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Adaptive least-squares space-time finite element methods
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abstract
We consider the numerical solution of an abstract operator equation $Bu=f$ by using a least-squares approach. We assume that $B: X \to Y^*$ is an isomorphism, and that $A : Y \to Y^*$ implies a norm in $Y$, where $X$ and $Y$ are Hilbert spaces. The minimizer of the least-squares functional $\frac{1}{2} \, \| Bu-f \|_{A^{-1}}^2$, i.e., the solution of the operator equation, is then characterized by the gradient equation $Su=B^* A^{-1}f$ with an elliptic and self-adjoint operator $S:=B^* A^{-1} B : X \to X^*$. When introducing the adjoint $p = A^{-1}(f-Bu)$ we end up with a saddle point formulation to be solved numerically by using a mixed finite element method. Based on a discrete inf-sup stability condition we derive related a priori error estimates. While the adjoint $p$ is zero by construction, its approximation $p_h$ serves as a posteriori error indicator to drive an adaptive scheme when discretized appropriately. While this approach can be applied to rather general equations, here we consider second order linear partial differential equations, including the Poisson equation, the heat equation, and the wave equation, in order to demonstrate its potential, which allows to use almost arbitrary space-time finite element methods for the adaptive solution of time-dependent partial differential equations.
Forward citations
Cited by 2 Pith papers
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Inf-sup stable space-time discretization of the wave equation based on a first-order-in-time variational formulation
A conforming space-time discretization of the wave equation using exponential time weights is proven unconditionally stable and quasi-optimal for general tensor product spaces.
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Paving the way to a $\operatorname{T}$-coercive method for the wave equation
A parameter-dependent transformation T_mu makes the weak form of u''+mu u=f coercive with mu-independent stability, a step toward a T-coercive space-time wave equation method.
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