MAMS
Points of Contact:
-
Anthony Guillory and Gary Jedlovec
-
Global Hydrology and Climate Center
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NASA/ Marshal Space Flight Center/ Code: SD60
- Huntsville, Alabame 35805
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Office Telephone: (256) 961-7894, (256) 961-7964
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FAX: (256) 961-7723
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E-mail: anthony.guillory@msfc.nasa.gov,
gary.jedlovec@msfc.nasa.gov
Brief Instrument Description of the
Multispectral Atmospheric Mapping Sensor (MAMS)
The MAMS is a multispectral scanner which measures reflected radiation
from the Earth's surface and clouds in 8 visible/near infrared channels
and thermal emission from the surface, clouds, and atmospheric constituents
(primarily water vapor) if four infrared bands. The scanner views a 37
kilometer wide scene of the Earth from the ER2 altitude of about 20 kilometers.
Each MAMS footprint (individual field of view) has a horizontal resolution
of 100 meters at nadir. Since the ER2 travels at about 208 meters per second,
a swath of MAMS data 37 by 740 kilometers is collected every hour. The
nominal duration of an ER2 flight is 6 hours (maximum of about 7 hours).
>A number of geophysical parameters can be derived from the MAMS data.
The resolution of each product varies because of the desired accuracy of
each parameter. The table below lists the parameters which can be derived
from MAMS for CAMEX research. Precipitable water and skin temperature (land
or sea surface) are derived from with a physical split window algorithm
(Jedlovec 1987; Guillory et al 1993; Suggs and Jedlovec 1986). The accuracy
of precipitable ranges between 2 -5 mm root mean square error based on
the MAMS calibration, quality of the first guess, the desired spatial resolution,
and the sounding environment (poor performance occurs where temperature
inversions exist). Sea surface temperature is retrieved quite accurately
and not subject to the temperature inversion problem. Varying surface emissivity
over land influences the quality of the land surface temperature retrieval.
Upper-level humidity is retrieved with an empirical method similar to Soden
and Bretherton (1993). Accuracy varies with MAMS calibration and the locally
generated retrieval coefficients. Clouds can be detected quite well with
the multispectral channels of MAMS (even thin cirrus). Cloud top temperature
and height assignment varies with MAMS absolute calibration and cloud emissivity.
Absolute calibration degrades at cold temperatures and therefore cloud
top information approaches worst values for the tallest (coldest clouds).
References
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Guillory, A.R., G.J. Jedlovec, and H.E.
Fuelberg, 1993: A Technique for Deriving Column-Integrated Water Content
Using VAS Split-Window Data. J. Appl. Meteor. 32, 1226-1241.
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Jedlovec, G.J. , 1987:
Determination of atmospheric moisture structure from high resolution MAMS
radiance data., Ph.D. dissertation. Ph.D. Degree. The University of Wisconsin-Madison,
University Microfilm International, Ann Arbor, MI. 187.
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Soden, B.J. and F.P. Bretherton, 1993:
Upper tropospheric relative humidity from the GOES 6.7um channel: Method
and climatology for July 1987. J. Geophys. Res. 98, 16669-16688.
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Suggs, R.J. and G.J. Jedlovec, 1996: Evaluation
of a split window technique for the retrieval of geophysical parameters
from GOES. In preparation for J. Appl. Meteor.
MAMS CAMEX Derived Parameters and Their Accuracy
|
Parameter
|
Resolution
|
Coverage
|
Accuracy
|
| Total Precipitable Water |
250 - 1000 m
|
over entire image
|
2 - 5 mm rms |
Land Surface Temperature
0.5 - 0.6 K (absolute) |
100 - 300 m
|
over entire image
|
0.1 - 1.0 K (relative) |
| Sea Surface Temperature |
100 - 300 m
|
over entire image
|
0.1 K (relative)
0.1 - 1.0 K (absolute) |
Upper-Level Humidity
(in weighting function layer) |
100 - 300 m
|
over entire image
|
1 - 2% (relative)
5 - 10 (absolute) |
| Cloud Detection |
100 - 200 m
|
over entire image
|
99% efficiency |
| Cloud Mean Top Temperature |
100 - 200 m
|
where cloud present
|
0.5 K (relative)
0.5 - 6.0 K (absolute) |
| Cloud Mean Height (Pressure) |
100 - 200 m
|
where cloud present
|
50 mb (relative)
50 - 200 mb (absolute) |
|