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1 Spatial Modelling of the Terrestrial Environment - Georeferencial

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66 <strong>Spatial</strong> <strong>Modelling</strong> <strong>of</strong> <strong>the</strong> <strong>Terrestrial</strong> <strong>Environment</strong><br />

canopy boundaries suppresses internal reflections in <strong>the</strong> canopy and associated interference<br />

patterns in <strong>the</strong> microwave emission (Lee et al., 2002a).<br />

Figures 4.1c and d show <strong>the</strong> time series <strong>of</strong> modelled and measured brightness temperatures<br />

for <strong>the</strong> same time periods as in Figure 4.1a and b but in <strong>the</strong> presence <strong>of</strong> a soy<br />

bean canopy. During drying period 2 (Figure 4.1c), <strong>the</strong> fresh weight <strong>of</strong> <strong>the</strong> canopy was<br />

3.45 kg m −2 and <strong>the</strong> height was 0.89 m, while during drying period 3 (Figure 4.1d), <strong>the</strong><br />

fresh weight <strong>of</strong> <strong>the</strong> canopy was 4.41 kg m −2 and <strong>the</strong> height was 1.15 m. The effect <strong>of</strong><br />

vegetation on <strong>the</strong> microwave emission from <strong>the</strong> soil is included using <strong>the</strong> extended Wilheit<br />

(1978) model (Lee et al., 2002a). As in <strong>the</strong> bare soil examples, <strong>the</strong> soil near-surface water<br />

contents range from 40% to 10% for drying period 2 (Figure 4.1c), and span a similar range<br />

for drying period 3 (Figure 4.1d). However, this is not as readily apparent in <strong>the</strong> presence<br />

<strong>of</strong> vegetation because <strong>the</strong> vegetation perturbs <strong>the</strong> emission from <strong>the</strong> soil.<br />

4.2.3 Potential Near-Future L-Band Missions<br />

The European Space Agency (ESA) has approved <strong>the</strong> Soil Moisture Ocean Salinity (SMOS)<br />

mission (SMOS homepage) with a proposed launch date between 2005 and 2007. The<br />

SMOS mission will be based on a dual polarization, L-band radiometer with an innovative<br />

aperture syn<strong>the</strong>sis concept (a two-dimensional interferometer) that can achieve an<br />

on-<strong>the</strong>-ground resolution <strong>of</strong> around 50 km and provide global measurements <strong>of</strong> microwave<br />

brightness temperature at a range <strong>of</strong> different angles. The proposed SMOS retrieval algorithm<br />

is based on a non-coherent model <strong>of</strong> emission from soil and vegetation using <strong>the</strong><br />

simple model discussed in section 4.2.2 and will simultaneously retrieve <strong>the</strong> soil moisture<br />

and <strong>the</strong> vegetation optical depth by exploiting <strong>the</strong> range <strong>of</strong> available look-angles (Kerr et al.,<br />

2001; Wigneron et al., 2000). Wigneron et al. (2000) used simulated SMOS observations<br />

(created by adding random and systematic errors to <strong>the</strong> model proposed for <strong>the</strong> SMOS<br />

retrieval algorithm) and showed that <strong>the</strong> retrieval lost accuracy as <strong>the</strong> number <strong>of</strong> available<br />

independent measures <strong>of</strong> microwave brightness temperatures at different angles decreased.<br />

NASA has selected <strong>the</strong> HYDROspheric States mission (HYDROS) as a reserve mission.<br />

It will consist <strong>of</strong> an L-band passive microwave radiometer with a resolution <strong>of</strong> around<br />

40 km and an active microwave radar with a resolution <strong>of</strong> up to 3 km. Both instruments<br />

will measure at multi-polarizations but constant look-angle.<br />

4.3 Discussion<br />

The use <strong>of</strong> coupled land surface and microwave emission models to explore potential solutions<br />

to three <strong>of</strong> <strong>the</strong> limitations <strong>of</strong> L-band passive microwave remote sensing is discussed.<br />

4.3.1 Accounting for Effects <strong>of</strong> Vegetation in Retrieval Algorithms<br />

Retrieval algorithms typically use <strong>the</strong> simple optical depth model to account for <strong>the</strong> effects<br />

<strong>of</strong> vegetation. If <strong>the</strong> only brightness temperature measurements available are at a single<br />

polarization and look-angle, such as those measured during <strong>the</strong> Sou<strong>the</strong>rn Great Plains<br />

1997 (SGP97) field experiment, <strong>the</strong> algorithms require ancillary information to estimate<br />

<strong>the</strong> optical depth. One commonly used method is to define <strong>the</strong> vegetation water content<br />

and opacity coefficient for each class <strong>of</strong> vegetation within a land cover classification, and

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