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.

42 CHAPTER 2. STATE OF THE ART<br />

Volumetric water content (-)<br />

Volumetric water content (-)<br />

50<br />

40<br />

30<br />

20<br />

10<br />

0<br />

50<br />

40<br />

30<br />

20<br />

10<br />

0<br />

Volumetric water content (-)<br />

50<br />

40<br />

30<br />

20<br />

10<br />

results Brooks <strong>an</strong>d Corey (1964) V<strong>an</strong> Genuchten (1980) a, n, m=1/(1-n) Experimental<br />

0<br />

Best fit Air-entry value<br />

Residual suction zone Residual<br />

(1980) Genuchten V<strong>an</strong> 0 1 10<br />

Suction (kPa)<br />

100<br />

50<br />

0 1 10<br />

Suction (kPa)<br />

100<br />

40<br />

Volumetric water content (-)<br />

0 1 10 100<br />

Suction (kPa)<br />

30<br />

20<br />

10<br />

0<br />

a, n, m Fredlund <strong>an</strong>d Xing (1994)<br />

0 1 10 100<br />

Suction (kPa)<br />

Figure 2.15: Experimental results for Hostun s<strong>an</strong>d from drainage: soil-water characteristic<br />

curve <strong>an</strong>d fitted results using empirical models<br />

(see Chapter 6) are fitted using the above mentioned equations. In general good agreement<br />

between observed <strong>an</strong>d calculated values was found for all used models. An disadv<strong>an</strong>tage <strong>of</strong><br />

the equation proposed by Brooks <strong>an</strong>d Corey is, that the calculated results in the region <strong>of</strong><br />

the air-entry value are not proper conform to the experimental results. The calculated results<br />

fit well to the experimental results in the saturated zone, tr<strong>an</strong>sition zone <strong>an</strong>d residual zone.<br />

Comparing the experimental <strong>an</strong>d calculated results using v<strong>an</strong> Genuchten’s equations it c<strong>an</strong> be<br />

observed that the calculated results in the region <strong>of</strong> the residual suction as well as the residual<br />

zone are in better agreement to the experimental results when using the flexible parameter<br />

m. Good fit was found when using Fredlund <strong>an</strong>d Xing’s equation. Whereas v<strong>an</strong> Genuchten’s<br />

equation does not tend to 0 in the residual zone, Fredlund <strong>an</strong>d Xing’s equation even considers<br />

the water content to be 0 at a suction <strong>of</strong> 10 6 kPa.<br />

The influence <strong>of</strong> the parameters α <strong>an</strong>d λ on the shape <strong>of</strong> the curve is given in Fig. 2.16<br />

for Brooks <strong>an</strong>d Corey’s equation. The parameter α is ch<strong>an</strong>ging while the parameter λ is kept<br />

const<strong>an</strong>t in Fig. 2.16 on the left h<strong>an</strong>d side. With decreasing α the curve is shifting to larger<br />

values <strong>of</strong> suction <strong>an</strong>d the air-entry value is increasing. When λ is decreasing the slope <strong>of</strong> the<br />

curve is decreasing.

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

Saved successfully!

Ooh no, something went wrong!