2019
DOI: 10.4208/nmtma.oa-2018-0058
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Optimal Rate Convergence Analysis of a Second Order Numerical Scheme for the Poisson-Nernst-Planck System

Abstract: In this work, we propose and analyze a second-order accurate numerical scheme, both in time and space, for the multi-dimensional Poisson-Nernst-Planck system. Linearized stability analysis is developed, so that the second order accuracy is theoretically justified for the numerical scheme, in both temporal and spatial discretization. In particularly, the discrete W 1,4 estimate for the electric potential field, which plays a crucial role in the proof, are rigorously established. In addition, various numerical t… Show more

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Cited by 17 publications
(9 citation statements)
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“…Notice that the definition of the boundary data ψ D and σ have been extended to the whole computational domain. In numerical implementation, the ghost points outside Ω are eliminated by coupling the discretization scheme ( 8) and boundary discretization ( 9) and (10). The coupled difference equations can be written in a matrix form…”
Section: Finite Difference Methods In Space 1) Spatial Discretization...mentioning
confidence: 99%
“…Notice that the definition of the boundary data ψ D and σ have been extended to the whole computational domain. In numerical implementation, the ghost points outside Ω are eliminated by coupling the discretization scheme ( 8) and boundary discretization ( 9) and (10). The coupled difference equations can be written in a matrix form…”
Section: Finite Difference Methods In Space 1) Spatial Discretization...mentioning
confidence: 99%
“…), (5.82) in which the a-priori estimates (5.53), (5.55) have been used in the second step, and the following inverse inequality has been applied in the last step: 4 ).…”
Section: A Rough Error Estimatementioning
confidence: 99%
“…Such a stability analysis has appeared in a few existing numerical works [11,23,27], while the unique solvability and positivity-preserving analysis have been missing. Furthermore, there have been a few existing works for the convergence analysis [4,31,35], while these convergence estimates have been based on the perfect Laplacian operator structure for n and p, instead of the H −1 gradient flow structure, so that the energy estimate is not available. Many other numerical schemes have been reported [13,16,27,28,33,36,40].…”
Section: Introductionmentioning
confidence: 99%
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“…We focus on the development of numerical methods for the PNPCH equations. Many efforts have been devoted to the development of numerical methods for the PNP-type equations, ranging from finite difference schemes to discontinuous Galerkin (DG) methods [9,10,16,18,37,41,42,50]. In order to obtain physically faithful numerical solutions, it is highly desirable and crucial to preserve physical properties of the analytical solutions, such as mass conservation, free-energy dissipation, and positivity, at the discrete level.…”
Section: Introductionmentioning
confidence: 99%