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SCHRIFTENREIHE Institut für Pflanzenernährung und Bodenkunde ...

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Chapter 6 Modeling of Coupled Water and Heat Transfer in Freezing and Thawing Soil<br />

described using the modified Richards equation (e.g., Hansson et al., 2004):<br />

∂h<br />

∂T<br />

∂h<br />

∂T<br />

[ ( h)<br />

+ K ( h)<br />

+ K ( h)<br />

+ K ( θ ) + K ( θ ) ] S<br />

∂θ<br />

( h) pi<br />

∂θi<br />

( T ) ∂<br />

∂t<br />

+ p t = z K<br />

w ∂ ∂ Lh ∂z<br />

Lh<br />

LT ∂z<br />

vh ∂z<br />

vT ∂z<br />

u −<br />

where θu [L 3 L -3 ] is the volumetric unfrozen water content (=θ+θv), θ is the<br />

volumetric liquid water content, θv is the volumetric vapor content, θi is the<br />

volumetric ice content, t is time, z is soil depth, pw and pi is the density of liquid<br />

and ice water, respectively, h is the pressure head, T is the temperature, and S is<br />

a sink/source term usually accounting for root water uptake.<br />

In Eq. 1, the first five terms on the right-hand side represent liquid flows due<br />

to gradient in pressure head (KLh, [L T -1 ]), gravity, and temperature (KLT, [L 2 T -1<br />

K -1 ]), and vapor flows due to gradient in pressure head (Kvh) and temperature<br />

gradients (KvT), respectively. Eq. 1 is nonlinear, namely dependencies of the<br />

water content and the hydraulic conductivity on the gradient of pressure head<br />

and temperature, i.e. θ(h), θi(T), KLh(h), and KLT(h). The KLh is described by the<br />

following expressions (van Genuchten, 1980):<br />

θ ( h)<br />

−θ<br />

r 1<br />

Se<br />

( h)<br />

= =<br />

n<br />

θ −θ<br />

[ 1+<br />

αh<br />

]<br />

s<br />

K ( h)<br />

−<br />

Lh<br />

r<br />

m<br />

l<br />

1/<br />

m m 2<br />

= Ks<br />

× 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, respectively; the symbols α [L -1 ], n, and m=1-1/n are empirical<br />

shape parameters, and the inverse of α is often referred to as the air entry value<br />

or bubbling pressure; Ks is the saturated hydraulic conductivity [L T -1 ], and L is a<br />

pore connectivity parameter, which normally a value of 0.5 is given.<br />

The hydraulic conductivity of frozen soil is significantly reduced by ice<br />

lenses, blocking parts of the pore space. To account for this blocking effect, the<br />

hydraulic conductivity in our study is reduced by an impedance factor, Ω (L<strong>und</strong>in,<br />

1990), which is multiplied by Q. Namely, the Ω reduces the hydraulic conductivity<br />

of the partially frozen soil, KfLh, as follows:<br />

KfLh =10 -ΩQ KLh [4]<br />

the parameter Q is the ratio of the ice content to the total water content,<br />

which accounts for the more significant blocking effects with the increase in ice<br />

[1]<br />

[2]<br />

119

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