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High energy solutions of general Kirchhoff type equations without the Ambrosetti-Rabinowitz type condition 不含Ambrosetti-Rabinowitz型条件的一般Kirchhoff型方程的高能解
IF 4.2 1区 数学 Q1 Mathematics Pub Date : 2023-01-01 DOI: 10.1515/anona-2022-0311
Jian Zhang, Hui Liu, J. Zuo
Abstract In this article, we study the following general Kirchhoff type equation: − M ∫ R 3 ∣ ∇ u ∣ 2 d x Δ u + u = a ( x ) f ( u ) in R 3 , -Mleft(mathop{int }limits_{{{mathbb{R}}}^{3}}| nabla u{| }^{2}{rm{d}}xright)Delta u+u=aleft(x)fleft(u)hspace{1em}{rm{in}}hspace{0.33em}{{mathbb{R}}}^{3}, where inf R + M > 0 {inf }_{{{mathbb{R}}}^{+}}Mgt 0 and f f is a superlinear subcritical term. By using the Pohozǎev manifold, we obtain the existence of high energy solutions of the aforementioned equation without the well-known Ambrosetti-Rabinowitz type condition.
摘要在这篇文章中,我们研究了以下一般的Kirchhoff型方程:在R3中,−MŞR 3ŞõuŞ2 d xΔu+u=a(x)f(u),-Mleft(mathop{int}limits_{{mathbb{R}}}^{3}}|nabla u{|}^{2}{rm{d}}xright)Delta u+u=aleft R}}}^{3},其中inf R+M>0{inf}_{{mathbb{R}}}^{+}Mgt 0并且f是超线性次临界项。利用Pohozлev流形,在不存在Ambrosetti-Rabinowitz型条件的情况下,我们得到了上述方程的高能解的存在性。
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引用次数: 4
Positive solutions for a class of singular (p, q)-equations 一类奇异(p, q)方程的正解
IF 4.2 1区 数学 Q1 Mathematics Pub Date : 2023-01-01 DOI: 10.1515/anona-2022-0300
S. Leonardi, Nikolaos S. Papageorgiou
Abstract We consider a nonlinear singular Dirichlet problem driven by the ( p , q ) left(p,q) -Laplacian and a reaction where the singular term u − η {u}^{-eta } is multiplied by a strictly positive Carathéodory function f ( z , u ) fleft(z,u) . By using a topological approach, based on the Leray-Schauder alternative principle, we show the existence of a smooth positive solution.
摘要考虑由(p,q) 左(p,q) -拉普拉斯算子驱动的非线性奇异Dirichlet问题,以及奇异项u−η {u}^{-eta}乘以严格正的carathacemoory函数f (z,u) f左(z,u)的反应。利用拓扑方法,基于Leray-Schauder交替原理,证明了光滑正解的存在性。
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引用次数: 1
Dynamical analysis of a reaction–diffusion mosquito-borne model in a spatially heterogeneous environment 空间异质环境下反应-扩散蚊媒模式的动力学分析
IF 4.2 1区 数学 Q1 Mathematics Pub Date : 2023-01-01 DOI: 10.1515/anona-2022-0295
Jinliang Wang, W. Wu, Chunyang Li
Abstract In this article, we formulate and perform a strict analysis of a reaction–diffusion mosquito-borne disease model with total human populations stabilizing at H(x) in a spatially heterogeneous environment. By utilizing some fundamental theories of the dynamical system, we establish the threshold-type results of the model relying on the basic reproduction number. Specifically, we explore the mutual impacts of the spatial heterogeneity and diffusion coefficients on the basic reproduction number and investigate the existence, uniqueness, and global attractivity of the nontrivial steady state by utilizing the arguments of asymptotically autonomous semiflows. For the case that all parameters are independent of space, the global attractivity of the nontrivial steady state is achieved by the Lyapunov function.
摘要在本文中,我们建立了一个反应-扩散蚊媒疾病模型,并对其进行了严格的分析,该模型在空间异质环境中总人口稳定在H(x)。利用动力系统的一些基本理论,建立了基于基本再生数的模型的阈值型结果。具体而言,我们利用渐近自治半流的自变量,探讨了空间异质性和扩散系数对基本繁殖数的相互影响,并研究了非平凡稳态的存在性、唯一性和全局吸引性。对于所有参数都独立于空间的情况,通过李雅普诺夫函数实现了非平凡稳态的全局吸引性。
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引用次数: 1
Fujita-type theorems for a quasilinear parabolic differential inequality with weighted nonlocal source term 具有加权非局部源项的拟线性抛物型微分不等式的Fujita型定理
IF 4.2 1区 数学 Q1 Mathematics Pub Date : 2023-01-01 DOI: 10.1515/anona-2022-0303
Yuepeng Li, Z. Fang
Abstract This work is concerned with the nonexistence of nontrivial nonnegative weak solutions for a quasilinear parabolic differential inequality with weighted nonlocal source term in the whole space, which involves weighted polytropic filtration operator or generalized mean curvature operator. We establish the new critical Fujita exponents containing the first and second types. The key ingredient of the technique in proof is the test function method developed by Mitidieri and Pohozaev. No use of comparison and maximum principles or assumptions on symmetry or behavior at infinity of the solutions are required.
研究了一类带加权非局部源项的拟线性抛物型微分不等式在整个空间中非平凡非负弱解的不存在性,涉及加权多向滤波算子或广义平均曲率算子。建立了包含第一类和第二类的新的临界Fujita指数。证明技术的关键要素是米蒂耶里和波霍扎耶夫提出的测试函数法。不需要使用比较和极大值原理或对解的对称性或无穷远处的行为的假设。
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引用次数: 1
Uniform decay estimates for the semi-linear wave equation with locally distributed mixed-type damping via arbitrary local viscoelastic versus frictional dissipative effects 基于任意局部粘弹性与摩擦耗散效应的具有局部分布混合阻尼的半线性波动方程的一致衰减估计
IF 4.2 1区 数学 Q1 Mathematics Pub Date : 2023-01-01 DOI: 10.1515/anona-2022-0285
Kun‐Peng Jin, Li Wang
Abstract We are concerned with the stabilization of the wave equation with locally distributed mixed-type damping via arbitrary local viscoelastic and frictional effects. Here, one of the novelties is: the viscoelastic and frictional damping together effect only in a part of domain, not in entire domain, which is only assumed to meet the piecewise multiplier geometric condition that their summed interior and boundary measures can be arbitrarily small. Furthermore, there is no other additional restriction for the location of the viscoelastic-effect region. That is, it is dropped that the viscoelastic-effect region includes a part of the system boundary, which is the fundamental condition in almost all previous literature even if when two types of damping together cover the entire system domain. The other distinct novelty is: in this article we remove the fundamental condition that the derivative of the relaxation function is controlled by relaxation function itself, which is a necessity in the previous literature to obtain the optimal uniform decay rate. Under such weak conditions, we successfully establish a series of decay theorems, which generalize and extend essentially the previous related stability results for viscoelastic model regardless of local damping case, entire damping case and mixed-type damping case.
摘要研究了具有局部分布混合型阻尼的波动方程在任意局部粘弹性和摩擦作用下的镇定问题。这里的一个新颖之处在于:粘弹性和摩擦阻尼共同作用仅在局部区域,而不是整个区域,这只是假设满足分段乘子几何条件,即它们的内部和边界测度之和可以任意小。此外,粘弹性效应区域的位置没有其他附加限制。即忽略了粘弹性效应区域包含系统边界的一部分,这是以往几乎所有文献的基本条件,即使两种阻尼共同覆盖了整个系统域。另一个明显的新颖之处在于:在本文中,我们去掉了松弛函数的导数由松弛函数本身控制的基本条件,而这在以前的文献中是获得最优均匀衰减率的必要条件。在这种弱条件下,我们成功地建立了一系列衰减定理,这些定理在本质上推广和推广了粘弹性模型在局部阻尼情况、整体阻尼情况和混合阻尼情况下的稳定性相关结果。
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引用次数: 2
Singularity for a nonlinear degenerate hyperbolic-parabolic coupled system arising from nematic liquid crystals 由向列液晶产生的非线性退化双曲-抛物耦合系统的奇异性
IF 4.2 1区 数学 Q1 Mathematics Pub Date : 2022-11-19 DOI: 10.1515/anona-2022-0268
Yan-bo Hu
Abstract This article focuses on the singularity formation of smooth solutions for a one-dimensional nonlinear degenerate hyperbolic-parabolic coupled system originating from the Poiseuille flow of nematic liquid crystals. Without assuming that the wave speed of the hyperbolic equation is a positive function, we show that its smooth solution will break down in finite time even for an arbitrarily small initial energy. Based on an estimate of the solution for the heat equation, we use the method of characteristics to control the wave speed and its derivative so that the wave speed does not degenerate and its derivative does not change sign in a period of time.
摘要本文研究了由向列相液晶的Poiseuille流引起的一维非线性退化双曲-抛物耦合系统光滑解的奇异性形成。在不假设双曲方程的波速是正函数的情况下,我们证明了即使初始能量任意小,其光滑解也会在有限时间内崩溃。基于对热方程解的估计,我们使用特征法来控制波速及其导数,使波速在一段时间内不退化,导数不变号。
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引用次数: 1
On a strongly damped semilinear wave equation with time-varying source and singular dissipation 具有时变震源和奇异耗散的强阻尼半线性波动方程
IF 4.2 1区 数学 Q1 Mathematics Pub Date : 2022-11-18 DOI: 10.1515/anona-2022-0267
Yi Yang, Z. Fang
Abstract This paper deals with the global well-posedness and blow-up phenomena for a strongly damped semilinear wave equation with time-varying source and singular dissipative terms under the null Dirichlet boundary condition. On the basis of cut-off technique, multiplier method, contraction mapping principle, and the modified potential well method, we establish the local well-posedness and obtain the threshold between the existence and nonexistence of the global solution (including the critical case). Meanwhile, with the aid of modified differential inequality technique, the blow-up result of the solutions with arbitrarily positive initial energy and the lifespan of the blow-up solutions are derived.
摘要本文研究了具有时变源和奇异耗散项的强阻尼双线性波动方程在零Dirichlet边界条件下的全局适定性和爆破现象。在截断技术、乘法器方法、收缩映射原理和改进势阱方法的基础上,我们建立了局部适定性,并得到了全局解(包括临界情况)存在与不存在之间的阈值。同时,借助于改进的微分不等式技术,导出了具有任意正初始能量的解的爆破结果和爆破解的寿命。
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引用次数: 6
A global compactness result with applications to a Hardy-Sobolev critical elliptic system involving coupled perturbation terms 一个全局紧性结果及其在含耦合扰动项的Hardy-Sobolev临界椭圆系统中的应用
IF 4.2 1区 数学 Q1 Mathematics Pub Date : 2022-11-16 DOI: 10.1515/anona-2022-0276
Lu Shun Wang, T. Yang, Xiao Long Yang
Abstract In this article, we study a Hardy-Sobolev critical elliptic system involving coupled perturbation terms: (0.1) − Δ u + V 1 ( x ) u = η 1 η 1 + η 2 ∣ u ∣ η 1 − 2 u ∣ v ∣ η 2 ∣ x ′ ∣ + α α + β Q ( x ) ∣ u ∣ α − 2 u ∣ v ∣ β , − Δ v + V 2 ( x ) v = η 2 η 1 + η 2 ∣ v ∣ η 2 − 2 v ∣ u ∣ η 1 ∣ x ′ ∣ + β α + β Q ( x ) ∣ v ∣ β − 2 v ∣ u ∣ α , left{begin{array}{c}-Delta u+{V}_{1}left(x)u=frac{{eta }_{1}}{{eta }_{1}+{eta }_{2}}frac{{| u| }^{{eta }_{1}-2}u{| v| }^{{eta }_{2}}}{| x^{prime} | }+frac{alpha }{alpha +beta }Qleft(x)| u{| }^{alpha -2}u| v{| }^{beta }, -Delta v+{V}_{2}left(x)v=frac{{eta }_{2}}{{eta }_{1}+{eta }_{2}}frac{{| v| }^{{eta }_{2}-2}v{| u| }^{{eta }_{1}}}{| x^{prime} | }+frac{beta }{alpha +beta }Qleft(x){| v| }^{beta -2}v{| u| }^{alpha },end{array}right. where n ≥ 3 nge 3 , 2 ≤ m < n 2le mlt n , x ≔ ( x ′ , x ″ ) ∈ R m × R n − m x:= left(x^{prime} ,{x}^{^{primeprime} })in {{mathbb{R}}}^{m}times {{mathbb{R}}}^{n-m} , η 1 , η 2 > 1 {eta }_{1},{eta }_{2}gt 1 , and η 1 + η 2 = 2 ( n − 1 ) n − 2 {eta }_{1}+{eta }_{2}=frac{2left(n-1)}{n-2} , α , β > 1 alpha ,beta gt 1 and α + β < 2 n n − 2 alpha +beta lt frac{2n}{n-2} , and V 1 ( x ) , V 2 ( x ) , Q ( x ) ∈ C ( R n ) {V}_{1}left(x),{V}_{2}left(x),Qleft(x)in Cleft({{mathbb{R}}}^{n}) . Observing that (0.1) is doubly coupled, we first develop two efficient tools (i.e., a refined Sobolev inequality and a variant of the “Vanishing” lemma). On the previous tools, we will establish a global compactness result (i.e., a complete description for the Palais-Smale sequences of the corresponding energy functional) and some existence result for (0.1) via variational method. Our strategy turns out to be very concise because we avoid the use of Levy concentration functions and truncation techniques.
摘要本文研究了一个包含耦合扰动项的Hardy-Sobolev临界椭圆系统:(0.1)−Δu+V1,−Δv+V2(x)v=η2η1+η2ÜvÜη2−2 vÜuÜη1Üx′Ü+βα+βQ{c}-三角洲u+{V}_{1} left(x)u=frac{eta}_{1}}_{1}-2}u{|v|}^{eta}_{2}}{|x^{prime}|}+frac{alpha}+{V}_{2} left(x)v=frac{eta}_{2}}_{2}-2}v{|u|}^{{eta}_{1}}}{|x^{prime}|}+frac{beta}{alpha+beta{Qleft(x)。其中n≥3 nge 3,2≤m1{eta}_{1},{eta}_{2}gt 1,η1+η2=2(n−1)n−2{1}+{2}=frac{2left(n-1)}{n-2},α,β>1alpha,β1和α+β<2 n−2α+βltfrac{2n}{n-2},以及V1(x),V2(x)、Q(x)∈C(Rn){V}_{1} left(x),{V}_{2} left(x),Qleft(x)在Cleft中({mathbb{R}}{^{n})。观察到(0.1)是双耦合的,我们首先开发了两个有效的工具(即,一个精化的Sobolev不等式和一个“消失”引理的变体)。在前面的工具上,我们将通过变分方法建立一个全局紧性结果(即对相应能量泛函的Palais-Smale序列的完整描述)和(0.1)的一些存在性结果。我们的策略非常简洁,因为我们避免使用Levy集中函数和截断技术。
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引用次数: 0
Touchdown solutions in general MEMS models 通用MEMS模型的触地解决方案
IF 4.2 1区 数学 Q1 Mathematics Pub Date : 2022-10-30 DOI: 10.1515/anona-2023-0102
R. Clemente, J. Marcos do Ó, Esteban da Silva, E. Shamarova
Abstract We study general problems modeling electrostatic microelectromechanical systems devices (Pλ ) φ ( r , − u ′ ( r ) ) = λ ∫ 0 r f ( s ) g ( u ( s ) ) d s , r ∈ ( 0 , 1 ) , 0 < u ( r ) < 1 , r ∈ ( 0 , 1 ) , u ( 1 ) = 0 , left{begin{array}{ll}varphi (r,-u^{prime} left(r))=lambda underset{0}{overset{r}{displaystyle int }}frac{fleft(s)}{gleft(uleft(s))}{rm{d}}s,hspace{1.0em}& rin left(0,1), 0lt uleft(r)lt 1,hspace{1.0em}& rin left(0,1), uleft(1)=0,hspace{1.0em}end{array}right. where φ varphi , g g , and f f are some functions on [ 0 , 1 ] left[0,1] and λ > 0 lambda gt 0 is a parameter. We obtain results on the existence and regularity of a touchdown solution to ( P λ {P}_{lambda } ) and find upper and lower bounds on the respective pull-in voltage. In the particular case, when φ ( r , v ) = r α ∣ v ∣ β v varphi left(r,v)={r}^{alpha }{| v| }^{beta }v , i.e., when the associated differential equation involves the operator r − γ ( r α ∣ u ′ ∣ β u ′ ) ′ {r}^{-gamma }left({r}^{alpha }{| u^{prime} | }^{beta }u^{prime} )^{prime} , we obtain an exact asymptotic behavior of the touchdown solution in a neighborhood of the origin.
摘要研究静电微机电系统器件(Pλ) φ (r, - u ' (r)) = λ∫0 r f (s) g (u (s)) d s, r∈(0,1),0 < u (r) < 1 , r ∈ ( 0 , 1 ) , u ( 1 ) = 0 , left { begin{array}{ll}varphi (r,-u^{prime} left(r))=lambda underset{0}{overset{r}{displaystyle int }}frac{fleft(s)}{gleft(uleft(s))}{rm{d}}s,hspace{1.0em}& rin left(0,1), 0lt uleft(r)lt 1,hspace{1.0em}& rin left(0,1), uleft(1)=0,hspace{1.0em}end{array}right . where φ varphi , g g , and f f are some functions on [ 0 , 1 ] left[0,1] and λ >< 1, r∈(0,1),u (1) = 0, {。其中φ , g g, f f是[> 0 lambdagt 0是参数。我们得到了(P λ P_ {}{lambda)触地解的存在性和规律性},并和下界。在特殊情况下,当φ (r,v)=r α∣v∣β v varphileft (r{,}v)=r^ {alpha | v| ^ }{}{beta v,即当相关}微分{方程涉及算子r−γ (r α∣}u '{∣β u ') ' r^- gamma}left (r^ {}{alpha | u^ }{{prime} | ^ }{beta u^ }{prime})^ {prime}时,我们得到了在原点附近的触地解的精确渐近行为。
{"title":"Touchdown solutions in general MEMS models","authors":"R. Clemente, J. Marcos do Ó, Esteban da Silva, E. Shamarova","doi":"10.1515/anona-2023-0102","DOIUrl":"https://doi.org/10.1515/anona-2023-0102","url":null,"abstract":"Abstract We study general problems modeling electrostatic microelectromechanical systems devices (Pλ ) φ ( r , − u ′ ( r ) ) = λ ∫ 0 r f ( s ) g ( u ( s ) ) d s , r ∈ ( 0 , 1 ) , 0 < u ( r ) < 1 , r ∈ ( 0 , 1 ) , u ( 1 ) = 0 , left{begin{array}{ll}varphi (r,-u^{prime} left(r))=lambda underset{0}{overset{r}{displaystyle int }}frac{fleft(s)}{gleft(uleft(s))}{rm{d}}s,hspace{1.0em}& rin left(0,1), 0lt uleft(r)lt 1,hspace{1.0em}& rin left(0,1), uleft(1)=0,hspace{1.0em}end{array}right. where φ varphi , g g , and f f are some functions on [ 0 , 1 ] left[0,1] and λ > 0 lambda gt 0 is a parameter. We obtain results on the existence and regularity of a touchdown solution to ( P λ {P}_{lambda } ) and find upper and lower bounds on the respective pull-in voltage. In the particular case, when φ ( r , v ) = r α ∣ v ∣ β v varphi left(r,v)={r}^{alpha }{| v| }^{beta }v , i.e., when the associated differential equation involves the operator r − γ ( r α ∣ u ′ ∣ β u ′ ) ′ {r}^{-gamma }left({r}^{alpha }{| u^{prime} | }^{beta }u^{prime} )^{prime} , we obtain an exact asymptotic behavior of the touchdown solution in a neighborhood of the origin.","PeriodicalId":51301,"journal":{"name":"Advances in Nonlinear Analysis","volume":null,"pages":null},"PeriodicalIF":4.2,"publicationDate":"2022-10-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"48254089","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":1,"RegionCategory":"数学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 1
Nonstationary Poiseuille flow of a non-Newtonian fluid with the shear rate-dependent viscosity 具有剪切速率相关粘度的非牛顿流体的非平稳Poiseuille流
IF 4.2 1区 数学 Q1 Mathematics Pub Date : 2022-10-26 DOI: 10.1515/anona-2022-0259
G. Panasenko, K. Pileckas
Abstract A nonstationary Poiseuille flow of a non-Newtonian fluid with the shear rate dependent viscosity is considered. This problem is nonlinear and nonlocal in time and inverse to the nonlinear heat equation. The provided mathematical analysis includes the proof of the existence, uniqueness, regularity, and stability of the velocity and the pressure slope for a given flux carrier and of the exponential decay of the solution as the time variable goes to infinity for the exponentially decaying flux.
考虑黏度随剪切速率变化的非牛顿流体的非平稳泊泽维尔流。这个问题在时间上是非线性和非局部的,与非线性热方程相反。所提供的数学分析包括证明给定通量载体的速度和压力斜率的存在性、唯一性、规律性和稳定性,以及指数衰减通量随时间变量趋于无穷时解的指数衰减。
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引用次数: 1
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Advances in Nonlinear Analysis
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