2:3.5 Lateral Flow

Lateral flow will be significant in areas with soils having high hydraulic conductivities in surface layers and an impermeable or semipermeable layer at a shallow depth. In such a system, rainfall will percolate vertically until it encounters the impermeable layer. The water then ponds above the impermeable layer forming a saturated zone of water, i.e. a perched water table. This saturated zone is the source of water for lateral subsurface flow.

SWAT+ incorporates a kinematic storage model for subsurface flow developed by Sloan et al. (1983) and summarized by Sloan and Moore (1984). This model simulates subsurface flow in a two-dimensional cross-section along a flow path down a steep hillslope. The kinematic approximation was used in its derivation.

This model is based on the mass continuity equation, or mass water balance, with the entire hillslope segment used as the control volume. The hillslope segment has a permeable soil surface layer of depth DpermD_{perm} and length LhillL_{hill} with an impermeable soil layer or boundary below it as shown in Figure 2:3-3. The hillslope segment is oriented at an angle αhill to the horizontal.

Figure 2:3-3: Conceptual representation of the hillslope segment.

The kinematic wave approximation of saturated subsurface or lateral flow assumes that the lines of flow in the saturated zone are parallel to the impermeable boundary and the hydraulic gradient equals the slope of the bed.

Figure 2:3-4: Behavior of the water table as assumed in the kinematic storage model.

From Figure 2:3-4, the drainable volume of water stored in the saturated zone of the hillslope segment per unit area, SWly,excessSW_{ly,excess}, is

SWly,excess=1000HoϕdLhill2SW_{ly,excess}=\frac{1000*H_o*\phi_d*L_{hill}}{2} 2:3.5.1

where SWly,excessSW_{ly,excess} is the drainable volume of water stored in the saturated zone of the hillslope per unit area (mm H2_2O), HoH_o is the saturated thickness normal to the hillslope at the outlet expressed as a fraction of the total thickness (mm/mm), ϕd\phi_d is the drainable porosity of the soil (mm/mm), LhillL_{hill} is the hillslope length (m), and 1000 is a factor needed to convert meters to millimeters. This equation can be rearranged to solve for HoH_o:

Ho=2SWly,excess1000ϕdLhillH_o=\frac{2*SW_{ly,excess}}{1000*\phi_d*L_{hill}} 2:3.5.2

The drainable porosity of the soil layer is calculated:

ϕd=ϕsoilϕfc\phi_d=\phi_{soil}-\phi_{fc} 2:3.5.3

where ϕd\phi_d is the drainable porosity of the soil layer (mm/mm), ϕsoil\phi_{soil} is the total porosity of the soil layer (mm/mm), and ϕfc\phi_{fc} is the porosity of the soil layer filled with water when the layer is at field capacity water content (mm/mm).

A soil layer is considered to be saturated whenever the water content of the layer exceeds the layer’s field capacity water content. The drainable volume of water stored in the saturated layer is calculated:

SWly,excess=SWlyFClySW_{ly,excess}=SW_{ly}-FC_{ly} if SWly>FClySW_{ly}> FC_{ly} 2:3.5.4

SWly,excess=0SW_{ly,excess}=0 if SWlyFClySW_{ly} \le FC_{ly} 2:3.5.5

where SWlySW_{ly} is the water content of the soil layer on a given day (mm H2_2O) and FClyFC_{ly} is the water content of the soil layer at field capacity (mm H2_2O).

The net discharge at the hillslope outlet, QlatQ_{lat}, is given by

Qlat=24HovlatQ_{lat}=24*H_o*v_{lat} 2:3.5.6

where QlatQ_{lat} is the water discharged from the hillslope outlet (mm H2_2O/day), HoH_o is the saturated thickness normal to the hillslope at the outlet expressed as a fraction of the total thickness (mm/mm), vlatv_{lat} is the velocity of flow at the outlet (mm h1^{-1}), and 24 is a factor to convert hours to days.

Velocity of flow at the outlet is defined as

vlat=Ksatsin(αhill)v_{lat}=K_{sat}*sin(\alpha_{hill}) 2:3.5.7

where KsatK_{sat} is the saturated hydraulic conductivity (mm h1^{-1}) and αhill\alpha_{hill} is the slope of the hillslope segment. The slope is input to SWAT+ as the increase in elevation per unit distance (slpslp) which is equivalent to tan(αhill)^{tan(\alpha_{hill})}. Because tan(αhill)sin(αhill)^{tan(\alpha_{hill}) \cong sin(\alpha_{hill})} , equation 2:3.5.3 is modified to use the value for the slope as input to the model:

vlat=Ksattan(αhill)=Ksatslpv_{lat}=K_{sat}*tan(\alpha_{hill})=K_{sat}*slp 2:3.5.8

Combining equations 2:3.5.2 and 2:3.5.8 with equation 2:3.5.6 yields the equation

Qlat=0.024(2SWly,excessKsatslpϕdLhill)Q_{lat}=0.024*(\frac{2*SW_{ly,excess}*K_{sat}*slp}{\phi_d*L_{hill}}) 2:3.5.9

where all terms are previously defined.

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