Because of scale disparity and uncertainties, it is important to derive convergence results that are independent of the physical parameters. One of my main research goals has been to develop innovative numerical methods that converge independent of physical parameters. The research I have been involved with is strongly motivated by many fundamental issues that arise in practical applications of flows in porous media. Below I describe my research in more details.
Subsurface flows are often affected by heterogeneities in a wide range of length scales. High-contrast in the media properties brings an additional small scale into the problem, expressed as the ratio between low and high conductivity values. Because of disparity of scales, it is prohibitevly expensive to do detailed fine-scale simulations. Some of the challenging issues in this are the design of reduced models on a coarse grid and robust and optimal preconditioners that converge independent of physical parameters, such as small scales and the contrast in the media properties. I have made some contributions in this direction in my papers [10,11,17,18,19]. A review of this results and some other important ideas is presented in [12].
To convey the main idea of my work, for simplicity I consider
two-level domain decomposition preconditioners for flow equations
In our papers [10,11,17,18,19] , we propose a special
coarse spaces for two-level domain decomposition
preconditioners that provide an optimal (w.r.t. physical
parameters) preconditioners. The main idea behind the construction
of these coarse spaces is the use of a local eigenvalue problem
of the form
with a modified weight function
. The weight function is computed
as the pointwise energy of (multiscale) basis functions that
are carefully selected.
We show that the spectrum of this eigenvalue problem has a spectral
gap that allows us to indentify important features of the solution
and basis functions that are needed. We show that
with such construction, the coarse spaces only needs to contain
information and features related to
long channels (high-conductivity regions that connect the boundaries of
the coarse block). Coarse spaces with dimension
related only to the number of channels are optimal size
since it is known that one has to include the channels information in the
coarse space. We prove that
the convergence of two-level preconditioners is independent
of physical parameters.
In [11], we discuss and analyze the coarse-scale approximation of the solution using our multiscale basis functions. In particular, we present an error analysis that shows that more basis functions are required to achieve reasonable accuracy. In [17], we extend two-level approaches to multi-level methods within the framework of spectral Algebraic Multigrid (AMG). Our main objective is to show that one can achieve optimal (in terms of physical parameters) convergence of multigrid methods if basis functions at each level are chosen appropriately. In this work, the coarse spaces are constructed hierarchically. We show that the hierarchical construction preserves important features of the solution. One of the difficulties I faced is guaranteeing that the coarse space dimension is minimal, i.e., at coarse levels, we do not represent the inclusions separately.
In [16] we show how to use our methodology to design a robust iterations for nonlinear problems (e.g., Richard's equation). In [15,14] we extended the framework introduced in [18,19,11,10,17] to other equations such as the mixed version of (1) and Brinkman. The results in [15] are general and can be applied to many equations with important physical parameters that adversely affect the performance of iterative methods. In order to apply our results to an equation with important physical parameters, we require that the problem can be formulated in a weak sense with positive bilinear forms. The dimension of the resulting coarse problem is problem dependent since the number of small eigenvalues of the resulting local generalize eigenvalue may differ for each problem. In particular, finding optimal dimension coarse space for equations such as highly anisotropic elliptic problems ([13]), elasticity, and other applications of the framework introduced in [18,19,11,10,17] is matter of current research.
Media properties contain uncertainties, especially at the fine resolution. As permeability data is also collected at finest scales such as core scales, detailed geological models are constructed that contain the information about uncertainties. At these scales, we deal with large uncertainties associated with the fine grid information and robust convergence estimates for stochastic discretization that take into account the fine-scale uncertainties are needed. In this case, it is more advantageous to work with infinite dimensional stochastic space due to a large dimension of the stochastic space.
In my work, I have considered
log-normal random
field so that
is Gaussian and its
distribution is determined by its mean
and
covariance function
This leads to the
problem
on a suitable probability space with infinite
stochastic dimensions. A main theoretical
challenge related to this log-normal coefficient
is dealing with the lack of uniform ellipticity
of the coefficient. One of the results in [21]
is a new framework introduced to overcome this difficulty
and to derive error estimates as described below.
In
[35], Roman and Sarkis use the
white noise framework
of Hida and others to pose the problem, see
[28,29,31].
The probability space is the the Schwartz space of rapidly decreasing functions
. They use the family
of Borel
subsets of
and the probability measure,
, is given by the Bochner-Minlos theorem. The triplet
is the
-dimensional white noise probability space, and
is
called the white noise measure. The measure
is also
often called the (normalized) Gaussian measure on
.
Roman and Sarkis assume that the coefficient
is
bounded away from zero.
They expand the solution with respect to special
basis of
made of multivariate
(Fourier-Hermite) polynomials
of random variables.
This series
is called the (Fourier-Hermite) chaos expansion.
They proposed a
finite element approximation of the problem by truncating the
chaos expansion of the solutions. They
provide neither a priori error estimate nor numerical experiments.
In
[21]
we introduced adequate norms in the space
and derive
a priori error estimates for the Finite Element approximations proposed
in [35]. See [2] and references therein.
This work uses tools from the white noise
calculus, also known as infinite dimensional calculus
(see [28,29,31,3,34] and references therein).
In the more theoretical and very interesting submitted manuscript [26], we proved the regularity
results required in [21]. In [26] we use tools from the white noise
calculus and the Malliavin calculus. In particular, we
prove equivalence of two important class of norms used
to define regular (in
) random functions
.
The first norms are weighted chaos norms used in [21] to get a priori
error estimates.
The other norms are Gaussian Sobolev norms, that is, the analogous
to Sobolev norms using the Gaussian measure
.
This second norms is more adequate to prove regularity
results, see [26].
Some numerical comparisons and possible numerical and theoretical advantages of using the framework in [21,26] are object of our current research.
In many porous media applications, it is important to consider the coupling of free flow (described by Stokes or Navier-Stokes flow) and porous media flows. This occurs, for example, in the coupling of flow in the reservoir (described by Darcy's equations) and well bore (described by Navier-Stokes equations). The interface conditions that are often used to couple porous media and Stokes flows are Beavers-Joseph-Saffman conditions that is some type of upscaling of Stokes flow near the interface. The main challenge is to design efficient coupling of the discretization of Stokes equations and Darcy equations (e.g., multiscale discretization of Darcy described earlier). This has been a part of my research.
The purpose of my research
is to analyze the coupling across an interface of fluid and
porous media flows. It is considered an incompressible fluid in a
region
that can flow
both ways across an interface
into a saturated porous medium domain
.
The model consists of Stokes equations in the
fluid region,
, and Darcy law for the filtration velocity in
the porous medium region,
. The transmission
conditions on the interface
are the Beavers-Joseph-Saffman
conditions (see [1,30,36]).
This model appears in several applications like well-reservoir
coupling in petroleum engineering, transport of substances across
groundwater and surface water, and (bio)fluid-organ
interactions.
In [20,25], we
consider this model. We analyze inf-sup conditions and optimal a priori error
estimates associated with the continuous and discrete
formulations of this Stokes-Darcy system.
The continuous inf-sup analysis uses tools developed in
[25] and [32].
For the discretization of this problem,
Taylor-Hood and Raviart-Thomas finite elements are used
for the free fluid and porous medium subdomains, respectively.
Using mortar finite element analysis and
appropriate scaled norms, we show that the constants that appear on the
a priori error bounds do not depend on the viscosity, permeability and
ratio of mesh parameters. Numerical experiments are presented to confirm
the theoretical results.
For standard choices of finite elements spaces
and due to the small value of the permeability parameter
of the porous medium, the resulting discrete symmetric saddle point
system is very ill conditioned. In [22,24],
we design and analyze two preconditioners for the non-matching
meshes case. One of the preconditioners is based on Balancing Domain
Decomposition (BDD) methods and
the other one based on Finite Element by Tearing and Interconnecting (FETI)
methods.
For both methods, we derive condition number
estimates of order
. In
case the fluid discretization is finer
than the porous side discretization, we derive a better estimate of
order
for the FETI preconditioner.
Here,
is the mesh size
of the porous side triangulation. The constants
and
are independent of the permeability
, the
fluid viscosity
, and
the mesh ratio across the interface.
Numerical experiments confirm the sharpness of
the theoretical estimates. These two solvers
are modular in the sense that they need the solution
of a whole Stokes and/or Darcy problem in each iteration.
This may represent a drawback of the method if these solves
are not available due to time or memory budget constrains.
In [23] we present some preliminary
and numerical
results of some (multisubdomain) FETI-DP methods
for the coupling of Stokes and Darcy. These new methods
allow solving the Stokes/Darcy coupled model
iteratively using solution in small
(either Darcy or either Stokes) subdomains.
Each subdomain is a subregion of the
Stokes or the Darcy
type. These works use the previous
multisubdomain solvers for Stokes [33]
and Darcy [38].
See also references therein.
The numerical analysis and
other aspects of the design of methods
similar to the methods we presented in [23]
are under current
research.
The pressure equation (1)
appears in the mathematical studies of the transport of pollutants in
ground-water and of oil recovery processes. When
is piecewise constant on
(or
close to a piecewise constant function),
a discontinuous Galerkin (DG) approximation of
these elliptic problems can be used.
DG methods are becoming more and more popular for the approximation of
PDEs since they are well suited for dealing with regions with
complex geometries or discontinuous coefficients. In my work,
we have extended the design and analysis of
classical domain decomposition methods to DG discretization
as described below.
The region
in (1)
is assumed to be a geometrically conforming union of disjoint polygonal subregions
.
The discontinuities of the coefficients occur across
. The problem is approximated by a
conforming finite element method (FEM) based on a
matching triangulation inside each
,
. We
allow these triangulations to be nonmatching across
,
. This kind of triangulation
and composite discretization is motivated, among a variety of reasons,
by the regularity of the solution of the problem being discussed.
The discrete problem is formulated using the symmetric DG
method with interior penalty terms on
,
with the harmonic average values of
discontinuous coefficients of the original problem on common
faces of substructures. See [4,9] and references therein.
In [8], we analyze Neumann-Neumann
(N-N) algorithms for the resulting discrete problem.
N-N methods
are
well known for the standard conforming and nonconforming
discretizations, see [37] and
references therein.
This work
was based on the previous work presented in a
technical report by Dryja and Sarkis where
they analyze several DG preconditioners of Neumann-Neumann type.
We present numerical experiments that verify the theoretical estimates.
In [5] and [6], we have also successfully extended these
preconditioners to the Balancing Domain Decomposition (BDD) method and
the Balancing Domain Decomposition with Constrains (BDDC) method,
respectively. Numerical experiments are presented.
In [7], we extend the BDD and BDDC algorithm for the
geometrically nonconforming case. We present numerical experiments
to verify the theory.
All the methods developed above assume particular distributions of the jumps of the coefficients. Our current research seeks to develop domain decomposition preconditioners for the case of more general distributions of coefficients and DG discretizations. In particular, we are studying optimal ways to apply some of the ideas introduced in [18,19,11,10,17] to this case.
With my Phd and my experience after it, I have mastered several important modeling, numerical and mathematical tools. Also, I have become aware of many other important tools and topics in pure and applied mathematics. I am confident I can easily continue with my current research areas and current collaborations. I plan to continue developing efficient numerical methods for heterogeneous problems with multiple scales and uncertainties. As mentioned in all the topics before, there is still several research directions that I can follow up and continue my research. These directions are valid important research topics. I am also confident that I will be adding some research topics of my interest as well as starting new collaborations. Some of these topics are motivated because they are fields where I can apply the tools and areas I already know. Some others are motivated by the fact that Ill be learning and developing new tools. Possible future new research directions I consider to include into my list of research topics are: mulstiscale finite element methods for flows on rough surfaces (already started and we have results and we are preparing manuscript) ensemble-level preconditioners for stochastic problems (already started and we have nice results), Free interface problems (already started and we have some preliminary results), abstract theory for non-symmetric domain decomposition solvers, multiscale model reduction methods for heterogeneous problems, optimal preconditioners for nonlinear problems, discretization of eigenvalue problems, inverse coefficient elliptic problems, solvers and multiscale finite element methods for Stokes/Darcy coupling for the case of complex heterogeneous porous media, parabolic problems with random coefficients and temporal noise, etc.