Progression of Wave Breaker Types on a Plane Impermeable Slope, Depending on Experimental Design
The objective of this research was to analyze the progression of breaker types on plane impermeable slopes. This study used dimensional analysis to demonstrate the relative water depth is a key explanatory quantity. The dominant breaker types depend on the incident wave characteristics at the foot o...
Gespeichert in:
Veröffentlicht in: | Journal of geophysical research. Oceans 2021-05, Vol.126 (5), p.n/a, Article 2021 |
---|---|
Hauptverfasser: | , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | n/a |
---|---|
container_issue | 5 |
container_start_page | |
container_title | Journal of geophysical research. Oceans |
container_volume | 126 |
creator | Moragues, M. V. Losada, M. Á. |
description | The objective of this research was to analyze the progression of breaker types on plane impermeable slopes. This study used dimensional analysis to demonstrate the relative water depth is a key explanatory quantity. The dominant breaker types depend on the incident wave characteristics at the foot of the slope. Accordingly, it is possible to combine values of H, T, and m. The physical experiments of Galvin, recent numerical results, and new experiments, performed on an impermeable 1:10 slope, were used to verify the result. It was thus possible to obtain the progression of breaker types in different sequences of pairs of combined wave H and T values. Once a sequence is defined, the expected progression of breaker types is predictable, and is well approximated by the log‐transform of the alternate similarity parameter. Since the classification of breaker types is discontinuous, the data assigned to each type were placed in horizontal lines, based on the value of log(χ). Given that the breaking of a wave train on a slope should be considered a continuous process, the location of some data was corrected to satisfy this assumption. There is thus a functional relationship between the sets of the experimental space and of the breaker types. This research also derives the non‐dimensional energy dissipation on the slope, considering the wave‐reflected energy flux on the slope. It is proportional to a dimensionless bulk dissipation coefficient which depends on the breaker type and, therefore, on the value of χ at the toe of the slope.
Plain Language Summary
The main objective of this research was to analyze the progression of breaker types on a plane impermeable slope. This study used dimensional analysis to demonstrate that the relative water depth is a key explanatory quantity. The dominant breaker types depend on the incident wave characteristics at the foot of the slope, h/L, and H/L, and also on the slope, m. Accordingly, different combinations of these three parameters can be made. Data from different data sets performed on an impermeable slope with a 1:10 slope angle were used to verify that result. After several analyses of different experimental techniques, it can be concluded that there is a functional relationship between the sets of the experimental space and the breaker types.
Key Points
The progression of breaker types depends on the slope and the wave characteristics at the toe of the slope. It is predictable
There is a functional relationship betwee |
doi_str_mv | 10.1029/2021JC017211 |
format | Article |
fullrecord | <record><control><sourceid>proquest_webof</sourceid><recordid>TN_cdi_webofscience_primary_000654462400021CitationCount</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2532085995</sourcerecordid><originalsourceid>FETCH-LOGICAL-a3683-30e37e3c6c99a5b966b1fe9a09d05d26c9bb75d221c2e6b95496b365e412df13</originalsourceid><addsrcrecordid>eNqNkV1LwzAYhYsoOObu_AEBL101H03aXGqdc2Pg0IGXNW3fjs4uqUmn7t-bsSFeibnJIec5yctJEJwTfEUwldcUUzJNMYkpIUdBjxIhQ0klOf7RMT8NBs6tsF8JSaJI9oLXuTVLC87VRiNToRf1AejWgnoDixbbFhzyhkLzRmlAk3ULdg0qbwA9N6aFIbqDFnRZ6-WOG315v16D7lTjHVcv9VlwUqnGweCw94PF_WiRPoSzx_EkvZmFiomEhQwDi4EVopBS8VwKkZMKpMKyxLyk_jjPYy8oKSiIXPJIipwJDhGhZUVYP7jYX9ta874B12Urs7Hav5hRzihOuJTcU8M9VVjjnIUqa_24ym4zgrNdi9nvFj1-ucc_ITeVK2rQBfxEfIuCR5GgkVd0Ryf_p9O6U53vPDUb3fkoO0TrBrZ_DpVNx08p9X_H2DcbgpJx</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2532085995</pqid></control><display><type>article</type><title>Progression of Wave Breaker Types on a Plane Impermeable Slope, Depending on Experimental Design</title><source>Access via Wiley Online Library</source><source>Web of Science - Science Citation Index Expanded - 2021<img src="https://exlibris-pub.s3.amazonaws.com/fromwos-v2.jpg" /></source><source>Wiley Online Library (Open Access Collection)</source><source>Alma/SFX Local Collection</source><creator>Moragues, M. V. ; Losada, M. Á.</creator><creatorcontrib>Moragues, M. V. ; Losada, M. Á.</creatorcontrib><description>The objective of this research was to analyze the progression of breaker types on plane impermeable slopes. This study used dimensional analysis to demonstrate the relative water depth is a key explanatory quantity. The dominant breaker types depend on the incident wave characteristics at the foot of the slope. Accordingly, it is possible to combine values of H, T, and m. The physical experiments of Galvin, recent numerical results, and new experiments, performed on an impermeable 1:10 slope, were used to verify the result. It was thus possible to obtain the progression of breaker types in different sequences of pairs of combined wave H and T values. Once a sequence is defined, the expected progression of breaker types is predictable, and is well approximated by the log‐transform of the alternate similarity parameter. Since the classification of breaker types is discontinuous, the data assigned to each type were placed in horizontal lines, based on the value of log(χ). Given that the breaking of a wave train on a slope should be considered a continuous process, the location of some data was corrected to satisfy this assumption. There is thus a functional relationship between the sets of the experimental space and of the breaker types. This research also derives the non‐dimensional energy dissipation on the slope, considering the wave‐reflected energy flux on the slope. It is proportional to a dimensionless bulk dissipation coefficient which depends on the breaker type and, therefore, on the value of χ at the toe of the slope.
Plain Language Summary
The main objective of this research was to analyze the progression of breaker types on a plane impermeable slope. This study used dimensional analysis to demonstrate that the relative water depth is a key explanatory quantity. The dominant breaker types depend on the incident wave characteristics at the foot of the slope, h/L, and H/L, and also on the slope, m. Accordingly, different combinations of these three parameters can be made. Data from different data sets performed on an impermeable slope with a 1:10 slope angle were used to verify that result. After several analyses of different experimental techniques, it can be concluded that there is a functional relationship between the sets of the experimental space and the breaker types.
Key Points
The progression of breaker types depends on the slope and the wave characteristics at the toe of the slope. It is predictable
There is a functional relationship between the sets of the relative water depth and wave steepness and of breaker types
A dimensionless bulk dissipation coefficient is defined which depends on the breaker type and on the relative water depth and wave steepness</description><identifier>ISSN: 2169-9275</identifier><identifier>EISSN: 2169-9291</identifier><identifier>DOI: 10.1029/2021JC017211</identifier><language>eng</language><publisher>WASHINGTON: Amer Geophysical Union</publisher><subject>Breaker types ; Breakers ; Data ; Design of experiments ; Dimensional analysis ; Energy dissipation ; Energy exchange ; Energy flux ; Energy transfer ; Experimental design ; Feet ; Geophysics ; Incident waves ; Oceanography ; Parameters ; Physical Sciences ; relative water depth ; Science & Technology ; Slopes ; smooth plane slopes ; Water depth ; wave steepness ; Wave trains</subject><ispartof>Journal of geophysical research. Oceans, 2021-05, Vol.126 (5), p.n/a, Article 2021</ispartof><rights>2021. The Authors.</rights><rights>2021. This article is published under http://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>true</woscitedreferencessubscribed><woscitedreferencescount>5</woscitedreferencescount><woscitedreferencesoriginalsourcerecordid>wos000654462400021</woscitedreferencesoriginalsourcerecordid><citedby>FETCH-LOGICAL-a3683-30e37e3c6c99a5b966b1fe9a09d05d26c9bb75d221c2e6b95496b365e412df13</citedby><cites>FETCH-LOGICAL-a3683-30e37e3c6c99a5b966b1fe9a09d05d26c9bb75d221c2e6b95496b365e412df13</cites><orcidid>0000-0003-3635-2553 ; 0000-0002-2071-3134</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://onlinelibrary.wiley.com/doi/pdf/10.1029%2F2021JC017211$$EPDF$$P50$$Gwiley$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://onlinelibrary.wiley.com/doi/full/10.1029%2F2021JC017211$$EHTML$$P50$$Gwiley$$Hfree_for_read</linktohtml><link.rule.ids>315,782,786,1419,1435,27931,27932,39265,45581,45582,46416,46840</link.rule.ids></links><search><creatorcontrib>Moragues, M. V.</creatorcontrib><creatorcontrib>Losada, M. Á.</creatorcontrib><title>Progression of Wave Breaker Types on a Plane Impermeable Slope, Depending on Experimental Design</title><title>Journal of geophysical research. Oceans</title><addtitle>J GEOPHYS RES-OCEANS</addtitle><description>The objective of this research was to analyze the progression of breaker types on plane impermeable slopes. This study used dimensional analysis to demonstrate the relative water depth is a key explanatory quantity. The dominant breaker types depend on the incident wave characteristics at the foot of the slope. Accordingly, it is possible to combine values of H, T, and m. The physical experiments of Galvin, recent numerical results, and new experiments, performed on an impermeable 1:10 slope, were used to verify the result. It was thus possible to obtain the progression of breaker types in different sequences of pairs of combined wave H and T values. Once a sequence is defined, the expected progression of breaker types is predictable, and is well approximated by the log‐transform of the alternate similarity parameter. Since the classification of breaker types is discontinuous, the data assigned to each type were placed in horizontal lines, based on the value of log(χ). Given that the breaking of a wave train on a slope should be considered a continuous process, the location of some data was corrected to satisfy this assumption. There is thus a functional relationship between the sets of the experimental space and of the breaker types. This research also derives the non‐dimensional energy dissipation on the slope, considering the wave‐reflected energy flux on the slope. It is proportional to a dimensionless bulk dissipation coefficient which depends on the breaker type and, therefore, on the value of χ at the toe of the slope.
Plain Language Summary
The main objective of this research was to analyze the progression of breaker types on a plane impermeable slope. This study used dimensional analysis to demonstrate that the relative water depth is a key explanatory quantity. The dominant breaker types depend on the incident wave characteristics at the foot of the slope, h/L, and H/L, and also on the slope, m. Accordingly, different combinations of these three parameters can be made. Data from different data sets performed on an impermeable slope with a 1:10 slope angle were used to verify that result. After several analyses of different experimental techniques, it can be concluded that there is a functional relationship between the sets of the experimental space and the breaker types.
Key Points
The progression of breaker types depends on the slope and the wave characteristics at the toe of the slope. It is predictable
There is a functional relationship between the sets of the relative water depth and wave steepness and of breaker types
A dimensionless bulk dissipation coefficient is defined which depends on the breaker type and on the relative water depth and wave steepness</description><subject>Breaker types</subject><subject>Breakers</subject><subject>Data</subject><subject>Design of experiments</subject><subject>Dimensional analysis</subject><subject>Energy dissipation</subject><subject>Energy exchange</subject><subject>Energy flux</subject><subject>Energy transfer</subject><subject>Experimental design</subject><subject>Feet</subject><subject>Geophysics</subject><subject>Incident waves</subject><subject>Oceanography</subject><subject>Parameters</subject><subject>Physical Sciences</subject><subject>relative water depth</subject><subject>Science & Technology</subject><subject>Slopes</subject><subject>smooth plane slopes</subject><subject>Water depth</subject><subject>wave steepness</subject><subject>Wave trains</subject><issn>2169-9275</issn><issn>2169-9291</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><sourceid>24P</sourceid><sourceid>WIN</sourceid><sourceid>HGBXW</sourceid><recordid>eNqNkV1LwzAYhYsoOObu_AEBL101H03aXGqdc2Pg0IGXNW3fjs4uqUmn7t-bsSFeibnJIec5yctJEJwTfEUwldcUUzJNMYkpIUdBjxIhQ0klOf7RMT8NBs6tsF8JSaJI9oLXuTVLC87VRiNToRf1AejWgnoDixbbFhzyhkLzRmlAk3ULdg0qbwA9N6aFIbqDFnRZ6-WOG315v16D7lTjHVcv9VlwUqnGweCw94PF_WiRPoSzx_EkvZmFiomEhQwDi4EVopBS8VwKkZMKpMKyxLyk_jjPYy8oKSiIXPJIipwJDhGhZUVYP7jYX9ta874B12Urs7Hav5hRzihOuJTcU8M9VVjjnIUqa_24ym4zgrNdi9nvFj1-ucc_ITeVK2rQBfxEfIuCR5GgkVd0Ryf_p9O6U53vPDUb3fkoO0TrBrZ_DpVNx08p9X_H2DcbgpJx</recordid><startdate>202105</startdate><enddate>202105</enddate><creator>Moragues, M. V.</creator><creator>Losada, M. Á.</creator><general>Amer Geophysical Union</general><general>Blackwell Publishing Ltd</general><scope>24P</scope><scope>WIN</scope><scope>BLEPL</scope><scope>DTL</scope><scope>HGBXW</scope><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/0000-0003-3635-2553</orcidid><orcidid>https://orcid.org/0000-0002-2071-3134</orcidid></search><sort><creationdate>202105</creationdate><title>Progression of Wave Breaker Types on a Plane Impermeable Slope, Depending on Experimental Design</title><author>Moragues, M. V. ; Losada, M. Á.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a3683-30e37e3c6c99a5b966b1fe9a09d05d26c9bb75d221c2e6b95496b365e412df13</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Breaker types</topic><topic>Breakers</topic><topic>Data</topic><topic>Design of experiments</topic><topic>Dimensional analysis</topic><topic>Energy dissipation</topic><topic>Energy exchange</topic><topic>Energy flux</topic><topic>Energy transfer</topic><topic>Experimental design</topic><topic>Feet</topic><topic>Geophysics</topic><topic>Incident waves</topic><topic>Oceanography</topic><topic>Parameters</topic><topic>Physical Sciences</topic><topic>relative water depth</topic><topic>Science & Technology</topic><topic>Slopes</topic><topic>smooth plane slopes</topic><topic>Water depth</topic><topic>wave steepness</topic><topic>Wave trains</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Moragues, M. V.</creatorcontrib><creatorcontrib>Losada, M. Á.</creatorcontrib><collection>Wiley Online Library (Open Access Collection)</collection><collection>Wiley Online Library (Open Access Collection)</collection><collection>Web of Science Core Collection</collection><collection>Science Citation Index Expanded</collection><collection>Web of Science - Science Citation Index Expanded - 2021</collection><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>Moragues, M. V.</au><au>Losada, M. Á.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Progression of Wave Breaker Types on a Plane Impermeable Slope, Depending on Experimental Design</atitle><jtitle>Journal of geophysical research. Oceans</jtitle><stitle>J GEOPHYS RES-OCEANS</stitle><date>2021-05</date><risdate>2021</risdate><volume>126</volume><issue>5</issue><epage>n/a</epage><artnum>2021</artnum><issn>2169-9275</issn><eissn>2169-9291</eissn><abstract>The objective of this research was to analyze the progression of breaker types on plane impermeable slopes. This study used dimensional analysis to demonstrate the relative water depth is a key explanatory quantity. The dominant breaker types depend on the incident wave characteristics at the foot of the slope. Accordingly, it is possible to combine values of H, T, and m. The physical experiments of Galvin, recent numerical results, and new experiments, performed on an impermeable 1:10 slope, were used to verify the result. It was thus possible to obtain the progression of breaker types in different sequences of pairs of combined wave H and T values. Once a sequence is defined, the expected progression of breaker types is predictable, and is well approximated by the log‐transform of the alternate similarity parameter. Since the classification of breaker types is discontinuous, the data assigned to each type were placed in horizontal lines, based on the value of log(χ). Given that the breaking of a wave train on a slope should be considered a continuous process, the location of some data was corrected to satisfy this assumption. There is thus a functional relationship between the sets of the experimental space and of the breaker types. This research also derives the non‐dimensional energy dissipation on the slope, considering the wave‐reflected energy flux on the slope. It is proportional to a dimensionless bulk dissipation coefficient which depends on the breaker type and, therefore, on the value of χ at the toe of the slope.
Plain Language Summary
The main objective of this research was to analyze the progression of breaker types on a plane impermeable slope. This study used dimensional analysis to demonstrate that the relative water depth is a key explanatory quantity. The dominant breaker types depend on the incident wave characteristics at the foot of the slope, h/L, and H/L, and also on the slope, m. Accordingly, different combinations of these three parameters can be made. Data from different data sets performed on an impermeable slope with a 1:10 slope angle were used to verify that result. After several analyses of different experimental techniques, it can be concluded that there is a functional relationship between the sets of the experimental space and the breaker types.
Key Points
The progression of breaker types depends on the slope and the wave characteristics at the toe of the slope. It is predictable
There is a functional relationship between the sets of the relative water depth and wave steepness and of breaker types
A dimensionless bulk dissipation coefficient is defined which depends on the breaker type and on the relative water depth and wave steepness</abstract><cop>WASHINGTON</cop><pub>Amer Geophysical Union</pub><doi>10.1029/2021JC017211</doi><tpages>21</tpages><orcidid>https://orcid.org/0000-0003-3635-2553</orcidid><orcidid>https://orcid.org/0000-0002-2071-3134</orcidid><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | ISSN: 2169-9275 |
ispartof | Journal of geophysical research. Oceans, 2021-05, Vol.126 (5), p.n/a, Article 2021 |
issn | 2169-9275 2169-9291 |
language | eng |
recordid | cdi_webofscience_primary_000654462400021CitationCount |
source | Access via Wiley Online Library; Web of Science - Science Citation Index Expanded - 2021<img src="https://exlibris-pub.s3.amazonaws.com/fromwos-v2.jpg" />; Wiley Online Library (Open Access Collection); Alma/SFX Local Collection |
subjects | Breaker types Breakers Data Design of experiments Dimensional analysis Energy dissipation Energy exchange Energy flux Energy transfer Experimental design Feet Geophysics Incident waves Oceanography Parameters Physical Sciences relative water depth Science & Technology Slopes smooth plane slopes Water depth wave steepness Wave trains |
title | Progression of Wave Breaker Types on a Plane Impermeable Slope, Depending on Experimental Design |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-04T20%3A59%3A10IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_webof&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Progression%20of%20Wave%20Breaker%20Types%20on%20a%20Plane%20Impermeable%20Slope,%20Depending%20on%20Experimental%20Design&rft.jtitle=Journal%20of%20geophysical%20research.%20Oceans&rft.au=Moragues,%20M.%20V.&rft.date=2021-05&rft.volume=126&rft.issue=5&rft.epage=n/a&rft.artnum=2021&rft.issn=2169-9275&rft.eissn=2169-9291&rft_id=info:doi/10.1029/2021JC017211&rft_dat=%3Cproquest_webof%3E2532085995%3C/proquest_webof%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=2532085995&rft_id=info:pmid/&rfr_iscdi=true |