115 research outputs found
Optimal control for the thin-film equation: Convergence of a multi-parameter approach to track state constraints avoiding degeneracies
We consider an optimal control problem subject to the thin-film equation
which is deduced from the Navier--Stokes equation. The PDE constraint lacks
well-posedness for general right-hand sides due to possible degeneracies; state
constraints are used to circumvent this problematic issue and to ensure
well-posedness, and the rigorous derivation of necessary optimality conditions
for the optimal control problem is performed. A multi-parameter regularization
is considered which addresses both, the possibly degenerate term in the
equation and the state constraint, and convergence is shown for vanishing
regularization parameters by decoupling both effects. The fully regularized
optimal control problem allows for practical simulations which are provided,
including the control of a dewetting scenario, to evidence the need of the
state constraint, and to motivate proper scalings of involved regularization
and numerical parameters
Optimal Strong Rates of Convergence for a Space-Time Discretization of the Stochastic Allen-Cahn Equation with multiplicative noise
The stochastic Allen-Cahn equation with multiplicative noise involves the
nonlinear drift operator . We use the fact that
satisfies a weak monotonicity property to deduce uniform bounds in strong norms
for solutions of the temporal, as well as of the spatio-temporal discretization
of the problem. This weak monotonicity property then allows for the estimate for all
small , where is the strong variational solution of the
stochastic Allen-Cahn equation, while solves a
structure preserving finite element based space-time discretization of the
problem on a temporal mesh of size which
covers
Convergent finite element discretizations of the nonstationary incompressible magnetohydrodynamics system
The incompressible MHD equations couple Navier-Stokes equations with Maxwell's equations
to describe the flow of a viscous, incompressible, and electrically conducting fluid in
a Lipschitz domain .
We verify convergence of iterates of different coupling and
decoupling fully discrete schemes towards weak solutions for
vanishing discretization parameters. Optimal first order of convergence is shown
in the presence of strong solutions for a splitting scheme which decouples
the computation of velocity field, pressure, and magnetic fields at
every iteration step
Error analysis of a mixed finite element method for the Cahn-Hilliard equation
Summary.: We propose and analyze a semi-discrete and a fully discrete mixed finite element method for the Cahn-Hilliard equation ut + Δ(ɛΔu−ɛ−1f(u)) = 0, where ɛ > 0 is a small parameter. Error estimates which are quasi-optimal order in time and optimal order in space are shown for the proposed methods under minimum regularity assumptions on the initial data and the domain. In particular, it is shown that all error bounds depend on only in some lower polynomial order for small ɛ. The cruxes of our analysis are to establish stability estimates for the discrete solutions, to use a spectrum estimate result of Alikakos and Fusco [2], and Chen [15] to prove a discrete counterpart of it for a linearized Cahn-Hilliard operator to handle the nonlinear term on a stretched time grid. The ideas and techniques developed in this paper also enable us to prove convergence of the fully discrete finite element solution to the solution of the Hele-Shaw (Mullins-Sekerka) problem as ɛ → 0 in [29
Multiscale resolution in the computation of crystalline microstructure
Summary.: This paper addresses the numerical approximation of microstructures in crystalline phase transitions without surface energy. It is shown that branching of different variants near interfaces of twinned martensite and austenite phases leads to reduced energies in finite element approximations. Such behavior of minimizing deformations is understood for an extended model that involves surface energies. Moreover, the closely related question of the role of different growth conditions of the employed bulk energy is discussed. By explicit construction of discrete deformations in lowest order finite element spaces we prove upper bounds for the energy and thereby clarify the question of the dependence of the convergence rate upon growth conditions and lamination orders. For first order laminates the estimates are optima
Stabilization methods in relaxed micromagnetism
The magnetization of a ferromagnetic sample solves a
non-convex variational problem, where its relaxation by convexifying
the energy density resolves relevant
macroscopic information.
The numerical analysis of the relaxed model
has to deal with a constrained convex
but degenerated, nonlocal energy functional in mixed formulation for
magnetic potential u and magnetization m.
In [C. Carstensen and A. Prohl, Numer. Math. 90
(2001) 65–99], the conforming P1 - (P0)d-element in d=2,3 spatial
dimensions is shown to lead to
an ill-posed discrete problem in relaxed micromagnetism, and suboptimal
convergence.
This observation motivated a
non-conforming finite element method which leads to
a well-posed discrete problem, with solutions converging at
optimal rate.
In this work, we provide both an a priori and a posteriori error analysis for two
stabilized conforming methods which account for inter-element jumps of the
piecewise constant magnetization.
Both methods converge at optimal rate;
the new approach is applied to a macroscopic nonstationary
ferromagnetic model [M. Kružík and A. Prohl, Adv. Math. Sci. Appl. 14 (2004) 665–681 – M. Kružík and T. Roubíček, Z. Angew. Math. Phys. 55 (2004) 159–182 ]
Data-dependent density estimation for the Fokker-Planck equation in higher dimensions
We present a new strategy to approximate the global solution of the
Fokker-Planck equation efficiently in higher dimensions and show its
convergence. The main ingredients are the Euler scheme to solve the associated
stochastic differential equation and a histogram method for tree-structured
density estimation on a data-dependent partitioning of the state space R^d
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