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Spent Fuel and Waste Science and Technology
Coupled THM modeling of In Situ Heater
Experiments at Mont Terri (Switzerland) and
Bure (France) Underground Laboratories
Jonny Rutqvist, Hao Xu, Jens Birkholzer
Lawrence Berkeley National Laboratory
SFWST WG Meeting in Las Vegas
Argillite/Crystalline Sessions
May 24, 2017
Spent Fuel and
Waste Science and
Technology
Stress-induced
fracture opening
or closure with
associated
permeability
change
Infiltration of
water from rock
to bentonite
Drying and
shrinkage
Heating of bentonite
and rock
Thermal
Stress
Wetting and
swelling of
bentonite
Vapor flow along
thermal gradient
away from heat
source
Stress-induced
fracture opening
or closure with
associated
permeability
change
Infiltration of
water from rock
to bentonite
Drying and
shrinkage
Heating of bentonite
and rock
Thermal
Stress
Wetting and
swelling of
bentonite
Vapor flow along
thermal gradient
away from heat
source
Bentonite 100%
Saturated with a
Swelling pressure
of ļ‚» 5 MPa
Temperature close
to ambient
Sealing of
fracture?
Remaining
ā€œpermanentā€
changes in rock
properties (e.g.
irreversible
fracture shear)?
Restored hydrostatic
fluid pressure
Excavation
Disturbed
Zone (EDZ)
Bentonite 100%
Saturated with a
Swelling pressure
of ļ‚» 5 MPa
Temperature close
to ambient
Sealing of
fracture?
Remaining
ā€œpermanentā€
changes in rock
properties (e.g.
irreversible
fracture shear)?
Restored hydrostatic
fluid pressure
Excavation
Disturbed
Zone (EDZ)
Short-Term THM Disturbance
(0 to 1000 years)
Long-Term Impact
(10,000 to 100,000 years)
ā€¢ Strongest during early time (excavation, waste emplacement and thermal
peak), but may cause permanent changes that could impact long-term
performance.
ā€¢ Complex, but can be analyzed with advanced numerical modeling supported
by lab and field experiments.
Coupled THM Processes and
Nuclear Waste Disposal
Spent Fuel and
Waste Science and
Technology
TOUGH2
Multiphase flow and
heat transport
FLAC3D
Geomechanics
ā€¢Linking two established codes (each
hundreds of users word-wide)
ā€¢Both codes continuously developed and
applied in their respective fields
ā€¢Large number of constitutive model
available and relatively easy to
implement new constitutive models
ā€¢First developed and applied in the Yucca Mountain Project (2000-2008)
for modeling high-temperature multiphase flow and geomechanics
ā€¢Modeling THM in bentonite and clay host rock (from 2010)
ā€¢Modeling THM in salt host rock (from 2013)
ā€¢Modeling of THM in deep borehole disposalā€¦
TOUGH-FLAC Simulator:
(Rutqvist et al., 2002; Rutqvist 2011; 2017)
LBNL THM Modeling of Nuclear
Waste Disposal
Spent Fuel and
Waste Science and
Technology
THM driven buffer/rock interactions: 1) Delayed buffer resaturation due to low rock
permeability, 2) thermal-pressurization in rock affects pressure and stress evolution in buffer
Opalinus clay:
15% fluid saturated porosity
5ļ‚“10-20 m2 permeability
ļƒž Strong THM coupling
COUPLED THM MODELING OF A
REPOSITORY IN CLAY
Rutqvist et al., (2014)
Spent Fuel and
Waste Science and
Technology
TOUGH-FLAC
1) Barcelona Basic Model (BBM)
A constitutive model for thermo-elasto-plastic
behavior of unsaturated soils (bentonite)
ā€¢ Shear strength and stiffness depends on saturation ( or suction)
ā€¢ Wetting-induced swelling or collapse strains
Deviatoric
(shear) stress
Suction
Netpressure(total
stresslessgaspressure)
Drying
Cam-clay yield
surface (fully
fluid saturated)
Deviatoric
(shear) stress
Suction
Netpressure(total
stresslessgaspressure)
Drying
Cam-clay yield
surface (fully
fluid saturated)
Bentonite block stored at different
relative humidity (Teodori et al 2011)
55%
75%
99%
2) Barcelona Expansive Model (BExM)
ā€¢ Micro- and macro-structure
ā€¢ Proper modeling of fluid flow through macro pores and their
changes with stress and saturation
ā€¢ Can provide a link for coupling mechanics with chemistry
TOUGH-FLAC THM Simulator
LBNL THM Model Developments
for Bentonite Backfill
Spent Fuel and
Waste Science and
Technology
ļ® Undertaken by NAGRA as an ultimate test
for the performance of geologic disposal
in Opalinus Clay, with focus on both the
EBS components and the host-rock
behavior
ļ® It will be one of the largest and longest
running heater tests worldwide
ļ® Thousands of sensors within the EBS and
surrounding rock for monitoring THMC
processes
(Figure from Tobias Vogt NAGRA)
2.5 m
Mont Terri Full-scale Emplacement (FE)
Experiment
International Partners
Spent Fuel and
Waste Science and
Technology
TOUGH-FLAC Model of FE Experiment
Access tunnel
Plug
Heaters
Heater
Bentonite
blocks
Bentonite
pellets
Shot crete
Spent Fuel and
Waste Science and
Technology
ā€¢ Anisotropic THM properties (thermal conductivity, permeability, strength)
of Opalinus Clay considering bedding
ā€¢ TH bentonite properties of granular bentonite and bentonite blocks
from laboratory scale and HE-E (half-scale) modeling
ā€¢ Basic Barcelona Model (BBM) properties for granular bentonite and
blocks (but too early to see significant swelling stress in the buffer)
THM Properties and Heat Load
Spent Fuel and
Waste Science and
Technology
Heater
Host
rock
Moisture Flow in Bentonite Buffer
During Heating
Heating
Drying
Wetting
ļ€Ø ļ€©zP
k
X ll
l
rlw
ll
w
l ļƒ‘ļ€­ļƒ‘ļ€­ļ€½ g
k
q ļ²
ļ­
ļ²
Liquid Darcy Flow:
Liquid pressure
gradient
w
g
w
ggg
w
g XDS ļƒ‘ļ€­ļ€½ Ii ļ“ļ¦ļ²
Vapor diffusion:
Water mass
fraction in gas
Effective
vapor diffusion
Spent Fuel and
Waste Science and
Technology
T IM E (d a y s )
TEMPERATURE(C
o
)
0 5 0 1 0 0 1 5 0 2 0 0 2 5 0 3 0 0 3 5 0 4 0 0
0
1 0
2 0
3 0
4 0
5 0
6 0
7 0
8 0
9 0
1 0 0
1 1 0
1 2 0
1 3 0
1 4 0
1 5 0
H e a te r S u rfa c e
1 0 c m fro m h e a te r
2 0 c m fro m h e a te r
A t tu n n e l w a ll
F ie ld d a ta
M o d e lin g
TIME (days)
TEMPERATURE(Co
)
0 50 100 150 200 250 300 350 400
0
50
100
150
Heater surface
10 cm from heater
20 cm from heater
Simulated and Observed Temperature
(mid heater) 1st year
ā€¢ Calibrated thermal properties of ā€œheaterā€ for temperature distribution on heater-
surface
ā€¢ Heater-surface temperature higher at granular bentonite (Tmax=126ļ‚°C) then at
bentonite block pedestal (Tmax=118ļ‚°C)
ā€¢ Excellent agreement between simulated and observed temperature
Granular Bentonite Bentonite Blocks
Spent Fuel and
Waste Science and
Technology
TIME (days)
RELATIVEHUMIDITY(-)
0 50 100 150 200 250 300 350 400
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
20 cm from heater
10 cm from heater
At tunnel wall
20 cm from heater
10 cm from heater
TIME (days)
RELATIVEHUMIDITY(-)
0 50 100 150 200 250 300 350 400
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
ā€¢ Good agreement for substantial reduction of the effective vapor diffusion
coefficient through a medium tortuosity factor as low as 0.14.
w
g
w
ggg
w
g XDS ļƒ‘ļ€­ļ€½ Ii ļ“ļ¦ļ²
Diffusion coefficient for vapor-
air mixture 2.13e-5 m2/s
Medium tortuosity,
best match for 0.14
Mass fraction
Simulated and Observed Moisture
Evolution (mid heater) 1st year
Spent Fuel and
Waste Science and
Technology
TIME (days)
TEMPERATURE(Co
)
0 100 200 300 400 500 600 700 800
0
10
20
30
40
50
60
70
80
90
100
110
120
130
140
150
Heater Surface
10 cm from heater
20 cm from heater
At tunnel wall
Field data
Modeling
20 cm from heater
10 cm from heater
At tunnel wall
TIME (days)
RELATIVEHUMIDITY(-)
0 100 200 300 400 500 600 700 800
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Comparison with 2 Years of Data
(Heater 2)
Heater 2
Spent Fuel and
Waste Science and
Technology
Comparison with 2 Years of Data
(Heater 3)
TIME (days)
RELATIVEHUMIDITY(-)
0 200 400 600 800
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
20 cm from heater
10 cm from heater
At tunnel wall
Field data
Modeling
TIME (days)
TEMPERATURE(Co
)
0 200 400 600 800
0
10
20
30
40
50
60
70
80
90
100
110
120
130
140
150
Heater Surface
10 cm from heater
20 cm from heater
At tunnel wall
Heater 3
Spent Fuel and
Waste Science and
Technology
Real Tunnel Shape vs Model
Blue line at
designed tunnel
radius of 1.4 m
Laser scan
of tunnel wall
Spent Fuel and
Waste Science and
Technology
TempƩrature
Pression
interstitielle
3 Borehole Heaters 12
to 16 m from drift wall
23 monitoring boreholes with
over 200 sensors (temperature,
pressure, displacement)
Temperature
Pressure
TED Borehole Heating Experiment at Bure
by ANDRA, France
Spent Fuel and
Waste Science and
Technology
Sample
scale
Borehole
scale
Micro-tunnel
scale
Repository
scale
ā€¢ Upscaling is an important issue for the repository design and safety
calculation: How to go from sample to a repository scale ?
ā€¢ Two in situ tests performed at the underground research laboratory in
Bure (France) will be interpreted and modeled
ā€¢ The host rock consists of Callovo-Oxfordian claystone (COx)
ā€¢ Thermally induced pore pressure build-up and stress changes around a
repositoryā€¦
Upscaling of THM Parameters
(DECOVALEX Task Led by ANDRA, France)
Spent Fuel and
Waste Science and
Technology
TOUGH-FLAC Model of TED Borehole
Heating Experiment
Entire Model
Heaters
(Biotā€™s coefficient)
Some basic
Cox Claystone
properties
Spent Fuel and
Waste Science and
Technology
Simulation Results with Comparison to
Measured Data - Temperature
Spent Fuel and
Waste Science and
Technology
Field Data
(dashed lines)
Simulations
(solid lines)
Simulation Results with Comparison to
Measured Data - Pressure
Spent Fuel and
Waste Science and
Technology
Concluding Remarks THM Modeling
ā€¢ 3 new journal papers published on DECOVALEX-2015 work
(modeling of Mont Terri experiments)
ā€¢ Continue modeling of FE- Experiment with access to field data
(2 years of heating)
- Opportunity for applying dual-structure (BExM) model in
collaboration with the Barcelona group
ā€¢ Continue work on ANDRAā€™s heater tests in Cox clay stone
associated with DECOVALEX-2019
ā€¢ Implementation and testing of continuum damage model for
EDZ and permeability evolution in clay host rock with
comparison to TOUGH-RBSN discrete fracture modelā€¦
20

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  • 1. Spent Fuel and Waste Science and Technology Coupled THM modeling of In Situ Heater Experiments at Mont Terri (Switzerland) and Bure (France) Underground Laboratories Jonny Rutqvist, Hao Xu, Jens Birkholzer Lawrence Berkeley National Laboratory SFWST WG Meeting in Las Vegas Argillite/Crystalline Sessions May 24, 2017
  • 2. Spent Fuel and Waste Science and Technology Stress-induced fracture opening or closure with associated permeability change Infiltration of water from rock to bentonite Drying and shrinkage Heating of bentonite and rock Thermal Stress Wetting and swelling of bentonite Vapor flow along thermal gradient away from heat source Stress-induced fracture opening or closure with associated permeability change Infiltration of water from rock to bentonite Drying and shrinkage Heating of bentonite and rock Thermal Stress Wetting and swelling of bentonite Vapor flow along thermal gradient away from heat source Bentonite 100% Saturated with a Swelling pressure of ļ‚» 5 MPa Temperature close to ambient Sealing of fracture? Remaining ā€œpermanentā€ changes in rock properties (e.g. irreversible fracture shear)? Restored hydrostatic fluid pressure Excavation Disturbed Zone (EDZ) Bentonite 100% Saturated with a Swelling pressure of ļ‚» 5 MPa Temperature close to ambient Sealing of fracture? Remaining ā€œpermanentā€ changes in rock properties (e.g. irreversible fracture shear)? Restored hydrostatic fluid pressure Excavation Disturbed Zone (EDZ) Short-Term THM Disturbance (0 to 1000 years) Long-Term Impact (10,000 to 100,000 years) ā€¢ Strongest during early time (excavation, waste emplacement and thermal peak), but may cause permanent changes that could impact long-term performance. ā€¢ Complex, but can be analyzed with advanced numerical modeling supported by lab and field experiments. Coupled THM Processes and Nuclear Waste Disposal
  • 3. Spent Fuel and Waste Science and Technology TOUGH2 Multiphase flow and heat transport FLAC3D Geomechanics ā€¢Linking two established codes (each hundreds of users word-wide) ā€¢Both codes continuously developed and applied in their respective fields ā€¢Large number of constitutive model available and relatively easy to implement new constitutive models ā€¢First developed and applied in the Yucca Mountain Project (2000-2008) for modeling high-temperature multiphase flow and geomechanics ā€¢Modeling THM in bentonite and clay host rock (from 2010) ā€¢Modeling THM in salt host rock (from 2013) ā€¢Modeling of THM in deep borehole disposalā€¦ TOUGH-FLAC Simulator: (Rutqvist et al., 2002; Rutqvist 2011; 2017) LBNL THM Modeling of Nuclear Waste Disposal
  • 4. Spent Fuel and Waste Science and Technology THM driven buffer/rock interactions: 1) Delayed buffer resaturation due to low rock permeability, 2) thermal-pressurization in rock affects pressure and stress evolution in buffer Opalinus clay: 15% fluid saturated porosity 5ļ‚“10-20 m2 permeability ļƒž Strong THM coupling COUPLED THM MODELING OF A REPOSITORY IN CLAY Rutqvist et al., (2014)
  • 5. Spent Fuel and Waste Science and Technology TOUGH-FLAC 1) Barcelona Basic Model (BBM) A constitutive model for thermo-elasto-plastic behavior of unsaturated soils (bentonite) ā€¢ Shear strength and stiffness depends on saturation ( or suction) ā€¢ Wetting-induced swelling or collapse strains Deviatoric (shear) stress Suction Netpressure(total stresslessgaspressure) Drying Cam-clay yield surface (fully fluid saturated) Deviatoric (shear) stress Suction Netpressure(total stresslessgaspressure) Drying Cam-clay yield surface (fully fluid saturated) Bentonite block stored at different relative humidity (Teodori et al 2011) 55% 75% 99% 2) Barcelona Expansive Model (BExM) ā€¢ Micro- and macro-structure ā€¢ Proper modeling of fluid flow through macro pores and their changes with stress and saturation ā€¢ Can provide a link for coupling mechanics with chemistry TOUGH-FLAC THM Simulator LBNL THM Model Developments for Bentonite Backfill
  • 6. Spent Fuel and Waste Science and Technology ļ® Undertaken by NAGRA as an ultimate test for the performance of geologic disposal in Opalinus Clay, with focus on both the EBS components and the host-rock behavior ļ® It will be one of the largest and longest running heater tests worldwide ļ® Thousands of sensors within the EBS and surrounding rock for monitoring THMC processes (Figure from Tobias Vogt NAGRA) 2.5 m Mont Terri Full-scale Emplacement (FE) Experiment International Partners
  • 7. Spent Fuel and Waste Science and Technology TOUGH-FLAC Model of FE Experiment Access tunnel Plug Heaters Heater Bentonite blocks Bentonite pellets Shot crete
  • 8. Spent Fuel and Waste Science and Technology ā€¢ Anisotropic THM properties (thermal conductivity, permeability, strength) of Opalinus Clay considering bedding ā€¢ TH bentonite properties of granular bentonite and bentonite blocks from laboratory scale and HE-E (half-scale) modeling ā€¢ Basic Barcelona Model (BBM) properties for granular bentonite and blocks (but too early to see significant swelling stress in the buffer) THM Properties and Heat Load
  • 9. Spent Fuel and Waste Science and Technology Heater Host rock Moisture Flow in Bentonite Buffer During Heating Heating Drying Wetting ļ€Ø ļ€©zP k X ll l rlw ll w l ļƒ‘ļ€­ļƒ‘ļ€­ļ€½ g k q ļ² ļ­ ļ² Liquid Darcy Flow: Liquid pressure gradient w g w ggg w g XDS ļƒ‘ļ€­ļ€½ Ii ļ“ļ¦ļ² Vapor diffusion: Water mass fraction in gas Effective vapor diffusion
  • 10. Spent Fuel and Waste Science and Technology T IM E (d a y s ) TEMPERATURE(C o ) 0 5 0 1 0 0 1 5 0 2 0 0 2 5 0 3 0 0 3 5 0 4 0 0 0 1 0 2 0 3 0 4 0 5 0 6 0 7 0 8 0 9 0 1 0 0 1 1 0 1 2 0 1 3 0 1 4 0 1 5 0 H e a te r S u rfa c e 1 0 c m fro m h e a te r 2 0 c m fro m h e a te r A t tu n n e l w a ll F ie ld d a ta M o d e lin g TIME (days) TEMPERATURE(Co ) 0 50 100 150 200 250 300 350 400 0 50 100 150 Heater surface 10 cm from heater 20 cm from heater Simulated and Observed Temperature (mid heater) 1st year ā€¢ Calibrated thermal properties of ā€œheaterā€ for temperature distribution on heater- surface ā€¢ Heater-surface temperature higher at granular bentonite (Tmax=126ļ‚°C) then at bentonite block pedestal (Tmax=118ļ‚°C) ā€¢ Excellent agreement between simulated and observed temperature Granular Bentonite Bentonite Blocks
  • 11. Spent Fuel and Waste Science and Technology TIME (days) RELATIVEHUMIDITY(-) 0 50 100 150 200 250 300 350 400 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 20 cm from heater 10 cm from heater At tunnel wall 20 cm from heater 10 cm from heater TIME (days) RELATIVEHUMIDITY(-) 0 50 100 150 200 250 300 350 400 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 ā€¢ Good agreement for substantial reduction of the effective vapor diffusion coefficient through a medium tortuosity factor as low as 0.14. w g w ggg w g XDS ļƒ‘ļ€­ļ€½ Ii ļ“ļ¦ļ² Diffusion coefficient for vapor- air mixture 2.13e-5 m2/s Medium tortuosity, best match for 0.14 Mass fraction Simulated and Observed Moisture Evolution (mid heater) 1st year
  • 12. Spent Fuel and Waste Science and Technology TIME (days) TEMPERATURE(Co ) 0 100 200 300 400 500 600 700 800 0 10 20 30 40 50 60 70 80 90 100 110 120 130 140 150 Heater Surface 10 cm from heater 20 cm from heater At tunnel wall Field data Modeling 20 cm from heater 10 cm from heater At tunnel wall TIME (days) RELATIVEHUMIDITY(-) 0 100 200 300 400 500 600 700 800 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 Comparison with 2 Years of Data (Heater 2) Heater 2
  • 13. Spent Fuel and Waste Science and Technology Comparison with 2 Years of Data (Heater 3) TIME (days) RELATIVEHUMIDITY(-) 0 200 400 600 800 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 20 cm from heater 10 cm from heater At tunnel wall Field data Modeling TIME (days) TEMPERATURE(Co ) 0 200 400 600 800 0 10 20 30 40 50 60 70 80 90 100 110 120 130 140 150 Heater Surface 10 cm from heater 20 cm from heater At tunnel wall Heater 3
  • 14. Spent Fuel and Waste Science and Technology Real Tunnel Shape vs Model Blue line at designed tunnel radius of 1.4 m Laser scan of tunnel wall
  • 15. Spent Fuel and Waste Science and Technology TempĆ©rature Pression interstitielle 3 Borehole Heaters 12 to 16 m from drift wall 23 monitoring boreholes with over 200 sensors (temperature, pressure, displacement) Temperature Pressure TED Borehole Heating Experiment at Bure by ANDRA, France
  • 16. Spent Fuel and Waste Science and Technology Sample scale Borehole scale Micro-tunnel scale Repository scale ā€¢ Upscaling is an important issue for the repository design and safety calculation: How to go from sample to a repository scale ? ā€¢ Two in situ tests performed at the underground research laboratory in Bure (France) will be interpreted and modeled ā€¢ The host rock consists of Callovo-Oxfordian claystone (COx) ā€¢ Thermally induced pore pressure build-up and stress changes around a repositoryā€¦ Upscaling of THM Parameters (DECOVALEX Task Led by ANDRA, France)
  • 17. Spent Fuel and Waste Science and Technology TOUGH-FLAC Model of TED Borehole Heating Experiment Entire Model Heaters (Biotā€™s coefficient) Some basic Cox Claystone properties
  • 18. Spent Fuel and Waste Science and Technology Simulation Results with Comparison to Measured Data - Temperature
  • 19. Spent Fuel and Waste Science and Technology Field Data (dashed lines) Simulations (solid lines) Simulation Results with Comparison to Measured Data - Pressure
  • 20. Spent Fuel and Waste Science and Technology Concluding Remarks THM Modeling ā€¢ 3 new journal papers published on DECOVALEX-2015 work (modeling of Mont Terri experiments) ā€¢ Continue modeling of FE- Experiment with access to field data (2 years of heating) - Opportunity for applying dual-structure (BExM) model in collaboration with the Barcelona group ā€¢ Continue work on ANDRAā€™s heater tests in Cox clay stone associated with DECOVALEX-2019 ā€¢ Implementation and testing of continuum damage model for EDZ and permeability evolution in clay host rock with comparison to TOUGH-RBSN discrete fracture modelā€¦ 20