2011 IEEE International Symposium of Circuits and Systems (ISCAS) 2011
DOI: 10.1109/iscas.2011.5938164
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Nonsmooth dynamics of electrical systems

Abstract: In this paper we briefly review the current knowledge on the nonsmooth phenomena in power electronic systems. We describe a method of investigating the stability of nonsmooth limit cycles, and demonstrate its application in investigating the nonsmooth phenomena in the current mode controlled boost converter-which exhibits interesting bifurcations involving tori.

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Cited by 3 publications
(4 citation statements)
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“…In sliding, the tangential force is proportional to the normal force, ∥f t ∥= µ k ∥f n ∥, (66). In the constrained sticking mode, the force vector is calculated from Lagrange multipliers as in (65).…”
Section: G Slip-stick Frictionmentioning
confidence: 99%
“…In sliding, the tangential force is proportional to the normal force, ∥f t ∥= µ k ∥f n ∥, (66). In the constrained sticking mode, the force vector is calculated from Lagrange multipliers as in (65).…”
Section: G Slip-stick Frictionmentioning
confidence: 99%
“…This will force n to be non zero and hence change the slope of ℎ. In this case, the switching manifold will be modified as: ℎ (X, 𝑡) = 𝐾 0 + 𝐾 1 X (𝑡) − (1 + 𝑏) 𝑀 (𝑥 1 (𝑡)) − 𝑉 𝑝 = 0, (10) where…”
Section: Adding a Small Component To The Inductor Current Signalmentioning
confidence: 99%
“…The reason for choosing the spectral radius of the Monodromy matrix at 0.99 is to limit the transient overshoot resulting from higher values of the variable (𝑏) needed for a smaller value of the spectral radius. If the overshoot reaches a high enough value, it might hit the unstable boundary, and the response of the system will be saturated as described in [10,11]. The behavior of the system is very sensitive to the initial conditions.…”
Section: Adding a Small Component To The Inductor Current Signalmentioning
confidence: 99%
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