2003
DOI: 10.1016/s0005-1098(03)00070-0
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A dual relation between port-Hamiltonian systems and the Brayton–Moser equations for nonlinear switched RLC circuits

Abstract: A dual relation between port-Hamiltonian systems and the Brayton-Moser equations for nonlinear switched RLC circuits Jeltsema, Dimitri; Scherpen, Jacquelien M.A. CopyrightOther than for strictly personal use, it is not permitted to download or to forward/distribute the text or part of it without the consent of the author(s) and/or copyright holder(s), unless the work is under an open content license (like Creative Commons).Take-down policy If you believe that this document breaches copyright please contact us… Show more

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Cited by 31 publications
(24 citation statements)
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“…so, by noting that J , h 11 and h 22 are skew symmetric, we verify thaṫ 15) which shows that the rate at which the stored energy increases equals the difference between the power delivered by the sources and the power dissipated by the resistors.…”
Section: Remark 22mentioning
confidence: 69%
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“…so, by noting that J , h 11 and h 22 are skew symmetric, we verify thaṫ 15) which shows that the rate at which the stored energy increases equals the difference between the power delivered by the sources and the power dissipated by the resistors.…”
Section: Remark 22mentioning
confidence: 69%
“…Note, however, that in the general nonlinear case, practical use of these procedures is impeded by the requirement of an explicit solution of (2.10). An alternative way to relax Assumption 2.3 is to enforce Kirchhoff's laws using the notion of port-Hamiltonian models with constraints [15].…”
Section: Remark 25mentioning
confidence: 99%
“…This property is of main importance in the following section. Other similarities and dualities between the BM equations and port-Hamiltonian systems can be found in [4]. …”
Section: A Non-switched Electrical Circuitsmentioning
confidence: 97%
“…Remark 1: In contrast to the Lagrangian or Hamiltonian functions, that are usually defined by the circuit's total (co-)energy, the mixed-potential consists of terms related to the power circulating in the circuit. However, it is easily seen that the circuit's total co-energy, denoted by , forms a fundamental part of the BM equations, e.g., [4], i.e., we may replace and in (1) by respectively. This property is of main importance in the following section.…”
Section: A Non-switched Electrical Circuitsmentioning
confidence: 99%
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