2005
DOI: 10.1002/rnc.1012
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Duality and eventually periodic systems

Abstract: SUMMARYThis paper employs semidefinite programming duality theory to develop new alternative linear matrix inequality (LMI) tools for eventually periodic systems. These tools are then utilized to rederive an important version of the Kalman-Yakubovich-Popov (KYP) Lemma for such systems, and further give new synthesis results.

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Cited by 24 publications
(10 citation statements)
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“…The work follows from [1][2][3] in their study of the Kalman-Yakubovich-Popov (KYP) lemma for LTV systems and [4,5] in their work on relaxing IQC theorems obtained from a dissipativity context. Previous work on robustness of LTV systems without IQCs is considerable.…”
Section: Introductionmentioning
confidence: 99%
“…The work follows from [1][2][3] in their study of the Kalman-Yakubovich-Popov (KYP) lemma for LTV systems and [4,5] in their work on relaxing IQC theorems obtained from a dissipativity context. Previous work on robustness of LTV systems without IQCs is considerable.…”
Section: Introductionmentioning
confidence: 99%
“…Eventually time‐invariant LPV models are NSLPV models such that the explicit time variation in the state‐space realization is eventually time‐invariant, ie, aperiodic for an initial amount of time and then time‐invariant afterwards. () The definition of the isomorphic system can be further extended to cover all negative time instants by simply setting the state‐space matrix‐valued functions for t <−1 equal to zero. The resulting system is then defined for all integers tfalse(,false) with A ( k ) ( t ,δ ( k ) ( t ))=0 for t <0 (in the isomorphic system, we have A ( k ) (−1, · )=0).…”
Section: Preliminariesmentioning
confidence: 99%
“…We show that, for such systems, the synthesis conditions in Corollary reduce to a finite‐dimensional semidefinite programming problem. An eventually periodic system arises when linearizing the nonlinear system equations about an eventually periodic trajectory. Such a trajectory can be arbitrary for an initial amount of time but then settles into a periodic orbit.…”
Section: Finite‐dimensional Synthesis Conditionsmentioning
confidence: 99%
“…Clearly, a γ ‐admissible synthesis for G is a 1‐admissible synthesis for trueG̃, where trueG̃ has the same realization as G except that trueC̃1i(tMathClass-punc,k)MathClass-rel=1γC1i(tMathClass-punc,k), trueD̃11(tMathClass-punc,k)MathClass-rel=1γD11(tMathClass-punc,k), and trueD̃12(tMathClass-punc,k)MathClass-rel=1γD12(tMathClass-punc,k) for all tMathClass-rel∈double-struckN0, k = 1,2,3,4, and i = 0,1, … , s . Furthermore, by employing the Schur complement formula, we can reformulate the synthesis conditions to be linear in γ 2 as in , Problem (16). With this said, let γ min denote the minimum γ , up to a certain tolerance, that is achievable by a ( 45,120)‐eventually periodic synthesis.…”
Section: Example: Distributed Control Of Hovercraftsmentioning
confidence: 99%
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