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RD&D-Programme 2004 - SKB

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These processes have been studied in the field mainly in conjunction with the wetting of<br />

the buffer in a number of full-scale tests in the Äspö HRL (Prototype Repository, Canister<br />

Retrieval Test and TBT). The water inflow and the change in the negative pore pressure can be<br />

determined by measurement and follow-up of the relative humidity in a large number of points.<br />

The temperature gradient is large in TBT, enabling the other major driving force for water,<br />

which leads to drying-out in the hot part, to be studied.<br />

An important update of computation capacity has been achieved by the purchase and testing of<br />

the finite element code Code Bright developed at UPC in Barcelona. The code is an excellent<br />

complement to Abaqus, since it models certain processes in water-unsaturated soil better. For<br />

example, it models all three components (particles, water and gas) in unsaturated soil, whereas<br />

Abaqus does not model the gas component (except for temperature-driven vapour flow). On the<br />

other hand, due to the well-developed models in Code Bright, the material models contain more<br />

parameters which are often difficult to determine. A great deal of work remains to be done in<br />

determining and validating these models for <strong>SKB</strong>’s buffer materials.<br />

Model calculations of water flow have mainly been done in conjunction with modelling of the<br />

field and laboratory tests. The following calculations in particular can be mentioned:<br />

• Modelling of TBT with existing models with both Abaqus and Code Bright and comparisons<br />

with measurement data. Evaluation is under way.<br />

• Modelling of the scale test of KBS-3H (1:10) with Abaqus. The final phase of the wetting<br />

went slower than predicted.<br />

• Updated calculations of the Canister Retrieval Test. Evaluation is under way.<br />

• Modelling of the saturation and maturity phase for Lasgit with Abaqus. A new and simplified<br />

material model developed for nearly saturated soil (over 95 percent) is used in these<br />

calculations. The model has been partially verified by comparisons between laboratory tests<br />

and modellings of the laboratory tests.<br />

• Modelling of the first 1,000 days of the Febex experiment in Grimsel, Switzerland. The wetting<br />

of the buffer and the thermo-hydro-mechanical effects in the rock have been modelled<br />

and the results compared with measurements. The most important result from a water transport<br />

viewpoint is that the wetting of the buffer agreed well with the measurement results,<br />

even for the simplified assumption that the rock acts as a filter with zero water pressure<br />

and supplies the bentonite with the water it needs. Another observation is that the measured<br />

hydraulic interaction between rock and buffer is not as strong as has been modelled due<br />

to the fact that the modelled media have been coupled together. A skin zone is needed to<br />

explain the absence of negative water pressures in the rock.<br />

<strong>Programme</strong><br />

The wetting process is a part of the THM modelling that will be included in the upcoming<br />

research programme. The programme is described in section 17.2.12 “Integrated studies – THM<br />

evolution in unsaturated buffer”.<br />

17.2.5 Water transport under saturated conditions<br />

Water transport in a saturated buffer is a complex interplay between a number of sub-processes<br />

on a microscopic scale. On a macroscopic level, the result is that the permeability of a saturated<br />

buffer is very low, and this is also the essential result for the safety assessment. Other uncertainties<br />

concern the effect of transformations, which are expected to result in higher hydraulic<br />

conductivity. Very high salinities are also of importance for the process, see section 17.2.15.<br />

A special case of water-saturated buffer may arise if the water pressure in the buffer is equal<br />

to the total external pressure. The effective pressure between the clay particles is then zero<br />

and the buffer loses strength and enters a state of liquefaction. In the case of certain soils (soft<br />

sand and soft illitic clay), this can occur as a result of strong vibration or water flows, but great<br />

204 RD&D-<strong>Programme</strong> <strong>2004</strong>

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