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dc.contributor.authorMorales, P.-
dc.contributor.authorJaramillo Arango, Daniel Esteban-
dc.contributor.authorOsorio Vélez, Jaime Alberto-
dc.date.accessioned2020-01-11T23:03:50Z-
dc.date.available2020-01-11T23:03:50Z-
dc.date.issued2016-
dc.identifier.citationMorales, P., Jaramillo Arango, D. E., & Osorio Vélez, J. A. (2016). Experimental aspects of the gyroscope’s movement. Revista Mexicana de Fisica, (62), 44-50.spa
dc.identifier.issn0035-001X-
dc.identifier.urihttp://hdl.handle.net/10495/13075-
dc.description.abstractABSTRACT: 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.spa
dc.format.mimetypeapplication/pdfspa
dc.language.isoengspa
dc.publisherSociedad Mexicana de Físicaspa
dc.type.hasversioninfo:eu-repo/semantics/publishedVersionspa
dc.rightsAtribución-NoComercial 2.5 Colombia (CC BY-NC 2.5 CO)*
dc.rightsinfo:eu-repo/semantics/openAccessspa
dc.rights.urihttp://creativecommons.org/licenses/by-nc/2.5/co/*
dc.titleExperimental aspects of the gyroscope’s movementspa
dc.typeinfo:eu-repo/semantics/articlespa
dc.publisher.groupGrupo Estado Sólidospa
oaire.versionhttp://purl.org/coar/version/c_970fb48d4fbd8a85spa
dc.rights.accessrightshttp://purl.org/coar/access_right/c_abf2spa
oaire.citationtitleRevista Mexicana de Físicaspa
oaire.citationstartpage44spa
oaire.citationendpage50spa
oaire.citationvolume62spa
oaire.citationissue62spa
dc.rights.creativecommonshttps://creativecommons.org/licenses/by-nc/4.0/spa
dc.publisher.placeMéxicospa
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1spa
dc.type.redcolhttps://purl.org/redcol/resource_type/ARTspa
dc.type.localArtículo de investigaciónspa
dc.subject.lembEcuaciones Euler-Lagrange-
dc.subject.lembLagrange equations-
dc.subject.agrovocGiroscopios-
dc.subject.agrovocGyroscopes-
dc.subject.proposalMovimiento de la peonzaspa
dc.subject.proposalMovimiento del giroscopiospa
dc.subject.agrovocurihttp://aims.fao.org/aos/agrovoc/c_63747380-
dc.description.researchgroupidCOL0008138spa
dc.relation.ispartofjournalabbrevRev. Mex. Fis.spa
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