2012
DOI: 10.1016/j.probengmech.2011.08.012
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Transient vibrational power flows in slender random structures: Theoretical modeling and numerical simulations

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Cited by 5 publications
(2 citation statements)
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“…The high-frequency limit ε → 0 in the previous setting shall be considered for quadratic observables of the wave displacement field u ε as explained now. We rely on the simple following example which was already discussed in [42,43]. The real function x → u ε (x) oscillating with an amplitude a(x) about its mean u(x):…”
Section: 3mentioning
confidence: 99%
“…The high-frequency limit ε → 0 in the previous setting shall be considered for quadratic observables of the wave displacement field u ε as explained now. We rely on the simple following example which was already discussed in [42,43]. The real function x → u ε (x) oscillating with an amplitude a(x) about its mean u(x):…”
Section: 3mentioning
confidence: 99%
“…However the theory of micro-local analysis of wave sytems shows that the energy density associated with their HF solutions satisfies radiative transfer equations [3]. In this model, heterogeneities are introduced along the same lines as done by Savin in [4]. Here they are modeled by fluctuations of the material properties of the medium represented by second order stochastic processes.…”
Section: Introductionmentioning
confidence: 99%