2015
DOI: 10.1098/rspa.2014.0402
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Damping-induced interplay between vibrations and waves in a forced non-dispersive elastic continuum with asymmetrically placed local attachments

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Cited by 14 publications
(3 citation statements)
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“…Recently, a nonresonant damped side branch has been used for spatial separation (localization) of acoustic traveling and standing waves in a duct with constant cross-sectional area (CSA), where the acoustic impedance of the side branch required to produce this localization is found analytically as a function of wavenumber and side-branch location. [1][2][3] In structural dynamics, spatial separation of traveling and standing waves has also been studied for a non-dispersive taut string with an attached spring-dashpot support and a vibration absorber, 4,5 a dispersive taut string on a partial viscoelastic foundation, 6 and an Euler-Bernoulli beam with one or two spring-dashpot supports. 7 The ducts, strings and beams stud-ied for localization of waves were all assumed to have constant geometries, as in the case of the duct 1,2 shown in Fig.…”
Section: Introductionmentioning
confidence: 99%
“…Recently, a nonresonant damped side branch has been used for spatial separation (localization) of acoustic traveling and standing waves in a duct with constant cross-sectional area (CSA), where the acoustic impedance of the side branch required to produce this localization is found analytically as a function of wavenumber and side-branch location. [1][2][3] In structural dynamics, spatial separation of traveling and standing waves has also been studied for a non-dispersive taut string with an attached spring-dashpot support and a vibration absorber, 4,5 a dispersive taut string on a partial viscoelastic foundation, 6 and an Euler-Bernoulli beam with one or two spring-dashpot supports. 7 The ducts, strings and beams stud-ied for localization of waves were all assumed to have constant geometries, as in the case of the duct 1,2 shown in Fig.…”
Section: Introductionmentioning
confidence: 99%
“…In particular, it can give rise to mode complexity, i. e., a non-trivial phase lag between the oscillations of different material points of a system [5,2]. Depending on the system parameters and the degree of asyncronicity of the oscillation, the dynamics may change completely from standing waves to a traveling waves [2,3]. It should be noted that non-unison vibrations can also occur in undamped nonlinear systems.…”
Section: Introductionmentioning
confidence: 99%
“…Non-classical damping, on the other hand, can generally lead to mode complexity; and if it is strong enough, it may even lead to a transition from standing to traveling waves, for example, as was recently shown for a locally damped linear string. 5,6 However, the extent of motion complexity is typically expected to remain small if damping is relatively weak. It should be noted that non-classical damping is quite common in many engineering applications: For instance, mechanical joints or attachments subject to dry friction may introduce a rather local dissipation source which leads to a highly non-classical damping distribution in the system.…”
Section: Introductionmentioning
confidence: 99%