Atmospheric
Soundings
An important application of satellite measurements is their ability to make soundings of the atmosphere- for example retrieving vertical profiles of water vapor and ozone (important trace gases) as well as profiles of temperature.
Two types of passive sounding techniques:
As we already observed in our review of data from the GOES sounder, sounding theory is based on the integrated form of Schwarzchild's equation , which can be simplified with the following statement:
Radiance detected by the satellite sensor comes from two sources
1) the surface term, which is a function of the radiance leaving the surface times the transmittance of the entire atmosphere along the slant path from surface to satellite.
2) the contribution of the atmosphere, the amount of radiance from discrete atmospheric layers which reach the satellite, integrated over all layers.
as we know radiation, that is not transmitted is absorbed and may interact with gases in the atmosphere in the following manner
Vertical temperature soundings (and trace gas concentrations) are based on vibrational transitions of atmospheric gases.
POES Sensors: Review
HIRS/2, high resolution infrared radiation sounder, operates like the AVHRR, but the HIRS/2 has more channels (20 versus 4 or 5).
Here is the main problem with retrieving profiles, we want to use the remotely sensed radiance and relate it to a unique temperature/trace gas profile. This is called the inversion problem. The opposite approach, the forward approach, is when temperatures and trace gas profiles are used to calculate outgoing radiance (obviously, this only works in regions which are not contaminated with clouds).
Review of Sounding Tutorial concepts presented in the GOES Tutorial (http://cimss.ssec.wisc.edu/sounder/profinfo.html)
Radiative
Transfer Equation Basic Principles
The upwelling radiation sensed by a satellite sensor is governed by a) emission from the earth's surface transmitted through the atmosphere and b) emission from the atmospheric layers transmitted through the outer layers of the atmosphere.
The surface contribution to the upwelling radiation sensed at the top of the atmosphere for wavelength lambda is a product of the surface emissivity, the Planck function at the surface temperature, and the vertical transmittance through the depth of the atmosphere. This is written as:
The transmittance of upwelling radiation through the atmosphere is diminished exponentially with increasing path length,
where k is the absorption coefficient of the atmosphere and u is the density weighted path length.
The formulation for a discrete atmospheric layer is similar to that for the surface contribution except that the appropriate layer emissivity, Planck function at layer temperature , and vertical transmittance would be used. The contribution for all atmospheric layers is then,
The radiative transfer equation combines the surface and atmospheric contributions and for an infinitely layered atmosphere can be written:
The term
in the radiative transfer equation is known as a weighting function. The weighting function, the derivative of transmittance with respect to height (pressure), specifies the relative contribution each atmospheric layer makes to the radiation emitted to space and thereby determines those regions of the atmosphere which are sensed from space at this wavelength. Sounding is accomplished with a group of spectral bands selected to detect radiation emitted from successively lower layers of the atmosphere.
The TOVS systems includes four modules
The preprocessor process digital count data and converts it to radiances, and each scan spot is located on the earths surface. The preprocessor also calculates the solar zenith angle, terrain elevations, and first guess of the skin temperature and surface albedo.