1958
DOI: 10.1016/0021-8928(58)90033-9
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On the stability of periodic motions

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Cited by 48 publications
(43 citation statements)
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“…Hiskens et al used this model to find the required jump map. Very briefly, just before the switching, the two conditions that must be satisfied are (14) where and are the state and algebraic variables immediately before the switching. Furthermore, by using the chain rule, the derivative of the state vector just before the switching is given by (15) where is the instant just before the switching.…”
Section: B Nonsmooth Systemsmentioning
confidence: 99%
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“…Hiskens et al used this model to find the required jump map. Very briefly, just before the switching, the two conditions that must be satisfied are (14) where and are the state and algebraic variables immediately before the switching. Furthermore, by using the chain rule, the derivative of the state vector just before the switching is given by (15) where is the instant just before the switching.…”
Section: B Nonsmooth Systemsmentioning
confidence: 99%
“…If there is no discontinuity (i.e., ), by using the linear approximation given in (7) for both sides of the switching, the map reduces to a simple form similar to the saltation matrix [14] and part of the Jacobian of the Poincaré map [27], [28].…”
Section: B Nonsmooth Systemsmentioning
confidence: 99%
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“…The eigenvalues of this matrix are called Floquet multipliers. For piecewise linear systems, as is the case for the system considered in this study, the monodromy matrix can be constructed from the product of the state transition matrices corresponding to each sub-cycle and the corresponding saltation matrix [Leine and Nijemeijer, 2004;Aizerman and Gantmakher, 1958;Fillipov, 1988;Giaouris et al, 2008]. Suppose a trajectory x(t) starts at time instant t i and is passing from the Configuration C i described by the vector field A i x+B i (t) := f i (x, t), intersects the switching boundary described by the equation σ i (x, t) = 0 at t i , and goes to Configuration C i+1 given by the vector field A i+1 x + B i+1 (t) := f i+1 (x, t).…”
Section: Floquet Theory and Fillipov Methodsmentioning
confidence: 99%
“…The first approach will be based on a Poincaré map function [El Aroudi et al, 2007]. The second approach is the Floquet theory ( [Aizerman and Gantmakher, 1958]) together with Fillipov methods for systems with discontinuous vector field [Fillipov, 1988], [Leine and Nijemeijer, 2004], [Giaouris et al, 2008]. The third approach is based on the FDM together with Floquet theory [Nayfeh et al, 2009], [Nayfeh and Balachandran, 1995].…”
Section: Closed-form Solutions Corresponding To the Different Linear mentioning
confidence: 99%