2022
DOI: 10.1016/j.jcp.2022.111612
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Multiple relaxation time lattice Boltzmann schemes for advection-diffusion equations with application to radar image processing

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Cited by 11 publications
(4 citation statements)
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“…The Rudin-Osher-Fatemi total variation minimization equation for image restoration [29] can be efficiently modeled using a nine-velocity LB scheme [30]. Nine-velocity MRT LB models are applied for the simulation of a nonlinear reaction-advection-diffusion equation with a constant diffusion coefficient and non-constant advection velocity, with applications in sea clutter denoising in marine radar images [31]. LB models simulating anisotropic diffusion equations can be used for the smoothing and segmentation of two-dimensional and three-dimensional medical images [32][33][34][35].…”
Section: Introductionmentioning
confidence: 99%
“…The Rudin-Osher-Fatemi total variation minimization equation for image restoration [29] can be efficiently modeled using a nine-velocity LB scheme [30]. Nine-velocity MRT LB models are applied for the simulation of a nonlinear reaction-advection-diffusion equation with a constant diffusion coefficient and non-constant advection velocity, with applications in sea clutter denoising in marine radar images [31]. LB models simulating anisotropic diffusion equations can be used for the smoothing and segmentation of two-dimensional and three-dimensional medical images [32][33][34][35].…”
Section: Introductionmentioning
confidence: 99%
“…Although they appear more complex, MRT LB schemes have significant advantages over simple SRT LB schemes, which explain their growing popularity. They allow, for instance, a gain in numerical stability [24] and a better handling of both boundary conditions [21] and physical quantities [9]. They include for instance cumulant [10] and entropic [18] LB schemes.…”
mentioning
confidence: 99%
“…Choosing equal relaxation times within the MRT collision operator leads to SRT collision operator. It is precisely because we can choose different relaxation times within the collision step that the numerical stability is improved (see for instance [24]). Following [15] and assuming all relaxation times s k nonzero for k = 1, 2, .…”
mentioning
confidence: 99%
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