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<strong>an</strong> icy fog that creeps up valleys <strong>an</strong>d allows for ice to accumulate on vegetation. These distinct<br />
distributions may also be <strong>an</strong> effect of grain size growth during <strong>the</strong> early winter months,<br />
influencing <strong>the</strong> scattering properties of <strong>the</strong> snowpack. At <strong>the</strong> 36.5 GHz frequency, emissivity<br />
decre<strong>as</strong>es proportional to <strong>an</strong> incre<strong>as</strong>e in grain size (Mätzler, 1994), <strong>an</strong>d so <strong>as</strong> <strong>the</strong> grains within <strong>the</strong><br />
snowpack grow early in <strong>the</strong> winter, <strong>the</strong>ir Tb decre<strong>as</strong>es from <strong>the</strong> upper distribution to <strong>the</strong> lower<br />
distribution (Fig. 3). As <strong>the</strong>se events both occur within <strong>the</strong> same time frame, fur<strong>the</strong>r investigation<br />
is required to identify <strong>the</strong> source of <strong>the</strong>se differing relationships.<br />
The second technique, examining a histogram of AMSR-E 36.5V GHz Tb distribution from <strong>the</strong><br />
Wheaton b<strong>as</strong>in for all 2004 <strong>an</strong>d 2005 data, also produced a Tb threshold of 252 K (Fig. 4). The<br />
frequency histogram, with a bin size of 2 K, displays a bimodal distribution from which it is<br />
interpreted that brightness temperatures less th<strong>an</strong> 252 K relate to frozen, non-melting snow <strong>an</strong>d<br />
brightness temperatures greater th<strong>an</strong> 252 K relate to wet, melting snow <strong>as</strong> well <strong>as</strong> no snow during<br />
<strong>the</strong> summer months. The sets of individual pixels, representing <strong>the</strong> upper (pixels A02 <strong>an</strong>d A03),<br />
middle (pixels B02 <strong>an</strong>d B03), <strong>an</strong>d lower (pixels C02 <strong>an</strong>d C03) portions of <strong>the</strong> Wheaton River<br />
b<strong>as</strong>in, do not have <strong>as</strong> clear a bimodal distribution but do have comparable minimum values around<br />
252 K (Fig. 4). This, along with <strong>the</strong> plots of Tb against air temperature, suggests that <strong>the</strong> Tb<br />
threshold is effective in differentiating between dry <strong>an</strong>d wet snow at <strong>the</strong> drainage b<strong>as</strong>in <strong>an</strong>d subdrainage<br />
b<strong>as</strong>in scales in this heterogeneous terrain.<br />
The DAV calculation, which involves taking <strong>the</strong> difference between night <strong>an</strong>d day observations,<br />
shows <strong>the</strong> daily contr<strong>as</strong>t in brightness temperatures at this time of year. The timing of <strong>the</strong> AMSR-<br />
E overp<strong>as</strong>ses for this region are around 03:30 <strong>an</strong>d 13:30 local time (PST), which are likely near<br />
<strong>the</strong> times of minimum <strong>an</strong>d maximum daily melt, <strong>an</strong>d so <strong>the</strong> difference in <strong>the</strong> Tb from <strong>the</strong>se times<br />
provides a good indicator of melting <strong>an</strong>d refreezing snow. The DAV threshold incre<strong>as</strong>ed due to<br />
<strong>the</strong> apparent incre<strong>as</strong>ed sensitivity of <strong>the</strong> AMSR-E sensor to daily Tb fluctuations (Fig. 6a). A new<br />
DAV threshold of ±18 K, which w<strong>as</strong> determined by comparing <strong>the</strong> AMSR-E DAV with SSM/I<br />
DAV for <strong>the</strong> Wheaton River pixels in 2005 (Fig. 6b), represents times when strong melt-refreeze<br />
cycles are occurring during <strong>the</strong> spring snowmelt tr<strong>an</strong>sition.<br />
The ch<strong>an</strong>ge in Tb <strong>an</strong>d DAV thresholds from SSM/I to AMSR-E (Table 2) is most likely <strong>the</strong><br />
result of differences in <strong>the</strong> times of data acquisition for <strong>the</strong> two sensors. Daily AMSR-E<br />
overp<strong>as</strong>ses for <strong>the</strong> area occur around 03:30 <strong>an</strong>d 13:30 PST, where<strong>as</strong> SSM/I overp<strong>as</strong>ses occur<br />
around 08:30 <strong>an</strong>d 18:30 PST. The AMSR-E sensor makes observations during <strong>the</strong> early morning,<br />
when temperatures <strong>an</strong>d corresponding Tb would be near <strong>the</strong>ir daily minimum, <strong>an</strong>d again in <strong>the</strong><br />
early afternoon, when much of <strong>the</strong> mountainous terrain would be near <strong>the</strong> daily maximum air <strong>an</strong>d<br />
brightness temperatures. This creates larger DAV in relation to <strong>the</strong> DAV from SSM/I, since <strong>the</strong><br />
timing of SSM/I overp<strong>as</strong>ses is fur<strong>the</strong>r from <strong>the</strong>se daily minimum <strong>an</strong>d maximum, <strong>an</strong>d <strong>the</strong>refore<br />
requires a larger DAV threshold. In addition, <strong>the</strong> DAV threshold must incre<strong>as</strong>e so <strong>as</strong> to not<br />
indicate that melting is occurring when large DAV are observed during <strong>the</strong> summer, when much<br />
of <strong>the</strong> l<strong>an</strong>d is snow-free (Fig. 6b).<br />
Field-observed snow liquid-water content me<strong>as</strong>urements from <strong>the</strong> Wheaton River b<strong>as</strong>in during<br />
<strong>the</strong> spring of 2005 support <strong>the</strong> Tb threshold of 252 K <strong>an</strong>d also show that <strong>the</strong> <strong>as</strong>sumed response in<br />
Tb to melting snow c<strong>an</strong> be directly attributed to snowmelt instead of o<strong>the</strong>r effects, such <strong>as</strong> liquid<br />
precipitation events. Surface (0 cm) <strong>an</strong>d near surface (0.5-2 cm) wetness me<strong>as</strong>urements relate<br />
very well to AMSR-E 36.5V GHz Tb observations obtained at coincident times (Figs. 5a <strong>an</strong>d 5b,<br />
Table 3). At wetness values below 2%, <strong>the</strong> Tb are clustered between 230 K <strong>an</strong>d 245 K, but <strong>as</strong> <strong>the</strong><br />
liquid-water content of <strong>the</strong> snowpack incre<strong>as</strong>es above 2% by volume, <strong>the</strong> Tb appear to incre<strong>as</strong>e<br />
near <strong>an</strong>d above <strong>the</strong> threshold of 252 K (Fig. 5a). For <strong>the</strong> period prior to <strong>an</strong>d including <strong>the</strong><br />
beginning of <strong>the</strong> spring tr<strong>an</strong>sition, <strong>the</strong> ch<strong>an</strong>ges in <strong>the</strong> snowpack wetness through time closely<br />
follow that of <strong>the</strong> AMSR-E Tb, <strong>an</strong>d at wetness values above 2%, <strong>the</strong> Tb are at or above <strong>the</strong> 252 K<br />
threshold (Fig. 5b). This relationship verifies that <strong>the</strong> Tb response is due to <strong>the</strong> presence of liquid<br />
water within melting snow.<br />
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