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Rogue waves in a reverse space nonlocal nonlinear Schrödinger equation 反向空间非局部非线性薛定谔方程中的乱流波
IF 2.7 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-08-05 DOI: 10.1016/j.physd.2024.134313

Rogue waves in a reverse space nonlocal nonlinear Schrödinger (NLS) equation with real and parity-symmetric nonlinearity-induced potential are considered. This equation has clear physical meanings since it can be derived from the Manakov system with a special reduction. The N-fold Darboux transformation and its generalized form for the nonlocal NLS equation are constructed. As an application, the multiparametric Nth-order rogue wave solution in terms of Schur polynomials for the nonlocal NLS equation with focusing case is derived by the limit technique. The significant differences of rogue wave dynamics between the nonlocal NLS equation and its usual (local) counterpart are illustrated through two types of specific rogue wave solutions. Unlike the eye-shaped (Peregrine type) rogue waves, the rogue wave doublets which involve an eye-shaped rogue wave and a dark/four-petaled rogue wave merging or separating with each other, and the rogue wave sextets that are characterized by the superpositions of three eye-shaped rogue waves and three dark/four-petaled rogue waves with fundamental, triangular and quadrilateral patterns are shown. Moreover, some wave characteristics including the difference between the light intensity and the plane-wave background, and the pulse energy of the rogue wave doublets are discussed.

研究考虑了反向空间非局域非线性薛定谔(NLS)方程中的流氓波,该方程具有实数和奇偶性对称的非线性诱导势。该方程具有明确的物理意义,因为它可以通过特殊的还原法从 Manakov 系统中导出。本文构建了非局部 NLS 方程的 N 折达布变换及其广义形式。作为应用,通过极限技术推导出了有聚焦情况下非局部 NLS 方程的舒尔多项式多参数 Nth 阶流氓波解。非局部 NLS 方程与通常(局部)NLS 方程的流氓波动力学之间的显著差异通过两类具体的流氓波求解得到了说明。与眼形(百灵鸟型)流氓波不同的是,流氓波双波涉及一个眼形流氓波和一个暗色/四瓣流氓波的相互合并或分离,而流氓波六波的特征是三个眼形流氓波和三个暗色/四瓣流氓波的叠加,具有基波、三角波和四边波的形态。此外,还讨论了一些波形特征,包括光强与平面波背景之间的差异,以及流氓波双联体的脉冲能量。
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引用次数: 0
Shear-imposed falling film on a vertical moving plate with disrupted time-reversal 垂直移动板上的剪切降膜,时间逆转紊乱
IF 2.7 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-08-03 DOI: 10.1016/j.physd.2024.134314

We propose a mathematical model to study the stability and dynamics of a shear-imposed thin film flow on a vertical moving plate, incorporating the influence of odd viscosity. This odd viscosity effect is vital in conventional fluids when there is a disruption in time-reversal symmetry. Our motivation to study the dynamics with odd viscosity arises from recent studies (Kirkinis & Andreev, vol. 878, 2019, pp. 169–189; Chattopadhyay & Ji, vol. 455, 2023, pp. 133883) where the odd viscosity effectively reduces flow instabilities under different scenarios. Utilizing a long wave perturbation method, we derive a nonlinear evolution equation at the liquid–air interface, which is influenced by the motion of the vertical plate, imposed shear, odd viscosity, and inertia. We first perform a linear stability analysis of the model to get firsthand information on various flow parameters. Three distinct conditions for the vertical plate, quiescent, upward-moving, and downward-moving, are considered, accounting the imposed shear and odd viscosity. Additionally, employing the method of multiple scales, we conduct a weakly nonlinear stability analysis for the traveling wave solution of the evolution equation and explore its bifurcation analysis. The bifurcation analysis reveals the existence of subcritical unstable and supercritical stable zones for crucial flow parameters: odd viscosity, imposed shear, and motion of the vertical plate. Both linear and weakly nonlinear stability analyses demonstrate that the destabilizing effect induced by the upward motion of the vertical plate can be alleviated by applying uphill shear, while the destabilizing effect of downhill shear can be mitigated when the vertical plate is in a downward motion. Moreover, we define an eigenvalue problem that mirrors the Orr–Sommerfeld (OS) model for analyzing normal modes and identifying the critical Reynolds number. We investigate the dynamics of surface waves through numerical solutions of the OS eigenvalue problem using the Chebyshev spectral collocation method. We observe the consistent enhancement of stabilization in the presence of odd viscosity. In the low to moderate Reynolds number range, vertical plate motion and odd viscosity show similar behavior in OS analysis, while imposed shear exhibits distinct changes. The Benney-type model does not agree with the OS problem when the Reynolds number is moderate with or without the three key parameters: vertical plate motion, imposed shear, and odd viscosity. However, when the Reynolds number is low with or without the three key parameters: vertical plate motion, imposed shear, and odd viscosity, the Benney-type model agrees with the OS. Further, numerical simulations of the evolution equation corroborate the results obtained from linear stability, weakly nonlinear stability, and OS analyses. Finally, the Hopf bifurcation analysis of the fixed point reveals that the wave speed is influenced by both the motion of the plate and

我们提出了一个数学模型来研究垂直运动板上的剪切薄膜流的稳定性和动力学,其中包含奇异粘度的影响。当时间反向对称性被破坏时,奇数粘度效应在传统流体中至关重要。我们研究奇数粘度动力学的动机来自近期的研究(Kirkinis & Andreev,vol. 878,2019,pp. 169-189;Chattopadhyay & Ji,vol. 455,2023,pp. 133883),在这些研究中,奇数粘度有效地降低了不同情况下的流动不稳定性。利用长波扰动法,我们推导出了液气界面的非线性演化方程,该方程受到竖板运动、外加剪切力、奇异粘度和惯性的影响。我们首先对模型进行了线性稳定性分析,以获得各种流动参数的第一手信息。考虑到外加剪切力和奇异粘度,我们对垂直板的静止、向上运动和向下运动三种不同情况进行了分析。此外,我们采用多尺度方法,对演化方程的行波解进行了弱非线性稳定性分析,并探讨了其分岔分析。分岔分析表明,在奇数粘度、外加剪切力和垂直板运动等关键流动参数下,存在亚临界不稳定区和超临界稳定区。线性和弱非线性稳定性分析表明,通过施加上坡剪切力,可减轻垂直板向上运动引起的失稳效应,而当垂直板向下运动时,可减轻下坡剪切力的失稳效应。此外,我们还定义了一个特征值问题,该问题反映了用于分析法向模式和确定临界雷诺数的奥尔-索默菲尔德(OS)模型。我们通过使用切比雪夫谱配位法对 OS 特征值问题进行数值求解,研究了表面波的动力学。我们观察到,在奇数粘度存在的情况下,稳定度持续增强。在中低雷诺数范围内,垂直板运动和奇数粘度在 OS 分析中表现出相似的行为,而外加剪切力则表现出明显的变化。当雷诺数为中等时,无论是否有三个关键参数:垂直板运动、外加剪切力和奇异粘度,本尼型模型都与 OS 问题不一致。然而,当雷诺数较低时,无论是否有三个关键参数:垂直板块运动、外加剪切力和奇数粘度,本尼型模型都与 OS 一致。此外,演化方程的数值模拟证实了线性稳定性、弱非线性稳定性和 OS 分析的结果。最后,对固定点的霍普夫分岔分析表明,波速受板块运动和外加剪切力的影响,而与奇数粘度无关。
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引用次数: 0
Pseudo grid-based physics-informed convolutional-recurrent network solving the integrable nonlinear lattice equations 基于伪网格的物理信息卷积递归网络求解可积分非线性网格方程
IF 2.7 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-07-30 DOI: 10.1016/j.physd.2024.134304

Traditional discrete learning methods involve discretizing continuous equations using difference schemes, necessitating considerations of stability and convergence. Integrable nonlinear lattice equations possess a profound mathematical structure that enables them to revert to continuous integrable equations in the continuous limit, particularly retaining integrable properties such as conservation laws, Hamiltonian structure, and multiple soliton solutions. The pseudo grid-based physics-informed convolutional-recurrent network (PG-PhyCRNet) is proposed to investigate the localized wave solutions of integrable lattice equations, which significantly enhances the model’s extrapolation capability to lattice points beyond the temporal domain. We conduct a comparative analysis of PG-PhyCRNet with and without pseudo grid by investigating the multi-soliton solutions and rational solitons of the Toda lattice and self-dual network equation. The results indicate that the PG-PhyCRNet excels in capturing long-term evolution and enhances the model’s extrapolation capability for solitons, particularly those with steep waveforms and high wave speeds. Finally, the robustness of the PG-PhyCRNet method and its effect on the prediction of solutions in different scenarios are confirmed through repeated experiments involving pseudo grid partitioning.

传统的离散学习方法涉及使用差分方案对连续方程进行离散化,因此必须考虑稳定性和收敛性。可积分非线性晶格方程具有深刻的数学结构,使其能够在连续极限中恢复为连续可积分方程,特别是保留了守恒定律、哈密顿结构和多重孤子解等可积分特性。我们提出了基于伪网格的物理信息卷积-并流网络(PG-PhyCRNet)来研究可积分晶格方程的局部波解,这大大增强了模型对时域以外晶格点的外推能力。我们通过研究户田晶格和自偶网络方程的多孤子解和有理孤子,对 PG-PhyCRNet 进行了有伪网格和无伪网格的对比分析。结果表明,PG-PhyCRNet 在捕捉长期演化方面表现出色,并增强了模型对孤子的外推能力,尤其是那些波形陡峭、波速较高的孤子。最后,PG-PhyCRNet 方法的稳健性及其对不同情况下预测解的影响通过涉及伪网格划分的反复实验得到了证实。
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引用次数: 0
Higher order mass aggregation terms in a nonlinear predator–prey model maintain limit cycle stability in Saturn’s F ring 非线性捕食者-猎物模型中的高阶质量聚集项维持土星 F 环的极限循环稳定性
IF 2.7 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-07-29 DOI: 10.1016/j.physd.2024.134311

We consider a generic higher order mass aggregation term for interactions between particles exhibiting oscillatory clumping and disaggregation behavior in the F ring of Saturn, using a novel predator–prey model that relates the mean mass aggregate (prey) and the square of the relative dispersion velocity (predator) of the interacting particles. The resulting cyclic dynamic behavior is demonstrated through time series plots, phase portraits and their stroboscopic phase maps.

Employing an eigenvalue stability analysis of the Jacobian of the system, we find out that there are two distinct regimes depending on the exponent and the amplitude of the higher order interactions of the nonlinear mass term. In particular, the system exhibits a limit cycle oscillatory stable behavior for a range of values of these parameters and a non-cyclic behavior for another range, separated by a curve across which phase transitions would occur between the two regimes. This shows that the observed clumping dynamics in Saturn’s F ring, corresponding to a limit cycle stability regime, can be systematically maintained in presence of physical higher order mass aggregation terms in the introduced model.

我们利用一个新颖的捕食者-猎物模型,考虑了土星 F 环中表现出振荡结块和分解行为的粒子之间相互作用的一般高阶质量聚集项,该模型将相互作用粒子的平均质量聚集(猎物)与相对分散速度(捕食者)的平方联系起来。通过时间序列图、相位图及其频闪相位图展示了由此产生的循环动态行为。
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引用次数: 0
Zero dissipation limit of the anisotropic Boussinesq equations with Navier-slip and Neumann boundary conditions 具有纳维-滑移和诺伊曼边界条件的各向异性布森斯克方程的零耗散极限
IF 2.7 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-07-25 DOI: 10.1016/j.physd.2024.134301

In this paper, we study the vanishing dissipation limit of the 2D anisotropic Boussinesq equations with the Navier-slip boundary condition for velocity field and the fixed flux boundary condition for temperature in the upper half plane. By constructing boundary layer correctors to compensate for the discrepancies between dissipative equations and non-dissipative equations at the boundary, we prove that the solutions of the anisotropic Boussinesq equations converge to the solutions of the non-dissipative Boussinesq equations in L2-norm. Particularly, we find that the anisotropic dissipation coefficients only affect the rate of convergence, which is different from the phenomenon of the Dirichlet problem of the anisotropic Boussinesq equations in Wang & Xu (2021).

本文研究了二维各向异性布森斯克方程的耗散消失极限,速度场采用纳维-滑移边界条件,温度在上半平面采用固定通量边界条件。通过构造边界层校正器来补偿耗散方程和非耗散方程在边界上的差异,我们证明了各向异性布辛斯方程的解在 L2 规范下收敛于非耗散布辛斯方程的解。特别是,我们发现各向异性耗散系数只影响收敛速度,这与 Wang & Xu (2021) 中各向异性 Boussinesq 方程的 Dirichlet 问题现象不同。
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引用次数: 0
Model reduction on manifolds: A differential geometric framework 流形上的模型还原:微分几何框架
IF 2.7 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-07-25 DOI: 10.1016/j.physd.2024.134299

Using nonlinear projections and preserving structure in model order reduction (MOR) are currently active research fields. In this paper, we provide a novel differential geometric framework for model reduction on smooth manifolds, which emphasizes the geometric nature of the objects involved. The crucial ingredient is the construction of an embedding for the low-dimensional submanifold and a compatible reduction map, for which we discuss several options. Our general framework allows capturing and generalizing several existing MOR techniques, such as structure preservation for Lagrangian- or Hamiltonian dynamics, and using nonlinear projections that are, for instance, relevant in transport-dominated problems. The joint abstraction can be used to derive shared theoretical properties for different methods, such as an exact reproduction result. To connect our framework to existing work in the field, we demonstrate that various techniques for data-driven construction of nonlinear projections can be included in our framework.

在模型缩减(MOR)中使用非线性投影和保留结构是当前活跃的研究领域。在本文中,我们为光滑流形上的模型还原提供了一个新颖的微分几何框架,它强调了相关对象的几何性质。其中的关键要素是构建低维子流形的嵌入和兼容的还原图,我们讨论了几种选择。我们的总体框架允许捕捉和概括现有的几种 MOR 技术,例如拉格朗日或哈密尔顿动力学的结构保持,以及使用非线性投影,例如与传输主导问题相关的非线性投影。联合抽象可用于推导不同方法的共享理论属性,如精确再现结果。为了将我们的框架与该领域的现有工作联系起来,我们证明了我们的框架可以包含各种数据驱动的非线性投影构建技术。
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引用次数: 0
Thermodynamically consistent Cahn–Hilliard–Navier–Stokes equations using the metriplectic dynamics formalism 使用元三体动力学形式主义的热力学一致的卡恩-希利亚德-纳维尔-斯托克斯方程
IF 2.7 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-07-24 DOI: 10.1016/j.physd.2024.134303

Cahn–Hilliard–Navier–Stokes (CHNS) systems describe flows with two-phases, e.g., a liquid with bubbles. Obtaining constitutive relations for general dissipative processes for such systems, which are thermodynamically consistent, can be a challenge. We show how the metriplectic 4-bracket formalism (Morrison and Updike, 2024) achieves this in a straightforward, in fact algorithmic, manner. First, from the noncanonical Hamiltonian formulation for the ideal part of a CHNS system we obtain an appropriate Casimir to serve as the entropy in the metriplectic formalism that describes the dissipation (e.g. viscosity, heat conductivity and diffusion effects). General thermodynamics with the concentration variable and its thermodynamics conjugate, the chemical potential, are included. Having expressions for the Hamiltonian (energy), entropy, and Poisson bracket, we describe a procedure for obtaining a metriplectic 4-bracket that describes thermodynamically consistent dissipative effects. The 4-bracket formalism leads naturally to a general CHNS system that allows for anisotropic surface energy effects. This general CHNS system reduces to cases in the literature, to which we can compare.

卡恩-希利亚德-纳维尔-斯托克斯(Cahn-Hilliard-Navier-Stokes,CHNS)系统描述的是两相流动,如带有气泡的液体。为这种系统获取热力学上一致的一般耗散过程的构成关系是一项挑战。我们展示了元三偏 4-bracket形式主义(莫里森和厄普代克,2024 年)如何以一种简单明了、实际上是算法化的方式实现这一目标。首先,从 CHNS 系统理想部分的非规范哈密顿公式中,我们得到了一个适当的卡西米尔(Casimir),作为描述耗散(如粘度、热传导和扩散效应)的元三偏形式主义中的熵。一般热力学包括浓度变量及其热力学共轭物--化学势。有了哈密顿(能量)、熵和泊松括号的表达式,我们描述了获得元折中 4 个括号的过程,该 4 个括号描述了热力学上一致的耗散效应。4-括号形式自然引出了允许各向异性表面能效应的一般 CHNS 系统。这个一般 CHNS 系统可还原为文献中的案例,我们可以与之进行比较。
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引用次数: 0
The dynamics around the collinear points of the elliptic three-body problem: A normal form approach 椭圆三体问题碰撞点周围的动力学:正态方法
IF 2.7 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-07-23 DOI: 10.1016/j.physd.2024.134302

We study the dynamics of the collinear points in the planar, restricted three-body problem, assuming that the primaries move on an elliptic orbit around a common barycenter. The equations of motion can be conveniently written in a rotating–pulsating barycentric frame, taking the true anomaly as independent variable. We consider the Hamiltonian modeling this problem in the extended phase space and we implement a normal form to make a center manifold reduction. The normal form provides an approximate solution for the Cartesian coordinates, which allows us to construct several kinds of orbits, most notably planar and vertical Lyapunov orbits, and halo orbits. We compare the analytical results with a numerical simulation, which requires special care in the selection of the initial conditions.

我们研究了平面受限三体问题中碰撞点的动力学,假设原点在围绕共同原心的椭圆轨道上运动。以真实反常为自变量,运动方程可以方便地写入旋转脉动重心框架。我们考虑了在扩展相空间中模拟这一问题的哈密顿模型,并采用了一种正则表达式来进行中心流形还原。正则表达式提供了笛卡尔坐标的近似解,使我们能够构建几种轨道,尤其是平面和垂直 Lyapunov 轨道以及晕轨道。我们将分析结果与数值模拟进行了比较,数值模拟需要特别注意初始条件的选择。
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引用次数: 0
Conceptual climate modelling 概念气候建模
IF 2.7 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-07-23 DOI: 10.1016/j.physd.2024.134285

Modelling the climate is notoriously difficult and generally associated with high-dimensional general circulation models that may be quite unwieldy from the mathematical perspective. At the other end of the spectrum are seemingly simple conceptual models that focus on underlying mechanisms, such as the roles of different types of delayed feedback loops and/or switching phenomena for a specific climate phenomenon. This special issue is designed to highlight the usefulness of conceptual modelling in climate. It presents a number of conceptual climate models, discusses the mathematical techniques available for their analysis, and showcases how relevant insights can be gained from them, including informing more realistic modelling of the climate.

气候建模是出了名的难事,一般都与高维大气环流模型有关,从数学角度看可能相当笨重。另一端是看似简单的概念模型,侧重于潜在机制,如不同类型的延迟反馈回路和/或特定气候现象的转换现象的作用。本特刊旨在突出气候概念模型的实用性。它介绍了一些概念性气候模型,讨论了可用于分析这些模型的数学技术,并展示了如何从这些模型中获得相关见解,包括为更现实的气候建模提供信息。
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引用次数: 0
Consistent and conservative lattice Boltzmann method for axisymmetric multiphase electrohydrodynamic flows 轴对称多相电流体的一致和保守晶格玻尔兹曼法
IF 2.7 3区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-07-20 DOI: 10.1016/j.physd.2024.134294

In this work, we first develop a consistent and conservative mathematical model to study multiphase electrohydrodynamic (EHD) flows, including the reduction-consistent and conservative Allen-Cahn equation for the multiphase field, the Laplace equation for the electric potential, and the consistent and conservative Navier–Stokes equations for the flow field. Owing to the reduction-consistent property, the present model can be used to handle a set of M (1MN) EHD fluids in N-phase system. Then a two-relaxation-time lattice Boltzmann (LB) method is proposed for axisymmetric multiphase EHD flows, which can correctly recover the axisymmetric governing equations through the direct Taylor expansion analysis. To test the capacity of the LB method, the deformations of a single two-phase droplet and a ternary-phase compound droplet under a uniform electric field are considered. It is found that different from a single droplet with two deformation modes, the compound droplet has four deformation modes, and additionally, the effects of the electric strength, the conductivity ratio and the permittivity ratio on the compound droplet are also investigated. Finally, the compound droplet in the quaternary-phase system is also explored, and there are eight deformation modes that have not been reported in the available literature.

在这项工作中,我们首先建立了一个一致和保守的数学模型来研究多相电流体动力学(EHD)流动,包括多相场的还原一致和保守的 Allen-Cahn 方程、电动势的拉普拉斯方程以及流场的一致和保守的 Navier-Stokes 方程。由于还原一致的特性,本模型可用于处理()EHD 流体的-相系统。然后,针对轴对称多相 EHD 流体提出了一种双松弛时间晶格玻尔兹曼(LB)方法,该方法可以通过直接泰勒展开分析正确恢复轴对称控制方程。为了检验 LB 方法的能力,考虑了单个两相液滴和三相复合液滴在均匀电场下的变形。结果发现,与单一液滴的两种变形模式不同,复合液滴有四种变形模式,此外,还研究了电强度、电导比和介电比对复合液滴的影响。最后,还探讨了四相体系中的复合液滴,其中有八种变形模式是现有文献未曾报道过的。
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引用次数: 0
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