1986
DOI: 10.1002/sapm198675295
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Solitary‐Wave Interactions in Elastic Rods

Abstract: The propagation of longitudinal deformation waves in an elastic rod is modelled by the nonlinear partial differential equationwith p = 3 or 5. This equation is first derived under a range of possible constraints. We then show that this equation and even certain generaliza.ions do not pass the Painleve test, and hence are probably not completely integrable. Finally, we study the head-on collision of two equal solitary waves numerically and also asymptotically for small and large amplitude.

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Cited by 150 publications
(62 citation statements)
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“…The equations (1.1) and (1.2) also cover another various physical phenomena such as the dynamics of stretched string [30,9], Fermi-Pasta-Ulam problems [10], the evolution of long internal waves of moderate amplitude [1], nonlinear Alvén waves [27] and so on.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…The equations (1.1) and (1.2) also cover another various physical phenomena such as the dynamics of stretched string [30,9], Fermi-Pasta-Ulam problems [10], the evolution of long internal waves of moderate amplitude [1], nonlinear Alvén waves [27] and so on.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…For each fixed ε 0 > 0, equation (E ε 0 ) is a special form of the so-called improved Boussinesq equation (see [3,19,20,31]) with damped term −Δu t , which was used to describe ion-sound waves in plasma by Makhankov [20,21] and also known to represent other sorts of 'propagation problems' of, for example, lengthways waves in nonlinear elastic rods and ion-sonic waves of space transformations by a weak nonlinear effect (see [3,10]). …”
Section: Introductionmentioning
confidence: 99%
“…The equations that fall into this class are known to represent some sort of 'propagation problems' (see [4,6,22]; also [19] and the references therein), among which a specific problem is (1.3)…”
Section: Introductory Notesmentioning
confidence: 99%
“…Here −A : D(A) ⊂ X → X is the generator of an exponentially decaying analytic semigroup of bounded linear operators in X and X 1 is the domain of A with the graph norm. The equations that fall into this class are known to represent some sort of 'propagation problems' (see [4,6,22]; also [19] and the references therein), among which a specific problem is Key words and phrases. Evolution equations of the second order in time, existence, uniqueness and continuous dependence of solutions on initial conditions, asymptotic behavior of solutions, attractors, regularity, critical exponents.…”
mentioning
confidence: 99%