Experimental aspects of the gyroscope’s movement

ABSTRACT: In presence of a uniform gravitational field, Euler equations for a gyroscope can be written as a non-linear equation for the components of Riemann’s stereographic projection of the symmetry axis over a horizontal plane. Under the approximation of nutations with low amplitude, the solution...

Full description

Autores:
Morales, P.
Jaramillo Arango, Daniel Esteban
Osorio Vélez, Jaime Alberto
Tipo de recurso:
Article of investigation
Fecha de publicación:
2016
Institución:
Universidad de Antioquia
Repositorio:
Repositorio UdeA
Idioma:
eng
OAI Identifier:
oai:bibliotecadigital.udea.edu.co:10495/13075
Acceso en línea:
http://hdl.handle.net/10495/13075
Palabra clave:
Ecuaciones Euler-Lagrange
Lagrange equations
Giroscopios
Gyroscopes
Movimiento de la peonza
Movimiento del giroscopio
http://aims.fao.org/aos/agrovoc/c_63747380
Rights
openAccess
License
https://creativecommons.org/licenses/by-nc/4.0/
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oai_identifier_str oai:bibliotecadigital.udea.edu.co:10495/13075
network_acronym_str UDEA2
network_name_str Repositorio UdeA
repository_id_str
dc.title.spa.fl_str_mv Experimental aspects of the gyroscope’s movement
title Experimental aspects of the gyroscope’s movement
spellingShingle Experimental aspects of the gyroscope’s movement
Ecuaciones Euler-Lagrange
Lagrange equations
Giroscopios
Gyroscopes
Movimiento de la peonza
Movimiento del giroscopio
http://aims.fao.org/aos/agrovoc/c_63747380
title_short Experimental aspects of the gyroscope’s movement
title_full Experimental aspects of the gyroscope’s movement
title_fullStr Experimental aspects of the gyroscope’s movement
title_full_unstemmed Experimental aspects of the gyroscope’s movement
title_sort Experimental aspects of the gyroscope’s movement
dc.creator.fl_str_mv Morales, P.
Jaramillo Arango, Daniel Esteban
Osorio Vélez, Jaime Alberto
dc.contributor.author.none.fl_str_mv Morales, P.
Jaramillo Arango, Daniel Esteban
Osorio Vélez, Jaime Alberto
dc.contributor.researchgroup.spa.fl_str_mv Grupo Estado Sólido
dc.subject.lemb.none.fl_str_mv Ecuaciones Euler-Lagrange
Lagrange equations
topic Ecuaciones Euler-Lagrange
Lagrange equations
Giroscopios
Gyroscopes
Movimiento de la peonza
Movimiento del giroscopio
http://aims.fao.org/aos/agrovoc/c_63747380
dc.subject.agrovoc.none.fl_str_mv Giroscopios
Gyroscopes
dc.subject.proposal.spa.fl_str_mv Movimiento de la peonza
Movimiento del giroscopio
dc.subject.agrovocuri.none.fl_str_mv http://aims.fao.org/aos/agrovoc/c_63747380
description ABSTRACT: In presence of a uniform gravitational field, Euler equations for a gyroscope can be written as a non-linear equation for the components of Riemann’s stereographic projection of the symmetry axis over a horizontal plane. Under the approximation of nutations with low amplitude, the solution of this equation corresponds to the sum of two rotating vectors with angular frequencies related to both angular velocities of nutation and precession. Such velocities are functions of rotation rapidity and inertia momentum of the gyroscope. From pictures of the movement projection of a commercial gyroscope, and using a laser that turn on during half revolution cycle of a disk, we can determine all kinematic quantities of the gyroscope, velocities of: rotation, precession and nutation, along with the angle of average inclination from axis. After complete a total of 120 experiments, we corroborate that the expressions given for velocities of precession and nutation, in function of rotation, match with experimental data. This is an easy experiment to implement, and can be used in advanced courses of mechanic.
publishDate 2016
dc.date.issued.none.fl_str_mv 2016
dc.date.accessioned.none.fl_str_mv 2020-01-11T23:03:50Z
dc.date.available.none.fl_str_mv 2020-01-11T23:03:50Z
dc.type.spa.fl_str_mv Artículo de investigación
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dc.identifier.citation.spa.fl_str_mv Morales, P., Jaramillo Arango, D. E., & Osorio Vélez, J. A. (2016). Experimental aspects of the gyroscope’s movement. Revista Mexicana de Fisica, (62), 44-50.
dc.identifier.issn.none.fl_str_mv 0035-001X
dc.identifier.uri.none.fl_str_mv http://hdl.handle.net/10495/13075
identifier_str_mv Morales, P., Jaramillo Arango, D. E., & Osorio Vélez, J. A. (2016). Experimental aspects of the gyroscope’s movement. Revista Mexicana de Fisica, (62), 44-50.
0035-001X
url http://hdl.handle.net/10495/13075
dc.language.iso.spa.fl_str_mv eng
language eng
dc.relation.ispartofjournalabbrev.spa.fl_str_mv Rev. Mex. Fis.
dc.relation.citationendpage.spa.fl_str_mv 50
dc.relation.citationissue.spa.fl_str_mv 62
dc.relation.citationstartpage.spa.fl_str_mv 44
dc.relation.citationvolume.spa.fl_str_mv 62
dc.relation.ispartofjournal.spa.fl_str_mv Revista Mexicana de Física
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dc.rights.accessrights.*.fl_str_mv Atribución-NoComercial 2.5 Colombia (CC BY-NC 2.5 CO)
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dc.publisher.spa.fl_str_mv Sociedad Mexicana de Física
dc.publisher.place.spa.fl_str_mv México
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spelling Morales, P.Jaramillo Arango, Daniel EstebanOsorio Vélez, Jaime AlbertoGrupo Estado Sólido2020-01-11T23:03:50Z2020-01-11T23:03:50Z2016Morales, P., Jaramillo Arango, D. E., & Osorio Vélez, J. A. (2016). Experimental aspects of the gyroscope’s movement. Revista Mexicana de Fisica, (62), 44-50.0035-001Xhttp://hdl.handle.net/10495/13075ABSTRACT: In presence of a uniform gravitational field, Euler equations for a gyroscope can be written as a non-linear equation for the components of Riemann’s stereographic projection of the symmetry axis over a horizontal plane. Under the approximation of nutations with low amplitude, the solution of this equation corresponds to the sum of two rotating vectors with angular frequencies related to both angular velocities of nutation and precession. Such velocities are functions of rotation rapidity and inertia momentum of the gyroscope. From pictures of the movement projection of a commercial gyroscope, and using a laser that turn on during half revolution cycle of a disk, we can determine all kinematic quantities of the gyroscope, velocities of: rotation, precession and nutation, along with the angle of average inclination from axis. After complete a total of 120 experiments, we corroborate that the expressions given for velocities of precession and nutation, in function of rotation, match with experimental data. This is an easy experiment to implement, and can be used in advanced courses of mechanic.COL0008138application/pdfengSociedad Mexicana de FísicaMéxicohttps://creativecommons.org/licenses/by-nc/4.0/http://creativecommons.org/licenses/by-nc/2.5/co/Atribución-NoComercial 2.5 Colombia (CC BY-NC 2.5 CO)info:eu-repo/semantics/openAccesshttp://purl.org/coar/access_right/c_abf2Experimental aspects of the gyroscope’s movementArtículo de investigaciónhttp://purl.org/coar/resource_type/c_2df8fbb1https://purl.org/redcol/resource_type/ARThttp://purl.org/coar/version/c_970fb48d4fbd8a85info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionEcuaciones Euler-LagrangeLagrange equationsGiroscopiosGyroscopesMovimiento de la peonzaMovimiento del giroscopiohttp://aims.fao.org/aos/agrovoc/c_63747380Rev. Mex. 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