WAVE-ICE INTERACTION

Three models are examined to study the transmission of ocean waves through an ice-field. In each case the effect of ice thickness, water depth, and the wave-length and angle of incidence of the incoming ocean wave is considered. In Model 1 the ice is assumed to consist of floating non- interacting m...

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Bibliographic Details
Main Authors: Evans, David V, Davies, Thomas V
Other Authors: STEVENS INST OF TECH HOBOKEN NJ DAVIDSON LAB
Format: Text
Language:English
Published: 1968
Subjects:
Ice
Online Access:http://www.dtic.mil/docs/citations/AD0674895
http://oai.dtic.mil/oai/oai?&verb=getRecord&metadataPrefix=html&identifier=AD0674895
id ftdtic:AD0674895
record_format openpolar
spelling ftdtic:AD0674895 2023-05-15T16:37:12+02:00 WAVE-ICE INTERACTION Evans, David V Davies, Thomas V STEVENS INST OF TECH HOBOKEN NJ DAVIDSON LAB 1968-08 text/html http://www.dtic.mil/docs/citations/AD0674895 http://oai.dtic.mil/oai/oai?&verb=getRecord&metadataPrefix=html&identifier=AD0674895 en eng http://www.dtic.mil/docs/citations/AD0674895 Approved for public release; distribution is unlimited. DTIC AND NTIS Physical and Dynamic Oceanography Snow Ice and Permafrost Numerical Mathematics *OCEAN WAVES *SEA ICE APPROXIMATION(MATHEMATICS) DIFFERENTIAL EQUATIONS DISTRIBUTION HYDRODYNAMICS INTEGRAL TRANSFORMS INTERACTIONS MATHEMATICAL MODELS PRESSURE REFLECTION SHALLOW WATER STABILITY THEOREMS THICKNESS WAVE PROPAGATION GRAPHS(CHARTS) Text 1968 ftdtic 2017-08-06T14:48:07Z Three models are examined to study the transmission of ocean waves through an ice-field. In each case the effect of ice thickness, water depth, and the wave-length and angle of incidence of the incoming ocean wave is considered. In Model 1 the ice is assumed to consist of floating non- interacting mass elements of varying thickness and the shallow-water approximation is utilized to simplify the equations. A simple cosine distribution varying in one direction only is assumed. In Model 11 the mass elements of constant thickness, interact through a bending stiffness force so that the ice acts as a thin elastic plate. The mass elements are connected through a surface tension force in Model 111 so that the ice is simulated by a stretched membrane. In both Models 11 and 111 the full linearized equations are solved. Because of the complexity of the resulting analysis, calculations of the reflection and transmission coefficients, and the pressure under the ice, are made in Model 11 on the basis of the shallow water approximation. Text Ice permafrost Sea ice 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 Physical and Dynamic Oceanography
Snow
Ice and Permafrost
Numerical Mathematics
*OCEAN WAVES
*SEA ICE
APPROXIMATION(MATHEMATICS)
DIFFERENTIAL EQUATIONS
DISTRIBUTION
HYDRODYNAMICS
INTEGRAL TRANSFORMS
INTERACTIONS
MATHEMATICAL MODELS
PRESSURE
REFLECTION
SHALLOW WATER
STABILITY
THEOREMS
THICKNESS
WAVE PROPAGATION
GRAPHS(CHARTS)
spellingShingle Physical and Dynamic Oceanography
Snow
Ice and Permafrost
Numerical Mathematics
*OCEAN WAVES
*SEA ICE
APPROXIMATION(MATHEMATICS)
DIFFERENTIAL EQUATIONS
DISTRIBUTION
HYDRODYNAMICS
INTEGRAL TRANSFORMS
INTERACTIONS
MATHEMATICAL MODELS
PRESSURE
REFLECTION
SHALLOW WATER
STABILITY
THEOREMS
THICKNESS
WAVE PROPAGATION
GRAPHS(CHARTS)
Evans, David V
Davies, Thomas V
WAVE-ICE INTERACTION
topic_facet Physical and Dynamic Oceanography
Snow
Ice and Permafrost
Numerical Mathematics
*OCEAN WAVES
*SEA ICE
APPROXIMATION(MATHEMATICS)
DIFFERENTIAL EQUATIONS
DISTRIBUTION
HYDRODYNAMICS
INTEGRAL TRANSFORMS
INTERACTIONS
MATHEMATICAL MODELS
PRESSURE
REFLECTION
SHALLOW WATER
STABILITY
THEOREMS
THICKNESS
WAVE PROPAGATION
GRAPHS(CHARTS)
description Three models are examined to study the transmission of ocean waves through an ice-field. In each case the effect of ice thickness, water depth, and the wave-length and angle of incidence of the incoming ocean wave is considered. In Model 1 the ice is assumed to consist of floating non- interacting mass elements of varying thickness and the shallow-water approximation is utilized to simplify the equations. A simple cosine distribution varying in one direction only is assumed. In Model 11 the mass elements of constant thickness, interact through a bending stiffness force so that the ice acts as a thin elastic plate. The mass elements are connected through a surface tension force in Model 111 so that the ice is simulated by a stretched membrane. In both Models 11 and 111 the full linearized equations are solved. Because of the complexity of the resulting analysis, calculations of the reflection and transmission coefficients, and the pressure under the ice, are made in Model 11 on the basis of the shallow water approximation.
author2 STEVENS INST OF TECH HOBOKEN NJ DAVIDSON LAB
format Text
author Evans, David V
Davies, Thomas V
author_facet Evans, David V
Davies, Thomas V
author_sort Evans, David V
title WAVE-ICE INTERACTION
title_short WAVE-ICE INTERACTION
title_full WAVE-ICE INTERACTION
title_fullStr WAVE-ICE INTERACTION
title_full_unstemmed WAVE-ICE INTERACTION
title_sort wave-ice interaction
publishDate 1968
url http://www.dtic.mil/docs/citations/AD0674895
http://oai.dtic.mil/oai/oai?&verb=getRecord&metadataPrefix=html&identifier=AD0674895
genre Ice
permafrost
Sea ice
genre_facet Ice
permafrost
Sea ice
op_source DTIC AND NTIS
op_relation http://www.dtic.mil/docs/citations/AD0674895
op_rights Approved for public release; distribution is unlimited.
_version_ 1766027497046016000