2008
DOI: 10.1109/tcsi.2008.916443
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Stability Analysis of the Continuous-Conduction-Mode Buck Converter Via Filippov's Method

Abstract: Abstract-To study the stability of a nominal cyclic steady state in power electronic converters, it is necessary to obtain a linearization around the periodic orbit. In many past studies, this was achieved by explicitly deriving the Poincaré map that describes the evolution of the state from one clock instant to the next and then locally linearizing the map at the fixed point. However, in many converters, the map cannot be derived in closed form, and therefore this approach cannot directly be applied. Alternat… Show more

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Cited by 202 publications
(155 citation statements)
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References 35 publications
(73 reference statements)
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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%
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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%
“…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). It has been shown, using the Fillipov method ( [Fillipov, 1988;Leine and Nijemeijer, 2004;Giaouris et al, 2008]), that when there is a transversal intersection, the state transition matrix across the switching boundary, called also the saltation matrix S i , is given by…”
Section: Floquet Theory and Fillipov Methodsmentioning
confidence: 99%
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“…Based on theory of monodromy matrix [24], [25], if the Floquet multipliers of the monodromy matrix are all within the unit circle, then the system is stable. If the maximum Floquet multiplier equals 1, then bifurcation occurs; otherwise, it is unstable.…”
Section: Monodromy Matrixmentioning
confidence: 99%
“…Thus it is essential to measure the undesired nonlinearity, in order to make sure the stable domain of the converter. Recently, a series of tools have become available for analyzing the dynamic behaviors in power electronics circuits, including Poincaré maps [3], the Filippov method [4], and the Lyapunov method [5], where, the maximal Lyapunov character exponent (mLCE) is the most extensive way to distinguish chaotic regimes from periodic regimes in a continuous system [6,7]. However, because of the non-differentiable point on the switching surface, the previous computation method of mLCE may cause error in the switching systems.…”
Section: Introductionmentioning
confidence: 99%