SDC Sphy Manual
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  • manual
    • SPHY Manual
      • 1. Introduction
      • 2. Theory
        • 2.1 Background
        • Modules
        • Reference and potential evaporation
        • Dynamic vegetation processes
        • Snow processes
        • Glacier processes
        • Soil water processes
        • Soil erosion processes
        • Routing
      • 3. Applications
        • Irrigation management in lowland areas
        • Snow- and glacier-fed river basins
        • Flow forecasting
      • 4. Installation of SPHY
      • 5. SPHY model GUI
        • 5.1 Map canvas layers and GUI interactions
        • 5.2 Top menu buttons
        • 5.3 General settings
        • 5.4 Climate
        • 5.5 Soils
        • 5.6 Groundwater
        • 5.7 Land use
        • 5.8 Glaciers
        • 5.9 Snow
        • 5.10 Routing
        • 5.11 Report options
        • 5.12 Running the model
        • 5.13 Visualizing model output
      • 6. SPHY model preprocessor v1.0
        • 6.1 Overview
        • 6.2 General settings
        • 6.3 Area selection
        • 6.4 Modules
        • 6.5 Basin delineation
        • 6.6 Stations
        • 5.7 Meteorological forcing
      • 7. Build your own SPHY-model
        • Select projection extent and resolution
        • Clone map
        • DEM and Slope
        • Delineate catchment and create local drain direction map
        • Preparing stations map and sub-basins map
        • Glacier fraction map
        • Soil hydraulic properties
        • Other static input maps
        • Meteorological forcing map series
        • Open water evaporation
        • Soil erosion model input
        • Sediment transport
        • Reporting
      • Appendix 1: Input and Output
      • Appendix 2: Hindu Kush-Himalaya database
      • References
      • Copyright
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  3. 2. Theory

Glacier processes

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

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 (Aci(mm))(A_{ci} (mm))(Aci​(mm)) is calculated as:

Equation 23

ACI,t{Tavg,t∗DDFCI∗FCIif Tavg,t>00if Tavg,t≤0}A_{CI,t}\begin{Bmatrix} T_{avg,t}*DDF_{CI}*F_{CI} &\text{if } & T_{avg,t}>0 \\ 0 &\text{if } & T_{avg,t}\le0 \end{Bmatrix}ACI,t​{Tavg,t​∗DDFCI​∗FCI​0​if if ​Tavg,t​>0Tavg,t​≤0​}

with DDFci(mm°C−1d−1)DDF_{ci} (mm \degree C^{-1}d^{-1})DDFci​(mm°C−1d−1) a calibrated degree-day factor for debris-free glaciers and Fci(−)F_{ci} (-)Fci​(−) the fraction of debris-free glaciers within the fractional glacier cover (GlacF) of a grid cell. The daily melt from debris-covered glaciers (ADC(mm))(A_{DC} (mm))(ADC​(mm)) is calculated in a similar way, but with a different degree-day factor:

Equation 24

ADC,t{Tavg,t∗DDFDC∗FDCif Tavg,t>00if Tavg,t≤0}A_{DC,t}\begin{Bmatrix} T_{avg,t}*DDF_{DC}*F_{DC} &\text{if } & T_{avg,t}>0 \\ 0 &\text{if } & T_{avg,t}\le0 \end{Bmatrix}ADC,t​{Tavg,t​∗DDFDC​∗FDC​0​if if ​Tavg,t​>0Tavg,t​≤0​}

where DDFDC(mm°C−1d−1)DDF_{DC} (mm \degree C^{-1}d^{-1})DDFDC​(mm°C−1d−1) is a degree-day factor for debris-covered glaciers and FDC(−)F_{DC} (-)FDC​(−) is the fraction of debris-covered glaciers within the fractional glacier cover of a grid cell. The total glacier melt per grid cell(AGLAC(mm))(A_{GLAC} (mm))(AGLAC​(mm)) 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

AGLAC,t=(ACI,t+ADC,t)⋅GlacFA_{GLAC,t}=(A_{CI,t}+A_{DC,t})\cdot GlacFAGLAC,t​=(ACI,t​+ADC,t​)⋅GlacF

Glacier runoff

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

GRot=AGLAC,t⋅GlacROFGRo_{t}=A_{GLAC,t} \cdot GlacROFGRot​=AGLAC,t​⋅GlacROF

Glacier percolation

The percolation from glacier melt to the groundwater (Gperc,t(mm))(G_{perc,t} (mm))(Gperc,t​(mm)) is defined as:

Equation 27

Gperc,t=AGLAC,t⋅(1−GlacROF)G_{perc,t}=A_{GLAC,t} \cdot (1-GlacROF)Gperc,t​=AGLAC,t​⋅(1−GlacROF)

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.

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