Annual simulations of Mars' atmosphere made with the NASA Ames Mars General Circulation Model have been used to extract and generate products to provide statistical products that detail the variability of Mars' atmosphere on fairly short time scales. These products are needed for the creation of a new version of Mars-GRAM, due for completion in June, 1999. The updated Mars-Gram, in turn, will provide guidance for forthcoming aerobraking and aerocapture activities. We have created files containing zonally-averaged fields (temperatures, densities, pressures, and winds, all on z-surfaces), as well as zonally-averaged diurnal and semidiurnal tidal amplitudes and phases. All fields represent a time averaged state (over either 5 or 30 sols), and all fields are available at each of 12 seasons for a Mars year (the seasons being 30deg of Ls apart). Files for low and moderate dust loading cases are liable via anonymous ftp. Files for a high dust case will be in place shortly

Bridger, Alison F. C.

Haberle, Robert M.

English

NASA Technical Reports Server

MARS CHARACTERIZATION FOR FUTURE MISSIONS
/
/
FINAL REPORT
Professor Alison F.C. Bridger
Meteorology Department
San Jose State University
San Jose CA 95192-0104
bridger@hellas.arc.nasa.gov
Dr. Robert M. Haberle
NASA Ames Research Center
MS 245-3
Moffett Field, CA
haberle@humbabe.arc.nasa.gov
Spring 1999
https://ntrs.nasa.gov/search.jsp?R=19990053337 2020-06-15T21:26:05+00:00Z
OVERVIEW
The purpose of this research project was to create statistical products which could
be of use to the engineering and scientific communities planning future missions to Mars.
This has been accomplished. Using simulations of Mars' atmosphere under a variety of
conditions, we have created statistical databases quantifying the behavior of Mars'
atmosphere under a variety of conditions expected to be encountered on forthcoming
missions. These data are now being incorporated into a new version of Mars-GRAM
EXPERIMENTS AND ANALYSIS
To generate the desired data products, we utilized the NASA Ames Mars General
Circulation Model (MGCM), a sophisticated computer model of Mars' atmosphere. The
MGCM is capable of simulating the atmosphere from pole-to-pole up to elevations of
about 80 km. Simulations can be for short periods [O(10's of days), simulating
"weather"], or for annual or even multiannual periods ("climate").
The MGCM incorporates sophisticated physics, including: radiative driving of
the atmosphere (visible and IR); realistic distributions and effects of suspended
atmospheric dust; allowed condensation of CO2; realistic topographical, albedo, and
thermal inertia distributions; a sophisticated boundary layer scheme; and an improved
soil scheme. Results of simulations under a variety of conditions have appeared in the
literature.
For the purposes of this study, we utilized results from a set of annual simulations
of the model. In these, the dust is assumed to be uniformly distributed in the horizontal,
and is not allowed to vary in time. In the vertical, dust is mixed uniformly up to a certain
height, above which its amount decays exponentially with height. Two such simulations
have been used, having dust opacities of r-0.3 (low dust) and _=l.0 (moderate dust; a
high dust z=3.0 simulation is pending, and results will be added to the database). These
choices were agreed upon following consultation with Dr. Jere Justus, and are in part
driven by values observed during the Viking mission and by recent MGS-TES
observations.
It was decided that an appropriate measure of the variability of the atmosphere
would be given by amplitudes and phases of atmospheric diurnal (one cycle per sol) and
semidiumal (two cycles per sol) thermal tides. These tides are excited by the sun's
radiative driving, and can attain substantial amplitudes during dusty conditions. Their
amplitudes generally increase with altitude, and thus they might sufficiently perturb the
higher atmosphere to impact aerobraking and aerocapture activities.
After some experimentation, it was decided to develop the following products:
1. zonally-averaged and time-averaged fields (temperatures, densities, horizontal wind
components, pressures on geopotential surfaces)
2. zonally-averaged tidal amplitudes of the above fields
3. zonally-averaged tidal phases
4. distributions of tidal amplitudes and phases at the two lowest levels in the MGCM, to
provide near-surface temperature intbrmation
RESULTS
The products outlined above have been developed, and are accessible via
anonymous ftp from mintz.arc.nasa.gov (/pub/mgcm/justus and directories below). At
this stage, it has not been decided to put the data on the web (as had been proposed),
since it can be readily accessed via ftp by those who immediately need it. However,
since other products from these MGCM simulations will be made available on the web as
part of the MGCM Climate Catalog, the products generated here may be added to that
site (in the form ifgifs and/or ascii data files).
The zonally-averaged fields are computed based on an average over 30 sols. In
part, this is determined by the structure of files archived from the annual simulations.
Twelve "mini-seasons" are defined for each simulation, each lasting 30 sols, and spaced
every 30 ° of areocentric longitude (Ls). The top panel of Fig. 1 shows an example of the
latitude-height distribution of zonally averaged temperatures at Ls 270 ° (northern mid-
winter). The distribution shows the warm, summer pole, and the cold winter polar
atmosphere, with a sharp north-souththermal gradient, indicative of an active baroclinic
zone in the north at this season.
For tidal fields, after experimentation it was decided to compute amplitudes based
on 5-sol composite fields, centered on the middle five sols of the 30 sol records
mentioned above. The chief reason for this is that there can be significant variation of
tidal amplitudes and phases over 30 sols, rendering 30-sol averages somewhat difficult to
interpret. In addition, and especially with tidal phases, we have encountered significant
longitudinal variations, again making averaging difficult (since products 1-3 are zonally-
averaged). To overcome this, a special zonal averaging procedure was developed for
phase fields. Taking the cosine and sine portions of the tidal field, we first form zonal
averages of these, and then form a final zonally-averaged phase from the ratio of these.
The lower two panels of Fig. 1 show the amplitudes (zonally-averaged) of the
diurnal and semidiumal temperature tide for the low dust case at Ls 270 °. They indicate
a diurnal tidal wave with amplitudes over 12.5 K (i.e., 25 K peak-to-peak temperature
swings). The semidiurnal wave has a somewhat smaller amplitude at this season.
A second set of products we proposed to create pertain to data for a near-surface
temperature model. This was accomplished again using the annual MGCM simulations
mentioned above. The products discussed above were provided following interpolation
to z-surfaces. The MGCM simulations however produce results on g-surfaces, where o
is related to the ratio p/Ps, with p = actual pressure and Ps = surface pressure. It was
decided to extract temperature information on the model's lowest two c surfaces,
corresponding to altitudes of approximately 5m AGL and 30m AGL. From these
temperature fields, diurnal and semidiurnal tidal amplitudes and phases were again
computed and stored in data files. From these, together with the temperature products
mentioned above, we can get a fairly detailed view of near-surface temperatures and their
variation through the day (as a function of season).
Figure 2 shows the latitude-longitude distribution of mean temperatures (upper
panel), as well as diurnal and semidiumal tidal amplitudes in the temperature field at the
lowesto-level in the model,againat Ls 270° and for the low dust case. In the mean
field, we see the north-south temperature gradient, as well as evidence of stationary wave
activity in the sub-tropics. Both tidal amplitude fields show considerable longitudinal
structure. This is indicative of the presence of non-migrating tides (sun-synchronous
tides propagate westwards, "following the sun". If these alone are present, we would
expect no longitudinal variations in amplitude. However, longitudinal variations of
topography, aibedo, and thermal inertia can produce non-sun-synchronous tidal
oscillations, yielding a complicated horizontal structure).
As mentioned above, all products have thus far been generated for both low and
moderate dust cases (144 files per annual simulation). Data from a third, high dust case
is pending. We may also choose to include (in consultation with Dr. Jere Justus of
MSFC) data from a shorter simulation (e.g., 30-50 sols) of a dust storm. For example, we
may include a simulation of the Noachis dust storm observed during MGS aerobraking
(simulation performed by Dr. Jim Murphy at NMSU), or simulations from Viking-era
dust storms.
SUMMARY
Annual simulations of Mars' atmosphere made with the NASA Ames Mars
General Circulation Model have been used to extract and generate products to provide
statistical products that detail the variability of Mars' atmosphere on fairly short time
scales. These products are needed for the creation of a new version of Mars-GRAM, due
for completion in June, 1999. The updated Mars-Gram, in turn, will provide guidance
for forthcoming aerobraking and aerocapture activities.
We have created files containing zonally-averaged fields (temperatures, densities,
pressures, and winds, all on z-surfaces), as well as zonally-averaged diurnal and
semidiumal tidal amplitudes and phases. All fields represent a time averaged state (over
either 5 or 30 sols), and all fields are available at each of 12 seasons for a Mars year (the
seasons being 30 ° of Ls apart). Files for low and moderate dust loading cases are
available via anonymous ftp. Files for a high dust case will be in place shortly.
FUTURE WORK
Two extensions from this work are possible. In the first (being funded through
the second year of this effort), we will provide products from these same simulations as
input to the Mars Thermospheric General Circulation Model (MTGCM, in consultation
with Dr. Steve Bougher at UA). We will provide data on tidal oscillations that are
needed to "drive" that model (i.e., Hough function amplitudes and phases). In a second
possible extension, it is clear that there are large-amplitude stationary waves in Mars'
atmosphere. These are expected, given Mars' large amplitude topography at large-scales.
Evidence of high-altitude stationary wave activity emerged during MGS aerobraking. It
may prove worthwhile to include a parameterization of this into Mars-GRAM Again,
products would be created from simulations of the MGCM.
4o
2O
ZONALLY-AVERAGEDTEMPERATURES (K) Run:98.27 Ls:270
TT_°_
--------79o____ _o _ _° -
---2oo / -
----_----21o____ _ ._9_-/_ \ \ I/
__._t2._o _ _ _ _ 20o "1)//_ -
- 230 )1//"
_ __ _2_o--... I ,'//// /_
0 , , I _ , 1 , ,
-gO -60 ,50 60 90
80
-3O 0
Lotituoe (deg)
DIURNAL TEMPERATURE AMPLITUDES (K) Run: 98.27 Ls: 270
I I ] I I
40
-90 -60 -30 0 30 60
Lotitude (deg)
SEMIDIURNAL TEMPERATURE AMPLITUDES (K) Run: 98.27 Ls: 270
80 i i i l i
2O
!
OL J j _._L_ ' l
-90 -60 -30 0 30 50
.o:,tuOe (deq)
9O
gO
UEAN TEMPERATURE FIELD (K) Run: 98.04 Ls: 270
90 i I i
6O
3O
--3O
-6O
-90 , , loan. , ..... I , , . . i .... c*..¢_ . .
-200 -lOO o lOO
Long;tuOe (deg)
DIURNAL TEMPERATURE FIELD (K) Run: 98.04 Ls: 270
°o_
_,o __ - _/_ __/_-_--_o-_
_,olilly ; i_ii:i J:ii:i ;i ilill iii ;;_
-200 ' -100 ' 0 lOW{)
LatituOe(de<J)
SEMI-DIURNAL TEMPERATURE FIELD (K) Run: 98.04 Ls: 270
i I i90
60 -
30
0
- 30
-60
-901 _
-200
2.5 _ 2.5
2.5 2.5 --
, , L ] I
-ioo o ioo
Lot,tuoe (deq)
2OO
2OO
200


Mars Characterization for Future Missions

Abstract

Similar works

Full text

Available Versions

NASA Technical Reports Server