SIAM Journal on Scientific Computing · 2015 · 39 citations · 24 references
ComputingComputer ScienceMathematicsAlgorithmsComputational PhysicsDynamical SystemsConvergence AnalysisNumerical AlgorithmsNumerical AnalysisNumerical ConvergenceNumerical IntegrationNumerical Methods For Differential EquationsConvergenceConvergence Rate AnalysisEigenvalue BoundsMesh ConvergencePositive Definite Functions
We analyze in this paper the convergence properties of the parareal algorithm for the symmetric positive definite problem $\mathbf{u}'+A\mathbf{u}=g$. The coarse propagator $\mathcal{G}$ is fixed to the backward-Euler method and three time integrators are chosen for the $\mathcal{F}$-propagator: the trapezoidal rule, the third-order diagonal implicit Runge--Kutta (RK) (DIRK) method, and the fourth-order Gauss RK method. It is well known that the Parareal-Euler algorithm using the backward-Euler method for $\mathcal{F}$ and $\mathcal{G}$ converges rapidly, but less is known when one uses for $\mathcal{F}$ the trapezoidal rule, or the fourth-order Gauss RK method, especially when the mesh ratio $J(=\Delta T/\Delta t)$ is small. We show that for a specified $\lambda_{\max}$(the maximal eigenvalue of $A$ or its upper bound), there exists some critical $J_{\rm cri}$ such that the parareal solvers derived from these three choices of $\mathcal{F}$ converge as fast as Parareal-Euler, provided $J\geq J_{\rm cri}$. Precisely, for $\mathcal{F}$ the trapezoidal rule and the fourth-order Gauss RK method, $J_{\rm cri}$ depends on $\Delta T, \Delta t$, and $\lambda_{\max}$ and we present concise formulas to calculate $J_{cri}$, while for $\mathcal{F}$ the third-order DIRK method, $J_{cri}=4$, independently of these parameters. Numerical examples with applications in fractional PDEs and uncertainty quantification are presented to support the theoretical predictions.
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