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Page 1: Managed by Triad National Security, LLC for the U.S ... · mixing in the basalt than standard diffusive theory . Results from the tracer test and simulations suggest that barometric

Managed by Triad National Security, LLC for the U.S. Department of Energy’s NNSA

Page 2: Managed by Triad National Security, LLC for the U.S ... · mixing in the basalt than standard diffusive theory . Results from the tracer test and simulations suggest that barometric

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High Rates of Tracer Gas Transport in a Deep

Fractured Basalt

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Sunday, September 22nd

Philip H. Stauffer

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Co-authors

9/9/2019 | 3Los Alamos National Laboratory

• T. Rahn , Los Alamos EES-14• J. P. Ortiz , Johns Hopkins• L. J. Salazar, N3B• H. Boukhalfa, Los Alamos EES-14• H. R. Behar, U. of Minnesota• E. E. Snyder, New Mexico Tech

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MOTIVATION

9/9/2019 | 4Los Alamos National Laboratory

Deep vadose contaminant transport at Los Alamos

Radionuclide gas migration from underground nuclear tests

2019 Behar, H.R., . . . P.H. Stauffer, An investigation of plume response to drum failure and soil vapor extraction at Material Disposal Area L, Los Alamos, NM, VadoseZone J., 18(1), doi: 10.2136/vzj2018.04.0080.

2019 Bourret, S.M., E.M. Kwicklis, T.A. Miller, and P.H. Stauffer, Evaluating the importance of barometric pumping for subsurface gas transport near an underground nuclear test site, Vadose Zone J., March 14, doi: 10.2136/vzj2018.07.0134 .

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Site Location

9/9/2019 | 5Los Alamos National LaboratorySlide 5

170 miA.

N

4 miB.

N

SVE -West

SVE-East

C.

= soil vapor extraction (SVE) well= monitoring borehole

New Mexico

Pajarito Plateau

Material Disposal

Area L (MDA L),

LANL

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Site Stratigraphy

9/9/2019 | 6Los Alamos National LaboratorySlide 6

Stauffer, P.H., Birdsell K.H., Witowski M.S., Hopkins J.K. 2005. Vadose zone transport of 1,1,1-trichloroethane: conceptual model validation through numerical simulation. Vadose Zone Journal. 760-773.

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Site Description

9/9/2019 | 7Los Alamos National LaboratorySlide 7

Basalt is nearly in phase and of the same amplitude as the atmosphere.

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Cerros del Rio Basalt

9/9/2019 | 8Los Alamos National LaboratorySlide 8

Massive columnar sections Fracture porosityHigh permeability

Thinner interflow brecciaRubble porosity 35%

High permeability

2017 Tracer test in the

Cerros del Rio Basalt

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Tracer Experiment April 2017

9/9/2019 | 9Los Alamos National LaboratorySlide 9

Sulfur Hexafluoride injection into the

Cerros del Rio Basalt Rubblized Basalt

Massive Basalt

Injection Borehole 0 m

172 m

201 m

179 m

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Tracer Experiment April 2017

9/9/2019 | 10Los Alamos National LaboratorySlide 10

Sulfur Hexafluoride injection into the

Cerros del Rio Basalt Rubblized Basalt

Massive Basalt

Casing

Injection Borehole 0 m

172 m

201 m

179 m

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Tracer Experiment April 2017

9/9/2019 | 11Los Alamos National LaboratorySlide 11

Sulfur Hexafluoride injection into the

Cerros del Rio Basalt Rubblized Basalt

Massive Basalt

Casing

Packer

Injection Borehole 0 m

172 m

201 m

179 m

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Tracer Experiment April 2017

9/9/2019 | 12Los Alamos National LaboratorySlide 12

Sulfur Hexafluoride injection into the

Cerros del Rio Basalt Rubblized Basalt

Massive Basalt

Casing

Injection + Sampling Port

Packer

Injection Borehole 0 m

172 m

201 m

179 m

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Tracer Experiment April 2017 – Tracer Details

9/9/2019 | 13Los Alamos National LaboratorySlide 13

Innova 1412i Photoacoustic Gas Monitor, installed in the field at MDA L, April 2017.

5 g of SF6 injected

Mixed in 1 L of air

10 min air purge

Pump reversed to sample

Presenter
Presentation Notes
Starting on 5 April 2017, a 1‐L bag (5‐g aliquot) of gas tracer SF6 was injected into borehole 54‐24399 at a depth of 173mthrough the injection/return flow tubing of the packer system (Figures S4 and S5). The tracer was subsequently monitored as it spread into the subsurface. Flow of about 2 L per minute to the packer outlet was continued for 10 min to ensure that the entire volume of tracer was flushed through the downhole tubing (approximate volume 2 L). After injection and flushing of the tubing to 173 m bgs, the pump was reversed and sampling was initiated with the INNOVA from 173 m bgs. INNOVA data were recorded approximately every 57 s.
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Tracer Experiment April 2017 – Tracer Data

9/9/2019 | 14Los Alamos National LaboratorySlide 14

Behavior was predicted by pre-test simulations

Tracer initially spikes, disappears, then returns, drops then increases.

Presenter
Presentation Notes
Starting on 5 April 2017, a 1‐L bag (5‐g aliquot) of gas tracer SF6 was injected into borehole 54‐24399 at a depth of 173mthrough the injection/return flow tubing of the packer system (Figures S4 and S5). The tracer was subsequently monitored as it spread into the subsurface. Flow of about 2 L per minute to the packer outlet was continued for 10 min to ensure that the entire volume of tracer was flushed through the downhole tubing (approximate volume 2 L). After injection and flushing of the tubing to 173 m bgs, the pump was reversed and sampling was initiated with the INNOVA from 173 m bgs. INNOVA data were recorded approximately every 57 s.
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Tracer Experiment April 2017 – Down-hole Pressure Data

9/9/2019 | 15Los Alamos National LaboratorySlide 15

Pressure gauge measuring below the packer

Basalt is nearly in phase and of the same amplitude as the atmosphere.

ATMdownhole

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Numerical Model of the Tracer Test

9/9/2019 | 16Los Alamos National LaboratorySlide 16

3-D long narrow slice of basalt

8 m vertical x 20 m wide x 2500 m long

0.07 m radius borehole

1 m spacing within 100 m of the borehole

Injection/Sample Port

Presenter
Presentation Notes
The mesh includes a high‐resolution borehole with a central radius of 0.07 m. The borehole runs the entire 8‐m vertical length of the domain, with the upper 3.5mof the borehole set to impermeable and nondiffusive, representing a cased/cemented interval. Porosity in the open section of the borehole is set to 0.999, while permeability in this section is fixed at 10−4 m2 based on downhole pressure loss matching. The third dimension of the mesh extends from 0 to 2,500 m, with borehole 54‐24399 located at 1,100 m (Figure S11). The 2,500‐m mesh allows the boundaries to be adjusted such that the measured atmospheric forcing can be moved to the point at which the measured pressure response beneath the packer is recreated in the simulations. Mesh spacing is 1 m in all directions within 100 m on either side of the borehole.
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Simulation Spin-up to atmospheric pressure

9/9/2019 | 17Los Alamos National LaboratorySlide 17

1 month of atmospheric pressure data used to create the initial state

Weather Station +

Simulated Atmosphere

Measured pressure below the packer

815

790

Pres

sure

(mB

ar)

3/1/2017 4/20/2017Date

Presenter
Presentation Notes
Measured atmospheric pressure, March 5 – April 17 at TA-54, simulated atmospheric pressure boundary, and measured downhole pressure beneath the packer in borehole 54-24399 at 173 m bgs.
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Parameters – calibrated to fit pressure and tracer data

9/9/2019 | 18Los Alamos National LaboratorySlide 18

Basalt permeability on order of 1000 darcies

Basalt porosity 35% rubble 0.4% massive fractured (4 mm fracture per m)

Lateral boundary for pressure drive at 1000 m from the sampling port

1000 mAtmospheric boundary

Presenter
Presentation Notes
The mesh includes a high‐resolution borehole with a central radius of 0.07 m. The borehole runs the entire 8‐m vertical length of the domain, with the upper 3.5mof the borehole set to impermeable and nondiffusive, representing a cased/cemented interval. Porosity in the open section of the borehole is set to 0.999, while permeability in this section is fixed at 10−4 m2 based on downhole pressure loss matching. The third dimension of the mesh extends from 0 to 2,500 m, with borehole 54‐24399 located at 1,100 m (Figure S11). The 2,500‐m mesh allows the boundaries to be adjusted such that the measured atmospheric forcing can be moved to the point at which the measured pressure response beneath the packer is recreated in the simulations. Mesh spacing is 1 m in all directions within 100 m on either side of the borehole.
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Results – Matching downhole pressure + tracer concentratoin

9/9/2019 | 19Los Alamos National LaboratorySlide 19

Presenter
Presentation Notes
The mesh includes a high‐resolution borehole with a central radius of 0.07 m. The borehole runs the entire 8‐m vertical length of the domain, with the upper 3.5mof the borehole set to impermeable and nondiffusive, representing a cased/cemented interval. Porosity in the open section of the borehole is set to 0.999, while permeability in this section is fixed at 10−4 m2 based on downhole pressure loss matching. The third dimension of the mesh extends from 0 to 2,500 m, with borehole 54‐24399 located at 1,100 m (Figure S11). The 2,500‐m mesh allows the boundaries to be adjusted such that the measured atmospheric forcing can be moved to the point at which the measured pressure response beneath the packer is recreated in the simulations. Mesh spacing is 1 m in all directions within 100 m on either side of the borehole.
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Implications – Contaminant Plume Migration

9/9/2019 | 20Los Alamos National LaboratorySlide 20

Atmospheric pressure drops will pull the plume into the basalt

10x to 100x more mixing in the basalt than standard diffusive theory

Presenter
Presentation Notes
Results from the tracer test and simulations suggest that barometric pumping induces 10x to 100x more mixing in the basalt than standard diffusive theory would predict. Further, within the basalt fractures, estimates of average linear velocity reach maximums of nearly 1000 m/day.
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Implications – Contaminant Plume Migration

9/9/2019 | 21Los Alamos National LaboratorySlide 21

Atmospheric pressure high pushes the plume back into the basalt

Average linear velocity reaches maximums of nearly 1000 m/day

Presenter
Presentation Notes
Results from the tracer test and simulations suggest that barometric pumping induces 10x to 100x more mixing in the basalt than standard diffusive theory would predict. Further, within the basalt fractures, estimates of average linear velocity reach maximums of nearly 1000 m/day.
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Implications – Nuclear gas transport

9/9/2019 | 22Los Alamos National LaboratorySlide 22

Basalt layer could provide a fast-path to the atmosphere, increasing probability of observing gas seepage

Presenter
Presentation Notes
Figure showing Model domain and mesh used for FEHM gas flow and transport �simulations for a site where an underground nuclear explosion was performed,�which includes hydrostratigraphic units, faults, and detonation-induced damage structure. �
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Questions ?

9/9/2019 | 23Los Alamos National LaboratorySlide 23

Presenter
Presentation Notes
The mesh includes a high‐resolution borehole with a central radius of 0.07 m. The borehole runs the entire 8‐m vertical length of the domain, with the upper 3.5mof the borehole set to impermeable and nondiffusive, representing a cased/cemented interval. Porosity in the open section of the borehole is set to 0.999, while permeability in this section is fixed at 10−4 m2 based on downhole pressure loss matching. The third dimension of the mesh extends from 0 to 2,500 m, with borehole 54‐24399 located at 1,100 m (Figure S11). The 2,500‐m mesh allows the boundaries to be adjusted such that the measured atmospheric forcing can be moved to the point at which the measured pressure response beneath the packer is recreated in the simulations. Mesh spacing is 1 m in all directions within 100 m on either side of the borehole.