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Correlation Coe.<br />

1<br />

0.9<br />

0.8<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20<br />

Points<br />

GTVN vs SWE SSI vs SWE GTH VS SWE<br />

112<br />

Winter 03-04<br />

Figure 7. Variation of correlations of SWE vs SSM/I scattering signatures for various points for winter 03–04<br />

The scatter plots of SWE versus <strong>the</strong> three SSM/I signatures (GTVN, GTH, SSI) have been<br />

produced for <strong>the</strong> all <strong>the</strong> test sites. Figure 8 illustrates <strong>the</strong> variation of SWE versus scattering<br />

signatures for selected test sites (2, 9, <strong>an</strong>d 18).<br />

RESULTS OF THE ANALYSIS<br />

The presented correlation coefficients in figures 6, 7 represent different winter se<strong>as</strong>ons from<br />

2001–2004. The <strong>an</strong>alysis of <strong>the</strong> results indicates <strong>the</strong> following:<br />

1) For test sites located in low latitudes, below 45N, (1, 2, 3, <strong>an</strong>d 4) only SSI exhibits some<br />

correlation with <strong>the</strong> snow depth. There is no noticeable correlation of GTH <strong>an</strong>d GTVN vs. <strong>the</strong><br />

snow depth. This is due to <strong>the</strong> saturation saturation effect in of ch<strong>an</strong>nel 85GHz which makes SSI<br />

only suitable for estimating properties of a shallow snow pack.<br />

2) Sites located in mid- latitudes, 45N–46N, (sites 6, 7, 8, 9) <strong>the</strong>re is some correlation between<br />

GTH <strong>an</strong>d GTVN vs. snow depth but SSI shows no correlation with <strong>the</strong> snow depth.<br />

3) No correlation is observed at sites that are very close to <strong>the</strong> lake (10, 11, 12, 13, <strong>an</strong>d 14). This<br />

is due to <strong>the</strong> different spatial resolution of SSM/I in various spectral b<strong>an</strong>ds. The sensors field of<br />

view incre<strong>as</strong>es from 37km at 37GHz to 69km for 19GHz. Therefore if a me<strong>as</strong>urement is made<br />

close to <strong>the</strong> lake, <strong>the</strong> effect of <strong>the</strong> open water may be different in two ch<strong>an</strong>nels.<br />

4) Test sites located in forested are<strong>as</strong> away from <strong>the</strong> lake show moderate correlations of snow<br />

with GTH <strong>an</strong>d GTVN. In addition, scatter plots show <strong>an</strong> attenuation of brightness temperature due<br />

to forested l<strong>an</strong>d cover.<br />

5) Both GTH <strong>an</strong>d GTVN show high correlations with physical characteristics of <strong>the</strong> snow pack<br />

which makes <strong>the</strong>m good potential estimators for snow depth <strong>an</strong>d SWE. The highest correlations<br />

are observed in north of <strong>the</strong> US which is due to larger amount of se<strong>as</strong>onal snow, colder wea<strong>the</strong>r<br />

<strong>an</strong>d less number of freeze/thaw events during a winter se<strong>as</strong>on.<br />

6) Table 3 presents <strong>the</strong> correlation between SSM/I spectral signatures <strong>an</strong>d SWE obtained from<br />

SNODAS. The results show higher <strong>an</strong>d more consistent correlation coefficients for SWE th<strong>an</strong> for<br />

snow depth.<br />

7) Figure (8) shows <strong>the</strong> scatter plots of SSM/I Signatures versus SWE (SNODAS) <strong>an</strong>d SSM/I<br />

Signatures versus <strong>Snow</strong> Depth (stations) for winter 2003–2004 in different test sites. Lines fitted<br />

to each graph have various slopes <strong>an</strong>d intercepts. This demonstrates that having one linear<br />

algorithm (e.g. Ch<strong>an</strong>g or Goodison-Walker) may not be enough for snow depth or SWE in a<br />

variety of environmental <strong>an</strong>d geographical conditions.

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