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arXiv 1206.2686math.NAcs.NA
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分数阶扩散和波动方程的不连续Galerkin方法的超收敛性

Superconvergence of a discontinuous Galerkin method for fractional diffusion and wave equations

KFUPM(国王法赫德国立石油与矿产大学);The University of New South Wales(新南威尔士大学)

Kassem Mustapha, William McLean

AI总结:

针对分数阶扩散和波动方程,提出时间不连续Galerkin与空间协调有限元结合的数值方法,证明在时间网格适当加密下解在时间层上具有超收敛性,并通过后处理推广到任意时间点。

摘要:

我们考虑一个初边值问题:$\partial_tu-\partial_t^{-α}\nabla^2u=f(t)$,即分数阶扩散($-1<α<0$)或波动($0<α<1$)方程。数值解通过在时间上应用分段线性不连续Galerkin方法,在空间上应用分段线性协调有限元方法得到。时间网格在$t=0$附近适当加密,但空间网格是拟均匀的。之前,我们证明了在空间$L_2$范数下,误差阶为$k^{2+α_-}+h^2\ell(k)$,在$t$上一致,其中$k$是最大时间步长,$h$是空间有限元最大直径,$α_-=\min(α,0)\le0$,$\ell(k)=\max(1,|\log k|)$。这里,我们推广了经典热方程(即$α=0$情况)的一个已知结果,表明在每个时间层$t_n$上,解关于$k$是超收敛的:误差阶为$(k^{3+2α_-}+h^2)\ell(k)$。此外,采用拉格朗日插值的简单后处理步骤可得到任意$t$的超收敛逼近。数值实验表明,当$α<0$时,我们的理论误差界是悲观的。忽略对数因子,我们观察到DG解在$t=t_n$处以及后处理后在所有$t$处的误差阶为$k^{3+α_-}+h^2$。

英文摘要:

We consider an initial-boundary value problem for $\partial_tu-\partial_t^{-α}\nabla^2u=f(t)$, that is, for a fractional diffusion ($-1<α<0$) or wave ($0<α<1$) equation. A numerical solution is found by applying a piecewise-linear, discontinuous Galerkin method in time combined with a piecewise-linear, conforming finite element method in space. The time mesh is graded appropriately near $t=0$, but the spatial mesh is quasiuniform. Previously, we proved that the error, measured in the spatial $L_2$-norm, is of order $k^{2+α_-}+h^2\ell(k)$, uniformly in $t$, where $k$ is the maximum time step, $h$ is the maximum diameter of the spatial finite elements, $α_-=\min(α,0)\le0$ and $\ell(k)=\max(1,|\log k|)$. Here, we generalize a known result for the classical heat equation (i.e., the case $α=0$) by showing that at each time level $t_n$ the solution is superconvergent with respect to $k$: the error is of order $(k^{3+2α_-}+h^2)\ell(k)$. Moreover, a simple postprocessing step employing Lagrange interpolation yields a superconvergent approximation for any $t$. Numerical experiments indicate that our theoretical error bound is pessimistic if $α<0$. Ignoring logarithmic factors, we observe that the error in the DG solution at $t=t_n$, and after postprocessing at all $t$, is of order $k^{3+α_-}+h^2$.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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