Loading…

Growth of unsteady wave groups by shear flows

A weakly nonlinear theory has been proposed and developed for calculating the energy- transfer rate to individual waves in a group. It is shown what portion of total energy- transfer rate, over the envelope of wave group, affects individual waves in the group. From this an expression for complex pha...

Full description

Saved in:
Bibliographic Details
Published in:arXiv.org 2017-04
Main Authors: Sajjadi, S G, Hunt, J C R, Drullion, F
Format: Article
Language:English
Subjects:
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by
cites
container_end_page
container_issue
container_start_page
container_title arXiv.org
container_volume
creator Sajjadi, S G
Hunt, J C R
Drullion, F
description A weakly nonlinear theory has been proposed and developed for calculating the energy- transfer rate to individual waves in a group. It is shown what portion of total energy- transfer rate, over the envelope of wave group, affects individual waves in the group. From this an expression for complex phase speed of individual waves is calculated. It is deduced that each wave in a group does not grow at the same rate. It is shown that the critical layer is no longer symmetrical compared with the ideal monochromatic waves. This asymmetry causes the critical layer height to be lower over the downwind part. Therefore the positive growth of the individual waves on the upwind part of the wave group exceeds the negative growth on the downwind part (which would not be true if \(z_c\), where the mean flow \(U\) is equal to the speed of the wave propagation, was the same over the whole group). This leads to the critical layer group effect producing a net horizontal force on the waves, in addition to the sheltering effect. Computational simulations over a non-growing wave group is also presented, which confirms the above postulation made by Sajjadi, Hunt and Drullion (2014) (SHD).
format article
fullrecord <record><control><sourceid>proquest</sourceid><recordid>TN_cdi_proquest_journals_2074351605</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2074351605</sourcerecordid><originalsourceid>FETCH-proquest_journals_20743516053</originalsourceid><addsrcrecordid>eNpjYuA0MjY21LUwMTLiYOAtLs4yMDAwMjM3MjU15mTQdS_KLy_JUMhPUyjNKy5JTUypVChPLEtVSC_KLy0oVkiqVCjOSE0sUkjLyS8v5mFgTUvMKU7lhdLcDMpuriHOHroFRfmFpanFJfFZ-aVFeUCpeCMDcxNjU0MzA1Nj4lQBAMVHMf0</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2074351605</pqid></control><display><type>article</type><title>Growth of unsteady wave groups by shear flows</title><source>ProQuest - Publicly Available Content Database</source><creator>Sajjadi, S G ; Hunt, J C R ; Drullion, F</creator><creatorcontrib>Sajjadi, S G ; Hunt, J C R ; Drullion, F</creatorcontrib><description>A weakly nonlinear theory has been proposed and developed for calculating the energy- transfer rate to individual waves in a group. It is shown what portion of total energy- transfer rate, over the envelope of wave group, affects individual waves in the group. From this an expression for complex phase speed of individual waves is calculated. It is deduced that each wave in a group does not grow at the same rate. It is shown that the critical layer is no longer symmetrical compared with the ideal monochromatic waves. This asymmetry causes the critical layer height to be lower over the downwind part. Therefore the positive growth of the individual waves on the upwind part of the wave group exceeds the negative growth on the downwind part (which would not be true if \(z_c\), where the mean flow \(U\) is equal to the speed of the wave propagation, was the same over the whole group). This leads to the critical layer group effect producing a net horizontal force on the waves, in addition to the sheltering effect. Computational simulations over a non-growing wave group is also presented, which confirms the above postulation made by Sajjadi, Hunt and Drullion (2014) (SHD).</description><identifier>EISSN: 2331-8422</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Computer simulation ; Horizontal loads ; Mathematical analysis ; Phase velocity ; Shear flow ; Wave groups ; Wave propagation</subject><ispartof>arXiv.org, 2017-04</ispartof><rights>2017. This work is published under http://creativecommons.org/publicdomain/zero/1.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.proquest.com/docview/2074351605?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>780,784,25752,37011,44589</link.rule.ids></links><search><creatorcontrib>Sajjadi, S G</creatorcontrib><creatorcontrib>Hunt, J C R</creatorcontrib><creatorcontrib>Drullion, F</creatorcontrib><title>Growth of unsteady wave groups by shear flows</title><title>arXiv.org</title><description>A weakly nonlinear theory has been proposed and developed for calculating the energy- transfer rate to individual waves in a group. It is shown what portion of total energy- transfer rate, over the envelope of wave group, affects individual waves in the group. From this an expression for complex phase speed of individual waves is calculated. It is deduced that each wave in a group does not grow at the same rate. It is shown that the critical layer is no longer symmetrical compared with the ideal monochromatic waves. This asymmetry causes the critical layer height to be lower over the downwind part. Therefore the positive growth of the individual waves on the upwind part of the wave group exceeds the negative growth on the downwind part (which would not be true if \(z_c\), where the mean flow \(U\) is equal to the speed of the wave propagation, was the same over the whole group). This leads to the critical layer group effect producing a net horizontal force on the waves, in addition to the sheltering effect. Computational simulations over a non-growing wave group is also presented, which confirms the above postulation made by Sajjadi, Hunt and Drullion (2014) (SHD).</description><subject>Computer simulation</subject><subject>Horizontal loads</subject><subject>Mathematical analysis</subject><subject>Phase velocity</subject><subject>Shear flow</subject><subject>Wave groups</subject><subject>Wave propagation</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><recordid>eNpjYuA0MjY21LUwMTLiYOAtLs4yMDAwMjM3MjU15mTQdS_KLy_JUMhPUyjNKy5JTUypVChPLEtVSC_KLy0oVkiqVCjOSE0sUkjLyS8v5mFgTUvMKU7lhdLcDMpuriHOHroFRfmFpanFJfFZ-aVFeUCpeCMDcxNjU0MzA1Nj4lQBAMVHMf0</recordid><startdate>20170416</startdate><enddate>20170416</enddate><creator>Sajjadi, S G</creator><creator>Hunt, J C R</creator><creator>Drullion, F</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope></search><sort><creationdate>20170416</creationdate><title>Growth of unsteady wave groups by shear flows</title><author>Sajjadi, S G ; Hunt, J C R ; Drullion, F</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-proquest_journals_20743516053</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Computer simulation</topic><topic>Horizontal loads</topic><topic>Mathematical analysis</topic><topic>Phase velocity</topic><topic>Shear flow</topic><topic>Wave groups</topic><topic>Wave propagation</topic><toplevel>online_resources</toplevel><creatorcontrib>Sajjadi, S G</creatorcontrib><creatorcontrib>Hunt, J C R</creatorcontrib><creatorcontrib>Drullion, F</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science &amp; Engineering Collection</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>ProQuest - Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Sajjadi, S G</au><au>Hunt, J C R</au><au>Drullion, F</au><format>book</format><genre>document</genre><ristype>GEN</ristype><atitle>Growth of unsteady wave groups by shear flows</atitle><jtitle>arXiv.org</jtitle><date>2017-04-16</date><risdate>2017</risdate><eissn>2331-8422</eissn><abstract>A weakly nonlinear theory has been proposed and developed for calculating the energy- transfer rate to individual waves in a group. It is shown what portion of total energy- transfer rate, over the envelope of wave group, affects individual waves in the group. From this an expression for complex phase speed of individual waves is calculated. It is deduced that each wave in a group does not grow at the same rate. It is shown that the critical layer is no longer symmetrical compared with the ideal monochromatic waves. This asymmetry causes the critical layer height to be lower over the downwind part. Therefore the positive growth of the individual waves on the upwind part of the wave group exceeds the negative growth on the downwind part (which would not be true if \(z_c\), where the mean flow \(U\) is equal to the speed of the wave propagation, was the same over the whole group). This leads to the critical layer group effect producing a net horizontal force on the waves, in addition to the sheltering effect. Computational simulations over a non-growing wave group is also presented, which confirms the above postulation made by Sajjadi, Hunt and Drullion (2014) (SHD).</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><oa>free_for_read</oa></addata></record>
fulltext fulltext
identifier EISSN: 2331-8422
ispartof arXiv.org, 2017-04
issn 2331-8422
language eng
recordid cdi_proquest_journals_2074351605
source ProQuest - Publicly Available Content Database
subjects Computer simulation
Horizontal loads
Mathematical analysis
Phase velocity
Shear flow
Wave groups
Wave propagation
title Growth of unsteady wave groups by shear flows
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-10T14%3A17%3A24IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest&rft_val_fmt=info:ofi/fmt:kev:mtx:book&rft.genre=document&rft.atitle=Growth%20of%20unsteady%20wave%20groups%20by%20shear%20flows&rft.jtitle=arXiv.org&rft.au=Sajjadi,%20S%20G&rft.date=2017-04-16&rft.eissn=2331-8422&rft_id=info:doi/&rft_dat=%3Cproquest%3E2074351605%3C/proquest%3E%3Cgrp_id%3Ecdi_FETCH-proquest_journals_20743516053%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=2074351605&rft_id=info:pmid/&rfr_iscdi=true