SCHRIFTENREIHE Institut für Pflanzenernährung und Bodenkunde ...
SCHRIFTENREIHE Institut für Pflanzenernährung und Bodenkunde ...
SCHRIFTENREIHE Institut für Pflanzenernährung und Bodenkunde ...
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Simulations of soil water and heat flow were performed with HYDRUS-1D<br />
(Šimůnek et al., 1998). HYDRUS-1D is a finite element model for simulating the<br />
one-dimensional movement of water, heat, and multiple solutes in variably<br />
saturated media. The program numerically solves the Richards’ equation for<br />
saturated and unsaturated water flow and Fickian-based advection dispersion<br />
equations for heat and solute transport. Variably saturated water flow is<br />
described by the modified Richards’ equation:<br />
∂h<br />
∂T<br />
[ ( h)<br />
+ K ( h)<br />
+ K ( h)<br />
S<br />
∂ ( h)<br />
∂ = K ∂t<br />
∂z<br />
h ∂z<br />
h<br />
T ∂z<br />
θ w ] −<br />
[1]<br />
where θw is the volumetric liquid water content, t is time, z is the spatial<br />
coordinate positive upward, h is the pressure head, T is the temperature, and S<br />
is a sink term usually accounting for root water uptake. Kh and KT donate<br />
hydraulic conductivity due to a gradient in h and T, respectively. Soil hydraulic<br />
properties are described by the following expressions (van Genuchten, 1980):<br />
S ( h)<br />
e<br />
θ ( h)<br />
−θ<br />
1<br />
w r = =<br />
[2]<br />
n m<br />
θs<br />
−θ<br />
r [ 1+<br />
αh<br />
]<br />
K ( h)<br />
−<br />
h<br />
l<br />
1/<br />
m m 2<br />
= K s × Se<br />
( 1−<br />
( 1 Se<br />
) )<br />
[3]<br />
where Se is the effective saturation, θs and θr are the saturated and residual<br />
water contents (L 3 L -3 ), respectively; the symbols α (L -1 ), n, and m=1-1/n are<br />
empirical shape parameters, and the inverse of α is often referred to as the air<br />
entry value or bubbling pressure; Ks is the saturated hydraulic conductivity (L<br />
T -1 ), and L is a pore connectivity parameter which normally is set to 0.5. The Eq.<br />
[2] was fitted to the measured water retention data (drying branch) using the<br />
RETC code (van Genuchten et al., 1991).<br />
The soil thermal regime is modeled with the conduction–convection heat<br />
flow equation (e.g., Nassar et al., 1992):<br />
∂T<br />
∂T<br />
[ λ(<br />
] − C q C ST<br />
∂ T ∂ C( ) = θ<br />
t z w)<br />
z w −<br />
∂ ∂<br />
∂<br />
∂z<br />
w<br />
θ [4]<br />
where C(θ) and Cw denote the volumetric heat capacity of the bulk soil and<br />
liquid phase, respectively. C(θ) is determined according to De Vries (1963):<br />
90<br />
C( θ ×<br />
6<br />
θ ) ≈ ( 1.<br />
92θ<br />
m + 2.<br />
51θ<br />
o + 4.<br />
18 w ) 10<br />
[5]