2018
DOI: 10.1016/j.jcp.2018.08.041
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Universal image systems for non-periodic and periodic Stokes flows above a no-slip wall

Abstract: It is well-known that by placing judiciously chosen image point forces and doublets to the Stokeslet above a flat wall, the no-slip boundary condition can be conveniently imposed on the wall [Blake, J. R. Math. Proc. Camb. Philos. Soc. 70(2), 1971: 303.]. However, to further impose periodic boundary conditions on directions parallel to the wall usually involves tedious derivations because single or double periodicity in Stokes flow may require the periodic unit to have no net force, which is not satisfied by t… Show more

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Cited by 20 publications
(19 citation statements)
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“…In the application example below, we employ the fast multi-pole boundary element method fastBEM [39,40], available for download at [64]. The open-source implementation of the fast boundary element method STKFMM directly incorporates the fundamental solution of the Stokes equation close to a no-slip boundary wall [65] and thus relieves the need for an explicit representation of the boundary as a triangulated mesh, yet currently only supports the computation of velocity fields from force distributions [66,67].…”
Section: Multi-scale Modeling: Numerical Implementationmentioning
confidence: 99%
“…In the application example below, we employ the fast multi-pole boundary element method fastBEM [39,40], available for download at [64]. The open-source implementation of the fast boundary element method STKFMM directly incorporates the fundamental solution of the Stokes equation close to a no-slip boundary wall [65] and thus relieves the need for an explicit representation of the boundary as a triangulated mesh, yet currently only supports the computation of velocity fields from force distributions [66,67].…”
Section: Multi-scale Modeling: Numerical Implementationmentioning
confidence: 99%
“…Ewald methods for Stokes flow based on image constructions have been developed for a single bottom wall using Fourier transforms in all directions [35] or FMMs [36,37]. However, the image construction for a no-slip wall for Stokes flow involves several types of image singularities [38], and this leads to substantial complexity and inefficiency compared to the approach we developed here for the Poisson equation.…”
Section: Discussionmentioning
confidence: 99%
“…It follows that the constant k = 0 basis function makes no contribution to K, and so we exclude it from the matrix. Note that two clamped ends cannot straightforwardly be fit into our approach, since it is difficult to write a basis like (69) when there is a constraint on L 0 τ (s) ds.…”
Section: Spectral Discretizationmentioning
confidence: 99%
“…We chose an Ewald approach because we are interested in triply-periodic systems; in free space a fast multipole method[24] is likely the best choice, and systems with mixed periodicity are an avenue of active research[37,69].…”
mentioning
confidence: 99%