2018
DOI: 10.1016/j.jcp.2018.01.044
|View full text |Cite
|
Sign up to set email alerts
|

Computation at a coordinate singularity

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

0
11
0

Year Published

2019
2019
2022
2022

Publication Types

Select...
5
3

Relationship

0
8

Authors

Journals

citations
Cited by 8 publications
(12 citation statements)
references
References 38 publications
0
11
0
Order By: Relevance
“…The governing Equations ( 1)-( 3) are discretised in a semi-implicit fashion, using a collocated lat-lon grid with its well-known pole problem [33]. In a nutshell, momentum equations are integrated with the trapezoidal rule…”
Section: The Discretised Modelmentioning
confidence: 99%
“…The governing Equations ( 1)-( 3) are discretised in a semi-implicit fashion, using a collocated lat-lon grid with its well-known pole problem [33]. In a nutshell, momentum equations are integrated with the trapezoidal rule…”
Section: The Discretised Modelmentioning
confidence: 99%
“…The major difficulty in increasing longitudinal resolution in spherical-geometry-based GCMs is that the explicit time stepping is constrained by the clustering azimuthal cells near the pole due to the Courant-Friedrichs-Lewy (CFL) condition (Courant et al, 1928). A number of attempts have been proposed to address this coordinate singularity issue (e.g., Purser, 1988;Bouaoudia and Marcus, 1991;Williamson et al, 1992;Takacs et al, 1999;Fukagata and Kasagi, 2002;Prusa, 2018). To use a time step that is larger than the global minimum requirement from CFL conditions, one common method used in a spherical GCM is to employ a low-pass Fourier filter at polar latitudes, which removes nonphysical, high-frequency zonal waves generated due to numerical instability caused by the local violation of CFL conditions (e.g., Skamarock et al, 2008).…”
Section: Introductionmentioning
confidence: 99%
“…A number of studies have been carried out to investigate these structures, including the formation and evolution of polar cap patches and tongues of ionization [Basu et al, 1995;Foster et al, 2005;Zhang et al, 2013], dynamics of ionospheric irregularities [Makela and Otsuka, 2012;Sun et al, 2015], variations of polar thermospheric density anomaly [Crowley et al, 2010;LĂŒhr et al, 2004], and the space weather effects of mesoscale electric field variability [Codrescu et al, 1995 The major difficulty in increasing longitudinal resolution in spherical geometry based GCMs is that the explicit time stepping is constrained by the clustering azimuthal cells near the pole due to the Courant-Friedrichs-Lewy (CFL) condition [Courant et al, 1928]. A number of attempts have been proposed to address this coordinate singularity issue ([e.g., Purser, 1988;Bouaoudia and Marcus, 1991;Williamson et al, 1992;Takacs, 1999;Fukagata and Kasagi, 2002;Prusa, 2018]). To use a time step that is larger than the global minimum requirement from the CFL conditions, one common method used in a spherical GCM is to employ a low-pass Fourier filter at polar latitudes, which removes non-physical, high-frequency zonal waves generated due to numerical instability caused by the local violation of the CFL conditions [e.g., Skamarock et al, 2008].…”
Section: Introductionmentioning
confidence: 99%
“…Ring Average filters used in the main The main Ring Average Algorithm in the TIE-GCM algorithms of the TIE-GCM, including the thermosphere solvers in Equations(25)(26)(27)(28)(29)(30)(31)(32)(33)(34), the ionosphere solver…”
mentioning
confidence: 99%