2004
DOI: 10.1134/1.1776219
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Localization of nonlinear waves in elastic bodies with inclusions

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Cited by 9 publications
(8 citation statements)
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“…At first, consider the simplest case p = v 0 δ(τ ) (p F = v 0 ) that corresponds to the initial conditions (9). To estimate asymptotically the integral in the righthand side of (27) for large times τ , we use the method of stationary phase [27,28].…”
Section: Inhomogeneous Non-stationary Problemmentioning
confidence: 99%
“…At first, consider the simplest case p = v 0 δ(τ ) (p F = v 0 ) that corresponds to the initial conditions (9). To estimate asymptotically the integral in the righthand side of (27) for large times τ , we use the method of stationary phase [27,28].…”
Section: Inhomogeneous Non-stationary Problemmentioning
confidence: 99%
“…We express Ψ ξ from (12) and substitute the result into Equation (10), having previously differentiated thereof for ξ. Neglecting the term εΨ ττ , we finally obtain…”
Section: The First Asymptoticsmentioning
confidence: 99%
“…The nonlinear fourth order equation is a resolving one for the main order of system ( 8)- (10), with respect to the small parameter ε. This equation can be called the generalized Boussinesq-Ostrovsky equation, since it contains dispersion terms specific to the usual and "improved" Boussinesq equation [17], as well as a linear term proportional to W, typical of the Ostrovsky equation [18][19][20][21].…”
Section: The First Asymptoticsmentioning
confidence: 99%
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“…This obviously relates to some facets of our problem. Note also that the phenomenon of trapped modes of oscillations also partake of the same class of dynamical phenomena (see, e.g., Indeitsev and Osipova [6]). …”
Section: Introductionmentioning
confidence: 98%