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Cross-hole electrical imaging of a controlled saline tracer injection.

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Cross-hole electrical imaging of a controlled saline tracer injection. / Slater, Lee; Binley, Andrew; Daily, W. et al.
In: Journal of Applied Geophysics, Vol. 44, No. 2-3, 05.2000, p. 85-102.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Slater, L, Binley, A, Daily, W & Johnson, R 2000, 'Cross-hole electrical imaging of a controlled saline tracer injection.', Journal of Applied Geophysics, vol. 44, no. 2-3, pp. 85-102. https://doi.org/10.1016/S0926-9851(00)00002-1

APA

Slater, L., Binley, A., Daily, W., & Johnson, R. (2000). Cross-hole electrical imaging of a controlled saline tracer injection. Journal of Applied Geophysics, 44(2-3), 85-102. https://doi.org/10.1016/S0926-9851(00)00002-1

Vancouver

Slater L, Binley A, Daily W, Johnson R. Cross-hole electrical imaging of a controlled saline tracer injection. Journal of Applied Geophysics. 2000 May;44(2-3):85-102. doi: 10.1016/S0926-9851(00)00002-1

Author

Slater, Lee ; Binley, Andrew ; Daily, W. et al. / Cross-hole electrical imaging of a controlled saline tracer injection. In: Journal of Applied Geophysics. 2000 ; Vol. 44, No. 2-3. pp. 85-102.

Bibtex

@article{14cf22dc70b24cb29a234455a91184bd,
title = "Cross-hole electrical imaging of a controlled saline tracer injection.",
abstract = "Electrical imaging of tracer tests can provide valuable information on the spatial variability of solute transport processes. This concept was investigated by cross-borehole electrical imaging of a controlled release in an experimental tank. A saline tracer (conductivity 8×103 ms/m volume 270 l) was injected into a tank facility (dimensions 10×10×3 m) consisting of alternating sand and clay layers. Injection was from 0.3 m below the surface, at a point where maximum interaction between tank structure and tracer transport was expected. Repeated imaging over a two-week period detected non-uniform tracer transport, partly caused by the sand/clay sequence. Tracer accumulation on two clay layers was observed and density-driven spill of tracer over a clay shelf was imaged. An additional unexpected flow pathway, probably caused by complications during array installation, was identified close to an electrode array. Pore water samples obtained following termination of electrical imaging generally supported the observed electrical response, although discrepancies arose when analysing the response of individual pixels. The pixels that make up the electrical images were interpreted as a large number of breakthrough curves. The shape of the pixel breakthrough-recession curve allowed some quantitative interpretation of solute travel time, as well as a qualitative assessment of spatial variability in advective-dispersive transport characteristics across the image plane. Although surface conduction effects associated with the clay layers complicated interpretation, the plotting of pixel breakthroughs was considered a useful step in the hydrological interpretation of the tracer test. The spatial coverage provided by the high density of pixels is the factor that most encourages the approach.",
keywords = "Resistivity, Tomography, Solute transport, Pixel-breakthroughs",
author = "Lee Slater and Andrew Binley and W. Daily and R. Johnson",
year = "2000",
month = may,
doi = "10.1016/S0926-9851(00)00002-1",
language = "English",
volume = "44",
pages = "85--102",
journal = "Journal of Applied Geophysics",
issn = "0926-9851",
publisher = "Elsevier",
number = "2-3",

}

RIS

TY - JOUR

T1 - Cross-hole electrical imaging of a controlled saline tracer injection.

AU - Slater, Lee

AU - Binley, Andrew

AU - Daily, W.

AU - Johnson, R.

PY - 2000/5

Y1 - 2000/5

N2 - Electrical imaging of tracer tests can provide valuable information on the spatial variability of solute transport processes. This concept was investigated by cross-borehole electrical imaging of a controlled release in an experimental tank. A saline tracer (conductivity 8×103 ms/m volume 270 l) was injected into a tank facility (dimensions 10×10×3 m) consisting of alternating sand and clay layers. Injection was from 0.3 m below the surface, at a point where maximum interaction between tank structure and tracer transport was expected. Repeated imaging over a two-week period detected non-uniform tracer transport, partly caused by the sand/clay sequence. Tracer accumulation on two clay layers was observed and density-driven spill of tracer over a clay shelf was imaged. An additional unexpected flow pathway, probably caused by complications during array installation, was identified close to an electrode array. Pore water samples obtained following termination of electrical imaging generally supported the observed electrical response, although discrepancies arose when analysing the response of individual pixels. The pixels that make up the electrical images were interpreted as a large number of breakthrough curves. The shape of the pixel breakthrough-recession curve allowed some quantitative interpretation of solute travel time, as well as a qualitative assessment of spatial variability in advective-dispersive transport characteristics across the image plane. Although surface conduction effects associated with the clay layers complicated interpretation, the plotting of pixel breakthroughs was considered a useful step in the hydrological interpretation of the tracer test. The spatial coverage provided by the high density of pixels is the factor that most encourages the approach.

AB - Electrical imaging of tracer tests can provide valuable information on the spatial variability of solute transport processes. This concept was investigated by cross-borehole electrical imaging of a controlled release in an experimental tank. A saline tracer (conductivity 8×103 ms/m volume 270 l) was injected into a tank facility (dimensions 10×10×3 m) consisting of alternating sand and clay layers. Injection was from 0.3 m below the surface, at a point where maximum interaction between tank structure and tracer transport was expected. Repeated imaging over a two-week period detected non-uniform tracer transport, partly caused by the sand/clay sequence. Tracer accumulation on two clay layers was observed and density-driven spill of tracer over a clay shelf was imaged. An additional unexpected flow pathway, probably caused by complications during array installation, was identified close to an electrode array. Pore water samples obtained following termination of electrical imaging generally supported the observed electrical response, although discrepancies arose when analysing the response of individual pixels. The pixels that make up the electrical images were interpreted as a large number of breakthrough curves. The shape of the pixel breakthrough-recession curve allowed some quantitative interpretation of solute travel time, as well as a qualitative assessment of spatial variability in advective-dispersive transport characteristics across the image plane. Although surface conduction effects associated with the clay layers complicated interpretation, the plotting of pixel breakthroughs was considered a useful step in the hydrological interpretation of the tracer test. The spatial coverage provided by the high density of pixels is the factor that most encourages the approach.

KW - Resistivity

KW - Tomography

KW - Solute transport

KW - Pixel-breakthroughs

U2 - 10.1016/S0926-9851(00)00002-1

DO - 10.1016/S0926-9851(00)00002-1

M3 - Journal article

VL - 44

SP - 85

EP - 102

JO - Journal of Applied Geophysics

JF - Journal of Applied Geophysics

SN - 0926-9851

IS - 2-3

ER -