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strings were buried 20 – 30 cm below <strong>the</strong> soil before snow accumulation beg<strong>an</strong> <strong>an</strong>d extended to<br />

80, 180, <strong>an</strong>d 200 cm above <strong>the</strong> ground surface; a guy wire tied to two trees at opposite ends of <strong>the</strong><br />

clearing w<strong>as</strong> used to te<strong>the</strong>r <strong>the</strong> tops of <strong>the</strong> <strong>the</strong>rmistor strings. During <strong>the</strong> study period <strong>the</strong><br />

<strong>the</strong>rmistor strings provided observations of soil, snow, <strong>an</strong>d air temperature.<br />

16<br />

12<br />

8<br />

4<br />

a<br />

day<br />

neutral<br />

night<br />

0<br />

0<br />

0 100 200 300 400 500 0 100 200 300 400 500<br />

upwind dist<strong>an</strong>ce, m<br />

Figure 2. (a) Normalized ch<strong>an</strong>ge in <strong>the</strong> understory turbulent flux (Q) with upwind dist<strong>an</strong>ce (x) during typical<br />

daytime (green), neutral (blue) <strong>an</strong>d nighttime (red) atmospheric stability conditions. (b) Cumulative ch<strong>an</strong>ge in<br />

<strong>the</strong> understory turbulent flux (Q) with upwind dist<strong>an</strong>ce (x) for typical daytime (green), neutral (blue) <strong>an</strong>d<br />

nighttime (red) atmospheric stability conditions.<br />

Eight water content reflectometers (Campbell Scientific model CS-615) were used to monitor<br />

soil moisture conditions surrounding <strong>the</strong> towers (Figure 3). These observations were used to<br />

ensure that latent heat fluxes were primarily allocated to sublimation <strong>as</strong> opposed to snowmelt <strong>an</strong>d<br />

to confirm that water from snowmelt had not entered <strong>the</strong> soil horizon which might trigger <strong>the</strong><br />

onset of tr<strong>an</strong>spiration.<br />

<strong>Snow</strong>pack properties<br />

Ground observations of snow depth <strong>an</strong>d snow density were derived from snow pits excavated<br />

weekly at two different locations (sub-c<strong>an</strong>opy <strong>an</strong>d within a small clearing adjacent to <strong>the</strong> flux<br />

towers). Within each snowpit, samples were taken at 10 cm vertical intervals over <strong>the</strong> <strong>entire</strong><br />

snowpit depth using a 1000 cc stainless steel cutter. <strong>Snow</strong> density stratigraphy <strong>an</strong>d bulk density<br />

<strong>an</strong>d snow water equivalent were calculated from weighted-average density values <strong>an</strong>d total<br />

snowpack depth.<br />

Observations of precipitation were used to determine <strong>the</strong> m<strong>as</strong>s input between <strong>the</strong> weekly<br />

snowpit observations, allowing us to approximate sublimation losses; ch<strong>an</strong>ges in snow water<br />

equivalent between <strong>the</strong> weekly snowpit observations result from input of m<strong>as</strong>s due to snowfall <strong>an</strong>d<br />

reduction in m<strong>as</strong>s due to sublimation. This provides a field b<strong>as</strong>ed technique for evaluating<br />

sublimation estimates from <strong>the</strong> sub-c<strong>an</strong>opy EC system. Precipitation observations were obtained at<br />

a height of 12 m from <strong>the</strong> above-c<strong>an</strong>opy EC tower; <strong>an</strong> Alter gauge shield w<strong>as</strong> used to improve<br />

precipitation gauge catch efficiency.<br />

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