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Hydro-Mechanical Properties of an Unsaturated Frictional Material

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7.5. VOLUMETRIC BEHAVIOR 161<br />

Table 7.3: Results for stiffness modulus in MPa for dense <strong>an</strong>d loose specimen<br />

Condition <strong>of</strong> S=1.0 ψ = 1.5 ψ = 3.0 ψ = 20.0 ψ = 50.0 dry<br />

specimen (-) kPa kPa kPa kPa (-)<br />

loose<br />

Eoed, σ = 100 23.4 25.8 24.7 25.7 23.9 15.1<br />

Eoed, σ = 12 4.9 7.0 6.5 7.1 5.2 6.8<br />

Eur, σ = 100 124.4 158.1 149.0 130.2 145.5 102.9<br />

Eur, σ = 12 13.6 15.1 14.2 15.9 16.7 7.6<br />

dense<br />

Eoed, σ = 100 24.4 30.5 29.3 36.1 28.1 21.5<br />

Eoed, σ = 12 6.0 6.5 7.9 7.6 5.4 10.4<br />

Eur, σ = 100 150.0 131.3 255.5 141.4 168.2 174.0<br />

Eur, σ = 12 9.5 13.6 9.7 14.8 15.1 8.3<br />

To investigate in detail the influence <strong>of</strong> suction on the stiffness behavior <strong>of</strong> s<strong>an</strong>d the<br />

compression index Cc <strong>an</strong>d the swelling index Cs were estimated. The results are given in<br />

Fig 7.19. The compression index decreases first for suction less then about 20 kPa, that is<br />

equal to <strong>an</strong> increase in stiffness, <strong>an</strong>d increases again for higher suction values, that is equal to<br />

a decrease in stiffness. As expected compression index <strong>of</strong> the dense specimen is less then the<br />

compression index <strong>of</strong> the loose one, which indicates a higher stiffness. No signific<strong>an</strong>t influence<br />

<strong>of</strong> the suction on the swelling index c<strong>an</strong> be observed.<br />

Cc, Cs (-)<br />

0.00<br />

0.01<br />

0.02<br />

0.03<br />

Matric suction (kPa)<br />

0 1 10 100 10 6<br />

ψ aev,loose<br />

ψ r,loose<br />

ψ aev,dense ψ r,dense<br />

Loose<br />

Loose<br />

Dense<br />

Cc<br />

Dense<br />

Cs Cs Cc<br />

Figure 7.19: Compression <strong>an</strong>d swelling index versus suction

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