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Direct Measurements of Mean Reynolds Stress and Ripple Roughness in the Presence of Energetic Forcing by Surface Waves
Direct covariance observations of the mean flow Reynolds stress and sonar images of the seafloor collected on a wave‐exposed inner continental shelf demonstrate that the drag exerted by the seabed on the overlying flow is consistent with boundary layer models for wave‐current interaction, provided t...
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Published in: | Journal of geophysical research. Oceans 2018-04, Vol.123 (4), p.2494-2512 |
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container_title | Journal of geophysical research. Oceans |
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creator | Scully, Malcolm E. Trowbridge, John H. Sherwood, Christopher R. Jones, Katie R. Traykovski, Peter |
description | Direct covariance observations of the mean flow Reynolds stress and sonar images of the seafloor collected on a wave‐exposed inner continental shelf demonstrate that the drag exerted by the seabed on the overlying flow is consistent with boundary layer models for wave‐current interaction, provided that the orientation and anisotropy of the bed roughness are appropriately quantified. Large spatial and temporal variations in drag result from nonequilibrium ripple dynamics, ripple anisotropy, and the orientation of the ripples relative to the current. At a location in coarse sand characterized by large two‐dimensional orbital ripples, the observed drag shows a strong dependence on the relative orientation of the mean current to the ripple crests. At a contrasting location in fine sand, where more isotropic sub‐orbital ripples are observed, the sensitivity of the current to the orientation of the ripples is reduced. Further, at the coarse site under conditions when the currents are parallel to the ripple crests and the wave orbital diameter is smaller than the wavelength of the relic orbital ripples, the flow becomes hydraulically smooth. This transition is not observed at the fine site, where the observed wave orbital diameter is always greater than the wavelength of the observed sub‐orbital ripples. Paradoxically, the dominant along‐shelf flows often experience lower drag at the coarse site than at the fine site, despite the larger ripples, highlighting the complex dynamics controlling drag in wave‐exposed environments with heterogeneous roughness.
Key Points
Covariance measurements of Reynolds stress are consistent with boundary layer models of wave‐current interaction if bed roughness is known
The drag experienced by the mean flow on wave‐exposed continental shelves can vary significantly in time and space
Drag depends on nonequilibrium ripple dynamics, ripple anisotropy, and the orientation of the ripples relative to the current |
doi_str_mv | 10.1002/2017JC013252 |
format | article |
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Key Points
Covariance measurements of Reynolds stress are consistent with boundary layer models of wave‐current interaction if bed roughness is known
The drag experienced by the mean flow on wave‐exposed continental shelves can vary significantly in time and space
Drag depends on nonequilibrium ripple dynamics, ripple anisotropy, and the orientation of the ripples relative to the current</description><identifier>ISSN: 2169-9275</identifier><identifier>EISSN: 2169-9291</identifier><identifier>DOI: 10.1002/2017JC013252</identifier><language>eng</language><publisher>Washington: Blackwell Publishing Ltd</publisher><subject>Anisotropy ; Bed roughness ; Boundary layer models ; Boundary layers ; Continental shelves ; Covariance ; Dependence ; Drag ; Dynamics ; Geophysics ; Ocean floor ; Orientation ; Reynolds stress ; Ripples ; Sand ; Sonar imagery ; Surface waves ; Temporal variations ; Wavelength</subject><ispartof>Journal of geophysical research. Oceans, 2018-04, Vol.123 (4), p.2494-2512</ispartof><rights>2018. American Geophysical Union. All Rights Reserved.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a3731-87ae1a317bc94c467b89608d029dc07bf14feab635bb493d64a0605a260717d43</citedby><cites>FETCH-LOGICAL-a3731-87ae1a317bc94c467b89608d029dc07bf14feab635bb493d64a0605a260717d43</cites><orcidid>0000-0002-8163-6857 ; 0000-0003-3373-3924 ; 0000-0001-6135-3553 ; 0000-0002-5267-4002</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27923,27924</link.rule.ids></links><search><creatorcontrib>Scully, Malcolm E.</creatorcontrib><creatorcontrib>Trowbridge, John H.</creatorcontrib><creatorcontrib>Sherwood, Christopher R.</creatorcontrib><creatorcontrib>Jones, Katie R.</creatorcontrib><creatorcontrib>Traykovski, Peter</creatorcontrib><title>Direct Measurements of Mean Reynolds Stress and Ripple Roughness in the Presence of Energetic Forcing by Surface Waves</title><title>Journal of geophysical research. Oceans</title><description>Direct covariance observations of the mean flow Reynolds stress and sonar images of the seafloor collected on a wave‐exposed inner continental shelf demonstrate that the drag exerted by the seabed on the overlying flow is consistent with boundary layer models for wave‐current interaction, provided that the orientation and anisotropy of the bed roughness are appropriately quantified. Large spatial and temporal variations in drag result from nonequilibrium ripple dynamics, ripple anisotropy, and the orientation of the ripples relative to the current. At a location in coarse sand characterized by large two‐dimensional orbital ripples, the observed drag shows a strong dependence on the relative orientation of the mean current to the ripple crests. At a contrasting location in fine sand, where more isotropic sub‐orbital ripples are observed, the sensitivity of the current to the orientation of the ripples is reduced. Further, at the coarse site under conditions when the currents are parallel to the ripple crests and the wave orbital diameter is smaller than the wavelength of the relic orbital ripples, the flow becomes hydraulically smooth. This transition is not observed at the fine site, where the observed wave orbital diameter is always greater than the wavelength of the observed sub‐orbital ripples. Paradoxically, the dominant along‐shelf flows often experience lower drag at the coarse site than at the fine site, despite the larger ripples, highlighting the complex dynamics controlling drag in wave‐exposed environments with heterogeneous roughness.
Key Points
Covariance measurements of Reynolds stress are consistent with boundary layer models of wave‐current interaction if bed roughness is known
The drag experienced by the mean flow on wave‐exposed continental shelves can vary significantly in time and space
Drag depends on nonequilibrium ripple dynamics, ripple anisotropy, and the orientation of the ripples relative to the current</description><subject>Anisotropy</subject><subject>Bed roughness</subject><subject>Boundary layer models</subject><subject>Boundary layers</subject><subject>Continental shelves</subject><subject>Covariance</subject><subject>Dependence</subject><subject>Drag</subject><subject>Dynamics</subject><subject>Geophysics</subject><subject>Ocean floor</subject><subject>Orientation</subject><subject>Reynolds stress</subject><subject>Ripples</subject><subject>Sand</subject><subject>Sonar imagery</subject><subject>Surface waves</subject><subject>Temporal variations</subject><subject>Wavelength</subject><issn>2169-9275</issn><issn>2169-9291</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNp9kE1Lw0AQhoMoWGpv_oAFr0b3K9nsUWJbLYqSKh7DZjNpU9JN3E0q-fcmVMSTc5mv552B1_MuCb4hGNNbiolYxZgwGtATb0JJKH1JJTn9rUVw7s2c2-EhIhJxLife4b60oFv0DMp1FvZgWofqYuwNSqA3dZU7tG4tOIeUyVFSNk0FKKm7zdaMw9KgdgvodSDAaBjFcwN2A22p0aK2ujQblPVo3dlCDfsPdQB34Z0VqnIw-8lT730xf4sf_KeX5WN89-QrJhjxI6GAKEZEpiXXPBRZJEMc5ZjKXGORFYQXoLKQBVnGJctDrnCIA0VDLIjIOZt6V8e7ja0_O3Btuqs7a4aXKcVccBYQiQfq-khpWztnoUgbW-6V7VOC09Hc9K-5A86O-FdZQf8vm66WSUwH5wn7Bp--egU</recordid><startdate>201804</startdate><enddate>201804</enddate><creator>Scully, Malcolm E.</creator><creator>Trowbridge, John H.</creator><creator>Sherwood, Christopher R.</creator><creator>Jones, Katie R.</creator><creator>Traykovski, Peter</creator><general>Blackwell Publishing Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7TG</scope><scope>7TN</scope><scope>F1W</scope><scope>H96</scope><scope>KL.</scope><scope>L.G</scope><orcidid>https://orcid.org/0000-0002-8163-6857</orcidid><orcidid>https://orcid.org/0000-0003-3373-3924</orcidid><orcidid>https://orcid.org/0000-0001-6135-3553</orcidid><orcidid>https://orcid.org/0000-0002-5267-4002</orcidid></search><sort><creationdate>201804</creationdate><title>Direct Measurements of Mean Reynolds Stress and Ripple Roughness in the Presence of Energetic Forcing by Surface Waves</title><author>Scully, Malcolm E. ; Trowbridge, John H. ; Sherwood, Christopher R. ; Jones, Katie R. ; Traykovski, Peter</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a3731-87ae1a317bc94c467b89608d029dc07bf14feab635bb493d64a0605a260717d43</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Anisotropy</topic><topic>Bed roughness</topic><topic>Boundary layer models</topic><topic>Boundary layers</topic><topic>Continental shelves</topic><topic>Covariance</topic><topic>Dependence</topic><topic>Drag</topic><topic>Dynamics</topic><topic>Geophysics</topic><topic>Ocean floor</topic><topic>Orientation</topic><topic>Reynolds stress</topic><topic>Ripples</topic><topic>Sand</topic><topic>Sonar imagery</topic><topic>Surface waves</topic><topic>Temporal variations</topic><topic>Wavelength</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Scully, Malcolm E.</creatorcontrib><creatorcontrib>Trowbridge, John H.</creatorcontrib><creatorcontrib>Sherwood, Christopher R.</creatorcontrib><creatorcontrib>Jones, Katie R.</creatorcontrib><creatorcontrib>Traykovski, Peter</creatorcontrib><collection>CrossRef</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Oceanic Abstracts</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>Meteorological & Geoastrophysical Abstracts - Academic</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><jtitle>Journal of geophysical research. Oceans</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Scully, Malcolm E.</au><au>Trowbridge, John H.</au><au>Sherwood, Christopher R.</au><au>Jones, Katie R.</au><au>Traykovski, Peter</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Direct Measurements of Mean Reynolds Stress and Ripple Roughness in the Presence of Energetic Forcing by Surface Waves</atitle><jtitle>Journal of geophysical research. Oceans</jtitle><date>2018-04</date><risdate>2018</risdate><volume>123</volume><issue>4</issue><spage>2494</spage><epage>2512</epage><pages>2494-2512</pages><issn>2169-9275</issn><eissn>2169-9291</eissn><abstract>Direct covariance observations of the mean flow Reynolds stress and sonar images of the seafloor collected on a wave‐exposed inner continental shelf demonstrate that the drag exerted by the seabed on the overlying flow is consistent with boundary layer models for wave‐current interaction, provided that the orientation and anisotropy of the bed roughness are appropriately quantified. Large spatial and temporal variations in drag result from nonequilibrium ripple dynamics, ripple anisotropy, and the orientation of the ripples relative to the current. At a location in coarse sand characterized by large two‐dimensional orbital ripples, the observed drag shows a strong dependence on the relative orientation of the mean current to the ripple crests. At a contrasting location in fine sand, where more isotropic sub‐orbital ripples are observed, the sensitivity of the current to the orientation of the ripples is reduced. Further, at the coarse site under conditions when the currents are parallel to the ripple crests and the wave orbital diameter is smaller than the wavelength of the relic orbital ripples, the flow becomes hydraulically smooth. This transition is not observed at the fine site, where the observed wave orbital diameter is always greater than the wavelength of the observed sub‐orbital ripples. Paradoxically, the dominant along‐shelf flows often experience lower drag at the coarse site than at the fine site, despite the larger ripples, highlighting the complex dynamics controlling drag in wave‐exposed environments with heterogeneous roughness.
Key Points
Covariance measurements of Reynolds stress are consistent with boundary layer models of wave‐current interaction if bed roughness is known
The drag experienced by the mean flow on wave‐exposed continental shelves can vary significantly in time and space
Drag depends on nonequilibrium ripple dynamics, ripple anisotropy, and the orientation of the ripples relative to the current</abstract><cop>Washington</cop><pub>Blackwell Publishing Ltd</pub><doi>10.1002/2017JC013252</doi><tpages>19</tpages><orcidid>https://orcid.org/0000-0002-8163-6857</orcidid><orcidid>https://orcid.org/0000-0003-3373-3924</orcidid><orcidid>https://orcid.org/0000-0001-6135-3553</orcidid><orcidid>https://orcid.org/0000-0002-5267-4002</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Anisotropy Bed roughness Boundary layer models Boundary layers Continental shelves Covariance Dependence Drag Dynamics Geophysics Ocean floor Orientation Reynolds stress Ripples Sand Sonar imagery Surface waves Temporal variations Wavelength |
title | Direct Measurements of Mean Reynolds Stress and Ripple Roughness in the Presence of Energetic Forcing by Surface Waves |
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