Finite difference approximations for fractional advection-dispersion flow equations
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...…i = 1, . . . , K − 1 and j = 1, . . . , K − 1 are defined by Ai,j = 1 − (ξi + ηi)g1 for j = i −(ξig2 + ηig0) for j = i − 1 −(ξig0 + ηig2) for j = i + 1 −ξigi−j+1 for j < i − 1 −ηigj−i+1 for j > i + 1 while A0,0 = 1, A0,j = 0 for j = 1, . . . , K, AK,K = 1, and AK,j = 0 for j = 0, . . . , K − 1....
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557 citations
Cites background or methods from "Finite difference approximations fo..."
...The standard Grünwald estimates generally yield unstable finite difference equations regardless of whether the resulting finite difference method is an explicit or an implicit system, see [9] for related discussion....
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...Several different first-order accurate numerical methods to solve fractional diffusion equations have been presented before [3,4,6,7,9,10]....
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546 citations
Cites methods from "Finite difference approximations fo..."
...The Riemann-Liouville fractional derivative can be discretized by the standard Grünwald-Letnikov form ula [18] with only the first order accuracy, but the difference scheme based on the Grünwald-Letnikov form ula for time dependent problems is unstable [12]....
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...In [12], the shifted Grünwald difference operator Ah,pu(x) = 1 hα ∞ ∑...
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Cites background or methods from "Finite difference approximations fo..."
...For the space fractional derivatives Dx uðxi; tkþ1Þ and Dxuðxi; tkþ1Þ, we adopted the Grünwald formula [11] and the shift Grünwald formula at level tk+1 [7], respectively Dx uðxi; tkþ1Þ 1⁄4 1 h Xi j1⁄40 g j uðxi jh; tkþ1Þ þOðhÞ; ð9Þ Dxuðxi; tkþ1Þ 1⁄4 1 h Xiþ1 j1⁄40 g j uðxi ðj 1Þh; tkþ1Þ þOðhÞ; ð10Þ...
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...[7] presented practical numerical methods to solve the one-dimensional space fractional ADE with variable coefficients on a finite domain....
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...The following lemma has been proved previously [7,14]: Lemma 1....
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