Td. Ringler et al., Modeling the atmospheric general circulation using a spherical geodesic grid: A new class of dynamical cores, M WEATH REV, 128(7), 2000, pp. 2471-2490
This paper documents the development and testing of a new type of atmospher
ic dynamical core. The model solves the vorticity and divergence equations
in place of the momentum equation. The model is discretized in the horizont
al using a geodesic grid that is nearly uniform over the entire globe. The
geodesic grid is formed by recursively bisecting the triangular faces of a
regular icosahedron and projecting those new vertices onto the surface of t
he sphere. All of the analytic horizontal operators are reduced to line int
egrals, which are numerically evaluated with second-order accuracy. In the
vertical direction the model can use a variety of coordinate systems, inclu
ding a generalized sigma coordinate that is attached to the top of the boun
dary layer. Terms related to gravity wave propagation are isolated and an e
fficient semi-implicit time-stepping scheme is implemented. Since this mode
l combines many of the positive attributes of both spectral models and conv
entional finite-difference models into a single dynamical core, it represen
ts a distinctively new approach to modeling the atmosphere's general circul
ation.
The model is tested using the idealized forcing proposed by Held and Suarez
. Results are presented for simulations using 2562 polygons (approximately
4.5 degrees x 4.5 degrees) and using 10 242 polygons (approximately 2.25 de
grees x 2.25 degrees). The results are compared to those obtained with spec
tral model simulations truncated at T30 and T63. In terms of first and seco
nd moments of stare variables such as the zonal wind, meridional wind, and
temperature, the geodesic grid model results using 2562 polygons are compar
able to those of a spectral model truncated at slightly less than T30, whil
e a simulation with 10 242 polygons is comparable to a spectral model simul
ation truncated at slightly less than T63.
In order to further demonstrate the viability of this modeling approach, pr
eliminary results obtained from a full-physics general circulation model th
at uses this dynamical core are presented. The dominant features of the DJF
climate are captured in the full-physics simulation.
In terms of computational efficiency, the geodesic grid model is somewhat s
lower than the spectral model used for comparison. Model timings completed
on an SGI Origin 2000 indicate that the geodesic grid model with 10 242 pol
ygons is 20% slower than the spectral model truncated at T63. The geodesic
grid model is more competitive at higher resolution than at lower resolutio
n, so further optimization and future trends toward higher resolution shoul
d benefit the geodesic grid model.