2018
DOI: 10.1016/j.jsv.2018.05.032
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Numerical and experimental study of a double physical pendulum with magnetic interaction

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Cited by 41 publications
(23 citation statements)
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“…Saeed and Kamel [43] gave an active magnetic bearing-based tuned controller to suppress lateral vibrations of a nonlinear Jeffcott rotor system. Wojna et al [44] gave the numerical and experimental study of a double physical pendulum with the magnetic interaction. Sun et al [45] investigated the nonlinear dynamic characteristics of the active magnetic bearing system based on the cell-mapping method with a case study.…”
Section: Introductionmentioning
confidence: 99%
“…Saeed and Kamel [43] gave an active magnetic bearing-based tuned controller to suppress lateral vibrations of a nonlinear Jeffcott rotor system. Wojna et al [44] gave the numerical and experimental study of a double physical pendulum with the magnetic interaction. Sun et al [45] investigated the nonlinear dynamic characteristics of the active magnetic bearing system based on the cell-mapping method with a case study.…”
Section: Introductionmentioning
confidence: 99%
“…This article extends our previous investigation 46,47 and includes a more detailed theoretical analysis and numerical investigation. It is organized in the following way.…”
Section: Introductionmentioning
confidence: 52%
“…Moreover, when k 1 0, k 2 0, k 1 p 1 − m 1 n 1 0, k 2 p 2 − m 2 n 2 0 are not held, (29) has an infinite number of solutions or no solutions, which leads to many periodic or no periodic solutions in the original system (6). For example, if k 1 0, k 2 0, k 1 p 1 − m 1 n 1 0, k 2 p 2 − m 2 n 2 = 0, (31) is equivalent to…”
Section: Periodic Solutionmentioning
confidence: 99%
“…When ϕ 11 u 2 − ϕ 21 u 1 0 or u 1 0 is true, Equation (37) has no solution. Hence, system (6) has no collision periodic solution. Note 1 Conditions (20) and (32) are sufficient and unnecessary conditions for system (6) with the first kind of collision periodic solution.…”
Section: Periodic Solutionmentioning
confidence: 99%
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