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SLTHERM Model initiation<br />

<strong>Snow</strong>pack properties for <strong>the</strong> 540 meteorological sub-environments were modeled with<br />

SLTHERM. SLTHERM is a new version of SNTHERM (Jord<strong>an</strong> 1991) that h<strong>as</strong> enh<strong>an</strong>ced<br />

capability to model moisture <strong>an</strong>d energy tr<strong>an</strong>sfer between <strong>the</strong> snowpack <strong>an</strong>d soil. SNTHERM is a<br />

well-tested <strong>an</strong>d internationally known physically b<strong>as</strong>ed snow process model. The simulation<br />

period initiated on 27 October (Juli<strong>an</strong> day 300) <strong>an</strong>d continued through snow accumulation <strong>an</strong>d<br />

finally snowmelt. An initial snow temperature profile w<strong>as</strong> available from Sleepers River Research<br />

Watershed (SRRW) at 900-m elevation <strong>an</strong>d lapsed at a rate of 6.5 °C over 1000 m to <strong>the</strong> lower<br />

elevations.<br />

<strong>Snow</strong> depth (m)<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

300 320 340 360 15 35 55 75 95 115<br />

Juli<strong>an</strong> day<br />

Figure 4. The modeled snow depth time-series for each of <strong>the</strong> 27 slope–azimuth c<strong>as</strong>es for sparse forest.<br />

The top line is <strong>the</strong> most north-facing, <strong>an</strong>d <strong>the</strong> bottom line <strong>the</strong> most south-facing modeled time series.<br />

RESULTS<br />

Shaped solution domains for snow depth<br />

The snow model solutions (Fig. 4) for sparse c<strong>an</strong>opy at 900-m elevation for each of <strong>the</strong> 27<br />

slope–azimuth c<strong>as</strong>es illustrate that <strong>the</strong> snow depths differentiate with time following snowfall<br />

events, <strong>an</strong>d that <strong>the</strong> differentiation becomes more pronounced in late winter <strong>an</strong>d spring <strong>as</strong> <strong>the</strong><br />

snowpack ablates. The slope–azimuth <strong>an</strong>d c<strong>an</strong>opy dependence of solar radiation is <strong>the</strong> driving<br />

force behind snow property differentiation. On day 60 <strong>the</strong> snowpack h<strong>as</strong> differentiated mildly with<br />

azimuth <strong>an</strong>d terrain slope (Figs. 4, 5), by day 82 additional snow h<strong>as</strong> fallen <strong>an</strong>d fur<strong>the</strong>r<br />

differentiation h<strong>as</strong> occurred, <strong>an</strong>d on day 110 <strong>the</strong> snowpack is shallow <strong>an</strong>d highly differentiated.<br />

The 540 model solutions generated output for 20 time-series plots such <strong>as</strong> Figure 4, one for each<br />

of <strong>the</strong> five forest <strong>an</strong>d four elevation combinations.<br />

A three-dimensional (3-D) solution domain in <strong>the</strong> shape of a pinched cone is suggested by <strong>the</strong><br />

terrain slope versus snow-depth plot (Fig. 5) if one visualizes <strong>the</strong> bold lines (e<strong>as</strong>t-facing azimuths)<br />

to be in <strong>the</strong> foreground <strong>an</strong>d <strong>the</strong> d<strong>as</strong>hed lines (west-facing azimuths) to be in <strong>the</strong> background. The<br />

cone vertex position along <strong>the</strong> x-axis (Fig. 5) represents <strong>the</strong> snow depth for <strong>the</strong> no-slope c<strong>as</strong>e <strong>an</strong>d<br />

<strong>the</strong> vertex tr<strong>an</strong>slates to <strong>the</strong> right along <strong>the</strong> x-axis in response to new snow (day 60 to day 82) or to<br />

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