2017
DOI: 10.1002/cpe.4216
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Parallel solvers for fractional power diffusion problems

Abstract: Summary Mathematical models with fractional‐order differential operators are computationally expensive due to the non‐local nature of these operators. In this work, we construct and investigate parallel solvers for problems described by fractional powers of elliptic operators, like fractional diffusion. Three state‐of‐the‐art approaches are used to transform the non‐local fractional‐order differential problem into local partial differential equation problems formulated in a space of higher dimension. Numerical… Show more

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Cited by 19 publications
(18 citation statements)
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“… The semi‐infinite cylinder is then truncated to allow numerical solution of elliptic problem in a bounded domain normalΩ×false[0,Tfalse]double-struckRd+1. In our previous studies,)this method has led to a worse parallel scalability compared to the remaining methods and it is not used for 3D problems in this work. M2 Transformation to a pseudo‐parabolic problem . Here, the new additional dimension is defined by the pseudo‐time.…”
Section: State Of the Art In Numerical Solution Methodsmentioning
confidence: 99%
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“… The semi‐infinite cylinder is then truncated to allow numerical solution of elliptic problem in a bounded domain normalΩ×false[0,Tfalse]double-struckRd+1. In our previous studies,)this method has led to a worse parallel scalability compared to the remaining methods and it is not used for 3D problems in this work. M2 Transformation to a pseudo‐parabolic problem . Here, the new additional dimension is defined by the pseudo‐time.…”
Section: State Of the Art In Numerical Solution Methodsmentioning
confidence: 99%
“…In the literature, several different numerical quadrature formulas are proposed to approximate integral . In our previous studies, we have used the quadrature formula based on a β ‐dependent graded mesh. However, initial computational experiments solving the current 3D test problem have shown superior results using another quadrature formula with uniformly distributed quadrature points y j = kj : alignleftalign-1UhM3=2ksin(πβ)πj=m1m2e2(β1)yje2yjIh+Lh1fh,align-2 where m 1 = ⌈ π 2 /(4 βk 2 )⌉ and m 2 = ⌈ π 2 /(4(1 − β ) k 2 )⌉.…”
Section: Quadrature Methods (M3)mentioning
confidence: 99%
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