5.3. Snow HydrologyΒΆ

ADELM updates the ground snow-water store and diagnoses snowmelt and snow sublimation from snowfall reaching the ground, air temperature, and the potential evaporative demand at the surface.

Coupling to other components

1. Snow storage balanceΒΆ

The snow-water store snow_water_storage [mm; State: snow water equivalent stored in the surface snowpack] satisfies

(5.3.1)ΒΆ\[W_{\mathrm{snow}}^{\,t+1} = W_{\mathrm{snow}}^{\,t} + P_{\mathrm{snow,ground}} - M_{\mathrm{snow}} - E_{\mathrm{snow}}\]

where \(W_{\mathrm{snow}}^{\,t}\) is the snow water storage at the start of the timestep, \(P_{\mathrm{snow,ground}}\) is snowfall reaching the ground (snowfall_to_ground_mmday [mm day-1; Flux: total snowfall reaching the ground, including direct throughfall and canopy unloading]), \(M_{\mathrm{snow}}\) is snowmelt (snowmelt_mmday [mm day-1; Flux: water flux released from the snowpack by melting]), and \(E_{\mathrm{snow}}\) is snow sublimation (snow_sublimation_mmday [mm day-1; Flux: water flux sublimated from the ground snowpack]).

2. Snow sublimationΒΆ

Snow sublimation snow_sublimation_mmday [mm day-1; Flux: water flux sublimated from the ground snowpack] occurs only in below-freezing conditions. It is limited by both an energy supply derived from net soil radiation and the available snow water:

(5.3.2)ΒΆ\[E_{\mathrm{snow}} = \min\!\Bigl(W_{\mathrm{snow}}^{\,t},\; \min\!\bigl(E_{\mathrm{snow}}^\ast,\; E_{\mathrm{energy}}\bigr)\Bigr) \cdot \mathbf{1}[T_{\mathrm{a}} < T_{\mathrm{freeze}}]\]

where \(E_{\mathrm{snow}}^\ast\) is potential_snow_sublimation [mm day-1; Diagnostic: atmospheric demand for sublimation from the ground snowpack] and the energy limit is

(5.3.3)ΒΆ\[E_{\mathrm{energy}} = \max\!\left( \frac{R_{\mathrm{soil,net}}\,t_{\mathrm{day}}}{L_{\mathrm{sub}}},\;0 \right)\]

with \(R_{\mathrm{soil,net}}\) the soil net radiation (soil_net_radiation_Wm2 [W m-2; Flux: net radiative flux at the soil surface]), \(t_{\mathrm{day}}\) the number of seconds per day, and \(L_{\mathrm{sub}}\) the latent heat of sublimation.

3. SnowmeltΒΆ

Snowmelt snowmelt_mmday [mm day-1; Flux: water flux released from the snowpack by melting] follows a degree-day formulation bounded by the snow water available after sublimation and new snowfall:

(5.3.4)ΒΆ\[M_{\mathrm{snow}} = \min\!\bigl(\max(T_{\mathrm{a}} - T_{\mathrm{freeze}},\,0)\,c_{\mathrm{melt}},\; W_{\mathrm{snow}}^{\,t} - E_{\mathrm{snow}} + P_{\mathrm{snow,ground}}\bigr)\]

where air temperature \(T_{\mathrm{a}}\) is ta_degC [degC; Driver: near-surface air temperature], the freezing threshold \(T_{\mathrm{freeze}}\) is freezing_point [default: 0 degC; Constant: temperature at which water freezes], and the melt coefficient \(c_{\mathrm{melt}}\) is snow_melt_coefficient [default: 3 mm degC-1 day-1; Fixed parameter: degree-day snowmelt coefficient: melt per degree above the freeze threshold per day].