Numerical
Mathematics Mini-symposia / Special Sessions in 47th BAMC –
4-7 April 2005
Tuesday
- Numer Math (I) |
14:00-14:45 |
A1 |
Prof Chris
J Budd (Invited) Scale Free Adaptive Methods for
Partial Differential Equations |
|
Numerical
PDE |
14:45-15:15 |
A2 |
Dr Keith
Davey Successive Preconditioning
For The Iterative Solution Of Non-Linear
Algebraic Equations |
|
Nonlinear
Iterations |
|
15:15-15:20 |
|
(Break) |
|
|
|
15:20-15:50 |
A3 |
Mr J
Savage / Dr K Chen / Prof W G Li Fast multilevel methods for
image processing |
|
Multigrid
Methods/Image |
|
15:50-16:20 |
A4 |
Dr Peter
J. Young Network Analysis through
Numerical Solution of Computer-generated Mathematical Equations |
DSTL |
Linear/Nonlinear
Iterations |
|
|
|
|
|
|
|
Wednesday
- Numer Math (II) |
09:15-09:45 |
B1 |
Dr
Sapna Somani A Wavelet
Preconditioner For Two Dimensional Elliptic Problem |
|
Wavelet
Poissons |
09:45-10:15 |
B2 |
Dr A.
Shidfar/R. Pourgholi An approximate stable solution for an
inverse heat conduction problem |
|
Numerical
Inverse Probs |
|
10:15-10:30 |
|
(Break) |
|
|
|
10:30-11:00 |
B3 |
Dr Dugald
B Duncan / Penny J Davies Numerical approximations of time domain
electromagnetic scattering |
|
Numerical
Scattering |
|
11:00-11:30 |
B4 |
Dr Stephen
Langdon / Prof S.N. Chandler-wilde A boundary element method for high
frequency scattering by convex polygons |
|
Numerical
Scattering |
|
|
|
|
|
|
|
Thursday -
Numer Math (III) |
09:15-09:40 |
C1 |
Prof
Ronald Smith / M K Bowen Compact Schemes for
Evolution Equations |
|
High Order
Time Stepping |
09:40-10:05 |
C2 |
Detecting small solutions
to a class of multi-delay differential equations: Two approaches |
|
Delay ODEs |
|
10:05-10:30 |
C3 |
Dr N B
Petrovskaya The Impact of Grid Cell Geometry
on the Least-Squares Gradient reconstruction |
|
Numerical
Least-squares |
|
10:30-10:45 |
|
(Break) |
|
|
|
10:45-11:10 |
C4 |
Dr Teijo
Arponen 2-tensor invariants in
numerical integration |
|
Numerical
Symplectic ODE |
|
11:10-11:35 |
C5 |
Dr.
A.Lukyanov A combined BIE-FE method
for dynamic wetting |
|
FEM-BEM
coupling |
|
|
|
|
|
|
|
A1
Prof Chris J
Budd (Invited)
Title = Scale Free Adaptive Methods for Partial
Differential
equations
Abstract =
One of the key qualitative features of the solution
of a nonlinear partial differential equation is the evolution of behaviour on
many different length scales. Examples are the continuum of length scales in
turbulence modelling, the formation of shocks in fluid mechanics and the
appearance of singularities in nonlinear optics. Traditional numerical methods
perform poorly in such situations as the discretisation imposes an artificial
length scale on the problem. Ideally, to give the correct qualitative behaviour
a numerical method should perform equally well at all length scales. I will
show in this talk that by using a mixture of ideas from Lie group theory to
meteorology it is possible to construct
adaptive numerical methods which can effectively
capture many different scales of behaviour. I will illustrate this with
examples from optics and combustion.
A2
Dr
K. DAVEY
\title{Successive
Preconditioning For The Iterative Solution Of
Non-Linear Algebraic Equations}
\abstract{ABSTRACT
Ill-conditioned
algebraic equations involving positive definite matrices arise in many physical
representations. A particular problem
of interest is ring rolling simulation using a constrained-flow formulation and
the finite element method, as this gives rise to poorly-conditioned non-linear
equations that require repeated solution.
The imposition of a volume-constancy constraint has the effect of
producing an eigen-spectrum with a cluster of relatively small
eigenvalues. This makes traditional
iterative solution methods such as the conjugate gradient method unreliable,
typically failing to converge. Some
success has been reported with the quasi-Newton method but again the eigenvalue
distribution makes for an unreliable performance. Direct methods are reliable but the
associated computational costs are extreme making the analysis impracticable. This work is concerned with a method
that unifies the conjugate gradient and the quasi-Newton method and is called
the Successive Preconditioned Conjugate Gradient Method (SPCGM). Both the conjugate gradient and
quasi-Newton methods possess quadratic termination, i.e. for exact arithmetic
the minimum for a quadratic function can be found within a maximum of n
iterations for an n-degree problem.
This property is shown to be preserved with the SPCGM, which in its
extreme form collapses to either the conjugate gradient or the quasi-Newton method. A feature of the method is the automatic
development of a suitable preconditioner that adapts as the equations
change. In the context of
non-linear problems the SPCGM can be classified as an inexact
[1]
C. T. Kelly, 'Iterative Methods for Linear and Non-linear Equations',
[2]
H. A. van der Vorst and C. Vuik, 'GMRESR: A Family of Nested GMRES Methods',
Numerical Linear Algebra and Applications, Vol. 1, pp. 369-386, (1994).
[3]
T. Eirola and O. Nevanlanna, 'Accelerating with Rank-One Updates', Linear
Algebra and its Applications, Vol. 121, pp. 511-520, (1989).
[4] O. Axelsson and P. S. Vassilevski, 'A Black Box
Generalised Conjugate Gradient Solver with Inner Iterations and Variable-step
Preconditioning',
A3
Mr
J Savage / Dr K Chen / Prof W G Li,
\title{Fast
multilevel methods for image processing}
ABSTRACT:
The variational partial
differential equation (PDE) approach for image denoising restoration leads to
PDEs with nonlinear and highly non-smooth coefficients. Such PDEs present
severe difficulties for the convergence of standard multigrid methods. In this
talk we shall present some of our recent work on developing fast algorithms in
several ways: (i) the linear multigrid methods in nonlinear iterations; (ii)
fully nonlinear multigrid methods; (Iii) the algebraic multigrid methods
(AMGs); (iv) the multigrid for the primal-dual system; (v) the multigrid
methods for the optimisation formulation. Experiments are shown to demonstrate
the improvements obtained.
A4
Dr
Peter J. Young
DSTL
\title{Network
Analysis through Numerical Solution of Computer-generated Mathematical
Equations}
\abstract{This presentation describes research that
has employed automatic generation of mathematical equations in symbolic form on
a computer for problem analysis and solution. The research was initiated
through the development of a computer model to permit analysis of call blocking
for a generic communications network in which inter-nodal bandwidths and
Poisson distributed, traffic calling patterns were specified. A novel approach
was developed in which the equations describing probability of call blocking
were automatically constructed in symbolic form for a user-specified
communications network. The resulting set of coupled, nonlinear equations was
then solved using an iterative numerical technique. The symbolic form of a
single equation consisted of nested collections of pointers to network
variables and mathematical operators. Given their symbolic forms, the equations
were parsed permitting recalculation of network variables from earlier
estimates until convergence was achieved. Verification of the
computer-generated equations was performed through comparison to equations
derived by hand for simple network configurations. The approach quickly
demonstrated its utility when larger, more complex networks were considered in
which the algebraic form of the equations becomes increasingly complicated.
Validation of the network communications model with
B1
Dr
Sapna Somani
\title{A
Wavelet Preconditioner For Two Dimensional Elliptic Problem}
\abstract{In
this paper we have made an attempt to solve Poisson's
equation
in two dimension using preconditioning concepts. We consider the representation
of
elliptic differential operators in wavelet bases and preconditioner based on
wavelet
methods.
The method for solving Poisson equation for two dimensions and three dimensions
has been implemented in Matlab based on work
of G. Beylkin [1]. In Galerkin
approach we
get
a ill-conditioned system. Here, we have made an attempt to show that the
condition
number of the reduced matrix is of size O(1)
using preconditioning.
References
[1].
G. Beylkin: On the representation
of operators in bases of compactly
supported
wavelets, SIAM J. on Numerical Analysis, vol. 6, No. 6, pp. 1716-1740
[2]
I. Daubechies, Orthonormal bases of compactly supported
wavelets,Comm.Pure.Appl.
Math.
41(1988), 909-996
B2
Dr
A. Shidfar/R. Pourgholi,
An
approximate stable solution for an inverse heat conduction problem
\abstract{
This paper deals the determination of a
stable solution for an Ill-posed
Inverse heat conduction
problem (IHCP). By using the Chebyshev polynomials based function an approximate stable solution
to the IHCP will be determined in
finite or infinite domain.
(Keywords: Inverse heat conduction
problem, Existence, Stability;
AMS Subject Classification: 35K05, 58G11,
93D05)}
B3
Dr
Dugald B Duncan / Dr Penny J Davies
\title{Numerical
approximations of time domain electromagnetic scattering}
\abstract{We
derive and analyse collocation approximations of retarded potential integral
equations (RPIEs) arising as models of
scattering
of waves from thin wire and strip antennas. We Fourier
analyse
the temporal stability of spatially exact piecewise
constant
and linear in time approximations of these three RPIEs.
Numerical
results are presented for practical schemes that are
piecewise
constant or linear in time and space, and these are in
close
agreement with the predictions of the Fourier analysis.}
B4
Dr
Stephen Langdon / Prof S.N. Chandler-Wilde
\title{A
boundary element method for high frequency scattering by convex polygons}
\abstract{Standard boundary or finite element
methods for problems of high frequency acoustic scattering by convex polygons
have a computational cost that grows in direct proportion to the frequency of
the incident wave. Here we present
a novel Galerkin boundary element method, using plane wave basis functions on a
graded mesh, for which the number of degrees of freedom required to achieve a
prescribed level of accuracy grows only logarithmically with respect to
frequency.}
C1
Prof
Ronald Smith / M K Bowen
\title{Compact Schemes for Evolution Equations}
\abstract{A method is given for the construction of
high-accuracy compact schemes for the numerical solution of linear evolution
equations. It brings together exact
time stepping and expansions for
the error in difference approximations to spatial derivatives. The accuracy permits the use of a smaller
computational module than is usual. Three points in $x$ suffice for the linear Korteweg de Vries equation with damping
$$
\partial_t c+\lambda \, c+\, u\, \partial_xc
-\kappa\partial_x^2 c +\frac{1}{6}h^2u\partial_x^3c =0
\quad
{\rm with} \quad \kappa,\, h \ge 0.
$$
Direct numerical modelling of $\partial_x^3 c$ would
have required at least four points
in $x$. For the severe
test-case of a delta-function initial condition, the computations fail to
replicate the sub-grid oscillatory tail far to the rear. However, the
resolvable part oscillatory tail and the forward skewness caused by the
$\partial_x^3 c$ term are
accurately replicated.
}
C2
Prof
Neville J Ford / Dr Patricia M. Lumb
\title{Detecting small solutions to a class of
multi-delay differential equations: Two approaches}
\abstract{Certain non-autonomous delay differential
equations are known to admit small solutions (solutions that are not
identically zero but which tend to zero more quickly than any exponential such
that $\lim_{t\rightarrow \infty}e^{kt}x(t)=0$, for all $k \in \bf{R}$). The detection of non-trivial small
solutions is a key tool for the mathematical analyst.\newline
\noindent We consider periodic delay differential
equations of the form
\[
\dot x(t)=\sum_{j=0}^{m}b_j(t)x(t-jw), x_s=\phi,
\mbox{ } t\ge s,
\]
where $b_j$, $j=0,1,...,m$ are continuous periodic
functions with period $\omega$.\newline
We are interested in detecting the presence, or
otherwise, of so-called \emph{small} solutions using a numerical method.
In our earlier work we have successfully detected
the presence of small solutions to linear periodic delay differential equations
with a single delay. We show how
our approach can be adapted for the multi-delay equation. We then develop a more sophisticated
approach using Floquet solutions.
We compare the two approaches and discuss the ease and clarity with
which the presence, or otherwise, of small solutions is detected. We present illustrative examples.
We have developed an algorithm that automates the
detection of small solutions to linear periodic delay differential equations
with a single delay. We indicate how our algorithm is adapted for equations
with multiple delays.
}
C3
Dr N B Petrovskaya
\title{The Impact of Grid Cell Geometry on the
Least-Squares Gradient reconstruction}
\abstract{Numerical solution of many modern problems
in physics and
engineering often requires to approximate the
solution gradient on
grid cells which are almost degenerate. We consider
the problem of
the least-squares gradient approximation on
two-dimensional
unstructured grids with "bad" cells. It
will be discussed how the
accuracy of the least-squares approximation depends
on the cell
geometry. We analyze a simple geometry and
demonstrate that
introducing weight coefficients into the problem may
essentially
help to improve the accuracy of the least-squares approximation.
Based on the results of our analysis, a heuristic
choice of the
weights in a general least-squares procedure is
suggested. Our
approach is illustrated by numerical tests.
}
C4
Dr Teijo Arponen
\title{2-tensor invariants in numerical integration}
\abstract{In numerical geometric integration of ODEs
one is concerned about preserving geometrical properties of the flow under
discretization. The best known examples are Hamiltonian ODEs which are
ubiquitous in applications. Today it is well known that conserving the
symplectic structure is the correct way to solve these Hamiltonian ODEs
numerically. Similar results are
known for Lie-group equations, to mention another class of applications.
But the key question in preserving "the"
structure is, how do we
define structure? In Hamiltonian case the answer is known:
it's the
symplectic structure. In this talk, I introduce
2-tensor-invariants.
These are defined for any ODE and they are and
algebraic generalization of symplectic structure.
This is work in progress and I present some
intermediate results which show this to be a promising approach to develop
geometric integrators to new classes of equations.
C5
Dr.
A.Lukyanov
\title{A combined BIE-FE method for dynamic wetting}
The method is applied to curtain coating where it
allows one to resolve the fine dynamics near the contact line and incorporate
the ``extra'' physics of interface formation, whereas the BIE component of the
method makes it capable of handling a wide range of shapes of the flow domain
with significant economy in computational time and memory. A combined Boundary
Integral Equation (BIE) and Finite Element (FE) technique is developed and
applied to curtain coating by high-viscosity liquids in the regime of creeping
flow. The idea of the new method is to combine advantages and compensate
limitations inherent in the BIEM and FEM. The BIEM uses the exact solution of
the Stokes equations in the bulk thus, on the one hand, reducing the problem to
integral equations along the boundary of the flow domain but, on the other
hand, it applies only when this boundary is smooth. The FEM can handle domains
with boundaries having such features as contact angles or cusps and it is not
limited to the Stokes equations (hence can incorporate extra physics that can
be important near such features). However, since the FEM makes it necessary to
tessellate the whole domain and solve the problem there, this becomes a
nontrivial and time-consuming task for domains with complex shapes. The
combined BIE-FE method employs finite elements to deal with the regions
comprising singularities of curvature of the boundary and utilizes the
boundary-integral representation for the rest of the flow. The two methods are
coupled along an internal boundary using mutually compatible representation of
the unknowns there.
The method is applied to curtain coating where it
allows one to resolve the fine dynamics near the contact line and incorporate
the ``extra'' physics of interface formation, whereas the BIE component of the
method makes it capable of handling a wide range of shapes of the flow domain
with significant economy in computational time and memory.
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END