Please use this identifier to cite or link to this item: https://scidar.kg.ac.rs/handle/123456789/12012
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dc.contributor.authorVeljovic, Ljiljana-
dc.contributor.authorRadakovic, Aleksandar-
dc.contributor.authorMilosavljevic, Dragan-
dc.contributor.authorBogdanovic, Gordana-
dc.date.accessioned2021-04-20T19:47:38Z-
dc.date.available2021-04-20T19:47:38Z-
dc.date.issued2015-
dc.identifier.issn0020-7462-
dc.identifier.urihttps://scidar.kg.ac.rs/handle/123456789/12012-
dc.description.abstract© 2014 Elsevier Ltd. All rights reserved. In this paper rigid body dynamic with coupled rotation around axes that are not intersecting is described by vectors connected to the pole and the axis. These mass moment vectors are defined by K. Hedrih. Dynamic equilibrium of rigid body dynamics with coupled rotations is described by vector equations. Also, they are used for obtaining differential equations to the rotor dynamics. In the case where one component of rotation is programmed by constant angular velocity, the non-linear differential equation of the system dynamics in the gravitational field is obtained and so is the corresponding equation of the phase trajectory. Series of phase trajectory transformations in relation with changes of some parameters of rigid body are presented.-
dc.rightsrestrictedAccess-
dc.sourceInternational Journal of Non-Linear Mechanics-
dc.titleRigid body coupled rotation around no intersecting axes-
dc.typearticle-
dc.identifier.doi10.1016/j.ijnonlinmec.2014.11.001-
dc.identifier.scopus2-s2.0-84939944427-
Appears in Collections:Faculty of Engineering, Kragujevac

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