P-wave velocity changes in freezing hard low-porosity rocks: a laboratory-based time-average model

P-wave refraction seismics is a key method in permafrost research but its applicability to low-porosity rocks, which constitute alpine rock walls, has been denied in prior studies. These studies explain p-wave velocity changes in freezing rocks exclusively due to changing velocities of pore infill,...

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Published in:The Cryosphere
Main Authors: D. Draebing, M. Krautblatter
Format: Article in Journal/Newspaper
Language:English
Published: Copernicus Publications 2012
Subjects:
Ice
Online Access:https://doi.org/10.5194/tc-6-1163-2012
https://doaj.org/article/25f3bbca8c584718831b9d18b307fd19
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spelling ftdoajarticles:oai:doaj.org/article:25f3bbca8c584718831b9d18b307fd19 2023-05-15T16:37:30+02:00 P-wave velocity changes in freezing hard low-porosity rocks: a laboratory-based time-average model D. Draebing M. Krautblatter 2012-10-01T00:00:00Z https://doi.org/10.5194/tc-6-1163-2012 https://doaj.org/article/25f3bbca8c584718831b9d18b307fd19 EN eng Copernicus Publications http://www.the-cryosphere.net/6/1163/2012/tc-6-1163-2012.pdf https://doaj.org/toc/1994-0416 https://doaj.org/toc/1994-0424 doi:10.5194/tc-6-1163-2012 1994-0416 1994-0424 https://doaj.org/article/25f3bbca8c584718831b9d18b307fd19 The Cryosphere, Vol 6, Iss 5, Pp 1163-1174 (2012) Environmental sciences GE1-350 Geology QE1-996.5 article 2012 ftdoajarticles https://doi.org/10.5194/tc-6-1163-2012 2022-12-31T01:32:25Z P-wave refraction seismics is a key method in permafrost research but its applicability to low-porosity rocks, which constitute alpine rock walls, has been denied in prior studies. These studies explain p-wave velocity changes in freezing rocks exclusively due to changing velocities of pore infill, i.e. water, air and ice. In existing models, no significant velocity increase is expected for low-porosity bedrock. We postulate, that mixing laws apply for high-porosity rocks, but freezing in confined space in low-porosity bedrock also alters physical rock matrix properties. In the laboratory, we measured p-wave velocities of 22 decimetre-large low-porosity (< 10%) metamorphic, magmatic and sedimentary rock samples from permafrost sites with a natural texture (> 100 micro-fissures) from 25 °C to −15 °C in 0.3 °C increments close to the freezing point. When freezing, p-wave velocity increases by 11–166% perpendicular to cleavage/bedding and equivalent to a matrix velocity increase from 11–200% coincident to an anisotropy decrease in most samples. The expansion of rigid bedrock upon freezing is restricted and ice pressure will increase matrix velocity and decrease anisotropy while changing velocities of the pore infill are insignificant. Here, we present a modified Timur's two-phase-equation implementing changes in matrix velocity dependent on lithology and demonstrate the general applicability of refraction seismics to differentiate frozen and unfrozen low-porosity bedrock. Article in Journal/Newspaper Ice permafrost The Cryosphere Directory of Open Access Journals: DOAJ Articles The Cryosphere 6 5 1163 1174
institution Open Polar
collection Directory of Open Access Journals: DOAJ Articles
op_collection_id ftdoajarticles
language English
topic Environmental sciences
GE1-350
Geology
QE1-996.5
spellingShingle Environmental sciences
GE1-350
Geology
QE1-996.5
D. Draebing
M. Krautblatter
P-wave velocity changes in freezing hard low-porosity rocks: a laboratory-based time-average model
topic_facet Environmental sciences
GE1-350
Geology
QE1-996.5
description P-wave refraction seismics is a key method in permafrost research but its applicability to low-porosity rocks, which constitute alpine rock walls, has been denied in prior studies. These studies explain p-wave velocity changes in freezing rocks exclusively due to changing velocities of pore infill, i.e. water, air and ice. In existing models, no significant velocity increase is expected for low-porosity bedrock. We postulate, that mixing laws apply for high-porosity rocks, but freezing in confined space in low-porosity bedrock also alters physical rock matrix properties. In the laboratory, we measured p-wave velocities of 22 decimetre-large low-porosity (< 10%) metamorphic, magmatic and sedimentary rock samples from permafrost sites with a natural texture (> 100 micro-fissures) from 25 °C to −15 °C in 0.3 °C increments close to the freezing point. When freezing, p-wave velocity increases by 11–166% perpendicular to cleavage/bedding and equivalent to a matrix velocity increase from 11–200% coincident to an anisotropy decrease in most samples. The expansion of rigid bedrock upon freezing is restricted and ice pressure will increase matrix velocity and decrease anisotropy while changing velocities of the pore infill are insignificant. Here, we present a modified Timur's two-phase-equation implementing changes in matrix velocity dependent on lithology and demonstrate the general applicability of refraction seismics to differentiate frozen and unfrozen low-porosity bedrock.
format Article in Journal/Newspaper
author D. Draebing
M. Krautblatter
author_facet D. Draebing
M. Krautblatter
author_sort D. Draebing
title P-wave velocity changes in freezing hard low-porosity rocks: a laboratory-based time-average model
title_short P-wave velocity changes in freezing hard low-porosity rocks: a laboratory-based time-average model
title_full P-wave velocity changes in freezing hard low-porosity rocks: a laboratory-based time-average model
title_fullStr P-wave velocity changes in freezing hard low-porosity rocks: a laboratory-based time-average model
title_full_unstemmed P-wave velocity changes in freezing hard low-porosity rocks: a laboratory-based time-average model
title_sort p-wave velocity changes in freezing hard low-porosity rocks: a laboratory-based time-average model
publisher Copernicus Publications
publishDate 2012
url https://doi.org/10.5194/tc-6-1163-2012
https://doaj.org/article/25f3bbca8c584718831b9d18b307fd19
genre Ice
permafrost
The Cryosphere
genre_facet Ice
permafrost
The Cryosphere
op_source The Cryosphere, Vol 6, Iss 5, Pp 1163-1174 (2012)
op_relation http://www.the-cryosphere.net/6/1163/2012/tc-6-1163-2012.pdf
https://doaj.org/toc/1994-0416
https://doaj.org/toc/1994-0424
doi:10.5194/tc-6-1163-2012
1994-0416
1994-0424
https://doaj.org/article/25f3bbca8c584718831b9d18b307fd19
op_doi https://doi.org/10.5194/tc-6-1163-2012
container_title The Cryosphere
container_volume 6
container_issue 5
container_start_page 1163
op_container_end_page 1174
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