** Papers:**

** Abstract.**
In this work we study a novel adaptive nonlinear filtering applied to the Leray-\(\alpha\) model. Unlike its classical counterpart, the new filtering requires the solution of a linear elliptic problem, with constant coefficients, at each time step. The action of the adaptive nonlinear filter throughout the integration time is refactorized as the solution of a linear system, with the same matrix and multiple right hand-sides. We discuss the theoretical properties of the new filtering approach applied to the BDF2 approximation of the Leray-\(\alpha\) model. Numerical tests demonstrate that the filtering damps the high wave number modes of the solution and has similar level of accuracy with the classical filter. Some benchmark results are also presented.

** Abstract.**
We propose a novel, time adaptive, strongly-coupled partitioned method for the interaction between a viscous, incompressible fluid and a thin elastic structure.
The time integration
is based on the refactorized Cauchy's one--legged `\(\theta-\)like' method, which consists of a backward Euler method using a \(\theta\tau_n\)--time step
and a forward Euler method using a \((1-\theta)\tau_n\)--time step.
The bulk of the computation is done by the backward Euler method, as
the forward Euler step is equivalent to (and implemented as) a linear extrapolation.
The variable \(\tau_n\)--time step integration scheme is
combined with the partitioned, kinematically coupled \(\beta-\)scheme, used to decouple the fluid and structure sub--problems. In the backward Euler step, the two sub--problems are solved in a partitioned sequential manner, and iterated until convergence.
Then, the fluid and structure sub--problems are
post--processed /extrapolated in the forward Euler step, and finally the \(\tau_n\)--time step is adapted.
The refactorized Cauchy's one--legged `\(\theta-\)like' method used in the development of the proposed method is equivalent to the midpoint rule when \(\theta\)=\(\frac12\), in which case the method is non--dissipative and second--order accurate.
We prove that the sub--iterative process of our algorithm is linearly convergent,
and that the method is unconditionally stable when \(\theta \geq \frac12\).
The numerical examples explore the properties of the method when both fixed and variable time steps are used, and in both cases shown an excellent agreement with the reference solution.

** Abstract.**
We analyze a second-order accurate implicit-symplectic (IMSP) scheme for reaction-diffusion systems modeling spatiotemporal dynamics of predator-prey populations. We prove stability and errors estimates of the semi- discrete-in-time approximations, under positivity assumptions. The numerical simulations confirm the theoretically derived rates of convergence and show an improved accuracy in the second-order IMSP in comparison with the first-order IMSP, at same computational cost.

** Abstract.**
The midpoint method can be implemented as a sequence of Backward Euler and Forward Euler solves with half time steps, allowing for improved performance of existing solvers for PDEs. We highlight the advantages of this refactorization by considering some specifics of implementation, conservation, error estimation, adaptivity, stability, and performance on several test problems.

** Abstract.**
The one-leg, two-step time-stepping scheme proposed by Dahlquist, Liniger and Nevanlinna
has clear advantages in complex, stiff numerical simulations: unconditional \(G\)-stability for variable time-steps and second-order accuracy.
Yet it has been underutilized due, partially, to its complexity of direct implementation.
We prove herein that this method is equivalent to the backward Euler method with pre- and post arithmetic steps added. This refactorization eases implementation in complex, possibly legacy codes.
The realization we develop
reduces complexity, including cognitive complexity
and increases accuracy over
both first order methods and constant time steps second order methods.

** Abstract.**
In this work, we develop a second-order nonlinear filter based stabilization scheme for high Reynolds number flows. We prove the unconditional stability of the method, establish the second order consistency and discuss the dynamical tuning of the relaxation parameter. The scheme is then validated against experimental data for an isothermal turbulent flow in a Staggered Tube Bundle at Reynolds number of 18000. Numerical results are found to be in an overall good qualitative and quantitative agreement with the benchmark results.

** Abstract.**
This work focuses on the derivation and the analysis of a novel, strongly-coupled partitioned method for fluid-structure interaction problems. The flow is assumed to be viscous and incompressible, and the structure is modeled using linear elastodynamic equations. We assume that the structure is thick, i.e., described in the same dimension as fluid. Our newly developed numerical method is based on generalized Robin boundary conditions, as well as on the refactorization of the Cauchy's one-legged `\(\theta\)-like' method, written as a sequence of Backward Euler - Forward Euler problems. This family of methods, parametrized by \(\theta\), is B-stable for any \(\theta\in [\frac{1}{2},1]\) and second-order accurate for \(\theta=\frac{1}{2}+ {\cal O}(\tau)\), where \(\tau\) is the time step. In the proposed algorithm, the fluid and structure sub-problems, discretized using the Backward Euler scheme, are first solved iteratively until convergence. Then, the variables are linearly extrapolated, equivalent to solving Forward Euler problems. We prove that the iterative procedure is convergent, and that the pro- posed method is stable provided \(\theta\in [\frac{1}{2},1]\). Numerical examples explore convergence rates using different values of parameters in the problem, and compare our method to other strongly-coupled partitioned schemes from the literature. We also compare our method to both a monolithic and a non-iterative partitioned solver on a benchmark problem with parameters within the physiological range of blood flow, obtaining an excellent agreement with the monolithic scheme.

** Abstract.**
An alternative formulation of the midpoint method is employed to analyze its advantages as an implicit second-order absolutely stable timestepping method. Legacy codes originally using the backward Euler method can be upgraded to this method by inserting a single line of new code. We show that the midpoint method, and a theta-like generalization, are B-stable. We outline three estimates of local truncation error that allow adaptive time-stepping.

** Abstract.**
The two-step time discretization proposed by Dahlquist, Liniger and
Nevanlinna is variable step \(G\)-stable. (In contrast, for increasing time
steps, the BDF2 method loses A-stability and suffers non-physical energy
growth in the approximate solution.) While unexplored, it is thus ideal for
time accurate approximation of the Navier-Stokes equations. This report
presents an analysis, for variable time-steps, of the method's stability and
convergence rates when applied to the NSE. It is proven that the method is
variable step,
unconditionally, long time stable and second order accurate. Variable step
error estimates are also proven. The results are supported by several
numerical tests.

** Abstract.**
We propose a BOundary Update using Resolvent (BOUR)
partitioned method, second-order accurate in time, unconditionally stable, for the interaction between a viscous, incompressible fluid and a thin structure. The method is algorithmically similar to the sequential Backward Euler - Forward Euler implementation of the midpoint quadrature rule. (i) The structure and fluid sub-problems are first solved using a Backward Euler scheme, (ii) the velocities of fluid and structure are updated on the boundary via a second- order consistent resolvent operator, and then (iii) the structure and fluid sub-problems are solved again, using a Forward Euler scheme. The stability analysis based on energy estimates shows that the scheme is unconditionally stable. Error analysis of the semi-discrete problem yields second-order convergence in time. The two numerical examples confirm the theoretical convergence analysis results and show an excellent agreement of the proposed partitioned scheme with the monolithic scheme.

** Abstract.**
The magnetohydrodynamics
flows are governed by the Navier-Stokes equations coupled with the
Maxwell equations.
We propose
a partitioned, variable step, second-order in time,
method for the evolutionary full MHD equations, at *high* magnetic Reynolds number.
The method is based on the refactorization of the midpoint rule.
We prove the convergence of the subiterates, the energy equality at the discrete time levels, and the conservation of energy, cross-helicity and magnetic helicity.

** Abstract.**
There has been a surge of work on models for coupling surface-water with groundwater flows which is at
its core the Stokes-Darcy problem, as well as methods for uncoupling the problem into subdomain, subphysics solves. The
resulting (Stokes-Darcy) fluid velocity is important because the flow transports contaminants. The numerical analysis and
algorithm development for the evolutionary transport problem has, however, focused on a quasi-static Stokes-Darcy model and
a single domain (fully coupled) formulation of the transport equation. This report presents a numerical analysis of a partitioned
method for contaminant transport for the fully evolutionary system. The algorithms studied are unconditionally stable with one
subdomain solve per step.

** Abstract.**
The existence of solutions to the Boussinesq system driven by random exterior forcing terms both in the velocity field
and the temperature is proven using a semigroup approach. We also obtain the existence and uniqueness of an invariant
measure via coupling methods.

** Abstract.**
We propose and analyze a novel, second order in time, partitioned method for the interaction between
an incompressible, viscous fluid and a thin, elastic structure. The proposed numerical method is based on the Crank-Nicolson discretization scheme, which is used to decouple the system into a fluid sub-problem and a structure subproblem.
The scheme is loosely coupled, and therefore at every time step, each sub-problem is solved only once.
Energy and error estimates for a fully discretized scheme using finite element spatial discretization are derived. We
prove that the scheme is stable under a CFL condition, second-order convergent in time and optimally convergent
in space. Numerical examples support the theoretically obtained results and demonstrate long time stability on a
realistic example of blood flow.

** Abstract.**
The explicit weakly-stable second-order accurate leapfrog scheme is widely used in the numerical models of weather and climate,
in conjunction with the Robert-Asselin (RA) and Robert-Asselin-Williams (RAW) time filters.
The RA and RAW filters successfully suppress the spurious computational mode associated with the leapfrog method,
but also weakly damp the physical mode and degrade the numerical accuracy to first-order.
The recent higher-order Robert-Asselin (hoRA) time filter reduces the undesired numerical damping of the RA and RAW
filters and increases the accuracy to second up-to third-order. We prove that the combination of leapfrog-hoRA and Williams'
step increases the stability by 25%, improves the accuracy of the amplitude of the physical mode up-to two significant digits,
effectively suppresses the computational modes, and further diminishes the numerical damping of the hoRA filter.

** Abstract.**
Magnetohydrodynamics (MHD) studies the dynamics of electrically conducting fluids, involving Navier-Stokes equations coupled with Maxwell equations via
Lorentz force and Ohm's law.
Monolithic methods, which solve fully coupled MHD systems, are computationally expensive.
Partitioned methods, on the other hand, decouple the full system and solve subproblems in parallel, and thus reduce the computational cost.
This paper is devoted to the design and analysis of a partitioned method for the MHD system in the Elsässer variables.
The stability analysis shows that for magnetic Prandtl number of order unity, the method is unconditionally stable.
We prove the error estimates and present computational tests that support the theory.

** Abstract.**
The numerical solution of reaction diffusion systems modelling predator-prey dynamics using implicit-symplectic (IMSP)
schemes is relatively new. When applied to problems with chaotic dynamics they perform well, both in terms of computational effort
and accuracy. However, until the current paper, a rigorous numerical analysis was lacking. We analyze the semi-discrete
in time approximations of a first-order IMSP scheme applied to spatially extended predator-prey systems.
We rigorously establish semi-discrete *a priori* bounds that guarantees positive and stable solutions,
and prove an optimal *a priori* error estimate. This analysis is an improvement on previous theoretical results
using standard implicit-explicit (IMEX) schemes. The theoretical results are illustrated via numerical experiments
in one and two space dimensions using fully-discrete finite element approximations.

** Abstract.**
This report presents a summary of the numerical analysis of time filters used to control the
unstable mode in the Crank-Nicolson-Leapfrog discretization of evolution equations.

** Abstract.**
We present the error analysis of three time-stepping schemes used
in the discretization of a nonlinear reaction-diffusion equation with Neumann
boundary conditions, relevant in phase transition. We prove\(L^1(L^1)\) stability by
maximum principle arguments, and derive error estimates using energy methods
for the implicit Euler, and two implicit-explicit approaches, a linearized
scheme and a fractional step method. A numerical experiment validates the
theoretical results, comparing the accuracy of the methods.

** Abstract.**
We propose a new numerical regularization for finite element spatial discretization of the Navier-Stokes equations (NSE),
a family of implicit-explicit (IMEX) second order timestepping schemes. The method combines a linear treatment of the advection term
and stabilization terms that are proportional to discrete curvature of the solutions in both velocity and pressure.
Only a linear Oseen problem needs to be solved at each timestep. We prove that the methods are unconditionally stable and second order
convergent. Numerical examples verify the convergence rate and show the stabilization term clearly improves the stability of the tested flow.

** Abstract.**
There has been a surge of work on models for coupling surface-water
with groundwater flows which is at its core the Stokes-Darcy problem. The resulting
(Stokes-Darcy) fluid velocity is important because the flow transports contaminants.
The analysis of models including the transport of contaminants has, however, focused on a
quasi-static Stokes-Darcy model. Herein we consider the fully evolutionary system including
contaminant transport and analyze its quasi-static limits.

** Abstract.**
We present the linear analysis of recent time filters used in numerical weather prediction. We focus on the accuracy and the stability of the
leapfrog scheme combined with the Robert-Asselin-Williams filter, the higher-order Robert-Asselin type time filter, the composite-tendency
Robert-Asselin-Williams filter and a more discriminating filter.

** Abstract.**
In this work, we present a comprehensive study of several partitioned methods for the coupling of flow and mechanics. We derive energy estimates for each method for the fully discrete problem. We write the obtained stability conditions in terms of a key control parameter defined as a ratio of the coupling strength and the speed of propagation. Depending on the parameters in the problem, give the choice of the partitioned method which allows the largest time step.

** Abstract.**
A method has been developed recently by the third author, that allows for decoupling of the evolutionary full MagnetoHydroDynamics
(MHD) system in the Elsässer variables. The method entails the implicit discretization of the subproblem terms and the
explicit discretization of coupling terms, and was proven to be unconditionally stable.
In this paper we build on that result by introducing a high-order accurate deferred correction method, which also decouples the MHD
system. We perform the full numerical analysis of the method, proving the unconditional stability and second order accuracy of the
two-step method. We also use a test problem to verify numerically the claimed convergence rate.

** Abstract.**
The Robert-Asselin (RA) time filter combined with leapfrog scheme is widely used in numerical models of weather and climate.
It successfully suppresses the spurious computational mode associated with the leapfrog method, but it also weakly dampens the physical mode
and degrades the numerical accuracy.
The Robert-Asselin-Williams (RAW) time filter is a modification of the RA filter that reduces the undesired numerical damping of RA filter
and increases the accuracy.
We propose a higher-order RA (hoRA) type time filter which effectively suppresses the computational modes and achieves *third-order* accuracy with the same
storage requirement as RAW filter. Like RA and RAW filters, the hoRA filter is non-intrusive, and so it would be easily implementable.
The leapfrog scheme with hoRA filter is almost as accurate, stable and efficient as the intrusive third-order Adams-Bashforth (AB3) method.

** Abstract.**
This paper addresses an open question of how to devise numerical schemes for approximate deconvolution fluid flow models that are
efficient, unconditionally stable, and optimally accurate. We propose, analyze and test a scheme for these models that has each of
these properties for the case of homogeneous Dirichlet velocity boundary conditions. There are several important components to the
derivation, both at the continuous and discrete levels, which allow for these properties to hold. The proofs of unconditional
stability and optimal convergence are carried out through the use of a special choice of test function and some technical estimates.
Numerical tests are provided that confirm the effectiveness of the scheme.

** Abstract.**
Stochastic collocation method has proved to be an efficient method and been widely applied to solve various
partial differential equations with random input data, including Navier-Stokes equations.
However, up to now, rigorous convergence analyses are limited to linear elliptic and parabolic equations;
its performance for Navier-Stokes equations was demonstrated mostly by numerical experiments.
In this paper, we present an error analysis of the stochastic collocation method for a semi-implicit
Backward Euler discretization for NSE and prove the exponential decay of the interpolation error in the probability space.
Our analysis indicates that due to the nonlinearity, as final time \(T\) increases and NSE solvers pile up,
the accuracy may be reduced significantly. Subsequently, an illustrative computational test of time dependent fluid flow
around a bluff body is provided.

** Abstract.**
Magnetohydrodynamics (MHD) studies the dynamics of electrically conducting fluids, involving Navier-Stokes (NSE) equations in fluid dynamics and Maxwell equations in eletromagnetism. The physical processes of fluid flows and electricity and magnetism are quite different and numerical simulations of non-model problems can require different meshes, time steps and methods. In most terrestrial applications, MHD flows occur at low magnetic Reynold numbers. We introduce two partitioned methods to solve evolutionary MHD equations in such cases. The methods we study allow us at each time step to call NSE and Maxwell codes separately, each possibly optimized for the subproblem's respective. Error analysis and experiments supporting the theory are given.

** Abstract.**
Geophysical flow simulations have evolved sophisticated implicit-explicit time stepping methods
(based on fast-slow wave splittings) followed by time filters to control any unstable models that result.
Time filters are modular and parallel. Their effect on stability of the overall process has been tested in numerous simulations.
In this paper, we study the stability of the Crank-Nicolson-Leapfrog scheme with the Robert-Asselin-Williams time filter.

** Abstract.**
A family of implicit-explicit second order time-stepping methods is analyzed for a system of ODEs motivated by
ones arising from spatial discretizations of evolutionary partial differential equations. The methods
we consider are implicit in local and stabilizing terms in the underlying PDE and explicit in nonlocal and unstabilizing
terms. Unconditional stability and convergence of the numerical scheme are proved by the energy method and by
algebraic techniques.
This is the first solution to the problem of finding a scheme for (1.1)
that is (provably) unconditionally stable and treats the *Cu* term explicitly. First order schemes were known in [2,10] and [10] gives a second order scheme stable provided all operators commute.

** Abstract.**
Stability is proven for an implicit-explicit, second order, two step method
for uncoupling a system of two evolution equations with exactly skew
symmetric coupling.
The form of the coupling studied arises in spatial discretizations of the Stokes-Darcy problem.
The method proposed is an interpolation of the Crank-Nicolson Leap Frog (CNLF) combination with the BDF2-AB2 combination,
being stable under the time step condition suggested by linear stability theory for the Leap-Frog scheme and BDF2-AB2.

** Abstract.**
The MHD flows are governed by the Navier-Stokes equations coupled with the Maxwell
equations through coupling terms. We prove the unconditional stability of a *partitioned* method for the
evolutionary full MHD equations, at high magnetic Reynolds number, in the Elsässer variables. The method
we analyze is a first order, one step scheme, which consists of implicit discretization of the subproblem terms
and explicit discretization of coupling terms.

** Abstract.**
We consider an uncoupled, modular regularization algorithm for approximation of the Navier-Stokes equations of the
Navier-Stokes equations. The method is: Step 1: Advance the NSE one time step,
Step 2: Regularize to obtain the approximation at the new time level.
The algorithmic key is that Step 2 is a modular regularization uncoupled from Step 1.
Previous analysis of this approach has been for simple time stepping methods in Step 1 and specific regularization operators
in Step 2
such as filter based stabilization. In this report we extend the mathematical support for uncoupled, modular stabilization to (i)
the more complex and better
performing BDF2 time discretization in Step 1, and (ii) general (linear or nonlinear) regularization operators in Step 2.
We give a
complete stability analysis, derive conditions on the Step 2 regularization operator for which the combination has good
stabilization effects,
characterize the numerical dissipation induced by Step 2, prove an asymptotic error estimate incorporating the numerical error of
the method used in
Step 1 and the regularization's consistency error in Step 2 and provide numerical tests. Some tests verify the presented
convergence
theory and some tests are beyond the theory developed. The latter suggest several directions for further development of modular
stabilization methods.

** Abstract.** We consider parameter identification for the classic Gierer-Meinhardt reaction-diffusion system.
The original Gierer-Meinhardt model [A. Gierer and H. Meinhardt, *Kybernetik*, 12 (1972), pp. 30-39]
was formulated with constant parameters and has been used as a prototype system for investigating pattern formation
in developmental biology. In our paper the parameters are extended in time and space and used as distributed control variables.
The methodology employs PDE-constrained optimization in the context of image-driven spatiotemporal pattern formation.
We prove the existence of optimal solutions, derive an optimality system, and determine optimal solutions.
The results of numerical experiments in 2D are presented using the finite element method, which illustrates the convergence
of a variable-step gradient algorithm for finding the optimal parameters of the system. A practical target function was
constructed for the optimal control algorithm corresponding to the actual image of a marine angelfish.

** Abstract.**
This paper concerns a second-order, three level piecewise linear finite element scheme 2-SBDF
[J. RUUTH, *Implicit-explicit methods for reaction-diffusion problems in pattern formation*, J. Math. Biol., 34 (1995), pp. 148-176] for approximating the stationary (Turing) patterns of a well-known experimental substrate-inhibition reaction-diffusion (`Thomas') system
[D. THOMAS, *Artificial enzyme membranes, transport, memory and oscillatory phenomena*, in Analysis and control of immobilized enzyme systems, D. Thomas and
J.P. Kernevez, eds., Springer, 1975, pp. 115-150]. A numerical analysis of the semi-discrete in time approximations leads to semi-discrete *a priori* bounds
and an optimal error estimate. The analysis highlights the technical challenges in undertaking the numerical analysis of multi-level ($?3$) schemes.
We illustrate the effectiveness of the numerical method by repeating an important classical experiment in mathematical biology, namely, to approximate the
Turing patterns of the Thomas system over a schematic mammal skin domain with fixed geometry at various scales. We also make some comments on the correct
procedure for simulating Turing patterns in general reaction-diffusion systems.

** Abstract.**
The most effective simulations of the multi-physics coupling of groundwater to surface water must involve employing the best
groundwater codes and the best surface water codes. Partitioned
methods, which solve the coupled problem by successively solving the sub-physics problems, have recently been studied for the
Stokes-Darcy coupling with convergence established over bounded
time intervals (with constants growing exponentially in t). This report analyzes and tests two such partitioned (non-iterative,
domain decomposition) methods for the fully evolutionary Stokes-Darcy
problem. Under a modest time step restriction of the form
\(C = C\)(*physical parameters*) we prove unconditional asymptotic (over \(0 \leq t < \infty\) stability of both partitioned methods.
From this we derive an optimal error estimate that is *uniform in time* over \(0 \leq t < \infty\).

** Abstract.**
MHD flows are governed by the Navier-Stokes equations coupled
with the Maxwell equations. Broadly, MHD flows in astrophysics occur at large
magnetic Reynolds numbers while those in terrestrial applications, such as liquid
metals, occur at small magnetic Reynolds numbers, the case considered
herein. The physical processes of fluid flows and electricity and magnetism
are quite different and numerical simulations of non-model problems can require
different meshes, time steps and methods. We introduce implicit-explicit
(IMEX) methods where the MHD equations can be evolved in time by calls
to the NSE and Maxwell codes, each possibly optimized for the subproblem's
respective physics.

** Abstract.**
Stability is proven for two second order, two step methods for
uncoupling a system of two evolution equations with exactly skew symmetric
coupling: the Crank-Nicolson Leap Frog (CNLF) combination and the BDF2-AB2
combination. The form of the coupling studied arises in spatial
discretizations of the Stokes-Darcy problem. For CNLF we prove stability for
the coupled system under the time step condition suggested by linear
stability theory for the Leap-Frog scheme. This seems
to be a first proof of a widely believed result. For BDF2-AB2 we prove
stability under a condition that is better than the one suggested by linear
stability theory for the individual methods.

** Abstract.**
We study adaptive nonlinear filtering in the Leray regularization model for
incompressible, viscous Newtonian flow. The filtering radius is locally adjusted
so that resolved flow regions and coherent flow structures are not `filtered-out', which is a common problem with these types of models. A numerical method is proposed that is unconditionally stable with respect to timestep, and
decouples the problem so that the filtering becomes linear at each timestep and is decoupled from the system. Several numerical examples are given that demonstrate the effectiveness of the method.

** Abstract.**
We study a new regularization of the Navier-Stokes equations, the
NS-\(\overline{\omega}\) model. This model has similarities to the
NS-\(\alpha\) model, but its structure is more amenable to be used as
a basis for numerical simulations of turbulent flows. In this report
we present the model and prove existence and uniqueness of strong
solutions as well as convergence (modulo a subsequence) to a weak
solution of the Navier-Stokes equations as the averaging radius
decreases to zero. We then apply turbulence phenomenology to the
model to obtain insight into its predictions.

** Abstract.** Stabilization using filters is intended to model and extract the energy lost
to resolved scales due to nonlinearity breaking down resolved scales to
unresolved scales. This process is highly nonlinear and yet current models
for it use linear filters to select the eddies that will be damped. In this
report we consider for the first time nonlinear filters which select eddies
for damping (simulating breakdown) based on knowledge of how nonlinearity
acts in real flow problems. The particular form of the nonlinear filter
allows for easy incorporation of more knowledge into the filter process and
its computational complexity is comparable to calculating a linear filter of
similar form. We then analyze nonlinear filter based stabilization for the
Navier-Stokes equations. We give a precise analysis of the numerical
diffusion and error in this process.

** Abstract.** When filtering through a wall with constant averaging radius, in addition to
the subfilter scale stresses, a non-closed commutator term arises. We consider
a proposal of Das and Moser to close the commutator error term by embedding it
in an optimization probem. This report shows that this optimization based
closure, with a small modification, leads to a well posed problem showing
existence of a minimizer. We also derive the associated first order optimality conditions.

** Abstract.** We investigate the mathematical properties of a model for the simulation of large
eddies in turbulent, electrically conducting, viscous, incompressible flows. We prove existence and
uniqueness of solutions for the simplest (zeroth) closed MHD model (1.7), we show that its solutions
converge to the solution of the MHD equations as the averaging radii converge to zero, and derive
a bound on the modeling error. Furthermore, we show that the model preserves the properties of
the 3D MHD equations: the kinetic energy and the magnetic helicity are conserved, while the cross
helicity is approximately conserved and converges to the cross helicity of the MHD equations, and
the model is proven to preserve the Alfvèn waves, with the velocity converging to that of the MHD,
as \(\delta_1\), \(\delta_2\) tend to zero. We perform computational tests that verify the accuracy
of the method and compare the conserved quantities of the model to those of the averaged MHD.

** Abstract.** We present a new algorithm for estimating parameters in reaction-diffusion systems that
display pattern formation via the mechanism of diffusion-driven instability. A Modified Discrete Optimal Control Algorithm (MDOCA) is illustrated with the Schnakenberg and Gierer-Meinhardt reaction-diffusion systems using PDE constrained optimization techniques. The MDOCA algorithm is a modification of a standard variable step gradient algorithm that yields a huge saving in computational cost. The results of numerical experiments demonstrate that the algorithm accurately estimated key parameters associated with stationary target functions generated from the models themselves. Furthermore, the robustness of the algorithm was verified by performing experiments with target functions perturbed with various levels of additive noise. The MDOCA algorithm could have important applications in the mathematical modeling of realistic Turing systems when experimental data are available.

** Abstract.** We consider a family of high accuracy, approximate deconvolution models of turbulent magnetohydrodynamic flows. For body force driven turbulence, we prove directly from the
model's equations of motion the following bounds on the model's time averaged energy dissipation
rate, time averaged cross helicity dissipation rate and magnetic helicity dissipation
rate, where U, B, L are the global velocity scale, global magnetic field scale and length
scale, R is a dimensionless constant related to fluid and magnetic Reynolds numbers, S is the reciprocal of the product of
fluid density times free-space permeability and \(\delta\) is the LES filter radius.

** Abstract.** We consider the family of approximate deconvolution models (ADM) for
the simulation of the large eddies in turbulent viscous,
incompressible, electrically conducting flows.
We prove the existence and uniqueness of solutions to the ADM-MHD equations, their weak converge to the solution of the MHD equations as the averaging radii tend to zero, and derive a
bound on the modeling error. We demonstrate that the energy and helicity
of the models are conserved, and the models preserve the Alfvèn waves.
We provide the results of the computational tests, that
verify the accuracy and physical fidelity of the models.

** Abstract.** We present the analysis of two reaction-diffusion systems modelling predator-prey interactions, where the
predator displays the Holling type II functional response, and in the absence of predators, the prey growth is logistic.
The local analysis is based on the
application of qualitative theory for ordinary differential equations and dynamical systems, while the global well-posedness depends on
invariant sets and differential inequalities. The key result is an \(L^{\infty}\)-stability estimate, which depends on a polynomial growth condition
for the kinetics. The existence of an a priori
\(L^{\infty}\)-uniform bounds,
given any
nonnegative \(L^{\infty}\)-estimate to general
reaction-diffusion systems is discussed, how the continuous results can be mimicked in the discrete case,
leading to stability estimates for a Galerkin finite-element method with piecewise linear continuous basis
functions. In order to verify the biological wave phenomena of solutions, numerical results are presented in
two-space dimensions, which have interesting ecological implications as they demonstrate that solutions
can be `trapped' in an invariant region of phase space.

** Abstract.** Fluid turbulence is usually characterized by the Navier-Stokes
equations with a large Reynolds number. The simulation of turbulence
model is known to be very difficult. In this paper, we use an artificial spectral
viscosity to make the simulation of turbulence tractable. The model
introduce various parameters and we pose a question whether an effective
choice of a parameter can be made using the mathematical analysis. We
show that the resulting partial differential equation is well-posed and its
consistency. Then, we consider a semi-implicit discretization of the equation
and investigate the stability.

** Abstract.** This report presents the mathematical foundation of
approximate deconvolution LES models together with the model
phenomenology downstream of the theory.

** Abstract.** We consider the mathematical formulation and the analysis of an
optimal control problem associated with the tracking of the
velocity and the magnetic field of a viscous, incompressible,
electrically conducting fluid in a bounded two-dimensional domain
through the adjustment of distributed controls. Existence of
optimal solutions is proved and first-order necessary conditions
for optimality are used to derive an optimality system of partial
differential equations whose solutions provide optimal states and
controls. Semidiscrete-in-time and fully discrete space-time
approximations are defined and their convergence to the exact
optimal solutions is shown.

** Abstract.** We present the numerical analysis of two well-known reaction-diffusion
systems modeling predator-prey interactions, where the local growth of prey is
logistic and the predator displays the Holling type II functional
response. Results are presented for two
fully-practical piecewise linear finite element methods. We establish
a priori estimates and error bounds for the semi-discrete and
fully-discrete finite element approximations. Numerical results
illustrating the theoretical results and spatiotemporal phenomena
(e.g., spiral waves and chaos) are presented in 1-D and 2-D.

** Abstract.** We consider the mathematical formulation and the
analysis of an optimal control problem associated with the tracking of
the velocity and the magnetic field of a viscous, incompressible,
electrically conducting fluid in a bounded three-dimensional domain
through the adjustment of distributed controls. The existence of
optimal solutions is shown, the Gateux differentiability for the MHD
system with respect to controls is proved, and the optimality system is
obtained.

** Abstract.** We consider the mathematical formulation, analysis,
and numerical solution of an optimal control problem for a nonlinear
`nutrient-phytoplankton-zooplankton-fish' reaction-diffusion system. We
study the existence of optimal
solutions, derive an optimality system, and determine optimal
solutions. In the original spatially homogeneous formulation the
dynamics of plankton were investigated as
a function of parameters for nutrient levels and fish predation rate
on zooplankton. In our paper the model is spatially extended and
the parameter for fish predation treated as a multiplicative control
variable. The
model has implications for the biomanipulation of food-webs in
eutrophic lakes to help improve water quality. In order to illustrate
the control of irregular spatiotemporal dynamics of plankton in
the model we implement a semi-implicit (in time) finite element method
with `mass lumping', and present the results of numerical experiments
in two space dimensions.

** Abstract.** We consider the mathematical formulation and analysis
of an optimal control problem associated with the tracking of the
velocity and the magnetic field of a viscous, incompressible,
electrically conducting fluid in a bounded two-dimensional domain
through the adjustment of distributed controls. Existence of optimal
solutions is proved and first-order necessary conditions for optimality
are used to derive an optimality system of partial differential
equations whose solutions provide optimal states and controls.
Semidiscrete-in-time approximations are defined and their convergence
to the exact optimal solutions is shown.

** Abstract.** This paper is concerned with the existence and the
maximum principle for the optimal control problem governed by the
Boussinesq equation. The case of internal controllers is examined.

** Abstract.**
This paper is concerned with the existence and the maximum principle
for the optimal control problems governed by the periodic
www-Bernoulli equation in one dimension with internal controllers.

** Abstract.** We characterize the value function by an appropriate
Hamilton Jacobi Bellman equation (in the viscosity sense) and derive
optimality conditions from the knowledge of the value function.

** Abstract.** We find explicitly the optimal control for an elliptic equation with respect to two different cost functionals.

** Abstract.**
Time-periodic systems governed by differential equations are somewhat
difficult to consider in the numerical setting because they may
possess many solutions. The number of solutions of such systems may
be finite or infinite. Further, some trajectories which are exactly
time-periodic over a given period might only approximately solve the
governing equation, whereas nearby trajectories which exactly solve
the governing equation might only be approximately time-periodic over
the given period. The difficulty of the time-periodic setting is
compounded in the case of systems governed by the Navier-Stokes
equation, as the solutions of such systems in the time-evolving
setting may be chaotic and multiscale. When considering the
optimization of controls for such systems in the time-periodic
setting, the situation is thus particularly delicate, as one doesn't
know a priori which time-periodic solution (or approximate solution)
one should design the controls for.
The present brief note motivates this work, presents the
structure of our analysis, and outlines the resulting numerical
algorithm.

** Abstract.**
This work is concerned with an approximation process
for the identification of nonlinearities in the nonlinear periodic wave
equation. It is based on the least-squares approach and on a splitting
method. A numerical algorithm of gradient type and the numerical
implementation are given.

** Abstract.**
This paper is concerned with the existence and the
maximum principle for the optimal control problem governed by the
periodic vibrating string equation with Dirichlet boundary conditions.
The case of internal controllers is examined.

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Last updated: September 15, 2020 by Catalin Trenchea |