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dc.contributor.authorSubramanian, Susheelkumar C.
dc.contributor.authorRedkar, Sangram
dc.date.accessioned2022-02-05T21:49:27Z
dc.date.available2022-02-05T21:49:27Z
dc.date.copyright11/11/2020 12:00:00 AM
dc.date.issued2020
dc.identifier.issn1555-1415
dc.identifier.othercnd_016_01_014502.pdf
dc.identifier.urihttp://yetl.yabesh.ir/yetl1/handle/yetl/4276412
dc.description.abstractIn this work, the authors draw comparisons between the Floquet theory and Normal Forms technique and apply them towards the investigation of stability bounds for linear time periodic systems. Though the Normal Forms technique has been predominantly used for the analysis of nonlinear equations, in this work, the authors utilize it to transform a linear time periodic system to a time-invariant system, similar to the Lyapunov–Floquet (L–F) transformation. The authors employ an intuitive state augmentation technique, modal transformation, and near identity transformations to facilitate the application of time-independent Normal Forms. This method provides a closed form analytical expression for the state transition matrix (STM). Additionally, stability analysis is performed on the transformed system and the comparative results of dynamical characteristics and temporal variations of a simple linear Mathieu equation are also presented in this work.
dc.publisherThe American Society of Mechanical Engineers (ASME)
dc.titleComparison of Poincaré Normal Forms and Floquet Theory for Analysis of Linear Time Periodic Systems
dc.typeJournal Paper
dc.journal.volume16
dc.journal.issue1
dc.journal.titleJournal of Computational and Nonlinear Dynamics
dc.identifier.doi10.1115/1.4048715
dc.journal.fristpage014502-1
dc.journal.lastpage014502-6
dc.page6
dc.treeJournal of Computational and Nonlinear Dynamics:;2020:;volume( 016 ):;issue: 001
dc.contenttypeFulltext


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