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Hydro-Mechanical Properties of an Unsaturated Frictional Material

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2.5. CONSTITUTIVE MODELS FOR HYDRAULIC FUNCTIONS 53<br />

Empirical Models<br />

Empirical models (Richards 1931, Gardner 1958, Brooks & Corey 1964) incorporate the sat-<br />

urated hydraulic conductivity <strong>an</strong>d a sufficient set <strong>of</strong> experimental data <strong>of</strong> unsaturated hy-<br />

draulic conductivity measurements, that are best fitted. One <strong>of</strong> the earliest equation, a linear<br />

function, was proposed by Richards (1931). The equations are either related to the suction<br />

(Richards 1931, Wind 1955, Gardner 1958) or to the volumetric water content (Gardner 1958,<br />

Campbell 1973, D<strong>an</strong>e & Klute 1977). Because water is only flowing through the water phase<br />

in soils unsaturated hydraulic conductivity <strong>an</strong>d soil-water characteristic curve are similar in<br />

shape. Thus soil-water characteristic curve parameters <strong>of</strong> well established soils c<strong>an</strong> also be<br />

used to determine unsaturated hydraulic conductivity function. Adv<strong>an</strong>tages <strong>an</strong>d disadv<strong>an</strong>-<br />

tages <strong>of</strong> direct <strong>an</strong>d indirect methods for obtaining the unsaturated hydraulic conductivity<br />

have been given by Leong & Rahardjo (1997a).<br />

Macroscopic Models<br />

Macroscopic models were developed on the assumption that laminar flow occurs on a micro-<br />

scopic scale that obeys Darcy´s law at the macroscopic level. Generally macroscopic models<br />

are based on the following general form:<br />

kr(ψ) = Se(ψ) δ<br />

(2.17)<br />

where Se is the effective degree <strong>of</strong> saturation, ψ is the suction <strong>an</strong>d the exponent δ is a<br />

fitting parameter. Depending on the type <strong>of</strong> soil the parameter δ is varying between 2 <strong>an</strong>d<br />

4. Averj<strong>an</strong>ov (1950) suggested δ = 3.5, Irmay (1954) suggested δ = 3.0 <strong>an</strong>d Corey (1954)<br />

suggested δ = 4.0. Brooks & Corey (1964) showed that the exponent δ = 3 is valid for<br />

uniform soils only. To account for the effect <strong>of</strong> pore-size distribution Brooks & Corey (1964)<br />

exp<strong>an</strong>ded the exponent to δ = (2 + 3λ)/λ, where λ is a pore-size distribution index. A<br />

knowledge <strong>of</strong> the soil-water characteristic curve <strong>an</strong>d the saturated hydraulic conductivity is<br />

required when using macroscopic models. The main disadv<strong>an</strong>tage <strong>of</strong> macroscopic models is,<br />

that the effect <strong>of</strong> pore-size distribution is neglected.<br />

Statistical Models<br />

Statistical models use the best-fitted suction-water content relation in connection with the<br />

saturated hydraulic conductivity to derive the relative hydraulic conductivity function. The<br />

unsaturated hydraulic conductivity function k(ψ) c<strong>an</strong> be calculated from the following rela-<br />

tionship:<br />

kr(ψ) = k(ψ)/ks; with kr(ψ) = 1 for ψ ≤ ψaev<br />

(2.18)<br />

where: kr is the relative hydraulic conductivity <strong>an</strong>d ks is the saturated hydraulic conductivity.<br />

Statistical models are based on the following assumptions (Mualem 1986):

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