2014
DOI: 10.1063/1.4902272
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Global behavior of the solutions to Boussinesq type equation with linear restoring force

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Cited by 4 publications
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“…By means of the properties of these functionals, the proof of blow up result follows from Lemma (i). An application of this method is given in for Klein–Gordon equation and in for generalized Boussinesq equation. The second approach uses directly the blow up results of Lemma ; see for Klein–Gordon equation and for generalized Boussinesq equation.Remark For α = 0, Theorem (ii) coincides with the result in Lemma , and the corresponding upper bounds of the blow up time are one and the same, that is, t2=tSK.…”
Section: Resultsmentioning
confidence: 84%
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“…By means of the properties of these functionals, the proof of blow up result follows from Lemma (i). An application of this method is given in for Klein–Gordon equation and in for generalized Boussinesq equation. The second approach uses directly the blow up results of Lemma ; see for Klein–Gordon equation and for generalized Boussinesq equation.Remark For α = 0, Theorem (ii) coincides with the result in Lemma , and the corresponding upper bounds of the blow up time are one and the same, that is, t2=tSK.…”
Section: Resultsmentioning
confidence: 84%
“…Let us recall that in case of subcritical and critical initial energy (0 < E (0)≤ d ), the global behaviour of the weak solutions is fully characterized by means of the potential well method, for example, – for Klein–Gordon equation – and – for generalized Boussinesq equation – with combined power‐type and exponential‐type nonlinearities. Here, d is the depth of the potential well, defined in , while the initial energy E (0) is given by and , respectively.…”
Section: Introductionmentioning
confidence: 99%
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