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Hydro-Mechanical Properties of an Unsaturated Frictional Material

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188 CHAPTER 9. NUMERICAL SIMULATION OF COLUMN TEST BY FEM<br />

Table 9.1: Input parameters for the soil-water characteristic<br />

V<strong>an</strong> Genuchten parameter Swr Snr α n<br />

Tr<strong>an</strong>sient state test - drainage 0.13 0.005 0.0005 8.0<br />

Tr<strong>an</strong>sient state test - imbibition 0.13 0.18 0.001 6.5<br />

Steady state test - drainage 0.05 0.01 0.00055 6.0<br />

Steady state test - imbibition 0.02 0.01 0.0015 2.8<br />

In the experiment <strong>an</strong>d also in the numerical simulations air is not allowed to reach the<br />

bottom <strong>of</strong> the s<strong>an</strong>d column <strong>an</strong>d <strong>of</strong> the model domain respectively. At the bottom <strong>of</strong> the<br />

numerical model, a Neum<strong>an</strong>n no-flow boundary condition is assigned to air, that ensures that<br />

no mass <strong>of</strong> air flows through the bottom. For the water phase, also a Neum<strong>an</strong>n boundary<br />

condition is applied. In this case, the amount <strong>of</strong> water flux in or out <strong>of</strong> the model domain<br />

is a predefined function <strong>of</strong> time as presented in Chapter 5. The fixed flux <strong>of</strong> water phase<br />

introduced by the Neum<strong>an</strong>n boundary condition implies that at a certain time a certain mass<br />

<strong>of</strong> water has entered the model domain. For inst<strong>an</strong>ce, during imbibition the total mass <strong>of</strong><br />

water in the domain does not depend on the hysteresis model, or even on whether hysteresis is<br />

taken into account at all, but only on the value <strong>of</strong> water influx at the bottom boundary. The<br />

same is true for the hydraulic properties <strong>of</strong> the s<strong>an</strong>d that are used as input in the numerical<br />

simulation. Permeability, porosity <strong>an</strong>d soil-water characteristic curve do not relate to the<br />

amount <strong>of</strong> water mass in the domain, but strongly influence how this mass distributes in it.<br />

The water mass outflow <strong>an</strong>d inflow is shown in Fig. 9.2.<br />

Two different sets <strong>of</strong> parameters for the hysteretic soil-water characteristic curve were<br />

identified that are given in Table 9.1. First the hysteretic soil-water characteristic curve is<br />

determined directly from the s<strong>an</strong>d column test results during the tr<strong>an</strong>sient state test. An<br />

additional hysteretic soil-water characteristic curve is determined based on the results from<br />

classical steady state experiment.<br />

9.4 Comparison <strong>of</strong> Simulation Results <strong>an</strong>d Experimental Results<br />

Experimental pore-water pressure <strong>an</strong>d volumetric water content versus time results <strong>an</strong>d nu-<br />

merical pore-water pressure <strong>an</strong>d volumetric water content versus time results as well as ex-<br />

perimental <strong>an</strong>d numerical soil-water characteristic curves are compared.<br />

- Comparison using soil-water characteristic curve from tr<strong>an</strong>sient state test:<br />

In the first numerical simulation, the soil-water characteristic curve parameters are used<br />

as input parameters directly measured by the TDR sensors <strong>an</strong>d tensiometer sensors.<br />

Simulation results are compared to the experimental results in terms <strong>of</strong> saturation versus

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