The problem of the body of revolution of minimal resistance

Detalhes bibliográficos
Autor(a) principal: Plakhov, A.
Data de Publicação: 2010
Outros Autores: Aleksenko, A.
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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spelling 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
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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
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