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melting occurs, where<strong>as</strong> at <strong>the</strong> higher elevations o<strong>the</strong>r snowfall events still occur, <strong>an</strong>d <strong>the</strong> curve<br />

becomes steeper. For <strong>the</strong> winter snowfall (Figure 11), <strong>the</strong> relation is almost linear for all <strong>the</strong><br />

elevations, <strong>as</strong> m<strong>an</strong>y o<strong>the</strong>r snowfall events had formerly occurred, <strong>an</strong>d <strong>the</strong>re is no melting.<br />

Concerning <strong>the</strong> early spring snowfall (Figure 12), just after <strong>the</strong> snowfall <strong>the</strong> relation is linear but<br />

after some days differential melting occurs at <strong>the</strong> lower elevations, this causes a steepening of <strong>the</strong><br />

curve <strong>an</strong>d <strong>an</strong> incre<strong>as</strong>e in its concavity, where<strong>as</strong> at <strong>the</strong> higher elevations <strong>the</strong>re is still snow<br />

accumulation.<br />

In conclusion, <strong>the</strong> relation between SWE <strong>an</strong>d elevation is more or less linear, but in autumn<br />

SWE is weekly dependent on elevation, where<strong>as</strong> <strong>the</strong> dependence is very strong in spring, due to<br />

differential melting <strong>an</strong>d to <strong>the</strong> succession of <strong>the</strong> snowfall events.<br />

Figure 13: Time evolution of <strong>the</strong> ratio between SWE averaged only in north facing pixels <strong>an</strong>d SWE<br />

averaged, for 2 elevation r<strong>an</strong>ks<br />

In Figure 13 <strong>the</strong> dependence of SWE on <strong>as</strong>pect is explored. The ratio between <strong>the</strong> SWE<br />

averaged in <strong>the</strong> north facing pixels <strong>an</strong>d <strong>the</strong> SWE averaged in all pixels for each of <strong>the</strong> elevation<br />

r<strong>an</strong>ks c<strong>an</strong> be <strong>an</strong> index to evaluate <strong>the</strong> import<strong>an</strong>ce of <strong>the</strong> effects exerted by radiation <strong>an</strong>d <strong>as</strong>pect. We<br />

consider <strong>as</strong> north facing pixels those characterized by <strong>as</strong>pect r<strong>an</strong>ging from -20° to +20°, being 0°<br />

<strong>the</strong> north <strong>as</strong>pect. Figure 13 shows <strong>the</strong> time evolution of this ratio for 2 different elevation r<strong>an</strong>ks,<br />

one characteristic of <strong>the</strong> bottom of <strong>the</strong> valley <strong>an</strong>d <strong>the</strong> o<strong>the</strong>r of <strong>the</strong> higher elevations. When <strong>the</strong> ratio<br />

is close to 1 no signific<strong>an</strong>t relation of SWE with <strong>as</strong>pect is present. When differential melting<br />

between N <strong>an</strong>d S facing slopes occurs, <strong>the</strong> ratio incre<strong>as</strong>es to very high values. It c<strong>an</strong> be noticed<br />

that in <strong>the</strong> bottom of <strong>the</strong> valley differential melting is always present all through <strong>the</strong> winter, except<br />

immediately after snowfalls. At <strong>the</strong> higher elevations, on <strong>the</strong> contrary, melting is <strong>as</strong>pect dominated<br />

only in autumn <strong>an</strong>d in spring.<br />

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