Euradwaste '08 - EU Bookshop - Europa
Euradwaste '08 - EU Bookshop - Europa Euradwaste '08 - EU Bookshop - Europa
within feldspars in the three granites were comparable but the most interesting difference was found between the various quartz grains. In some granite where quartz minerals showed no accessible PMMA porosity, uranium access was subject to the existence of micro-cracks or intergranular fissures. Figure 2 shows the RBS spectra of Grimsel granite obtained on quartz, feldspar and biotite. In the Table below, the values of apparent diffusion coefficients obtained for each mineral type and its porosity are shown. The RBS technique was also used to quantify Cs diffusion on single minerals in Czech granites [24]. Energy (MeV) Normalized Yield 7 6 5 4 3 2 1 1.4 1.6 1.8 2.0 Grimsel Quartz + U 1 day Grimsel Feldspar + U 1 day Grimsel biotite + U 1 day Simulations 0 500 600 700 Channel 800 900 Sorption “Sorption” is the general term used to define an unknown retention mechanism at a solid surface. RN sorption may take place at the fracture walls, but also on the materials filling the fractures. In PA, sorption is handled as a reversible attachment of dissolved species to surfaces using the “Kd approach”. The Kd is experimentally derived, generally from static “batch” experiments under sitespecific conditions. Pore surface of the rock matrix is considered to dominate sorption, while the sorption on fracture or infills is minor and neglected in PA. Limitations of the Kd concept are fully recognised: in particular, the Kd-approach do not take into account the chemistry of the pore solution and its variability. Besides, other relevant processes as precipitation /co-precipitation and solid solution formation may be hidden in Kd values. Mechanistic approach to sorption and retention processes is widely treated in RTDC 1. In RTDC 4, two main problems related to Kd values are being evaluated: Kd are not obtained directly on intact rocks [1] and, furthermore, the effect of the heterogeneities is totally neglected. Different “visualisation” techniques are available to observe the regions in which radionuclides interacts (e.g. modern autoradiography method [24]), and to perform sorption studies on intact rocks. The main challenge is to quantify RN retention at a mineral level, therefore sorption experiments were carried out with small rock pieces using the particle induced X-ray emission technique ( PIXE). A mapping of the single elements on the solid surface allows identifying both the main minerals present and the reactive areas where the RN is sorbed. The quantification of RN retention in single minerals can be done only by specific analyses of the individual PIXE spectra in each scanned point within 2x2 mm 2 areas and this methodology was developed in RTDC4. Small regions within single minerals can be selected as shown in Figure 3 where uranium is preferentially sorbed in a biotite. The variability of the surface distribution coefficient (Ka) was analysed as the studied areas increased. This investigation tried to understand how the distribution coefficients must be upscaled for consideration of the mineralogical heterogeneity found in any natural system. 332 Mineral Da (m2/s) Porosity Feldspar (1.5 0.5) E-13 0.5 % Quartz (1.1 0.5) E-13 0.5 % Dark minerals (5.2 0.5) E-13 > 1.4 % Figure 2: RBS spectra of Grimsel granite main minerals after contact with U solution 1 day: (�) Quartz, (�) Feldspar and (�) Biotite. Simulations are plotted as continuous lines. In the table, the values of apparent diffusion coefficients obtained for each mineral type and its porosity are shown.
Q B Si P K - 333 Fe Figure 3: Elemental distribution maps (Si, K, Fe and U) obtained by PIXE on a 2x2 mm 2 granite area after the contact with uranium (10 days). Red squares refer to the areas selected to obtain the individual PIXE spectra for a quantitative analysis, identified here as (Q) quartz; (B) biotite; (P) plagioclase. 3. Transport in crystalline rocks: Effects of colloids. To play a role in RN migration, colloids must exist in a non-negligible concentration, be mobile, stable and be able to adsorb radionuclides in irreversible form [25]. These conditions must be verified investigating scenarios, geochemistry, hydrogeology, and other physical factors as well as possible artefacts that could bias data interpretation. In poorly mineralized waters, such as those present at the GTS, bentonite colloids may fulfil several of the above-mentioned conditions, so that the determination of the effects on radionuclide migration has to be studied in depth. The hydration and loss of density of the bentonite backfill are necessary conditions for the colloids to be formed at the bentonite/granite interface [4, 26] but the quantification, in realistic conditions, of the colloid source term from the engineered barriers is still an open issue [1, 27]. In-situ transport studies at the GTS in the CRR project [5, 28] demonstrated that bentonite colloid migration was not retarded with respect to the water flow; the colloid recovery depended on not very well identified filtration processes taking place along the flow path as size exclusion, rock/colloid interactions and diffusion in the rock matrix. The recovery of bentonite colloids and highly sorbing tri- and tetravalent elements was very high [29] but water flow conditions were not fully representative of those expected in a geological repository. Thus, it was considered necessary to perform more experimental studies at a laboratory scale, under constrained conditions as similar as possible to the real ones. In RTDC4, different processes related to bentonite colloids were analysed: generation [30], stability and effects on RN speciation (31), recovery under different flow rates [32], diffusion in the rock matrix [33]. Other studies on transport and rock/colloid interactions related with colloid properties (size or surface charge) were carried out also with model colloids (Au, quantum dots composed of CdSe/ZnS). The generation of bentonite colloids from compacted clay in contact with stagnant water was analysed. Figure 3 (left) shows that colloid concentration initially increases but a steady state is reached in a relatively short time. The higher the clay dry density, the higher the quantity of colloids generated. Water chemistry controls the stability, size and concentration of the generated colloids: the concentration of colloids increase, when the salinity of the water decreases (Figure 3, right) and when pH increases. + U
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Q<br />
B<br />
Si<br />
P<br />
K<br />
-<br />
333<br />
Fe<br />
Figure 3: Elemental distribution maps (Si, K, Fe and U) obtained by PIXE on a 2x2 mm 2 granite<br />
area after the contact with uranium (10 days). Red squares refer to the areas selected to obtain the<br />
individual PIXE spectra for a quantitative analysis, identified here as (Q) quartz; (B) biotite; (P)<br />
plagioclase.<br />
3. Transport in crystalline rocks: Effects of colloids.<br />
To play a role in RN migration, colloids must exist in a non-negligible concentration, be mobile,<br />
stable and be able to adsorb radionuclides in irreversible form [25]. These conditions must be verified<br />
investigating scenarios, geochemistry, hydrogeology, and other physical factors as well as possible<br />
artefacts that could bias data interpretation. In poorly mineralized waters, such as those present<br />
at the GTS, bentonite colloids may fulfil several of the above-mentioned conditions, so that the<br />
determination of the effects on radionuclide migration has to be studied in depth. The hydration and<br />
loss of density of the bentonite backfill are necessary conditions for the colloids to be formed at the<br />
bentonite/granite interface [4, 26] but the quantification, in realistic conditions, of the colloid source<br />
term from the engineered barriers is still an open issue [1, 27].<br />
In-situ transport studies at the GTS in the CRR project [5, 28] demonstrated that bentonite colloid<br />
migration was not retarded with respect to the water flow; the colloid recovery depended on not<br />
very well identified filtration processes taking place along the flow path as size exclusion,<br />
rock/colloid interactions and diffusion in the rock matrix. The recovery of bentonite colloids and<br />
highly sorbing tri- and tetravalent elements was very high [29] but water flow conditions were not<br />
fully representative of those expected in a geological repository. Thus, it was considered necessary<br />
to perform more experimental studies at a laboratory scale, under constrained conditions as similar<br />
as possible to the real ones.<br />
In RTDC4, different processes related to bentonite colloids were analysed: generation [30], stability<br />
and effects on RN speciation (31), recovery under different flow rates [32], diffusion in the rock<br />
matrix [33]. Other studies on transport and rock/colloid interactions related with colloid properties<br />
(size or surface charge) were carried out also with model colloids (Au, quantum dots composed of<br />
CdSe/ZnS).<br />
The generation of bentonite colloids from compacted clay in contact with stagnant water was analysed.<br />
Figure 3 (left) shows that colloid concentration initially increases but a steady state is<br />
reached in a relatively short time. The higher the clay dry density, the higher the quantity of colloids<br />
generated. Water chemistry controls the stability, size and concentration of the generated colloids:<br />
the concentration of colloids increase, when the salinity of the water decreases (Figure 3,<br />
right) and when pH increases.<br />
+<br />
U