This page describes a set of numerical simulations at progressively coarser
resolution to compare with the
Andes07 results, which
use 500 m isotropic mesh spacing. Four new simulations were conducted, having
horizontal resolutions of 1000, 2000, 4000 and 8000 m.
This series utilizes an identical vertical mesh as the original Andes07 run.
Mesh Comparison
Horizontal Spacings
Each computational grid uses the same strategy as in Andes07 with uniform high
resolution used over the Andes and then progressively coarser mesh in the
horizontal directions when moving towards the lateral boundaries. The white
lines in the image below show the region of uniform spacing and this is
identical to what was used in the Andes07 simulation. The only difference is
that the horizontal spacings in the high-resolution zone is increased from 500
m in the Andes07 simulation to 1000, 2000, 4000, and 8000 m here. The dotted
white line in the image below indicates the location of the x-z views shown
below.
Region of uniform mesh (solid lines) and x-z plane location (dotted line).
(Δ 4000 m case).
Each computational domain extends to an altitude of 200 km and uses 500 m
resolution at the surface to an altitude of 144 km. Very gentle stretching
is used to the top of the domain.
Stretching
The the rate at which the mesh is stretched in all three directions is
approximately equal ~1.6%, which is nearly identical to what was used in
the Andes07 run.
Wind and Thermodynamic Profiles
Forcing
Forcing terms gradually introduce winds near the surface with the
objective of achieving the wind profile within a twelve hour period.
A hyperbolic tangent function is used in order to produce gentle
acceleration of the wind near the beginning and end of the forcing period.
The maximum forcing rate is equivalent to that of a linear ramp with a
duration of four hours.
The wind profile and forcing strategy are idetical to what was done in
the Andes07 run.
Results in xz Plane over the South Peak
Results in yz Plane at x = 50km
Results in xy Planes at Altitudes 50km, 70km, 100km, 150km, 180km
50 km
North Peak 2km Anomaly over the Interval 8.0-9.0 hr
Upon futher investigation and analysis it was determined that the 2km case
produces a large-scale coherent vortex that extends down to 50 km as
turbulence starts to develop during the 8.0-9.0 hr. time period. The vortex
is most evidient at a time of 8.5 hr., and the solutions for the 0.5 km and 2 km
resolution cases are shown in the images below. As expected, the 0.5 km
resolution case produces much smaller-scale turbulent motions with no coherent
large-scale vortices present. The 1 km resolution case (not shown) is
similar, but with less small-scale detail (but still no large-scale vortex).
Vorticity Magnitude for an xz plane over the North Peak (line at 50km)
The choherent vortex in the 2 km case gives rise to large momentum fluxes and
these superimpose with the GW momentum fluxes to create the anomoly in the
momentum flux seen in the plot for the 8-9 hr. averaging window above. The
figures below showing traces of u', w', and u'w' over the North Peak at an
altitude of 50 km demonstrate the enhanced momentum flux due to the vortex in
the 2 km case. The abrupt sign change in w' at x~50 km is an indication of the
vortex in the 2km case. Meanwhile u' for the 2 km case is roughly constant at
a minimum value around x=50 km, with the net result that u'w' also undergoes a
sign change close to x=50 km and achieves large peak values on either side of
the zero crossing.
Gaussian Averaged with FWHM of 200km along x and 50km along y
70 km
Gaussian Averaged with FWHM of 300km along x and 100km along y
100 km
Gaussian Averaged with FWHM of 400km along x and 200km along y
150 km
Gaussian Averaged with FWHM of 400km along x and 400km along y
180 km
Gaussian Averaged with FWHM of 400km along x and 400km along y