2022
DOI: 10.1016/j.jsv.2021.116673
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Non-stationary oscillation of a string on the Winkler foundation subjected to a discrete mass–spring system non-uniformly moving at a sub-critical speed

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Cited by 4 publications
(38 citation statements)
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“…If the instantaneous value of the vector of the zeroth order system parameters (2.30) at ξ = 0 leaves the localization domain, then we expect very fast vanishing of the displacements U(t). In a particular case, this was demonstrated numerically in [19]. Later, we have shown that at least for ǫ = 0 the displacement U(t) in the composite system vanishes asymptotically faster than in the corresponding pure continuum system.…”
Section: Remark 23mentioning
confidence: 54%
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“…If the instantaneous value of the vector of the zeroth order system parameters (2.30) at ξ = 0 leaves the localization domain, then we expect very fast vanishing of the displacements U(t). In a particular case, this was demonstrated numerically in [19]. Later, we have shown that at least for ǫ = 0 the displacement U(t) in the composite system vanishes asymptotically faster than in the corresponding pure continuum system.…”
Section: Remark 23mentioning
confidence: 54%
“…This formula cannot be obtained as a particular case of general formulae (5.6), (5.7). The results given by the correct formula derived later in [19], see also Sect. 6.5, are very close to ones given by (6.6) and differ considerably only for large enough mass M (see Sect.…”
Section: A Non-uniformly Moving Inertial Loadmentioning
confidence: 71%
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