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Hydro-Mechanical Properties of an Unsaturated Frictional Material

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46 CHAPTER 2. STATE OF THE ART<br />

fitting parameters bi <strong>an</strong>d di for imbibition curve c<strong>an</strong> be calculated using:<br />

� �<br />

(w1i − c)(wu − w2i)<br />

log<br />

(wu − w1i)(w2i − c)<br />

di =<br />

, bi =<br />

log(ψ2i/ψ1i)<br />

(w1i − c)ψ di<br />

1i<br />

wu − w1i<br />

(2.15)<br />

The parameters bd <strong>an</strong>d dd in Eq. 2.13 are replaced by the determined parameters bi<br />

<strong>an</strong>d di used for estimation <strong>of</strong> the main imbibition curve. Exemplary main drainage <strong>an</strong>d<br />

imbibition curve are given in Fig 2.20 for Hostun s<strong>an</strong>d, where the additional two points<br />

for deriving the main imbibition curve from the main drainage curve are included.<br />

Physical Models<br />

Domain models are based on physical properties <strong>of</strong> the soil. Domain models are divided into<br />

independent domain models <strong>an</strong>d dependent domain models. Based on Néel´s diagram (Néel<br />

1942, 1943) or Mualem´s diagram (Mualem 1974), where the distribution <strong>of</strong> water in a soil<br />

is defined during drainage <strong>an</strong>d imbibition processes, the hysteresis was described by Everett<br />

& Smith (1954), Everett (1955), Poulovassilis (1962), Philip (1964), Mualem (1974, 1984a),<br />

Hogarth et al. (1988) (independent domain models) <strong>an</strong>d Mualem & Dag<strong>an</strong> (1975), Mualem<br />

(1984b), Topp (1971b), Poulovassilis & El-Gharmy (1978) (dependent domain models). De-<br />

pendent models were derived from independent models <strong>an</strong>d additionally consider the effect<br />

<strong>of</strong> pore water blockage against the air-entry value <strong>an</strong>d the water-entry value in a soil during<br />

drainage <strong>an</strong>d imbibition. Poulovassilis (1962) performed drainage-imbibition tests on glass<br />

bead porous medium <strong>an</strong>d was one <strong>of</strong> the first who applied the domain theory to hysteresis.<br />

He obtained good agreement between predicted values <strong>an</strong>d observed values. Further models<br />

were suggested by Everett (1967), Topp (1971b). For these models a set <strong>of</strong> measured suction-<br />

water content data at the sc<strong>an</strong>ning curves is required. To reduce the amount <strong>of</strong> required<br />

experimental data Philip (1964), Mualem (1974) proposed similarity hypothesis. Based on<br />

similarity hypothesis Mualem proposed several models (Mualem 1977, 1984b). These models<br />

require boundary drainage curve for prediction.<br />

The measurement <strong>of</strong> suction water content relationship in the field <strong>an</strong>d also in the labo-<br />

ratory is a time consuming procedure. Sometimes it is useful to estimate the suction water<br />

content before. Physical models are capable to estimate the relation between saturation <strong>an</strong>d<br />

suction based on typical soil parameters as grain-size distribution or porosity. Physical models<br />

based on soil parameters (e.g. grain-size distribution, void ratio) <strong>an</strong>d/or pore geometry were<br />

suggested amongst others by Arya & Paris (1981), Haverkamp & Parl<strong>an</strong>ge (1986), Fredlund<br />

et al. (1997), Zapata et al. (2000), Aubertin et al. (2003), Zou (2003, 2004). These models<br />

utilize soil properties as well as geometric properties to estimate the suction water content<br />

relationship. Rojas & Rojas (2005) suggested a probabilistic model that is based on the phys-<br />

ical description <strong>of</strong> a porous system. Therefore two different elements, the sites (cavities) <strong>an</strong>d<br />

bonds (throats) are considered each with a proper size distribution. Whereas most models

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