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of depth hoar. The growth of depth hoar is favored when <strong>the</strong> difference between soil <strong>an</strong>d air<br />

temperatures is greater <strong>an</strong>d when vegetation buried within <strong>the</strong> snow results in a high porosity of<br />

snow cover near <strong>the</strong> snow–soil interface (Zh<strong>an</strong>g et al., 1997). Natural convection of air in snow<br />

c<strong>an</strong> occur to form depth hoar if a critical temperature gradient is exceeded. The convective flux<br />

c<strong>an</strong> be determined from <strong>the</strong> relationship between <strong>the</strong> thickness of <strong>the</strong> snow cover <strong>an</strong>d <strong>the</strong><br />

temperature gradient (Fig 44 of Akitaya, 1974).<br />

<strong>Snow</strong>/Soil Interface<br />

M<strong>as</strong>s <strong>an</strong>d energy tr<strong>an</strong>sfer at <strong>the</strong> snow/soil interface in SSVAT are b<strong>as</strong>ed on <strong>the</strong> algorithms from<br />

LSP (Liou, 1996). The infiltration model for soil c<strong>an</strong> be estimated using a qu<strong>as</strong>i-<strong>an</strong>alytic solution<br />

to Richard’s equation for vertical infiltration in a homogeneous soil (Liou, 1996; Judge, 1999). To<br />

precisely capture m<strong>as</strong>s <strong>an</strong>d energy tr<strong>an</strong>sfer at <strong>the</strong> soil/snow interface, snow <strong>an</strong>d soil layers at <strong>the</strong><br />

soil/snow interface should be thin.<br />

Figure 3. Simulations of temperature <strong>an</strong>d liquid water content for a thatch layer(modified from Chung et al.,<br />

2006)<br />

Heat tr<strong>an</strong>sfer at <strong>the</strong> snow/soil interface c<strong>an</strong> be affected by vegetation. A thatch layer in LSP w<strong>as</strong><br />

defined <strong>as</strong> a 2cm layer of org<strong>an</strong>ic matter at <strong>the</strong> b<strong>as</strong>e of <strong>the</strong> gr<strong>as</strong>s c<strong>an</strong>opy that is subject to <strong>the</strong> heat<br />

exch<strong>an</strong>ge with <strong>the</strong> atmosphere, <strong>the</strong> c<strong>an</strong>opy <strong>an</strong>d <strong>the</strong> underlying soil (Liou, 1996). To see if this<br />

thatch layer buried within <strong>the</strong> snow is import<strong>an</strong>t for heat exch<strong>an</strong>ges in SSVAT, a simulation w<strong>as</strong><br />

run for two weeks using a forcing data from Feburary 23, 2003 in CLPX (Chung et al., 2006). Our<br />

results showed that a thatch layer did not affect moisture <strong>an</strong>d temperature profiles of ei<strong>the</strong>r snow<br />

or soil when <strong>the</strong> thatch fraction varied (Fig 3). SSVAT thus ignores thatch at <strong>the</strong> snow/soil<br />

interface.<br />

RESULTS<br />

Study Area<br />

Fig 4 shows <strong>the</strong> study area at <strong>the</strong> Local Scale Observation Site (LSOS) of <strong>the</strong> NASA Cold L<strong>an</strong>d<br />

Processes Field Experiment (CLPX). SSVAT requires temperature, moisture <strong>an</strong>d grain size<br />

profiles for initialization, which were taken from <strong>the</strong> Micrometeorological Data <strong>an</strong>d <strong>Snow</strong><br />

Me<strong>as</strong>urements (Cline et al., 2002; Engl<strong>an</strong>d, 2003). SSVAT also requires precipitation data, which<br />

were taken from Ground B<strong>as</strong>ed P<strong>as</strong>sive Microwave Radiometer Data (Graf et al, 2003). Data for<br />

model validation came from snow pit me<strong>as</strong>urements of density <strong>an</strong>d grain size profiles <strong>an</strong>d subc<strong>an</strong>opy<br />

meteorological observations for late winter <strong>an</strong>d early spring (Cline et al., 2002; Hardy et<br />

al., 2002).<br />

6

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