2013
DOI: 10.1016/j.jsv.2013.02.024
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Shock transmission in a coupled beam system

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Cited by 17 publications
(6 citation statements)
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“…In the case of periodic structures, the perfect symmetry yields repeated eigenvalues, for example k 1 ¼ k 2 . However, in the presence of parametric uncertainties the symmetry is broken and the repeating eigenvalues are split into distinct values [30][31][32]. This change in the eigenvector, due to some variation of the mass and stiffness matrices in the system, is what has to be quantified.…”
Section: Background Of Mode Veeringmentioning
confidence: 99%
“…In the case of periodic structures, the perfect symmetry yields repeated eigenvalues, for example k 1 ¼ k 2 . However, in the presence of parametric uncertainties the symmetry is broken and the repeating eigenvalues are split into distinct values [30][31][32]. This change in the eigenvector, due to some variation of the mass and stiffness matrices in the system, is what has to be quantified.…”
Section: Background Of Mode Veeringmentioning
confidence: 99%
“…, where in the presence of parametric uncertainties the symmetry is broken and the repeating eigenvalues are split into distinct values [8][9][10]. Examining the derivative of the eigenvector expressed by [11] can provide an insight into the curve veering phenomena…”
Section: Background Of Mode Veeringmentioning
confidence: 99%
“…Dynamic characteristics (stiffness and damping matrices) can provide insights into the fatigue life of the structure. The stiffened structure was modeled as a coupled system comprising of two subsystems along with a coupling element [27,28,42,43]. For an assembly of welding joints having the same dimension, the joint parameters could be different for each case due to uncertainties.…”
Section: Introductionmentioning
confidence: 99%