2003
DOI: 10.1137/s003614290138437x
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Adaptive Mesh Methods for One- and Two-Dimensional Hyperbolic Conservation Laws

Abstract: Abstract. We develop efficient moving mesh algorithms for one-and two-dimensional hyperbolic systems of conservation laws. The algorithms are formed by two independent parts: PDE evolution and mesh-redistribution. The first part can be any appropriate high-resolution scheme, and the second part is based on an iterative procedure. In each iteration, meshes are first redistributed by an equidistribution principle, and then on the resulting new grids the underlying numerical solutions are updated by a conservativ… Show more

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Cited by 266 publications
(367 citation statements)
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“…In general, monitor functions depend on the underlying solution to be adapted and its derivatives. More terms can be added to the functional (17) to control other aspects of the adaptive mesh such as orthogonality and mesh alignment with a given vector field [14,34]. In this work, the adaptive mesh is determined by the corresponding Euler-Lagrange equations:…”
Section: Mesh Generationmentioning
confidence: 99%
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“…In general, monitor functions depend on the underlying solution to be adapted and its derivatives. More terms can be added to the functional (17) to control other aspects of the adaptive mesh such as orthogonality and mesh alignment with a given vector field [14,34]. In this work, the adaptive mesh is determined by the corresponding Euler-Lagrange equations:…”
Section: Mesh Generationmentioning
confidence: 99%
“…to replace the convectional (17), where G 1 and G 2 are again the monitor functions and∇ = (* , * ) T . The corresponding Euler-Lagrange equations are then of the form:…”
Section: Mesh Generationmentioning
confidence: 99%
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“…The necessary number of grid points to meet the tolerance is then computed, and a new grid {x j } constructed by inverse linear interpolation of ξ(x) in the same manner as in (10). In [35], Tang and Tang use calculus of variations and seek ξ(x) such that…”
mentioning
confidence: 99%