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Hydro-Mechanical Properties of an Unsaturated Frictional Material

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7.2. SOIL-WATER CHARACTERISTIC CURVE 145<br />

Influence <strong>of</strong> net stress<br />

In contrast to cohesive soils the influence <strong>of</strong> net stress on the shape <strong>of</strong> the soil-water charac-<br />

teristic curve is small for Hostun s<strong>an</strong>d as c<strong>an</strong> be seen in Fig. 6.4. Ch<strong>an</strong>ges in void ratio are<br />

negligible small during the whole experimental procedure. After saturation process <strong>an</strong>d after<br />

application <strong>of</strong> net stress main ch<strong>an</strong>ges in void ratio take place. While wetting the s<strong>an</strong>d spec-<br />

imen with water small ch<strong>an</strong>ges in settlements were measured <strong>an</strong>d thus no signific<strong>an</strong>t ch<strong>an</strong>ges<br />

in void ratio were observed.<br />

7.2.3 Tr<strong>an</strong>sient State Test Results<br />

The experimental results <strong>of</strong> s<strong>an</strong>d column tests I <strong>an</strong>d the best curve fits respectively are given<br />

in in Appendix B in Figs. B.5 to B.8 for loose <strong>an</strong>d dense specimens. Soil-water characteristic<br />

curves θ(ψ) <strong>an</strong>d S(ψ) are presented for the tests performed under tr<strong>an</strong>sient state condition<br />

with a flow rate <strong>of</strong> 30 ml/min as well as 100 ml/min. The saturated volumetric water content<br />

is θs = 46% for the loose specimen <strong>an</strong>d θs = 39% for the dense specimen under initially<br />

saturated condition. Caused by the occluded air after first imbibition process the saturated<br />

volumetric water content reduces to θ ′ s = 39% for the loose specimen <strong>an</strong>d θ ′ s = 35% for the<br />

dense specimen. For the experimental results <strong>of</strong> the tr<strong>an</strong>sient state test <strong>an</strong> air-entry value<br />

<strong>of</strong> approximately ψaev = 1.6 kPa was found for the loose specimen <strong>an</strong>d ψaev = 2.1 kPa for<br />

the dense specimen. Up to the air-entry value the soil-water characteristic curve is located<br />

in the saturated zone. After reaching the air-entry value, the water content decreases rapidly<br />

for both s<strong>an</strong>d specimens <strong>an</strong>d reaches the tr<strong>an</strong>sition zone. The tr<strong>an</strong>sition zone is between<br />

ψaev = 1.6 kPa to ψr = 2.7 kPa (θr = 5%) for the loose specimen <strong>an</strong>d between ψaev = 2.1 kPa<br />

to ψr = 3.0 kPa (θr = 6%) for the dense specimen. The residual zone starts at a relatively<br />

low suction value in the drainage cycle for both s<strong>an</strong>d specimens.<br />

In Fig. B.9 <strong>an</strong>d B.10 the experimental results <strong>an</strong>d the curve fits <strong>of</strong> the tr<strong>an</strong>sient state<br />

tests performed in the column testing device II are shown. A saturated volumetric water<br />

content <strong>of</strong> θs = 47% was measured for the loose specimen <strong>an</strong>d θs = 41% for the dense<br />

one. The volumetric water content is not ch<strong>an</strong>ging till reaching the air-entry value, that is<br />

ψaev = 1.7 kPa for the loose specimen <strong>an</strong>d ψaev = 1.9 kPa for the dense specimen (saturated<br />

zone). When passing the air-entry value the volumetric water content is rapidly decreasing<br />

<strong>an</strong>d the soil reaches unsaturated condition. The tr<strong>an</strong>sition zone extends from the air-entry<br />

value up to residual suction <strong>an</strong>d the residual volumetric water content <strong>of</strong> ψr = 3.6 <strong>an</strong>d θr = 6%<br />

for the loose specimen <strong>an</strong>d ψr = 3.8 <strong>an</strong>d θr = 8% for the dense specimen. Similar to all derived<br />

results the residual zone begins at low suction value.

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