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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Main Authors: D. Draebing, M. Krautblatter
Format: Article
Language:English
Published: Copernicus Publications 2012-10-01
Series:The Cryosphere
Online Access:http://www.the-cryosphere.net/6/1163/2012/tc-6-1163-2012.pdf
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spelling doaj-25f3bbca8c584718831b9d18b307fd192020-11-24T22:53:49ZengCopernicus PublicationsThe Cryosphere1994-04161994-04242012-10-01651163117410.5194/tc-6-1163-2012P-wave velocity changes in freezing hard low-porosity rocks: a laboratory-based time-average modelD. DraebingM. KrautblatterP-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.http://www.the-cryosphere.net/6/1163/2012/tc-6-1163-2012.pdf
collection DOAJ
language English
format Article
sources DOAJ
author D. Draebing
M. Krautblatter
spellingShingle D. Draebing
M. Krautblatter
P-wave velocity changes in freezing hard low-porosity rocks: a laboratory-based time-average model
The Cryosphere
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
series The Cryosphere
issn 1994-0416
1994-0424
publishDate 2012-10-01
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.
url http://www.the-cryosphere.net/6/1163/2012/tc-6-1163-2012.pdf
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