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Hydro-Mechanical Properties of an Unsaturated Frictional Material

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130 CHAPTER 6. EXPERIMENTAL RESULTS<br />

Vertical strain (-)<br />

Void ratio (-)<br />

0.000<br />

0.005<br />

0.010<br />

0.015<br />

0.020<br />

0.885<br />

0.880<br />

0.875<br />

0.870<br />

0.865<br />

0.860<br />

0.855<br />

Applied suction:<br />

kPa 3.0 kPa 20.0 kPa 50.0 kPa 1.5<br />

1·106 kPa Reihe4<br />

1 10 100<br />

0 kPa<br />

1000<br />

0.890<br />

1 10 100 1000<br />

Vertical net stress (kPa)<br />

specimen Initial void ratio = 0.89 Loose<br />

Figure 6.15: Experimental results <strong>of</strong> one dimensional compression rebound test for const<strong>an</strong>t<br />

suction condition (loose specimen)<br />

- Observation during unloading path:<br />

The unloading path shows that the initial strain is not reached again. The strain from<br />

sliding between particles or fracturing is <strong>an</strong> irreversible process. Some reverse sliding<br />

during unloading is observed. This is due elastic energy within few particles.<br />

A comparison between the experimental results <strong>of</strong> the loose specimen <strong>an</strong>d the dense specimen<br />

in Fig. 6.15 <strong>an</strong>d Fig. 6.16 shows that as <strong>an</strong>ticipated the stiffness for dense specimens is<br />

higher then for loose specimens. The difference in void ration during loading path is larger<br />

for the loose specimens with approximately ∆e = 0.025 th<strong>an</strong> for the dense specimens with<br />

approximately ∆e = 0.015, which indicates a higher stiffness for the dense one. From the test<br />

results for both loose <strong>an</strong>d dense specimens it is observed, that the ch<strong>an</strong>ge in void ratio for<br />

the specimens with applied suctions up to ψ = 20 kPa is smaller th<strong>an</strong> for the dry as well as<br />

saturated (S = 1) specimens. The results <strong>of</strong> the test with applied suction ψ = 50 kPa are close

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