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Euradwaste '08 - EU Bookshop - Europa

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)<br />

a)<br />

e)<br />

d)<br />

f)<br />

d)<br />

e)<br />

f)<br />

c)<br />

Figure 3.1: Overcoring of the strike-parallel SELFRAC [9] borehole at Mont Terri; a) conceptual<br />

model; b) modelling result for volumetric strain from Nagra (2002)[3]; c) 300 mm diameter slice<br />

of the overcore. The old borehole position is visible in the centre (the circular element is a section<br />

of the resin injection pipe); d) regularly spaced fractures in the collapsed region that follow the<br />

bedding planes; e) non-continuous cracks that limit collapsed regions cross-cut the bedding<br />

planes; f) cracks along the central region of the collapsed zone also cross-cutting the bedding.<br />

Sigma 1 orientation is sub-vertical.<br />

The self-sealing behaviour which is obvious for plastic clays was also investigated for indurated<br />

clays in laboratory tests. Here, this process is dominated by the combined impact of recompaction<br />

and clay swelling. A self-sealing test on a large fractured Opalinus Clay sample (L/D= 600 mm /<br />

260 mm) from the Mont Terri Rock Laboratory was performed by GRS within the framework of<br />

NF-PRO. As a result of coring and a long storage time without sufficient confinement, the sample<br />

was already highly damaged and desaturated before testing started (Fig. 3.2). Along the bedding<br />

planes, multiple macro-fractures developed through the whole sample more or less parallel to its<br />

axis. This damaged state may represent the situation in-situ near the drift wall. The large-scale sealing<br />

test focused on examining the effect of normal stress and water resaturation on gas permeability<br />

along fractures.<br />

The fractured sample had a high initial permeability of 5·10 -14 m 2 , which was measured with a radial<br />

stress of 3 MPa and an axial stress of 19 MPa. Keeping the axial stress constant, the radial stress<br />

normal to the fractures was increased stepwise to 18 MPa, resulting in a drastic decrease in permeability<br />

down to 10 -19 m 2 , which is around five orders of magnitude lower than the initial value.<br />

When the radial stress was reduced again to its initial level, the measured permeability of 10 -16 m 2<br />

was still two orders of magnitude lower than the initial value.<br />

208

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