25.01.2013 Views

Hydro-Mechanical Properties of an Unsaturated Frictional Material

Hydro-Mechanical Properties of an Unsaturated Frictional Material

Hydro-Mechanical Properties of an Unsaturated Frictional Material

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

160<br />

CHAPTER 7. ANALYSIS AND INTERPRETATION OF THE EXPERIMENTAL<br />

RESULTS<br />

state tests. In the unsaturated hydraulic conductivity versus volumetric water content curve<br />

slight hysteresis was found for loose <strong>an</strong>d dense specimens in the intermediate r<strong>an</strong>ge.<br />

7.5 Volumetric Behavior<br />

To investigate the influence <strong>of</strong> suction on mech<strong>an</strong>ical behavior <strong>of</strong> Hostun s<strong>an</strong>d the stiffness<br />

modulus, the compression as well as swelling index, the collapse potential <strong>an</strong>d the preconsol-<br />

idation pressure are determined from the experimental results.<br />

7.5.1 Stiffness Modulus, Compression <strong>an</strong>d Swelling Index<br />

Test results from one dimensional compression rebound tests were presented in Figs. 6.15<br />

<strong>an</strong>d 6.16, where the applied vertical net stress is plotted versus volumetric strain <strong>an</strong>d void<br />

ratio for loose <strong>an</strong>d dense specimen. 3D plots <strong>of</strong> the oedometer results for loose <strong>an</strong>d dense<br />

s<strong>an</strong>d specimen are added in this section in Fig. 7.18. As already mentioned in Chapter 6 from<br />

Figs. 6.15, 6.16 <strong>an</strong>d Fig. 7.18 one c<strong>an</strong> see that as <strong>an</strong>ticipated the stiffness for dense specimen<br />

is higher then for loose specimen.<br />

The stiffness increases with matric suction from ψ = 1.5 kPa, 3.0 kPa <strong>an</strong>d 20.0 kPa for<br />

the tests carried out for dense specimen. Lowest stiffness results from the test with a matric<br />

suction <strong>of</strong> ψ = 50.0 kPa, for the dry <strong>an</strong>d the saturated specimen. Similarly to the dense<br />

specimens for the loose one the lowest stiffness was calculated for the specimen with matric<br />

suction ψ = 50.0 kPa, for the dry <strong>an</strong>d the saturated specimen. With increase in matric suction<br />

from ψ = 1.5 kPa to 20.0 kPa the stiffness is slightly increasing. Comparison <strong>of</strong> the results<br />

from the unloading path <strong>of</strong> all tests one c<strong>an</strong> state that, there is a similar behavior for all the<br />

specimens.<br />

Void ratio [-]<br />

0.665<br />

0.660<br />

0.655<br />

0.650<br />

0.645<br />

0.640<br />

0.635<br />

0.630<br />

Matric suction [kPa]<br />

1<br />

10<br />

100<br />

1000<br />

100<br />

10<br />

Vertical net stress [kPa]<br />

1<br />

Void ratio [-]<br />

0.885<br />

0.880<br />

0.875<br />

0.870<br />

0.865<br />

0.860<br />

0.855<br />

0.850<br />

Matric suction [kPa]<br />

1<br />

10<br />

100<br />

1000<br />

100<br />

10<br />

Vertical net stress [kPa]<br />

Figure 7.18: 3D plots <strong>of</strong> oedometer test results for dense (left) <strong>an</strong>d loose (right) specimen<br />

1

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!