Glacier processes
Last updated
Last updated
Since the SPHY model usually operates at a spatial resolution between 250m and 1km, the dynamics of glaciers such as ice flow cannot be resolved explicitly. However, SPHY has a mass conserving glacier evolution algorithm to represent changes in glacier cover through time.
Glacier melt is calculated with a degree-day modeling approach as well (Hock 2005). Because glaciers that are covered with debris melt at different rates than debris-free glaciers (Reid et al. 2012), a distinction can be made between different degree-day factors for both types. The daily melt from debris-free glaciers is calculated as:
Equation 23
with a calibrated degree-day factor for debris-free glaciers and the fraction of debris-free glaciers within the fractional glacier cover (GlacF) of a grid cell. The daily melt from debris-covered glaciers is calculated in a similar way, but with a different degree-day factor:
Equation 24
where is a degree-day factor for debris-covered glaciers and is the fraction of debris-covered glaciers within the fractional glacier cover of a grid cell. The total glacier melt per grid cell is then calculated by summing the melt from the debris-covered and debris-free glacier types and multiplying by the fractional glacier cover, according to:
Equation 25
In SPHY, a fraction of the glacier melt percolates to the groundwater while the remaining fraction runs off. The distribution of both is defined by a calibrated glacier melt runoff factor (GlacROF (–)) that can have any value ranging from 0 to 1. Thus, the generated runoff GRo (mm) from glacier melt is defined as:
Equation 26
Equation 27
The percolated glacier water is added to the water that percolates from the soil layers of the non-glacierized part of the grid cell (Section 2.7.1 and 2.7.7), which eventually recharges the groundwater.
The percolation from glacier melt to the groundwater is defined as: