“…(1) If J(φ) < 0, then we can easily get from the definitions of J and I in (12) and (13) respectively that I(φ) < 0. So we have φ ∈ W if J(φ) < 0.…”
Section: Notations and Main Resultsmentioning
confidence: 99%
“…The homogeneous problem, i.e. σ = 0, was studied in [3,4,5,7,9,10,13,15,16,21,24,25,26,27,28,29]. Especially, for the Cauchy problem (i.e.…”
Section: Introductionmentioning
confidence: 99%
“…In [28], Yang et al proved that for p > p c , there is a secondary critical exponent α c = 2/(p − 1) such that the solution blows up in finite time for u 0 behaving like |x| −α at |x| → ∞ if α = (0, α c ); and there are global solutions for for u 0 behaving like |x| −α at |x| → ∞ if α = (α c , n). For the zero Dirichlet boundary problem in a bounded domain Ω, in [13,25,26], the authors studied the properties of global existence and blow-up by potential well method (which was firstly introduced by Sattinger [19] and Payne and Sattinger [18], then developed by Liu and Zhao in [14]), and they showed the global existence, blowup and asymptotic behavior of solutions with initial energy at subcritical, critical and supercritical energy level. The results of [13,25,26] were extended by Luo [15] and Xu and Zhou [24] by studying the lifespan (i.e.…”
This paper deals with the global existence and blow-up of solutions to a inhomogeneous pseudo-parabolic equation with initial value u 0 in the Sobolev space H 1 0 (Ω), where Ω ⊂ R n (n ≥ 1 is an integer) is a bounded domain. By using the mountain-pass level d (see (14)), the energy functional J (see (12)) and Nehari function I (see (13)), we decompose the space H 1 0 (Ω) into five parts, and in each part, we show the solutions exist globally or blow up in finite time. Furthermore, we study the decay rates for the global solutions and lifespan (i.e., the upper bound of blow-up time) of the blow-up solutions. Moreover, we give a blow-up result which does not depend on d. By using this theorem, we prove the solution can blow up at arbitrary energy level, i.e. for any M ∈ R, there exists u 0 ∈ H 1 0 (Ω) satisfying J(u 0) = M such that the corresponding solution blows up in finite time.
“…(1) If J(φ) < 0, then we can easily get from the definitions of J and I in (12) and (13) respectively that I(φ) < 0. So we have φ ∈ W if J(φ) < 0.…”
Section: Notations and Main Resultsmentioning
confidence: 99%
“…The homogeneous problem, i.e. σ = 0, was studied in [3,4,5,7,9,10,13,15,16,21,24,25,26,27,28,29]. Especially, for the Cauchy problem (i.e.…”
Section: Introductionmentioning
confidence: 99%
“…In [28], Yang et al proved that for p > p c , there is a secondary critical exponent α c = 2/(p − 1) such that the solution blows up in finite time for u 0 behaving like |x| −α at |x| → ∞ if α = (0, α c ); and there are global solutions for for u 0 behaving like |x| −α at |x| → ∞ if α = (α c , n). For the zero Dirichlet boundary problem in a bounded domain Ω, in [13,25,26], the authors studied the properties of global existence and blow-up by potential well method (which was firstly introduced by Sattinger [19] and Payne and Sattinger [18], then developed by Liu and Zhao in [14]), and they showed the global existence, blowup and asymptotic behavior of solutions with initial energy at subcritical, critical and supercritical energy level. The results of [13,25,26] were extended by Luo [15] and Xu and Zhou [24] by studying the lifespan (i.e.…”
This paper deals with the global existence and blow-up of solutions to a inhomogeneous pseudo-parabolic equation with initial value u 0 in the Sobolev space H 1 0 (Ω), where Ω ⊂ R n (n ≥ 1 is an integer) is a bounded domain. By using the mountain-pass level d (see (14)), the energy functional J (see (12)) and Nehari function I (see (13)), we decompose the space H 1 0 (Ω) into five parts, and in each part, we show the solutions exist globally or blow up in finite time. Furthermore, we study the decay rates for the global solutions and lifespan (i.e., the upper bound of blow-up time) of the blow-up solutions. Moreover, we give a blow-up result which does not depend on d. By using this theorem, we prove the solution can blow up at arbitrary energy level, i.e. for any M ∈ R, there exists u 0 ∈ H 1 0 (Ω) satisfying J(u 0) = M such that the corresponding solution blows up in finite time.
We consider a coefficient identification problem for a mathematical model with free boundary related to ductal carcinoma in situ (DCIS). This inverse problem aims to determine the nutrient consumption rate from additional measurement data at a boundary point. We first obtain a global‐in‐time uniqueness of our inverse problem. Then based on the optimization method, we present a regularization algorithm to recover the nutrient consumption rate. Finally, our numerical experiment shows the effectiveness of the proposed numerical method.
“…A powerful technique for treating problem (1.2) is the so called "potential well method", which was established by Sattinger [22], Payne and Sattinger [21], and then improved by Liu and Zhao [17] by introducing a family of potential wells. Recently, there are some interesting results about the global existence and blow-up of solutions for problem (1.2) in [3], in which Chen and Tian proved global existence, blow-up at +∞, the behavior of vacuum isolation and asymptotic behavior of solutions with initial energy J(u 0 ) ≤ d. For other related works, we refer the readers to [2,11,6,15] and the references therein.…”
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