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Convergence analysis of the geometric thin-film equation 几何薄膜方程的收敛性分析
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-10-01 Epub Date: 2026-01-20 DOI: 10.1016/j.nonrwa.2026.104601
Lennon Ó Náraigh , Khang Ee Pang , Richard J. Smith
The Geometric Thin-Film Equation is a mathematical model of droplet spreading in the long-wave limit, which includes a regularization of the contact-line singularity. We show that the weak formulation of the problem, given initial Radon data, admits solutions that are globally defined for all time and are expressible as push-forwards of Borel measurable functions whose behaviour is governed by a set of ordinary differential equations (ODEs). The existence is first demonstrated in the special case of a finite weighted sum of delta functions whose centres evolve over time – these are known as ‘particle solutions’. In the general case, we construct a convergent sequence of particle solutions whose limit yields a solution of the above form. Moreover, we demonstrate that all weak solutions constructed in this way are 1/2-Hölder continuous in time and are uniquely determined by the initial conditions.
几何薄膜方程是液滴在长波极限下扩散的数学模型,它包含了接触线奇点的正则化。我们表明,在给定初始Radon数据的情况下,问题的弱公式承认在所有时间内全局定义的解决方案,并且可以表示为Borel可测量函数的前推,其行为由一组常微分方程(ode)控制。这种存在性首先在中心随时间演化的有限加权函数和的特殊情况下得到证明——这些函数被称为“粒子解”。在一般情况下,我们构造一个粒子解的收敛序列,其极限产生上述形式的解。此外,我们证明了用这种方法构造的所有弱解在时间上是1/2-Hölder连续的,并且是由初始条件唯一确定的。
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引用次数: 0
Limit cycles of discontinuous piecewise hybrid rigid systems separated by a straight line 以直线分隔的不连续分段混合刚性系统的极限环
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-10-01 Epub Date: 2026-01-31 DOI: 10.1016/j.nonrwa.2026.104607
Jaume Llibre , Angela C.T. Sánchez , Durval J. Tonon
A hybrid dynamical system is one whose behavior is governed by both continuous and discrete dynamics; that is, it exhibits both flows and jumps. The field of hybrid dynamical systems is relatively recent and encompasses a broad range of phenomena, and is often used to model various natural processes. In this paper, we investigate the maximum number of limit cycles that can arise in certain classes of discontinuous piecewise differential systems. These systems consist of two hybrid rigid subsystems separated by a straight line, where each rigid subsystem is composed of a linear center perturbed by a homogeneous polynomial of degree 2, 3, 4, 5 or 6. For these classes of piecewise systems, we address the extended 16th Hilbert problem.
混合动力系统是其行为同时受连续和离散动力控制的系统;也就是说,它既表现出流动,也表现出跳跃。混合动力系统领域是相对较新的,包含了广泛的现象,经常被用来模拟各种自然过程。本文研究了一类不连续分段微分系统中可能出现的最大极限环数。这些系统由两个以直线分隔的混合刚性子系统组成,其中每个刚性子系统由一个受2、3、4、5或6次齐次多项式扰动的线性中心组成。对于这类分段系统,我们讨论了扩展的16阶希尔伯特问题。
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引用次数: 0
Global existence of weak solutions to a quasilinear parabolic chemotaxis system 一类拟线性抛物型趋化系统弱解的整体存在性
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-10-01 Epub Date: 2026-01-27 DOI: 10.1016/j.nonrwa.2026.104606
Chun Wu
This paper deals with the following quasilinear chemotaxis system{ut=·(umuvv)+aubu2,(x,t)Ω×(0,),vt=Δvuv,(x,t)Ω×(0,)under the homogeneous Neumann boundary condition in ΩRn(n1) with smooth boundary ∂Ω, where the parameters a, b > 0 and m > 1. It is shown that there is at least one global weak solution for the system being discussed.
摘要下面的拟线性趋化性系统{ut =∇·(∇嗯−紫外线∇v) +非盟−bu2, (x, t)∈Ω×(0,∞),vt =Δv−紫外线,(x, t)∈Ω×(0,∞)齐次纽曼边界条件下Ω⊂Rn (n≥1)光滑边界∂Ω,在参数a, b 祝辞 0和m 祝辞 1。结果表明,所讨论的系统至少存在一个全局弱解。
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引用次数: 0
Modelling spatiotemporal prey-predator interactions incorporating fear effect and variable handling time 包含恐惧效应和可变处理时间的时空捕食者相互作用建模
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-10-01 Epub Date: 2025-12-30 DOI: 10.1016/j.nonrwa.2025.104582
Shri Harine P, Ankit Kumar
Classical prey-predator models often assume that the predator’s handling time is constant. However, in real ecosystems, a predator’s handling time can vary due to several biotic and abiotic factors. Based on this, we modified the Holling Type II functional response by incorporating a nonlinear handling time function. Fear in prey can lead to notable population reductions, predominantly through decreased foraging and reproduction. Considering these essential factors, we developed a prey-predator model encompassing temporal dynamics, self-diffusion and cross-diffusion. For the temporal model, we investigated the non-negativity, boundedness, and stability conditions of the existing steady states. Furthermore, bifurcations such as Hopf, transcritical, and Bautin were observed with respect to parameters like the cost of fear and the maximal achievable handling time. Bistability behaviour was observed through the analysis involving these two parameters. Sensitivity analysis was conducted to understand the influence of parameters contributing to the coexistence of prey and predator populations. Stability conditions for both spatiotemporal models (with self and cross-diffusion) were established, highlighting the role of cross-diffusion coefficients in inducing Turing instability and pattern formation. Spatial patterns such as spots and vertically aligned chains were observed. An increase in the maximal achievable handling time was found to support prey occupation in high-density regions, promoting coexistence, whereas excessively high maximal handling time can lead to predator extinction.
经典的捕食者-猎物模型通常假设捕食者的处理时间是恒定的。然而,在真实的生态系统中,掠食者的处理时间可能会因几种生物和非生物因素而变化。在此基础上,通过引入非线性处理时间函数对Holling II型函数响应进行了修正。对猎物的恐惧会导致显著的种群减少,主要是通过减少觅食和繁殖。考虑到这些重要因素,我们建立了一个包含时间动力学、自扩散和交叉扩散的捕食者-捕食者模型。对于时间模型,我们研究了现有稳态的非负性、有界性和稳定性条件。此外,在恐惧成本和最大可实现处理时间等参数方面,观察到Hopf、跨临界和Bautin等分岔。通过对这两个参数的分析,观察到双稳性行为。通过敏感性分析了解各参数对食饵种群和捕食者种群共存的影响。建立了两种时空模型(自扩散和交叉扩散)的稳定性条件,突出了交叉扩散系数在诱导图灵不稳定性和模式形成中的作用。观察到斑点和垂直排列的链等空间模式。在高密度区域,最大可达处理时间的增加有利于猎物的占领,促进共存,而过大的最大处理时间可能导致捕食者灭绝。
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引用次数: 0
The pointwise estimates for the incompressible Navier–Stokes–Maxwell system with Ohm’s law 用欧姆定律对不可压缩Navier-Stokes-Maxwell系统的逐点估计
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-10-01 Epub Date: 2025-12-25 DOI: 10.1016/j.nonrwa.2025.104572
Guanghui Wang , Mingying Zhong
The pointwise estimates of the Green’s function for the incompressible Navier–Stokes–Maxwell system with Ohm’s law in 3D are given in this paper. It is shown that the Green’s function consists of the heat kernels, the diffusive waves at low-frequency, the hyperbolic waves at high-frequency with time decaying exponentially, and the singular short waves. In addition, we establish the pointwise estimate of the global solution to the nonlinear incompressible Navier–Stokes–Maxwell system with Ohm’s law based on the Green’s function. To solve the new problem that the nonlinear terms contain the nonlocal operators divΔ1 and ××Δ1 which arise from the fluid-electromagnetic decomposition, we develop some new estimates of the nonlocal operators.
本文给出了三维中具有欧姆定律的不可压缩Navier-Stokes-Maxwell系统的Green函数的点态估计。结果表明,格林函数由热核、低频扩散波、高频随时间指数衰减的双曲波和奇异短波组成。此外,基于格林函数,利用欧姆定律建立了非线性不可压缩Navier-Stokes-Maxwell系统全局解的点估计。为了解决由流体电磁分解引起的非线性项包含非局部算子∇divΔ−1和∇×∇×Δ−1的新问题,我们提出了一些新的非局部算子估计。
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引用次数: 0
Existence and decay of solutions for Timoshenko-type equation with variable exponents and the supercritical damping 变指数和超临界阻尼timoshenko型方程解的存在性和衰减性
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-10-01 Epub Date: 2026-01-30 DOI: 10.1016/j.nonrwa.2026.104611
Rongrong Yan , Bin Guo , Xiangyu Zhu
In this paper, we consider an initial boundary value problem for the following Timoshenko equation with variable exponents:utt+Δ2uM(u2)Δu+|ut|m(x)2ut=|u|q(x)2u.
First of all, we combine the truncation method, energy estimate method and Banach fixed point theorem as well as Galerkin method to prove the existence of local solutions with the exponent q(x) satisfying 2(n2)n4<q(x)<2nn4. Subsequently, for the supercritical case(m(x)>2nn4), owing to the failure of the embedding inequality, the well-known multiplier technique is unsuccessful in our problem. To end this, our strategy is to give a priori estimate for the weighted integral Ω(2+t)1m(x)|u|m(x)dx, and then to apply modified weighted multiplier method and potential well method to prove that the energy functional decays logarithmically under this condition. In particular, these results reveal the explicit relationship between decay rate of solutions and the weak damping term. These results improved and extended the existing results [1, 2].
本文考虑了下述变指数Timoshenko方程的初边值问题:utt+Δ2u−M(∥∇u∥2)Δu+| but | M(x)−2ut=|u|q(x)−2u。首先,结合截断法、能量估计法和Banach不动点定理以及Galerkin方法,证明了指数q(x)满足2(n−2)n−4<q(x)<;2nn−4的局部解的存在性。随后,对于超临界情况(m(x)>2nn−4),由于嵌入不等式的失效,众所周知的乘子技术在我们的问题中是不成功的。为此,我们的策略是对加权积分∫Ω(2+t)1−m(x)|u|m(x)dx进行先验估计,然后应用改进的加权乘数法和势阱法证明能量泛函在这种情况下呈对数衰减。特别地,这些结果揭示了解的衰减率与弱阻尼项之间的显式关系。这些结果是对已有结果的改进和扩展[1,2]。
{"title":"Existence and decay of solutions for Timoshenko-type equation with variable exponents and the supercritical damping","authors":"Rongrong Yan ,&nbsp;Bin Guo ,&nbsp;Xiangyu Zhu","doi":"10.1016/j.nonrwa.2026.104611","DOIUrl":"10.1016/j.nonrwa.2026.104611","url":null,"abstract":"<div><div>In this paper, we consider an initial boundary value problem for the following Timoshenko equation with variable exponents:<span><span><span><math><mrow><msub><mi>u</mi><mrow><mi>t</mi><mi>t</mi></mrow></msub><mo>+</mo><msup><mstyle><mi>Δ</mi></mstyle><mn>2</mn></msup><mspace></mspace><mi>u</mi><mo>−</mo><msup><mrow><mi>M</mi><mo>(</mo><mo>∥</mo><mi>∇</mi><mi>u</mi><mo>∥</mo></mrow><mn>2</mn></msup><mrow><mo>)</mo><mstyle><mi>Δ</mi></mstyle><mi>u</mi><mo>+</mo><mo>|</mo></mrow><msub><mi>u</mi><mi>t</mi></msub><msup><mrow><mo>|</mo></mrow><mrow><mi>m</mi><mo>(</mo><mi>x</mi><mo>)</mo><mo>−</mo><mn>2</mn></mrow></msup><msub><mi>u</mi><mi>t</mi></msub><mo>=</mo><msup><mrow><mo>|</mo><mi>u</mi><mo>|</mo></mrow><mrow><mi>q</mi><mo>(</mo><mi>x</mi><mo>)</mo><mo>−</mo><mn>2</mn></mrow></msup><mi>u</mi><mo>.</mo></mrow></math></span></span></span></div><div>First of all, we combine the truncation method, energy estimate method and Banach fixed point theorem as well as Galerkin method to prove the existence of local solutions with the exponent <em>q</em>(<em>x</em>) satisfying <span><math><mrow><mfrac><mrow><mn>2</mn><mo>(</mo><mi>n</mi><mo>−</mo><mn>2</mn><mo>)</mo></mrow><mrow><mi>n</mi><mo>−</mo><mn>4</mn></mrow></mfrac><mo>&lt;</mo><mi>q</mi><mrow><mo>(</mo><mi>x</mi><mo>)</mo></mrow><mo>&lt;</mo><mfrac><mrow><mn>2</mn><mi>n</mi></mrow><mrow><mi>n</mi><mo>−</mo><mn>4</mn></mrow></mfrac><mo>.</mo></mrow></math></span> Subsequently, for the supercritical case(<span><math><mrow><mi>m</mi><mrow><mo>(</mo><mi>x</mi><mo>)</mo></mrow><mo>&gt;</mo><mfrac><mrow><mn>2</mn><mi>n</mi></mrow><mrow><mi>n</mi><mo>−</mo><mn>4</mn></mrow></mfrac></mrow></math></span>), owing to the failure of the embedding inequality, the well-known multiplier technique is unsuccessful in our problem. To end this, our strategy is to give a priori estimate for the weighted integral <span><math><mstyle><mrow><msub><mo>∫</mo><mstyle><mi>Ω</mi></mstyle></msub><msup><mrow><mo>(</mo><mn>2</mn><mo>+</mo><mi>t</mi><mo>)</mo></mrow><mrow><mn>1</mn><mo>−</mo><mi>m</mi><mo>(</mo><mi>x</mi><mo>)</mo></mrow></msup><msup><mrow><mo>|</mo><mi>u</mi><mo>|</mo></mrow><mrow><mi>m</mi><mo>(</mo><mi>x</mi><mo>)</mo></mrow></msup><mrow><mi>d</mi></mrow><mi>x</mi></mrow></mstyle></math></span>, and then to apply modified weighted multiplier method and potential well method to prove that the energy functional decays logarithmically under this condition. In particular, these results reveal the explicit relationship between decay rate of solutions and the weak damping term. These results improved and extended the existing results [1, 2].</div></div>","PeriodicalId":49745,"journal":{"name":"Nonlinear Analysis-Real World Applications","volume":"91 ","pages":"Article 104611"},"PeriodicalIF":1.8,"publicationDate":"2026-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"146077474","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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: 0
Describing smooth small-data solutions to a quasilinear hyperbolic-parabolic system by W1,p energy analysis 用W1,p能量分析描述拟线性双曲抛物型系统的光滑小数据解
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-10-01 Epub Date: 2025-12-24 DOI: 10.1016/j.nonrwa.2025.104580
Leander Claes , Michael Winkler
<div><div>In bounded <em>n</em>-dimensional domains with <em>n</em> ≥ 1, this manuscript examines an initial-boundary value problem for the system<span><span><span><math><mtable><mtr><mtd><mrow><mo>{</mo><mtable><mtr><mtd><mrow><msub><mi>u</mi><mrow><mi>t</mi><mi>t</mi></mrow></msub><mo>=</mo><mi>∇</mi><mo>·</mo><mrow><mo>(</mo><mi>γ</mi><mrow><mo>(</mo><mstyle><mi>Θ</mi></mstyle><mo>)</mo></mrow><mi>∇</mi><msub><mi>u</mi><mi>t</mi></msub><mo>)</mo></mrow><mo>+</mo><mi>a</mi><mi>∇</mi><mo>·</mo><mrow><mo>(</mo><mi>γ</mi><mrow><mo>(</mo><mstyle><mi>Θ</mi></mstyle><mo>)</mo></mrow><mi>∇</mi><mi>u</mi><mo>)</mo></mrow><mo>+</mo><mi>∇</mi><mo>·</mo><mi>f</mi><mrow><mo>(</mo><mstyle><mi>Θ</mi></mstyle><mo>)</mo></mrow><mo>,</mo></mrow></mtd></mtr><mtr><mtd><mrow><msub><mstyle><mi>Θ</mi></mstyle><mi>t</mi></msub><mo>=</mo><mi>D</mi><mstyle><mi>Δ</mi></mstyle><mstyle><mi>Θ</mi></mstyle><mo>+</mo><mstyle><mi>Γ</mi></mstyle><mrow><mo>(</mo><mstyle><mi>Θ</mi></mstyle><mo>)</mo></mrow><msup><mrow><mo>|</mo><mi>∇</mi><msub><mi>u</mi><mi>t</mi></msub><mo>|</mo></mrow><mn>2</mn></msup><mo>+</mo><mi>F</mi><mrow><mo>(</mo><mstyle><mi>Θ</mi></mstyle><mo>)</mo></mrow><mo>·</mo><mi>∇</mi><msub><mi>u</mi><mi>t</mi></msub><mo>,</mo></mrow></mtd></mtr></mtable></mrow></mtd></mtr></mtable></math></span></span></span>which in the case <span><math><mrow><mi>n</mi><mo>=</mo><mn>1</mn></mrow></math></span> and with <em>γ</em> ≡ Γ as well as <em>f</em> ≡ <em>F</em> reduces to the classical model for the evolution of displacement and temperatures in thermoviscoelasticity. Unlike in previous related studies, the focus here is on situations in which besides <em>f</em> and <em>F</em>, also the core ingredients <em>γ</em> and Γ may depend on the temperature variable Θ. Firstly, a statement on local existence of classical solutions is derived for arbitrary <em>a</em> > 0, <em>D</em> > 0 as well as 0 < <em>γ</em> ∈ <em>C</em><sup>2</sup>([0, ∞)) and 0 ≤ Γ ∈ <em>C</em><sup>1</sup>([0, ∞)), for functions <span><math><mrow><mi>f</mi><mo>∈</mo><msup><mi>C</mi><mn>2</mn></msup><mrow><mo>(</mo><mrow><mo>[</mo><mn>0</mn><mo>,</mo><mi>∞</mi><mo>)</mo></mrow><mo>;</mo><msup><mi>R</mi><mi>n</mi></msup><mo>)</mo></mrow></mrow></math></span> and <span><math><mrow><mi>F</mi><mo>∈</mo><msup><mi>C</mi><mn>1</mn></msup><mrow><mo>(</mo><mrow><mo>[</mo><mn>0</mn><mo>,</mo><mi>∞</mi><mo>)</mo></mrow><mo>;</mo><msup><mi>R</mi><mi>n</mi></msup><mo>)</mo></mrow></mrow></math></span> with <span><math><mrow><mi>F</mi><mo>(</mo><mn>0</mn><mo>)</mo><mo>=</mo><mn>0</mn></mrow></math></span>, and for suitably regular initial data of arbitrary size. Secondly, it is seen that under an additional assumption on smallness of <em>a, f</em>′ and <em>F</em>, as well as on the deviation of the initial data from the constant state given by <span><math><mrow><mi>u</mi><mo>=</mo><mn>0</mn></mrow></math></span> and <span><math><mrow><mstyle><mi>Θ</mi></mstyle><mo>=</mo><msub><mstyle><mi>Θ</mi></mstyle><mi>★</mi>
在有界与n n维域 ≥ 1,这手稿检查系统的初边值问题{utt =∇·(γ(Θ)∇ut) +一个∇·(γ(Θ)∇u) +∇·f(Θ)Θt = DΔΘ+Γ(Θ)|∇ut | 2 + f(Θ)·∇ut,对于n = 1和γ ≡ Γ以及f ≡ f减少的经典模型的进化在thermoviscoelasticity位移和温度。与以往的相关研究不同,这里的重点是除了f和f之外,核心成分γ和Γ也可能取决于温度变量Θ的情况。首先,声明对当地古典解的存在性推导出任意一个 祝辞 0 D 祝辞 0 0 & lt; γ ∈ C2([0,∞))和0 ≤ Γ ∈ C1([0,∞)),函数f∈C2([0,∞);Rn), F∈C1([0,∞);Rn), F(0)=0,对于任意大小的适当规则初始数据。其次,我们可以看到,在附加假设a, f '和f的小性,以及初始数据与任意固定的Θ - ≥ 0给出的u=0和Θ=Θ★的恒定状态的偏差下,在凸域上,这些解在时间上实际上是全局的,并且具有∇ut,∇u和∇Θ在Lp中呈指数级快速衰减的性质。这是通过在Lp空间中检测涉及这些梯度范数的泛函的合适耗散性质来实现的。
{"title":"Describing smooth small-data solutions to a quasilinear hyperbolic-parabolic system by W1,p energy analysis","authors":"Leander Claes ,&nbsp;Michael Winkler","doi":"10.1016/j.nonrwa.2025.104580","DOIUrl":"10.1016/j.nonrwa.2025.104580","url":null,"abstract":"&lt;div&gt;&lt;div&gt;In bounded &lt;em&gt;n&lt;/em&gt;-dimensional domains with &lt;em&gt;n&lt;/em&gt; ≥ 1, this manuscript examines an initial-boundary value problem for the system&lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;mtable&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;mo&gt;{&lt;/mo&gt;&lt;mtable&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;∇&lt;/mi&gt;&lt;mo&gt;·&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;γ&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mstyle&gt;&lt;mi&gt;Θ&lt;/mi&gt;&lt;/mstyle&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mi&gt;∇&lt;/mi&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/msub&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;a&lt;/mi&gt;&lt;mi&gt;∇&lt;/mi&gt;&lt;mo&gt;·&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;γ&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mstyle&gt;&lt;mi&gt;Θ&lt;/mi&gt;&lt;/mstyle&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mi&gt;∇&lt;/mi&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;∇&lt;/mi&gt;&lt;mo&gt;·&lt;/mo&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mstyle&gt;&lt;mi&gt;Θ&lt;/mi&gt;&lt;/mstyle&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mrow&gt;&lt;msub&gt;&lt;mstyle&gt;&lt;mi&gt;Θ&lt;/mi&gt;&lt;/mstyle&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;D&lt;/mi&gt;&lt;mstyle&gt;&lt;mi&gt;Δ&lt;/mi&gt;&lt;/mstyle&gt;&lt;mstyle&gt;&lt;mi&gt;Θ&lt;/mi&gt;&lt;/mstyle&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mstyle&gt;&lt;mi&gt;Γ&lt;/mi&gt;&lt;/mstyle&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mstyle&gt;&lt;mi&gt;Θ&lt;/mi&gt;&lt;/mstyle&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;mi&gt;∇&lt;/mi&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/msub&gt;&lt;mo&gt;|&lt;/mo&gt;&lt;/mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msup&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;F&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mstyle&gt;&lt;mi&gt;Θ&lt;/mi&gt;&lt;/mstyle&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;·&lt;/mo&gt;&lt;mi&gt;∇&lt;/mi&gt;&lt;msub&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/msub&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;/mtable&gt;&lt;/mrow&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;/mtable&gt;&lt;/math&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;which in the case &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; and with &lt;em&gt;γ&lt;/em&gt; ≡ Γ as well as &lt;em&gt;f&lt;/em&gt; ≡ &lt;em&gt;F&lt;/em&gt; reduces to the classical model for the evolution of displacement and temperatures in thermoviscoelasticity. Unlike in previous related studies, the focus here is on situations in which besides &lt;em&gt;f&lt;/em&gt; and &lt;em&gt;F&lt;/em&gt;, also the core ingredients &lt;em&gt;γ&lt;/em&gt; and Γ may depend on the temperature variable Θ. Firstly, a statement on local existence of classical solutions is derived for arbitrary &lt;em&gt;a&lt;/em&gt; &gt; 0, &lt;em&gt;D&lt;/em&gt; &gt; 0 as well as 0 &lt; &lt;em&gt;γ&lt;/em&gt; ∈ &lt;em&gt;C&lt;/em&gt;&lt;sup&gt;2&lt;/sup&gt;([0, ∞)) and 0 ≤ Γ ∈ &lt;em&gt;C&lt;/em&gt;&lt;sup&gt;1&lt;/sup&gt;([0, ∞)), for functions &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;msup&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msup&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;[&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;∞&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;;&lt;/mo&gt;&lt;msup&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;F&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;msup&gt;&lt;mi&gt;C&lt;/mi&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/msup&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mrow&gt;&lt;mo&gt;[&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;∞&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;;&lt;/mo&gt;&lt;msup&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;mi&gt;n&lt;/mi&gt;&lt;/msup&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; with &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;F&lt;/mi&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt;, and for suitably regular initial data of arbitrary size. Secondly, it is seen that under an additional assumption on smallness of &lt;em&gt;a, f&lt;/em&gt;′ and &lt;em&gt;F&lt;/em&gt;, as well as on the deviation of the initial data from the constant state given by &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/math&gt;&lt;/span&gt; and &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mstyle&gt;&lt;mi&gt;Θ&lt;/mi&gt;&lt;/mstyle&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msub&gt;&lt;mstyle&gt;&lt;mi&gt;Θ&lt;/mi&gt;&lt;/mstyle&gt;&lt;mi&gt;★&lt;/mi&gt;","PeriodicalId":49745,"journal":{"name":"Nonlinear Analysis-Real World Applications","volume":"91 ","pages":"Article 104580"},"PeriodicalIF":1.8,"publicationDate":"2026-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145841569","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"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: 0
Mathematical analysis of a levitation model 悬浮模型的数学分析
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-10-01 Epub Date: 2025-12-23 DOI: 10.1016/j.nonrwa.2025.104573
Rafael Muñoz-Sola
The aim of this paper is to study a model of electromagnetic levitation for a metallic rigid body. The model is constituted by the transient linear model of eddy currents under the hypothesis of axisymmetry, written in terms of a magnetic potential vector, coupled with an ODE which governs the vertical motion of the body. The electromagnetic model is a parabolic-elliptic PDE which parabolicity region is the position occupied by the body, which changes with time. Besides, Lorentz force appears in the RHS of the ODE. Thus, the model exhibits a coupling of geometrical nature. We establish the existence and uniqueness of solution of the coupled problem and we study its maximally defined solution. In particular, we prove that a blow-up of the velocity of the body cannot happen. Our techniques involve: a reformulation of the coupled problem as a causal differential equation, an adaptation of the theory about this kind of equations and a result of locally Lipschitz dependence of the magnetic potential vector with respect to the velocity of the body.
本文的目的是研究金属刚体的电磁悬浮模型。该模型是在轴对称假设下涡流的瞬态线性模型,用磁势向量表示,加上控制物体垂直运动的ODE。电磁模型为抛物-椭圆偏微分方程,抛物区域为物体所占位置,抛物区域随时间变化。此外,洛伦兹力出现在ODE的RHS中。因此,该模型表现出几何性质的耦合。建立了该耦合问题解的存在唯一性,并研究了其最大定义解。特别地,我们证明了物体的速度不可能突然增大。我们的技术包括:耦合问题作为因果微分方程的重新表述,关于这类方程的理论的改编,以及磁势矢量相对于物体速度的局部利普希茨依赖的结果。
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引用次数: 0
An epidemic model for bovine rabies transmission by bats with spatial diffusion 具有空间扩散的蝙蝠传播牛狂犬病的流行模型
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-10-01 Epub Date: 2026-01-19 DOI: 10.1016/j.nonrwa.2026.104603
José Paulo Carvalho dos Santos , Evandro Monteiro , Nelson Henrique Teixeira Lemes , Ana Claudia Pereira
The focus of this research is an epidemic model that examines the spread of rabies in the bovine population, with the spatial diffusion in the bat population, which serves as the vector population. The study investigates both the well-posedness and qualitative behavior of equilibrium points. The paper establishes the well-posedness of the model through Semigroup theory of sectorial operators and existence results for abstract parabolic differential equations. The research also addresses the definition of the basic reproduction number, R0, which acts as a threshold index point using linearization theory for reaction-diffusion equations in the disease-free equilibrium point. Additionally, the global asymptotic stability is established through the use of a Lyapunov function and energy estimates.
本研究的重点是研究狂犬病在牛种群中的传播,以及作为媒介种群的蝙蝠种群的空间扩散的流行病模型。研究了平衡点的适定性和定性行为。本文利用扇形算子的半群理论和抽象抛物型微分方程的存在性结果,建立了该模型的适定性。研究还讨论了基本繁殖数R0的定义,R0作为无病平衡点反应扩散方程的线性化理论的阈值指标点。此外,利用Lyapunov函数和能量估计建立了系统的全局渐近稳定性。
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引用次数: 0
Effect of diffusion rates on a nonlocal SIS model with distinct dispersal kernels and logistic source 扩散速率对具有不同扩散核和逻辑源的非局部SIS模型的影响
IF 1.8 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2026-10-01 Epub Date: 2026-01-31 DOI: 10.1016/j.nonrwa.2026.104613
Boubakr Lamouri , Ahmed Boudaoui , Salih Djilali
We investigate a nonlocal SIS epidemic model that incorporates distinct mobility patterns for susceptible and infected individuals, together with a logistic growth. The model includes distinct nonlocal diffusion kernels, denoted by J1(x) and J2(x), which represent different mobility strategies of the susceptible and infected populations, respectively. This formulation enhances the biological realism of the model by allowing greater flexibility in the representation of individual movement behaviors. Consequently, it introduces additional mathematical challenges in the analysis while providing a more accurate modelling for studying the spatial spread of infectious diseases. We establish the well-posedness, positivity, and uniform boundedness of solutions, and prove the existence of a global attractor. The basic reproduction number R0 is derived, and persistence theory is used to show the existence of an endemic steady state when R0>1. We further analyze the asymptotic profiles of the endemic steady states under extreme diffusion limits, highlighting the impact of mobility on disease persistence.
我们研究了一个非本地SIS流行病模型,该模型结合了易感和感染个体的不同流动模式,以及逻辑增长。模型包含不同的非局部扩散核,分别用J1(x)和J2(x)表示,分别代表易感种群和感染种群的不同迁移策略。这个公式通过允许更大的灵活性来表示个体运动行为,从而增强了模型的生物真实感。因此,它在为研究传染病的空间传播提供更准确的模型的同时,在分析中引入了额外的数学挑战。我们建立了解的适定性、正性和一致有界性,并证明了全局吸引子的存在性。导出了基本繁殖数R0,并利用持续理论证明了在R0>;1时存在地方性稳态。我们进一步分析了极端扩散极限下地方性稳态的渐近分布,强调了流动性对疾病持久性的影响。
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引用次数: 0
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Nonlinear Analysis-Real World Applications
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