2016
DOI: 10.1016/j.nonrwa.2016.01.009
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Singular solutions for a class of traveling wave equations arising in hydrodynamics

Abstract: We give an exhaustive characterization of singular weak solutions for some singular ordinary differential equations. Our motivation stems from the fact that in the context of hydrodynamics several prominent equations are reducible to an equation of this form upon passing to a moving frame. We construct peaked and cusped waves, fronts with finite-time decay and compact solitary waves. We prove that one cannot obtain peaked and compactly supported traveling waves for the same equation. In particular, a peaked t… Show more

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Cited by 9 publications
(8 citation statements)
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“…Furthermore, we obtain negative smooth as well as anti-peaked and anti-cusped solitary waves with compact support, that is, the wave profile attains a constant value outside a finite interval. For comparison notice that it was shown to be impossible for moderate amplitude models to have peaks with compact support in [21]. Finally let us assert that we also recover all known smooth and singular traveling wave solutions of CH type equations.…”
Section: 42mentioning
confidence: 53%
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“…Furthermore, we obtain negative smooth as well as anti-peaked and anti-cusped solitary waves with compact support, that is, the wave profile attains a constant value outside a finite interval. For comparison notice that it was shown to be impossible for moderate amplitude models to have peaks with compact support in [21]. Finally let us assert that we also recover all known smooth and singular traveling wave solutions of CH type equations.…”
Section: 42mentioning
confidence: 53%
“…[31]. Moreover, equation (1) admits peaked and cusped solutions with compact support, which was shown to be impossible for CH type equations in [21]. As we will see, the existence of such solutions requires the presence of third order terms exhibiting nonlinearities of at least cubic order in the evolution equation.…”
mentioning
confidence: 97%
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“…For a wellposedness result in the context of Besov spaces we refer the reader to [25], whereas a result on low regularity solutions with 1 < s ≤ 3/2 may be found in [22], and for global conservative solutions and continuation of solutions beyond wave breaking we point out [29]. The equation admits smooth as well as cusped and peaked solitary and periodic traveling wave solutions, and also solitary traveling waves with compact support [14,15,16]. Furthermore, the smooth solitary traveling wave solutions are known to be orbitally stable [10].…”
Section: Introductionmentioning
confidence: 99%
“…The equation admits smooth as well as cusped and peaked solitary and periodic traveling wave solutions, and also solitary traveling waves with compact support [14,15,16]. Furthermore, the smooth solitary traveling wave solutions are known to be orbitally stable [10].…”
Section: Introductionmentioning
confidence: 99%