2005
DOI: 10.1016/j.jcp.2004.07.018
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A fourth order accurate discretization for the Laplace and heat equations on arbitrary domains, with applications to the Stefan problem

Abstract: In this paper, we first describe a fourth order accurate finite difference discretization for both the Laplace equation and the heat equation with Dirichlet boundary conditions on irregular domains. In the case of the heat equation we use an implicit time discretization to avoid the stringent time step restrictions associated with explicit schemes. We then turn our focus to the Stefan problem and construct a third order accurate method that also includes an implicit time discretization. Multidimensional comput… Show more

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Cited by 231 publications
(242 citation statements)
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“…In [34] and [36], we extended the ghost cell method to attain second-order accuracy on interior problems (i.e., p is constant in Ω c ) with boundary conditions that depend upon the geometry (e.g., curvature) and without a jump condition on the normal derivative. A similar extension to the ghost cell method was presented in [19] to solve Laplace's equation without geometric boundary conditions and yielded fourth-order convergence on fixed domains and third-order convergence on moving boundaries. In [38], we extended our approach to solve systems like (18) in the case where h = 0 and D was constant in Ω and Ω c (with different constants).…”
Section: The Ghost Cell Methodsmentioning
confidence: 96%
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“…In [34] and [36], we extended the ghost cell method to attain second-order accuracy on interior problems (i.e., p is constant in Ω c ) with boundary conditions that depend upon the geometry (e.g., curvature) and without a jump condition on the normal derivative. A similar extension to the ghost cell method was presented in [19] to solve Laplace's equation without geometric boundary conditions and yielded fourth-order convergence on fixed domains and third-order convergence on moving boundaries. In [38], we extended our approach to solve systems like (18) in the case where h = 0 and D was constant in Ω and Ω c (with different constants).…”
Section: The Ghost Cell Methodsmentioning
confidence: 96%
“…(The diffusion constant may be discontinuous across the interface Σ; this case is treated below.) If (x i−1 , y j ), (x i , y j ), and (x i+1 , y j ) are all in the same region, i.e., (19) or (20) then we can use the standard second-order discretization (21) Suppose, however, that (x i , y j ) and (x i+1 , y j ) are not in the same region. Assume without loss of generality that (x i , y j ) ∈ Ω and (x i+1 , y j ) ∈ Ω c ; the case where (x i , y j ) ∈ Ω c and (x i+1 , y j ) ∈ Ω is treated similarly.…”
Section: Ghost Cell Extrapolations For the Diffusionalmentioning
confidence: 99%
“…This methodology has been applied to a wide range of applications including deflagration in Fedkiw et al [43], compressible/incompressible fluids in Caiden et al [24], flame propagation in Nguyen et al [97], the Poisson equation with jump conditions in Liu et al [78], free surface flows in Enright et al [40], as well as in computer graphics [96,39]. It was developed for the Poisson and the diffusion equations on irregular domains with Dirichlet boundary conditions and their applications in Gibou et al [47,45,44,46]. In what follows, we describe the algorithms, point out common misconceptions and describe how to properly implement those methods.…”
Section: The Ghost-fluid Methods For the Diffusion And The Poisson Equmentioning
confidence: 99%
“…• In the case where third-or fourth-order accuracy is desired, the second-order central differencing used in equations (8) and (9) are replaced by the standard fourth-order accurate central differencing (see [45]). …”
Section: Remarksmentioning
confidence: 99%
“…We now describe a second-order accurate extension of the ghost fluid method (Fedkiw et al, 1999;Liu et al, 2000;Gibou et al, 2002Gibou et al, , 2003Gibou and Fedkiw, 2005) to solve the Poisson-like system…”
Section: A Improvements To the Ghost Fluid Methodsmentioning
confidence: 99%