Spinning rigid bodies driven by orbital forcing: the role of dry friction

Detalhes bibliográficos
Autor(a) principal: de Castro, Pablo [UNESP]
Data de Publicação: 2022
Outros Autores: Lima, Tiago Araújo, Parisio, Fernando
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositório Institucional da UNESP
Texto Completo: http://dx.doi.org/10.1007/s11071-021-07175-8
http://hdl.handle.net/11449/230192
Resumo: A “circular orbital forcing” makes a chosen point on a rigid body follow a circular motion while the body spins freely around that point. We investigate this problem for the planar motion of a body subject to dry friction. We focus on the effect called reverse rotation (RR), where spinning and orbital rotations are antiparallel. Similar reverse dynamics include the rotations of Venus and Uranus, journal machinery bearings, tissue production reactors, and chiral active particles. Due to dissipation, RRs are possible only as a transient. Here, the transient or flip time tf depends on the circular driving frequency ω, unlike the viscous case previously studied. We find tf∼ ωγ-1μ-γ/2, where μ is the friction coefficient and γ= 0 (γ= 2) for low (high) ω. Whether RRs really occur depends on the initial conditions as well as on μ and H, a geometrical parameter. The critical Hc(μ) where RRs become possible follows a q-exponential with q≃ 1.9 , a more restrictive RR scenario than in the wet case. We use animations to visualize the different dynamical regimes that emerge from the highly nonlinear dissipation mechanism of dry friction. Our results are valid across multiple investigated rigid body shapes.
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spelling Spinning rigid bodies driven by orbital forcing: the role of dry frictionCircular orbital forcingDry frictionReverse rotationsRigid-body dynamicsA “circular orbital forcing” makes a chosen point on a rigid body follow a circular motion while the body spins freely around that point. We investigate this problem for the planar motion of a body subject to dry friction. We focus on the effect called reverse rotation (RR), where spinning and orbital rotations are antiparallel. Similar reverse dynamics include the rotations of Venus and Uranus, journal machinery bearings, tissue production reactors, and chiral active particles. Due to dissipation, RRs are possible only as a transient. Here, the transient or flip time tf depends on the circular driving frequency ω, unlike the viscous case previously studied. We find tf∼ ωγ-1μ-γ/2, where μ is the friction coefficient and γ= 0 (γ= 2) for low (high) ω. Whether RRs really occur depends on the initial conditions as well as on μ and H, a geometrical parameter. The critical Hc(μ) where RRs become possible follows a q-exponential with q≃ 1.9 , a more restrictive RR scenario than in the wet case. We use animations to visualize the different dynamical regimes that emerge from the highly nonlinear dissipation mechanism of dry friction. Our results are valid across multiple investigated rigid body shapes.ICTP South American Institute for Fundamental Research & Instituto de Física Teórica - UNESPSer Educacional S.A., PernambucoDepartamento de Física Universidade Federal de Pernambuco, PernambucoICTP South American Institute for Fundamental Research & Instituto de Física Teórica - UNESPUniversidade Estadual Paulista (UNESP)Ser Educacional S.A.Universidade Federal de Pernambuco (UFPE)de Castro, Pablo [UNESP]Lima, Tiago AraújoParisio, Fernando2022-04-29T08:38:19Z2022-04-29T08:38:19Z2022-01-01info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articlehttp://dx.doi.org/10.1007/s11071-021-07175-8Nonlinear Dynamics.1573-269X0924-090Xhttp://hdl.handle.net/11449/23019210.1007/s11071-021-07175-82-s2.0-85122540660Scopusreponame:Repositório Institucional da UNESPinstname:Universidade Estadual Paulista (UNESP)instacron:UNESPengNonlinear Dynamicsinfo:eu-repo/semantics/openAccess2022-04-29T08:38:20Zoai:repositorio.unesp.br:11449/230192Repositório InstitucionalPUBhttp://repositorio.unesp.br/oai/requestopendoar:29462024-08-05T18:01:26.790946Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP)false
dc.title.none.fl_str_mv Spinning rigid bodies driven by orbital forcing: the role of dry friction
title Spinning rigid bodies driven by orbital forcing: the role of dry friction
spellingShingle Spinning rigid bodies driven by orbital forcing: the role of dry friction
de Castro, Pablo [UNESP]
Circular orbital forcing
Dry friction
Reverse rotations
Rigid-body dynamics
title_short Spinning rigid bodies driven by orbital forcing: the role of dry friction
title_full Spinning rigid bodies driven by orbital forcing: the role of dry friction
title_fullStr Spinning rigid bodies driven by orbital forcing: the role of dry friction
title_full_unstemmed Spinning rigid bodies driven by orbital forcing: the role of dry friction
title_sort Spinning rigid bodies driven by orbital forcing: the role of dry friction
author de Castro, Pablo [UNESP]
author_facet de Castro, Pablo [UNESP]
Lima, Tiago Araújo
Parisio, Fernando
author_role author
author2 Lima, Tiago Araújo
Parisio, Fernando
author2_role author
author
dc.contributor.none.fl_str_mv Universidade Estadual Paulista (UNESP)
Ser Educacional S.A.
Universidade Federal de Pernambuco (UFPE)
dc.contributor.author.fl_str_mv de Castro, Pablo [UNESP]
Lima, Tiago Araújo
Parisio, Fernando
dc.subject.por.fl_str_mv Circular orbital forcing
Dry friction
Reverse rotations
Rigid-body dynamics
topic Circular orbital forcing
Dry friction
Reverse rotations
Rigid-body dynamics
description A “circular orbital forcing” makes a chosen point on a rigid body follow a circular motion while the body spins freely around that point. We investigate this problem for the planar motion of a body subject to dry friction. We focus on the effect called reverse rotation (RR), where spinning and orbital rotations are antiparallel. Similar reverse dynamics include the rotations of Venus and Uranus, journal machinery bearings, tissue production reactors, and chiral active particles. Due to dissipation, RRs are possible only as a transient. Here, the transient or flip time tf depends on the circular driving frequency ω, unlike the viscous case previously studied. We find tf∼ ωγ-1μ-γ/2, where μ is the friction coefficient and γ= 0 (γ= 2) for low (high) ω. Whether RRs really occur depends on the initial conditions as well as on μ and H, a geometrical parameter. The critical Hc(μ) where RRs become possible follows a q-exponential with q≃ 1.9 , a more restrictive RR scenario than in the wet case. We use animations to visualize the different dynamical regimes that emerge from the highly nonlinear dissipation mechanism of dry friction. Our results are valid across multiple investigated rigid body shapes.
publishDate 2022
dc.date.none.fl_str_mv 2022-04-29T08:38:19Z
2022-04-29T08:38:19Z
2022-01-01
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://dx.doi.org/10.1007/s11071-021-07175-8
Nonlinear Dynamics.
1573-269X
0924-090X
http://hdl.handle.net/11449/230192
10.1007/s11071-021-07175-8
2-s2.0-85122540660
url http://dx.doi.org/10.1007/s11071-021-07175-8
http://hdl.handle.net/11449/230192
identifier_str_mv Nonlinear Dynamics.
1573-269X
0924-090X
10.1007/s11071-021-07175-8
2-s2.0-85122540660
dc.language.iso.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv Nonlinear Dynamics
dc.rights.driver.fl_str_mv info:eu-repo/semantics/openAccess
eu_rights_str_mv openAccess
dc.source.none.fl_str_mv Scopus
reponame:Repositório Institucional da UNESP
instname:Universidade Estadual Paulista (UNESP)
instacron:UNESP
instname_str Universidade Estadual Paulista (UNESP)
instacron_str UNESP
institution UNESP
reponame_str Repositório Institucional da UNESP
collection Repositório Institucional da UNESP
repository.name.fl_str_mv Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP)
repository.mail.fl_str_mv
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