2007
DOI: 10.2151/jmsj.85b.241
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The Evolution of Dynamical Cores for Global Atmospheric Models

Abstract: The evolution of global atmospheric model dynamical cores from the first developments in the early 1960s to present day is reviewed. Numerical methods for atmospheric models are not straightforward because of the so-called pole problem. The early approaches include methods based on composite meshes, on quasi-homogeneous grids such as spherical geodesic and cubed sphere, on reduced grids, and on a latitude-longitude grid with short time steps near the pole, none of which were entirely successful. This resulted … Show more

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Cited by 191 publications
(154 citation statements)
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References 140 publications
(138 reference statements)
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“…The efficiency and robustness achieved with SISL is not easily replaced by alternative choices [110], although the better scalability that can be exploited on future HPC architectures, due to less reliance on communication exchanges beyond nearest neighborhoods will work in favor of techniques with compact stencils, e.g. finite volume (FV) and spectral element methods (SEM), coupled with EBTI-based approaches.…”
Section: Discussion and Concluding Remarksmentioning
confidence: 99%
“…The efficiency and robustness achieved with SISL is not easily replaced by alternative choices [110], although the better scalability that can be exploited on future HPC architectures, due to less reliance on communication exchanges beyond nearest neighborhoods will work in favor of techniques with compact stencils, e.g. finite volume (FV) and spectral element methods (SEM), coupled with EBTI-based approaches.…”
Section: Discussion and Concluding Remarksmentioning
confidence: 99%
“…Semi-Lagrangian (SL) transport schemes are an integral part of many atmospheric models (Williamson, 2007). They are robust and stable even at large Courant number.…”
Section: Introductionmentioning
confidence: 99%
“…In the context of climate studies, a crucial additional requirement is that it be conservative: the discretized system should enforce the exact conservation of a discrete approximation of the total mass, momentum and, if possible, energy and enstrophy. For an in-depth review of the evolution of dynamical cores, the reader is referred to Williamson (2007). Although a single optimal scheme has not emerged yet, most dynamical cores in use today use one of two methods: the finite-difference method (Arakawa, 1966;Sadourny, 1975;Arakawa and Lamb, 1981) or the spectral-transform method (Orszag, 1970;Swarztrauber, 1996), both using a structured latitude-longitude grid.…”
Section: Introductionmentioning
confidence: 99%
“…This so-called 'pole problem' can be overcome by applying latitude-dependent zonal Fourier filters near the Poles. Although widely adopted, this fix remains 'unsatisfying' (Williamson, 2007) and may introduce discretization errors (Purser, 1988). Furthermore, Fourier filtering incurs an asymptotic cost of O(N 2 log N).…”
Section: Introductionmentioning
confidence: 99%
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