The problem of the body of revolution of minimal resistance
Autor(a) principal: | |
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Data de Publicação: | 2010 |
Outros Autores: | |
Tipo de documento: | Artigo |
Idioma: | eng |
Título da fonte: | Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos) |
Texto Completo: | http://hdl.handle.net/10773/6310 |
Resumo: | Newton's problem of the body of minimal aerodynamic resistance is traditionally stated in the class of convex axially symmetric bodies with fixed length and width. We state and solve the minimal resistance problem in the wider class of axially symmetric but generally nonconvex bodies. The infimum in this problem is not attained. We construct a sequence of bodies minimizing the resistance. This sequence approximates a convex body with smooth front surface, while the surface of approximating bodies becomes more and more complicated. The shape of the resulting convex body and the value of minimal resistance are compared with the corresponding results for Newton's problem and for the problem in the intermediate class of axisymmetric bodies satisfying the single impact assumption [Comte and Lachand-Robert, J. Anal. Math. 83 (2001) 313-335]. In particular, the minimal resistance in our class is smaller than in Newton's problem; the ratio goes to 1/2 as (length)/(width of the body) → 0, and to 1/4 as (length)/(width) → +∞. © EDP Sciences, SMAI, 2008. |
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The problem of the body of revolution of minimal resistanceBilliardsBodies of minimal resistanceCalculus of variationsNewton's problemAerodynamic resistanceAxially symmetricAxisymmetric bodiesBody of revolutionCalculus of variationsConvex bodyFront surfacesNonconvexResistance problemsAerodynamicsAerospace vehiclesCalculationsImpact resistanceBodies of revolutionNewton's problem of the body of minimal aerodynamic resistance is traditionally stated in the class of convex axially symmetric bodies with fixed length and width. We state and solve the minimal resistance problem in the wider class of axially symmetric but generally nonconvex bodies. The infimum in this problem is not attained. We construct a sequence of bodies minimizing the resistance. This sequence approximates a convex body with smooth front surface, while the surface of approximating bodies becomes more and more complicated. The shape of the resulting convex body and the value of minimal resistance are compared with the corresponding results for Newton's problem and for the problem in the intermediate class of axisymmetric bodies satisfying the single impact assumption [Comte and Lachand-Robert, J. Anal. Math. 83 (2001) 313-335]. In particular, the minimal resistance in our class is smaller than in Newton's problem; the ratio goes to 1/2 as (length)/(width of the body) → 0, and to 1/4 as (length)/(width) → +∞. © EDP Sciences, SMAI, 2008.2012-02-14T10:34:36Z2010-01-01T00:00:00Z2010info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articleapplication/pdfhttp://hdl.handle.net/10773/6310eng1292-811910.1051/cocv:2008070Plakhov, A.Aleksenko, A.info:eu-repo/semantics/openAccessreponame:Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos)instname:Agência para a Sociedade do Conhecimento (UMIC) - FCT - Sociedade da Informaçãoinstacron:RCAAP2024-02-22T11:09:50Zoai:ria.ua.pt:10773/6310Portal AgregadorONGhttps://www.rcaap.pt/oai/openaireopendoar:71602024-03-20T02:44:05.257341Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos) - Agência para a Sociedade do Conhecimento (UMIC) - FCT - Sociedade da Informaçãofalse |
dc.title.none.fl_str_mv |
The problem of the body of revolution of minimal resistance |
title |
The problem of the body of revolution of minimal resistance |
spellingShingle |
The problem of the body of revolution of minimal resistance Plakhov, A. Billiards Bodies of minimal resistance Calculus of variations Newton's problem Aerodynamic resistance Axially symmetric Axisymmetric bodies Body of revolution Calculus of variations Convex body Front surfaces Nonconvex Resistance problems Aerodynamics Aerospace vehicles Calculations Impact resistance Bodies of revolution |
title_short |
The problem of the body of revolution of minimal resistance |
title_full |
The problem of the body of revolution of minimal resistance |
title_fullStr |
The problem of the body of revolution of minimal resistance |
title_full_unstemmed |
The problem of the body of revolution of minimal resistance |
title_sort |
The problem of the body of revolution of minimal resistance |
author |
Plakhov, A. |
author_facet |
Plakhov, A. Aleksenko, A. |
author_role |
author |
author2 |
Aleksenko, A. |
author2_role |
author |
dc.contributor.author.fl_str_mv |
Plakhov, A. Aleksenko, A. |
dc.subject.por.fl_str_mv |
Billiards Bodies of minimal resistance Calculus of variations Newton's problem Aerodynamic resistance Axially symmetric Axisymmetric bodies Body of revolution Calculus of variations Convex body Front surfaces Nonconvex Resistance problems Aerodynamics Aerospace vehicles Calculations Impact resistance Bodies of revolution |
topic |
Billiards Bodies of minimal resistance Calculus of variations Newton's problem Aerodynamic resistance Axially symmetric Axisymmetric bodies Body of revolution Calculus of variations Convex body Front surfaces Nonconvex Resistance problems Aerodynamics Aerospace vehicles Calculations Impact resistance Bodies of revolution |
description |
Newton's problem of the body of minimal aerodynamic resistance is traditionally stated in the class of convex axially symmetric bodies with fixed length and width. We state and solve the minimal resistance problem in the wider class of axially symmetric but generally nonconvex bodies. The infimum in this problem is not attained. We construct a sequence of bodies minimizing the resistance. This sequence approximates a convex body with smooth front surface, while the surface of approximating bodies becomes more and more complicated. The shape of the resulting convex body and the value of minimal resistance are compared with the corresponding results for Newton's problem and for the problem in the intermediate class of axisymmetric bodies satisfying the single impact assumption [Comte and Lachand-Robert, J. Anal. Math. 83 (2001) 313-335]. In particular, the minimal resistance in our class is smaller than in Newton's problem; the ratio goes to 1/2 as (length)/(width of the body) → 0, and to 1/4 as (length)/(width) → +∞. © EDP Sciences, SMAI, 2008. |
publishDate |
2010 |
dc.date.none.fl_str_mv |
2010-01-01T00:00:00Z 2010 2012-02-14T10:34:36Z |
dc.type.status.fl_str_mv |
info:eu-repo/semantics/publishedVersion |
dc.type.driver.fl_str_mv |
info:eu-repo/semantics/article |
format |
article |
status_str |
publishedVersion |
dc.identifier.uri.fl_str_mv |
http://hdl.handle.net/10773/6310 |
url |
http://hdl.handle.net/10773/6310 |
dc.language.iso.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
1292-8119 10.1051/cocv:2008070 |
dc.rights.driver.fl_str_mv |
info:eu-repo/semantics/openAccess |
eu_rights_str_mv |
openAccess |
dc.format.none.fl_str_mv |
application/pdf |
dc.source.none.fl_str_mv |
reponame:Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos) instname:Agência para a Sociedade do Conhecimento (UMIC) - FCT - Sociedade da Informação instacron:RCAAP |
instname_str |
Agência para a Sociedade do Conhecimento (UMIC) - FCT - Sociedade da Informação |
instacron_str |
RCAAP |
institution |
RCAAP |
reponame_str |
Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos) |
collection |
Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos) |
repository.name.fl_str_mv |
Repositório Científico de Acesso Aberto de Portugal (Repositórios Cientìficos) - Agência para a Sociedade do Conhecimento (UMIC) - FCT - Sociedade da Informação |
repository.mail.fl_str_mv |
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1799137491393970176 |