CREEP OF SNOW AND ICE.

Constant load creep tests in uniaxial unconfined compression were performed on samples of sintered snow and bubbly polycrystalline ice. Nominal axial stresses were in the range 0.1 to 1.0 kgf/sq cm for snow, and 0.5 to 20 kgf/sq cm for ice. The range of temperatures investigated was from -0.5 to -34...

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Main Authors: Mellor,Malcolm, Smith,James H.
Other Authors: COLD REGIONS RESEARCH AND ENGINEERING LAB HANOVER N H
Format: Text
Language:English
Published: 1966
Subjects:
Ice
Online Access:http://www.dtic.mil/docs/citations/AD0649367
http://oai.dtic.mil/oai/oai?&verb=getRecord&metadataPrefix=html&identifier=AD0649367
id ftdtic:AD0649367
record_format openpolar
spelling ftdtic:AD0649367 2023-05-15T16:37:20+02:00 CREEP OF SNOW AND ICE. Mellor,Malcolm Smith,James H. COLD REGIONS RESEARCH AND ENGINEERING LAB HANOVER N H 1966-12 text/html http://www.dtic.mil/docs/citations/AD0649367 http://oai.dtic.mil/oai/oai?&verb=getRecord&metadataPrefix=html&identifier=AD0649367 en eng http://www.dtic.mil/docs/citations/AD0649367 APPROVED FOR PUBLIC RELEASE DTIC AND NTIS Snow Ice and Permafrost (*SNOW CREEP) (*ICE STRESSES STRAIN(MECHANICS) DENSITY TEMPERATURE HEAT OF ACTIVATION Text 1966 ftdtic 2016-02-18T19:58:26Z Constant load creep tests in uniaxial unconfined compression were performed on samples of sintered snow and bubbly polycrystalline ice. Nominal axial stresses were in the range 0.1 to 1.0 kgf/sq cm for snow, and 0.5 to 20 kgf/sq cm for ice. The range of temperatures investigated was from -0.5 to -34.5C. Assuming creep to follow the Arrhenius relation, values of apparent activation energy for secondary creep under a nominal axial stress of 0.5 kgf/sq cm varied from 10.7 kcal/mole for ice of density 0.83 g/cu cm to 17.8 kcal/mole for snow of density 0.44 g/cu cm. The dependence of strain rate epsilon on stress sigma for polycrystalline ice subjected to stresses in the range 0.5 to 20 kgf/sq cm at temperatures of -4 and -10C could best be described by a relation of the form epsilon = C sub 1 sigma + C sub 2 sigma to the 3.5 power where C sub 1 and C sub 2 are constants for a given ice type. It is suggested that the creep of polycrystalline ice depends on at least two distinct mechanisms in the stress range studied. If each mechanism has its own characteristic activation energy, the apparent activation energy measured in creep experiments may well vary with stress level. In snow subjected to a given nominal stress, such an effect should be reflected in variation of apparent activation energy with bulk density. (Author) Text Ice permafrost Defense Technical Information Center: DTIC Technical Reports database
institution Open Polar
collection Defense Technical Information Center: DTIC Technical Reports database
op_collection_id ftdtic
language English
topic Snow
Ice and Permafrost
(*SNOW
CREEP)
(*ICE
STRESSES
STRAIN(MECHANICS)
DENSITY
TEMPERATURE
HEAT OF ACTIVATION
spellingShingle Snow
Ice and Permafrost
(*SNOW
CREEP)
(*ICE
STRESSES
STRAIN(MECHANICS)
DENSITY
TEMPERATURE
HEAT OF ACTIVATION
Mellor,Malcolm
Smith,James H.
CREEP OF SNOW AND ICE.
topic_facet Snow
Ice and Permafrost
(*SNOW
CREEP)
(*ICE
STRESSES
STRAIN(MECHANICS)
DENSITY
TEMPERATURE
HEAT OF ACTIVATION
description Constant load creep tests in uniaxial unconfined compression were performed on samples of sintered snow and bubbly polycrystalline ice. Nominal axial stresses were in the range 0.1 to 1.0 kgf/sq cm for snow, and 0.5 to 20 kgf/sq cm for ice. The range of temperatures investigated was from -0.5 to -34.5C. Assuming creep to follow the Arrhenius relation, values of apparent activation energy for secondary creep under a nominal axial stress of 0.5 kgf/sq cm varied from 10.7 kcal/mole for ice of density 0.83 g/cu cm to 17.8 kcal/mole for snow of density 0.44 g/cu cm. The dependence of strain rate epsilon on stress sigma for polycrystalline ice subjected to stresses in the range 0.5 to 20 kgf/sq cm at temperatures of -4 and -10C could best be described by a relation of the form epsilon = C sub 1 sigma + C sub 2 sigma to the 3.5 power where C sub 1 and C sub 2 are constants for a given ice type. It is suggested that the creep of polycrystalline ice depends on at least two distinct mechanisms in the stress range studied. If each mechanism has its own characteristic activation energy, the apparent activation energy measured in creep experiments may well vary with stress level. In snow subjected to a given nominal stress, such an effect should be reflected in variation of apparent activation energy with bulk density. (Author)
author2 COLD REGIONS RESEARCH AND ENGINEERING LAB HANOVER N H
format Text
author Mellor,Malcolm
Smith,James H.
author_facet Mellor,Malcolm
Smith,James H.
author_sort Mellor,Malcolm
title CREEP OF SNOW AND ICE.
title_short CREEP OF SNOW AND ICE.
title_full CREEP OF SNOW AND ICE.
title_fullStr CREEP OF SNOW AND ICE.
title_full_unstemmed CREEP OF SNOW AND ICE.
title_sort creep of snow and ice.
publishDate 1966
url http://www.dtic.mil/docs/citations/AD0649367
http://oai.dtic.mil/oai/oai?&verb=getRecord&metadataPrefix=html&identifier=AD0649367
genre Ice
permafrost
genre_facet Ice
permafrost
op_source DTIC AND NTIS
op_relation http://www.dtic.mil/docs/citations/AD0649367
op_rights APPROVED FOR PUBLIC RELEASE
_version_ 1766027622248087552