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Hydro-mechanical behaviour of compacted bentonite-sand mixture used as sealing materials in radioactive waste disposal

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HAL Id: hal-00588065

https://hal-enpc.archives-ouvertes.fr/hal-00588065

Submitted on 22 Apr 2011

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Hydro-mechanical behaviour of compacted

bentonite-sand mixture used as sealing materials in radioactive waste disposal

Simona Saba, Q. Wang, Anh Minh Tang, Yu-Jun Cui, Jean-Dominique Barnichon

To cite this version:

Simona Saba, Q. Wang, Anh Minh Tang, Yu-Jun Cui, Jean-Dominique Barnichon. Hydro-mechanical behaviour of compacted bentonite-sand mixture used as sealing materials in radioactive waste disposal.

Mechanics and Physics of Porous Solids (MPPS)- A tribute to Prof. Olivier Coussy. 18/04/2011-

20/04/2011, Apr 2011, Champs sur Marne Marne La Vallée, France. �hal-00588065�

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Blocks start being saturated from their surface and swell forming a  loose gel that will grow to fill the technological void.

S. Saba

1,2

, Q. Wang

1

, A.M. Tang

1

, Y.J. Cui

1

, J.D. Barnichon

2

1

UR Navier/CERMES, Ecole des Ponts ParisTech, F‐77455, Marne la Vallée Cedex 

2

IRSN/DEI/SARG/LR2S, BP 17, F‐92262 Fontenay‐aux‐Roses Cedex [email protected][email protected]

Studying the buffer as a homogeneous material Studying the buffer as a non‐homogeneous material

Two Approaches

Host rock Technological void

Gel formation Compacted bentonite-sand block A better understanding of this changing gel formation is essential in 

assessing the performance of the total sealing structure.

The state of the gel formation is  changing with time in parallel  with a constant evolution of the  hydro‐mechanical conditions.

Methodology

Follow the swelling of a block immersed in water  by time‐lapse photography

Follow the swelling of a block immersed in water  by time‐lapse photography

Fixing weight Water container Support Bentonite‐sand block Transparent plate

Camera controlled via PC and takes photos automatically after a fixed time 

interval

‐ Image  processing  to investigate the  kinetics of swelling  and its limitations

‐ Compare  with  a  free swell test 

‐ Image  processing  to investigate the  kinetics of swelling  and its limitations

‐ Compare  with  a  free swell test 

First images

‐ The annular void have been  filled in 2h30min

‐ The  filling  material  has  different  state  than  the  central material

‐ The filling material is a loose  gel which state is changing  with time

‐ Generation of lateral swelling  pressure      

‐ The annular void have been  filled in 2h30min

‐ The  filling  material  has  different  state  than  the  central material

‐ The filling material is a loose  gel which state is changing  with time

‐ Generation of lateral swelling  pressure      

Initial State Final State (Annular void: 50%)

Perspectives

‐ From a mechanical point of  view,  due  to  this  non  homogeneity, the swelling  pressure generated radially  will be compared to the  axial one

‐ Investigation  of  an  anisotropic behavior

‐ From a mechanical point of  view,  due  to  this  non  homogeneity, the swelling  pressure generated radially  will be compared to the  axial one

‐ Investigation  of  an  anisotropic behavior

Swelling pressure

– No effect of technological void on the swelling pressure  – The final dry density controls the swelling pressure – No effect of technological void on the swelling pressure  – The final dry density controls the swelling pressure

Saturated hydraulic conductivity

Mock up test

‐ Objective:

‐Investigate the recovery capacity of compacted bentonite‐sand  mixture when considering a 14% of technological void

‐Provide useful information about the effectiveness of field design

‐ Methodology: Design a small scale (1/10) of the in situ SEALEX experiment model test 

‐ Objective:

‐Investigate the recovery capacity of compacted bentonite‐sand  mixture when considering a 14% of technological void

‐Provide useful information about the effectiveness of field design

‐ Methodology: Design a small scale (1/10) of the in situ SEALEX experiment model test 

Obvious effect of technological void - The hydraulic conductivities with      

technological void are higher than  those  determined  in  constant  volume condition

- That evidences  the preferential  pathway of water in the zone of  technological void (filling material  is more permeable)

Obvious effect of technological void - The hydraulic conductivities with      

technological void are higher than  those  determined  in  constant  volume condition

- That evidences  the preferential  pathway of water in the zone of  technological void (filling material  is more permeable)

20 %

(1) Initial saturation (2) Recovery of void (3) Confinement 

Technological  void

Displacement  transducer

Force sensor Force sensor

Sample

Phenomenon studied

Compacted block

water

Compacted state

Loose gel

50mm35mm

Karnland, O., Nilsson, U., Weber, H., and Wersin, P., 2008. Sealing ability of Wyoming bentonite pellets foreseen as buffer material‐Laboratory results. Physics and Chemistry of the Earth, Parts A/B/C, 33:S472–S475.

Gatabin C. 2008. ESDRED Project Module1 Selection and THM Characterisation of the Buffer Material, ESDRED International Conference, 16‐18 June 2008, Czech Technical University – Prague, Czech Republic 0.01

0.1 1 10

0.5 1 1.5 2

Final dry density of mixture (Mg/m3)

Swelling pressure (MPa)

With technological void (Present work) Constant volume (Karland et al.,2008)

1E-15 1E-14 1E-13 1E-12 1E-11 1E-10

1.4 1.6 1.8 2

Dry density of mixture (Mg/m3)

Hydraulic conductivity (m/s)

With technological void (Casagrande method) With technological void (Darcy's law - inflow) Constant volume (Darcy's law - inflow,Gatabin 2008) Constant volume (Darcy's law - outflow,Gatabin 2008)

Technological void

Sample

35 mm 38 mm

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