only the preproduction F-18E model
encounters wing drop conditions, while the AV-8B model develops only the wing
rock motion (i.e. limit-cycle oscillations). It is also found that wing rock
motion in the tunnel on a free-to-roll test rig is mainly caused by the nonlinear
damping effect of the time rate of sideslip angle, not the traditional roll
damping due to roll rate.
6. Weizhang Huang, A mathematical theory for anisotropic mesh adaptation.
In
this talk I will present a mathematical theory of anisotropic mesh adaptation
for the numerical solution of partial differential equations. Two principles,
equidistribution and alignment, will be shown to be necessary and sufficient
for a complete control of the size, shape, and orientation of mesh elements.
Applications and numerical results will be presented to demonstrate that the
developed equidistribution and alignment principles are useful tools for use in
designing reliable and robust algorithms for adaptive anisotropic mesh
generation.
7. Hongguo Xu, Krylov matrix and matrix functions.
Let A be an n-by-n matrix and b be a column
vector. The matrix [b,Ab,...,A^{n-1}b] is a Krylov matrix of A. Krylov matrix
is a basic tool in numerical linear algebra. It appears in numerical solution
of large scale system of linear equations and numerical eigenvalue problem. Can
Krylov matrix do more? We will give a positive answer in this talk. We will
show that when all the eigenvalues of A has a single Jordan block, f(A) can be
formulated by a Krylov matrix. Here f(t) can be a polynomial, a rational
function, an exponential, or just an analytic function. The formulation may
reduce the cost for computing f(A) from at least O(n^4) to O(n^3).
8. Myunghyun
Oh, A brief survey on
nonlinear stability.
For a spectrally stable traveling wave, we
consider the stability of the wave for the full partial differential equation.
We survey available methods and difficulties of them. We introduce the pointwise
semigroup method which has been used for traveling waves in conservation laws.
9. Xianping Li, Effect of
regularization on numerical simulation of phase change.
Regularization is commonly used in numerical
simulation of phase change problems. The choice of regularization method and
the parameter used therein affects greatly the accuracy of solution. A
numerical study of the issue will be presented in this talk.
10. Milenna Stanislavova, Nonlinear stability
and instability for Hamiltonian systems with symmetries.
The study of nonlinear stability of coherent
structures, such as soliton solutions, is very important and numerous
analytical techniques have been developed. From the spectrum of the
linearization one can typically produce stability results for dissipative
systems and only nonlinear instability results for conservative systems. I will
describe the available global techniques for proving orbital stability
(instability) results in the case of Hamiltonian systems with symmetries. The
main focus will be on particular examples of PDEs for which one can apply the
abstract theory with or without modifications.
11. Ventsislav
Ivanov, Chaotic
Synchronization.
The first usage of the logistic map can be
traced back to Pierre Francois Verhulst, a Belgian mathematician with a quest
for refining the Malthusian demographic model. Later usages include modeling
the surplus produced by species in the presence of population limiting factors
such as finite resources and death. Much interest in the map's chaotic regions,
formed by multiple period doubling bifurcations, has produced its latest usage
for generating random numbers. This talk will present the current state and
results generated by a chaos analysis tool aimed at analyzing the behavior
inside the map's chaotic regions. The goal of the research is to exploit this
apperant randomness, design a secure digital communication channel
(corresponding to the map's biotic potential value) and effectively transmit
sensitive information across arbitrary communication mediums.
12. Jingtang Ma, Convergence of
Moving Mesh Methods for Time-Dependent PDEs.
I will present the recent progress on the
convergence of the moving mesh methods for time-dependent PDEs. Two typical PDEs
whose solutions contain small layers and behave blow-up will be discussed. Brief
history and open questions will also be outlined in this talk.
This page is maintained by
Weizhang Huang.