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Hydro-Mechanical Properties of an Unsaturated Frictional Material

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7.2. SOIL-WATER CHARACTERISTIC CURVE 143<br />

Volumetric water content (%)<br />

Volumetric water content (%)<br />

50<br />

40<br />

30<br />

20<br />

10<br />

0<br />

θs= 40% θs=46%<br />

specimen - drainage Loose specimen - imbibition Dense specimen - drainage Dense specimen - imbibition Loose<br />

0.1 1 10<br />

ψaev= 1.4 kPa (loose)<br />

ψaev= 1.9 kPa (dense)<br />

100<br />

2.1 kPa (loose)<br />

Suction (kPa)<br />

kPa (dense) θr= 5%, ψr= 2.8 kPa (loose)<br />

θr= 2%, ψr= 3.3 kPa (dense)<br />

50<br />

θs=θ's<br />

40<br />

ψwev= 2.6 ψwev=<br />

41% ψaev= 1.2 kPa ψaev= 1.9 kPa<br />

θs= 46% θs=<br />

30<br />

20<br />

10<br />

0<br />

0.1 1 10 100<br />

Suction<br />

θr= 6%, ψr= 3.0 kPa<br />

(kPa) 5%, ψr= 2.7 kPa Loose specimen Initial void ratio = 0.89 Dense specimen<br />

θr=<br />

void ratio = 0.66<br />

Figure 7.4: Influence <strong>of</strong> void ratio on the shape <strong>of</strong> the soil-water characteristic curve (steady<br />

state tests)<br />

Initial<br />

derived from modified pressure plate apparatus <strong>an</strong>d the initial drainage curve derived from<br />

s<strong>an</strong>d column test I. As c<strong>an</strong> be observed from the curves the void ratio is influencing the shape<br />

<strong>of</strong> both, the drainage <strong>an</strong>d the imbibition curve. The saturated volumetric water content <strong>of</strong><br />

the loose specimens is larger then for the dense specimens (θs,loose > θs,dense). Here the larger<br />

voids <strong>of</strong> the loose specimen retain larger amount <strong>of</strong> water. Overall behavior is that with<br />

decreasing void ratio the soil-water characteristic curve is shifting to slightly higher suction<br />

values. This leads to higher air-entry value, residual suction as well as residual volumetric<br />

water content during drainage path <strong>an</strong>d also higher water-entry value during imbibition path.<br />

Due to the smaller voids in the dense specimen the water is retained up to higher suction<br />

values (ψaev,dense > ψaev,loose) when draining the saturated specimen. However, this is also<br />

causing higher residual volumetric water contents (θr,dense > θr,loose) for the dense specimens.<br />

When wetting the specimen the smaller voids <strong>of</strong> the dense specimens do absorb water at<br />

slightly higher suction values th<strong>an</strong> loose specimens (ψwev,dense > ψwev,loose). The saturated<br />

volumetric water content θs is reached first for the dense specimen.

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