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CACTUS 1 & 2
 
EXPERIMENT'S NAME
ChAracterisation of Clay under Thermal loading for Underground Storage
LAST MODIFIED
2004-05-13
EXPERIMENT'S ACRONYM
CACTUS 1 and 2
TYPE OF TEST
Clay characterization

PERSON RESPONSIBLE
Name : L. Ortiz
Email : lortiz@sckcen.be

COLLABORATIONS
SCK•CEN, G3S

FINANCING ORGANISM(S)
EC, ANDRA

GLOBAL BUDGET (k€)
900

Phenomena
Components
Safety (sub) functions concerned (if relevant)

i

Thermal
Host rock
SF
D
L
SSF
C1
R1
ii
Hydro-mechanical
Host rock
SF
C
D
L
SSF
C1
C2
R1
 
Background
In a HLW repository, the presence of canisters in the storage galleries, as a thermal source, will provoke an increase of the temperature in the surrounding host rock. This temperature variation will directly affect the hydro-mechanical properties of this rock. To study the long-term safety of a storage site, it is necessary to assess the influence of this thermal loading, on the host rock characteristics. Since Boom Clay is a potential host formation for HLW storage, two instrumented demonstration tests have been elaborated in the HADES URL.
 
Objective of the experiment
The aim of the experiment is to study the THM behaviour of the Boom Clay formation around a vertical lineic thermal source representing a stacking of HLW canisters. The experimental scale was chosen as close as possible to the real scale. Globally, it was necessary to measure the THM response of the clay host rock to this thermal loading. A derivated objective was to measure the amplitude of expected independent or coupled processes in order to identify a bottom line of the observed phenomena and to propose a relevant conceptual model for the near-field behaviour.
 
Description of the experiment

Design:
Protocol/explanation :
The external diameter of the thermal probes is equal to 30 cm (to be compared to the 43 cm diameter of the COGEMA canisters) and the length of the heated part is 2 metres. The "CACTUS" programme is composed of two in situ tests. The first test (CACTUS 1) served as preliminary approach. Each test is composed, in addition to a thermal probe placed in a large diameter central borehole, of a peripheral instrumentation located in six small diameter boreholes. The peripheral instrumentation has been installed first, in order to record stabilized the hydro-mechanical parameters prior to the drilling of the central borehole. The physionomy of the instrumentation is identical for both tests.
 
Instrumentation :
  • Two boreholes per test are dedicated to the measurement of total stress with Glötzl cells. Each borehole is equipped with five cells place at the level of the thermal probe between 12 and 15.5 m depth from the gallery. Three cells have their axis oriented towards the central borehole (radial component) and the other two have their axis oriented perpendicularly to the other three cells' axis.
  • One borehole per test is equipped with twenty PT 100 thermocouples located near the thermal probe (between 11.1 and 16.9 m depth).
  • One (slightly oblic) borehole per test is equipped with an extensometer comprising seven anchoring points distributed over the whole borehole length. This device, providing the distance variations between each anchoring point, allows to calculate the deformations in the host rock in the borehole direction. The distance between two anchored points varies between 1 m (near the thermal probe) and 3 m (near the gallery).
  • One borehole is equipped with a central tube allowing the measurement of local water content and density with a neutron-gamma probe.
  • One borehole per test is equipped with five piezometers located at the level of the thermal probe
 
Status/timing/planning :
These tests and their interpretation has been completed in the frame of the 4th EC framework programme.
 
CACTUS 1
  • From December 1989 till March 1990: peripheral drillings andinstallation of the instrumentation
  • May 1990: Drilling of the central borehole and installation of the thermal probe
  • September, 26 1990: 1st heating phase· November, 12 1990: cooling phase
  • March 14, 1991: 2nd heating phase
  • January 6, 1992: cooling phase
  • March 1993: end of the test
 
CACTUS 2
  • From February till July 1990: peripheral drillings and installation of the instrumentation
  • December 1991: Drilling of the central borehole and installation of the thermal probe
  • February 10, 1992: heating phase
  • March 4, 1993: cooling phase
 
Associated works :
  • Modelling work of the THM behaviour of the Boom Clay
  • C. Trentesaux, "Modelling of thermo-hydro-mechanical behaviour of the Boom Clay 'Cactus test'", Final report, EUR 17558, 1997.
 
Results of the experiment :

Before the excavation, it seems that the mechanical influence zone of the access gallery on the clay host rock has an extension that is larger than seven times its radius. During the excavation of the first central borehole, that lasted two days, a brutal response is observed: a drop of the interstitial pressure around the excavation, a drop of radial stress and an increase of the orthoradial stress. An increase of the water content is observed, while the density does not vary a lot. During the excavation of the second central borehole (CACTUS 2), an increase of the radial and orthoradial stresses are first observed during the drilling prior a decrease in the following days. In both cases, the deviatoric stress, defined by the difference between radial and orthoradial stresses has increased during the excavation. According to analytical calculations, the deviatoric stress is proportional to the excavation radius, and inversely proportional to the square of the distance from the borehole axis.

After the excavation, the interstitial pressures and the total stress components tend to their original values. In CACTUS 2, the equilibrium of the interstitial pressures was not reached yet when the heating phase was started. A re-consolidation of the clay host rock is observed after the excavation.

During the heating phase, the temperature measurements are coherent. The temperature field has an axisymetric configuration around the probe. The temperature rapidly decreases with the distance from the heat source. After one year of heating, the temperature increase is equal to 130-140°C on the probe, while it does not go beyond 20°C at a distance of 1.5m. The thermal analysis is made independently from the hydro-mechanical analysis, for the principal heat transfer process is conduction. The experimental measurements are successfully modelled by a numerical simulation with the following parameters:
Boom Clay thermal conductivity: 1.7 W.m-1.K-1
Boom Clay thermal diffusivity: 6 10-7 m2.s-1

Three phases are observed for the THM parameters evolution in a given point of the host rock:

  • Initial phase: the heating phase is started, but due to the thermal inertia, no temperature variation is observed at this point;
  • Transient phase: the temperature rapidly increases;
  • Near equilibrium phase: the temperature slowly and steadily increases near the probe.

The hydro-mechanical response vary according to these phase:

At the initial phase, the response is limited. We note a decrease of the orthoradial stress, an increase of the radial stress and of the interstitial pressures.

At the transient phase both radial and orthoradial stresses increase, as well as the interstitial pressures. A decrease of the water content is observed. The thermal dilation of the hot zone is hampered by the surrounding clay massif producing compressions in this zone. The thermal dilation coefficient of water is much higher than the constitutive minerals of Boom Clay. In an undrained situation, the interstitial water is overpressurized. A hydraulic gradient appears between the warm and cold zones leading to the dissipation of the overpressures.

At the near equilibrium phase, there is almost no variation of the total stress components. The interstitial pressure decrease and stabilize. The compressions appeared during the transient phase are maintained, even after the dissipation of the interstitial overpressures. Considering the water content and the strain, they are evolving towards the original state. The strain evolution is elapsed over a long period of time, which might indicate a creep due to the visco-platic properties of Boom Clay.

During the cooling phase, the THM parameters inversely evolve in comparison with the heating phase, on a very similar way. This observation tends to indicate that an important part of the observed variations are reversible.. Nevertheless, it is essential to identify the irreversibilities that subsist., i.e.:

  • A modification of the water content during the first heating phase of CACTUS 1;
  • Displacements in the massif of low amplitude;
  • A slight increase of the density.

The most interesting observation concerns the water content variation: the irreversibilities established during the first heating phase do not appear during the next cycle of similar amplitude.

 
Conclusions :

All the measurements could be used for the prediction of the hydro-mechanical response of a saturated clay host rock under the effect of a thermal loading. The results of the two tests coincide.

The observed THM couplings are different in nature:

  • On a short-term basis, the steep increase in temperature in the clay host rock gives rise to local interstitial overpressures These overpressures dissipate slowly due to the low permeability of the medium. The stress variations result from the thermal dilatation of the hot zone in the host rock and from the evolution of the interstitial overpressures
  • On a long-term basis, in a permanent regime, the hydraulic field has slightly changed while the compression state due to the heating is still noticed.
 
Bibliography :
  • J. M. Picard, B. Bazargan, G. Rousset, "Essai thermo-hydro-mécanique dans une argile profonde: 'Essai Cactus'", Final report, EUR 15482, 1994.