An immersed structure approach for fluid-vegetation interaction
•A method for modeling the interaction between fluids and vegetation.•Separate meshes for fluids and structures allows complex geometry.•Plant flexibility modeled with beam model.•Velocity profile and bulk drag compared to experiments.•Captures important trends for bulk drag coefficient. We present...
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Veröffentlicht in: | Advances in water resources 2015-06, Vol.80, p.1-16 |
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creator | Mattis, Steven A. Dawson, Clint N. Kees, Christopher E. Farthing, Matthew W. |
description | •A method for modeling the interaction between fluids and vegetation.•Separate meshes for fluids and structures allows complex geometry.•Plant flexibility modeled with beam model.•Velocity profile and bulk drag compared to experiments.•Captures important trends for bulk drag coefficient.
We present an immersed structure approach for modeling the interaction between surface flows and vegetation. Fluid flow and rigid and flexible vegetative obstacles are coupled through a local drag relation that conserves momentum. In the presented method, separate meshes are used for the fluid domain and vegetative obstacles. Taking techniques from immersed boundary finite element methods, the effects of the fluid on the vegetative structures and vice versa are calculated using integral transforms. Using a simple elastic structure model we incorporate bending and moving vegetative obstacles. We model flexible vegetation as thin, elastic, inextensible cantilever beams. Using the immersed structure approach, a fully coupled fluid-vegetation interaction model is developed assuming dynamic fluid flow and quasi-static bending. This relatively computationally inexpensive model allows for thousands of vegetative obstacles to be included in a simulation without requiring an extremely refined fluid mesh. The method is validated with comparisons to mean velocity profiles and bent vegetation heights from experiments that are reproduced computationally. We test the method on several channel flow setups. We calculate the bulk drag coefficient in these flow scenarios and analyze their trends with changing model parameters including stem population density and flow Reynolds number. Bulk drag models are the primary method of incorporating small-scale drag from individual plants into a value that can be used in larger-scale models. Upscaled bulk drag quantities from this method may be utilized in larger-scale simulations of flow through vegetation regions. |
doi_str_mv | 10.1016/j.advwatres.2015.02.014 |
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We present an immersed structure approach for modeling the interaction between surface flows and vegetation. Fluid flow and rigid and flexible vegetative obstacles are coupled through a local drag relation that conserves momentum. In the presented method, separate meshes are used for the fluid domain and vegetative obstacles. Taking techniques from immersed boundary finite element methods, the effects of the fluid on the vegetative structures and vice versa are calculated using integral transforms. Using a simple elastic structure model we incorporate bending and moving vegetative obstacles. We model flexible vegetation as thin, elastic, inextensible cantilever beams. Using the immersed structure approach, a fully coupled fluid-vegetation interaction model is developed assuming dynamic fluid flow and quasi-static bending. This relatively computationally inexpensive model allows for thousands of vegetative obstacles to be included in a simulation without requiring an extremely refined fluid mesh. The method is validated with comparisons to mean velocity profiles and bent vegetation heights from experiments that are reproduced computationally. We test the method on several channel flow setups. We calculate the bulk drag coefficient in these flow scenarios and analyze their trends with changing model parameters including stem population density and flow Reynolds number. Bulk drag models are the primary method of incorporating small-scale drag from individual plants into a value that can be used in larger-scale models. Upscaled bulk drag quantities from this method may be utilized in larger-scale simulations of flow through vegetation regions.</description><identifier>ISSN: 0309-1708</identifier><identifier>EISSN: 1872-9657</identifier><identifier>DOI: 10.1016/j.advwatres.2015.02.014</identifier><language>eng</language><publisher>Elsevier Ltd</publisher><subject>Computational fluid dynamics ; Computer simulation ; Drag ; Environmental modeling ; Fluid dynamics ; Fluid flow ; Fluids ; Fluid–structure interaction ; Mathematical models ; Obstacles ; Vegetation</subject><ispartof>Advances in water resources, 2015-06, Vol.80, p.1-16</ispartof><rights>2015 Elsevier Ltd</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c381t-e85c3ffb07265c3b9692f2771cb4d0eaab4cc70434d1cd82311618c66c8e0bff3</citedby><cites>FETCH-LOGICAL-c381t-e85c3ffb07265c3b9692f2771cb4d0eaab4cc70434d1cd82311618c66c8e0bff3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1016/j.advwatres.2015.02.014$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,777,781,3537,27905,27906,45976</link.rule.ids></links><search><creatorcontrib>Mattis, Steven A.</creatorcontrib><creatorcontrib>Dawson, Clint N.</creatorcontrib><creatorcontrib>Kees, Christopher E.</creatorcontrib><creatorcontrib>Farthing, Matthew W.</creatorcontrib><title>An immersed structure approach for fluid-vegetation interaction</title><title>Advances in water resources</title><description>•A method for modeling the interaction between fluids and vegetation.•Separate meshes for fluids and structures allows complex geometry.•Plant flexibility modeled with beam model.•Velocity profile and bulk drag compared to experiments.•Captures important trends for bulk drag coefficient.
We present an immersed structure approach for modeling the interaction between surface flows and vegetation. Fluid flow and rigid and flexible vegetative obstacles are coupled through a local drag relation that conserves momentum. In the presented method, separate meshes are used for the fluid domain and vegetative obstacles. Taking techniques from immersed boundary finite element methods, the effects of the fluid on the vegetative structures and vice versa are calculated using integral transforms. Using a simple elastic structure model we incorporate bending and moving vegetative obstacles. We model flexible vegetation as thin, elastic, inextensible cantilever beams. Using the immersed structure approach, a fully coupled fluid-vegetation interaction model is developed assuming dynamic fluid flow and quasi-static bending. This relatively computationally inexpensive model allows for thousands of vegetative obstacles to be included in a simulation without requiring an extremely refined fluid mesh. The method is validated with comparisons to mean velocity profiles and bent vegetation heights from experiments that are reproduced computationally. We test the method on several channel flow setups. We calculate the bulk drag coefficient in these flow scenarios and analyze their trends with changing model parameters including stem population density and flow Reynolds number. Bulk drag models are the primary method of incorporating small-scale drag from individual plants into a value that can be used in larger-scale models. Upscaled bulk drag quantities from this method may be utilized in larger-scale simulations of flow through vegetation regions.</description><subject>Computational fluid dynamics</subject><subject>Computer simulation</subject><subject>Drag</subject><subject>Environmental modeling</subject><subject>Fluid dynamics</subject><subject>Fluid flow</subject><subject>Fluids</subject><subject>Fluid–structure interaction</subject><subject>Mathematical models</subject><subject>Obstacles</subject><subject>Vegetation</subject><issn>0309-1708</issn><issn>1872-9657</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNqNkEtPwzAQhC0EEuXxG8iRS8LaTmznhKqKl1SJC5wtx1mDqzyK7RTx70lVxBVOO4eZ0exHyBWFggIVN5vCtLtPkwLGggGtCmAF0PKILKiSLK9FJY_JAjjUOZWgTslZjBsAUKVkC3K7HDLf9xgitllMYbJpCpiZ7TaMxr5nbgyZ6ybf5jt8w2SSH-fAkDAYu9cX5MSZLuLlzz0nr_d3L6vHfP388LRarnPLFU05qspy5xqQTMyqqUXNHJOS2qZsAY1pSmsllLxsqW0V45QKqqwQViE0zvFzcn3onXd9TBiT7n202HVmwHGKmkoJvBKsqv9h5UxRVvNytsqD1YYxxoBOb4PvTfjSFPSert7oX7p6T1cD0zPdObk8JHF-eucx6Gg9DhZbH9Am3Y7-z45vHVmIFg</recordid><startdate>201506</startdate><enddate>201506</enddate><creator>Mattis, Steven A.</creator><creator>Dawson, Clint N.</creator><creator>Kees, Christopher E.</creator><creator>Farthing, Matthew W.</creator><general>Elsevier Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7QH</scope><scope>7ST</scope><scope>7TG</scope><scope>7UA</scope><scope>C1K</scope><scope>F1W</scope><scope>H96</scope><scope>KL.</scope><scope>L.G</scope><scope>SOI</scope><scope>8FD</scope><scope>FR3</scope><scope>KR7</scope></search><sort><creationdate>201506</creationdate><title>An immersed structure approach for fluid-vegetation interaction</title><author>Mattis, Steven A. ; Dawson, Clint N. ; Kees, Christopher E. ; Farthing, Matthew W.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c381t-e85c3ffb07265c3b9692f2771cb4d0eaab4cc70434d1cd82311618c66c8e0bff3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><topic>Computational fluid dynamics</topic><topic>Computer simulation</topic><topic>Drag</topic><topic>Environmental modeling</topic><topic>Fluid dynamics</topic><topic>Fluid flow</topic><topic>Fluids</topic><topic>Fluid–structure interaction</topic><topic>Mathematical models</topic><topic>Obstacles</topic><topic>Vegetation</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Mattis, Steven A.</creatorcontrib><creatorcontrib>Dawson, Clint N.</creatorcontrib><creatorcontrib>Kees, Christopher E.</creatorcontrib><creatorcontrib>Farthing, Matthew W.</creatorcontrib><collection>CrossRef</collection><collection>Aqualine</collection><collection>Environment Abstracts</collection><collection>Meteorological & Geoastrophysical Abstracts</collection><collection>Water Resources Abstracts</collection><collection>Environmental Sciences and Pollution Management</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><collection>Environment Abstracts</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>Civil Engineering Abstracts</collection><jtitle>Advances in water resources</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Mattis, Steven A.</au><au>Dawson, Clint N.</au><au>Kees, Christopher E.</au><au>Farthing, Matthew W.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>An immersed structure approach for fluid-vegetation interaction</atitle><jtitle>Advances in water resources</jtitle><date>2015-06</date><risdate>2015</risdate><volume>80</volume><spage>1</spage><epage>16</epage><pages>1-16</pages><issn>0309-1708</issn><eissn>1872-9657</eissn><abstract>•A method for modeling the interaction between fluids and vegetation.•Separate meshes for fluids and structures allows complex geometry.•Plant flexibility modeled with beam model.•Velocity profile and bulk drag compared to experiments.•Captures important trends for bulk drag coefficient.
We present an immersed structure approach for modeling the interaction between surface flows and vegetation. Fluid flow and rigid and flexible vegetative obstacles are coupled through a local drag relation that conserves momentum. In the presented method, separate meshes are used for the fluid domain and vegetative obstacles. Taking techniques from immersed boundary finite element methods, the effects of the fluid on the vegetative structures and vice versa are calculated using integral transforms. Using a simple elastic structure model we incorporate bending and moving vegetative obstacles. We model flexible vegetation as thin, elastic, inextensible cantilever beams. Using the immersed structure approach, a fully coupled fluid-vegetation interaction model is developed assuming dynamic fluid flow and quasi-static bending. This relatively computationally inexpensive model allows for thousands of vegetative obstacles to be included in a simulation without requiring an extremely refined fluid mesh. The method is validated with comparisons to mean velocity profiles and bent vegetation heights from experiments that are reproduced computationally. We test the method on several channel flow setups. We calculate the bulk drag coefficient in these flow scenarios and analyze their trends with changing model parameters including stem population density and flow Reynolds number. Bulk drag models are the primary method of incorporating small-scale drag from individual plants into a value that can be used in larger-scale models. Upscaled bulk drag quantities from this method may be utilized in larger-scale simulations of flow through vegetation regions.</abstract><pub>Elsevier Ltd</pub><doi>10.1016/j.advwatres.2015.02.014</doi><tpages>16</tpages></addata></record> |
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subjects | Computational fluid dynamics Computer simulation Drag Environmental modeling Fluid dynamics Fluid flow Fluids Fluid–structure interaction Mathematical models Obstacles Vegetation |
title | An immersed structure approach for fluid-vegetation interaction |
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