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In this paper, we present import<strong>an</strong>t progress toward development of such <strong>an</strong> approach. We have<br />

found that <strong>the</strong> solution domains for snow depth, snow water equivalent, <strong>an</strong>d snow density have a<br />

predictable shape that c<strong>an</strong> be approximated by <strong>an</strong> <strong>an</strong>alytical equation with only two coefficients.<br />

Figure 1. <strong>Snow</strong> depth across a l<strong>an</strong>dscape showing shallow snow (dark) at south-facing point A<br />

<strong>an</strong>d deeper snow (light tone) on north-facing slope <strong>an</strong>d higher elevation point B.<br />

BACKGROUND AND APPROACH<br />

The approach taken w<strong>as</strong> to investigate snow properties <strong>as</strong> a function of slope, azimuth,<br />

elevation, <strong>an</strong>d forest c<strong>an</strong>opy tr<strong>an</strong>smissivity using a snow model that h<strong>as</strong> a proven record of<br />

accurately representing snowpack processes. The model solution domain w<strong>as</strong> <strong>an</strong>alyzed for<br />

structure in snow property differentiation without mapping to <strong>an</strong>y particular l<strong>an</strong>dscape.<br />

SNTHERM (Jord<strong>an</strong> 1991), SHAW (Flerchinger et al. 1994), UEB (Tarboton <strong>an</strong>d Luce 1996), <strong>an</strong>d<br />

ISNOBAL (Marks 1999) are examples of physically b<strong>as</strong>ed models that accurately simulate m<strong>as</strong>s<br />

<strong>an</strong>d energy tr<strong>an</strong>sfer in snowpacks. The complexity <strong>an</strong>d computational intensity of <strong>the</strong> models <strong>an</strong>d<br />

meteorological driver requirements usually restrict <strong>the</strong>ir use to point simulations or small research<br />

drainage b<strong>as</strong>ins (Marks 1999). With <strong>the</strong> exception of ISNOBAL, <strong>the</strong>se models are not intended for<br />

explicit mapping (pixel by pixel). We chose SNTHERM (Jord<strong>an</strong> 1991) because of p<strong>as</strong>t experience<br />

with <strong>the</strong> model (Melloh et al. 2004) <strong>an</strong>d used a recent update (SLTHERM) that includes m<strong>as</strong>s <strong>an</strong>d<br />

energy tr<strong>an</strong>sfer between <strong>the</strong> snow <strong>an</strong>d soil.<br />

We designed a method that would be broadly applicable to a hilly, forested l<strong>an</strong>dscape in New<br />

Hampshire or Vermont similar to <strong>the</strong> l<strong>an</strong>dscapes of <strong>the</strong> Sleepers River Research Watershed near<br />

D<strong>an</strong>ville, Vermont; Hubbard Brook Experimental Forest near Thornton, New Hampshire; <strong>an</strong>d <strong>the</strong><br />

Eth<strong>an</strong> Allen Firing R<strong>an</strong>ge near Jericho, Vermont. The first pl<strong>an</strong>ned application of <strong>the</strong> method<br />

developed here is for a high-resolution mobility model of <strong>the</strong> Eth<strong>an</strong> Allen Firing R<strong>an</strong>ge. Hubbard<br />

Brook, Sleepers River, <strong>an</strong>d Eth<strong>an</strong> Allen all have similar climate, topography, <strong>an</strong>d elevation r<strong>an</strong>ges<br />

from approximately 200 to 1000 m. The tree species are predomin<strong>an</strong>tly nor<strong>the</strong>rn deciduous<br />

hardwoods, including sugar maple (Acer sacharum), beech (Fagus gr<strong>an</strong>difoia) <strong>an</strong>d yellow birch<br />

(Betula allegheniensis). White <strong>as</strong>h (Fraximus americ<strong>an</strong>a) is found at middle <strong>an</strong>d lower elevations.<br />

Red spruce (Picea rubens), balsam fir (Abies balsamea), <strong>an</strong>d white birch (Betula papyrifera var.<br />

cordifolia) occur at <strong>the</strong> higher elevations <strong>an</strong>d on rock outcrops. Hemlock (Tsunga c<strong>an</strong>adensis) is<br />

found along <strong>the</strong> streams.<br />

Solar radiation, when calculated <strong>as</strong> a function of slope <strong>an</strong>d azimuth <strong>an</strong>d visualized in <strong>an</strong> array,<br />

displays a gradually ch<strong>an</strong>ging symmetrical pattern across <strong>the</strong> array <strong>an</strong>d with calendar progression<br />

(Fig. 2). It seemed plausible that snowmelt differentiation due to slope <strong>an</strong>d azimuth would also<br />

follow a tractable pattern. Slope–azimuth combinations were selected by examining plots of clearsky<br />

solar radiation over <strong>the</strong> snow se<strong>as</strong>on (Fig. 2). South- <strong>an</strong>d north-facing exposures were<br />

emph<strong>as</strong>ized over e<strong>as</strong>t- <strong>an</strong>d west-facing exposures in <strong>the</strong> selection of slope–azimuth combinations<br />

because <strong>the</strong> magnitude of daily solar radiation varies less with terrain slope for e<strong>as</strong>t <strong>an</strong>d west<br />

exposures. Modifications were made to <strong>the</strong> b<strong>as</strong>e meteorological data to drive <strong>the</strong> snowpack energy<br />

232

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