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Low rank approximation in the computation of first kind integral equations with TauToolbox 用 TauToolbox 计算第一类积分方程时的低级近似值
IF 2.2 2区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-07-04 DOI: 10.1016/j.apnum.2024.06.022
Paulo B. Vasconcelos , Laurence Grammont , Nilson J. Lima

Tau Toolbox is a mathematical library for the solution of integro-differential problems, based on the spectral Lanczos' Tau method. Over the past few years, a class within the library, called polynomial, has been developed for approximating functions by classical orthogonal polynomials and it is intended to be an easy-to-use yet efficient object-oriented framework.

In this work we discuss how this class has been designed to solve linear ill-posed problems and we provide a description of the available methods, Tikhonov regularization and truncated singular value expansion. For the solution of the Fredholm integral equation of the first kind, which is built from a low-rank approximation of the kernel followed by a numerical truncated singular value expansion, an error estimate is given.

Numerical experiments illustrate that this approach is capable of efficiently compute good approximations of linear discrete ill-posed problems, even facing perturbed available data function, with no programming effort. Several test problems are used to evaluate the performance and reliability of the solvers.

The final product of this paper is the numerical solution of a first-kind integral equation, which is constructed using only two inputs from the user: the kernel and the right-hand side.

Tau Toolbox 是一个基于 Lanczos'Tau 光谱法的数学库,用于求解积分微分问题。在过去几年中,该库中开发了一个名为 "多项式 "的类,用于用经典正交多项式逼近函数,该类旨在成为一个易于使用且高效的面向对象框架。对于第一类弗雷德霍姆积分方程的求解,我们给出了误差估计值,该误差估计值是由核的低阶近似值和数值截断奇异值展开建立的。本文的最终成果是对一元积分方程的数值求解,用户只需输入内核和右边两个参数即可构建该方程。
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引用次数: 0
Energetic spectral-element time marching methods for phase-field nonlinear gradient systems 相场非线性梯度系统的能量谱元时间行进方法
IF 2.2 2区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-06-27 DOI: 10.1016/j.apnum.2024.06.021
Shiqin Liu , Haijun Yu

We propose two efficient energetic spectral-element methods in time for marching nonlinear gradient systems with the phase-field Allen–Cahn equation as an example: one fully implicit nonlinear method and one semi-implicit linear method. Different from other spectral methods in time using spectral Petrov-Galerkin or weighted Galerkin approximations, the presented implicit method employs an energetic variational Galerkin form that can maintain the mass conservation and energy dissipation property of the continuous dynamical system. Another advantage of this method is its superconvergence. A high-order extrapolation is adopted for the nonlinear term to get the semi-implicit method. The semi-implicit method does not have superconvergence, but can be improved by a few Picard-like iterations to recover the superconvergence of the implicit method. Numerical experiments verify that the method using Legendre elements of degree three outperforms the 4th-order implicit-explicit backward differentiation formula and the 4th-order exponential time difference Runge-Kutta method, which were known to have best performances in solving phase-field equations. In addition to the standard Allen–Cahn equation, we also apply the method to a conservative Allen–Cahn equation, in which the conservation of discrete total mass is verified. The applications of the proposed methods are not limited to phase-field Allen–Cahn equations. They are suitable for solving general, large-scale nonlinear dynamical systems.

我们以相场 Allen-Cahn 方程为例,针对行进非线性梯度系统提出了两种高效的时间谱元方法:一种是全隐式非线性方法,另一种是半隐式线性方法。与其他使用频谱 Petrov-Galerkin 或加权 Galerkin 近似的时间频谱方法不同,本文介绍的隐式方法采用了一种能量变分 Galerkin 形式,可以保持连续动力系统的质量守恒和能量耗散特性。该方法的另一个优点是其超收敛性。对非线性项采用高阶外推法得到半隐式方法。半隐式方法不具有超收敛性,但可以通过几次类似皮卡尔迭代的改进来恢复隐式方法的超收敛性。数值实验证明,使用三阶 Legendre 元素的方法优于四阶隐式-显式反向微分公式和四阶指数时差 Runge-Kutta 方法,而这两种方法在求解相场方程时性能最佳。除了标准 Allen-Cahn 方程,我们还将该方法应用于保守 Allen-Cahn 方程,其中离散总质量守恒得到了验证。所提方法的应用不仅限于相场 Allen-Cahn 方程。它们适用于求解一般的大规模非线性动力学系统。
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引用次数: 0
An efficient hybrid conjugate gradient method with an adaptive strategy and applications in image restoration problems 具有自适应策略的高效混合共轭梯度法及其在图像复原问题中的应用
IF 2.2 2区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-06-26 DOI: 10.1016/j.apnum.2024.06.020
Zibo Chen , Hu Shao , Pengjie Liu , Guoxin Li , Xianglin Rong

In this study, we introduce a novel hybrid conjugate gradient method with an adaptive strategy called asHCG method. The asHCG method exhibits the following characteristics. (i) Its search direction guarantees sufficient descent property without dependence on any line search. (ii) It possesses strong convergence for the uniformly convex function using a weak Wolfe line search, and under the same line search, it achieves global convergence for the general function. (iii) Employing the Armijo line search, it provides an approximate guarantee for worst-case complexity for the uniformly convex function. The numerical results demonstrate promising and encouraging performances in both unconstrained optimization problems and image restoration problems.

在本研究中,我们介绍了一种新颖的混合共轭梯度法,该方法采用自适应策略,称为 asHCG 方法。asHCG 方法具有以下特点。(i) 其搜索方向保证了充分下降特性,而不依赖于任何线性搜索。(ii) 对均匀凸函数采用弱沃尔夫线性搜索,具有很强的收敛性;对一般函数采用相同的线性搜索,可实现全局收敛。(iii) 利用 Armijo 行搜索,它为均匀凸函数的最坏情况复杂度提供了近似保证。数值结果表明,该方法在无约束优化问题和图像复原问题上都有令人鼓舞的良好表现。
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引用次数: 0
An optimized algorithm for numerical solution of coupled Burgers equations 耦合布尔格斯方程数值解的优化算法
IF 2.2 2区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-06-26 DOI: 10.1016/j.apnum.2024.06.019
Anurag Kaur , V. Kanwar , Higinio Ramos

Investigation of the solutions of the coupled viscous Burgers system is crucial for realizing and understanding some physical phenomena in applied sciences. Particularly, Burgers equations are used in the modeling of fluid mechanics and nonlinear acoustics. In the present study, a modified meshless quadrature method based on radial basis functions is used to discretize the partial derivatives in the spatial variable. A technique to find the best value of the shape parameter is introduced. A high-resolution optimized hybrid block method is then used to solve the problem in the temporal variable. To validate the proposed method, several test problems are considered and the simulated results are compared with exact solutions and previous works. Moreover, a sensitivity analysis for parameter c is conducted, and the unconditional stability of the proposed algorithm has been validated.

研究耦合粘性布尔格斯系统的解对于实现和理解应用科学中的某些物理现象至关重要。特别是在流体力学和非线性声学建模中,布尔格斯方程被广泛应用。本研究采用基于径向基函数的修正无网格正交法来离散空间变量中的偏导数。研究还引入了一种寻找形状参数最佳值的技术。然后使用高分辨率优化混合分块法解决时间变量中的问题。为了验证所提出的方法,我们考虑了几个测试问题,并将模拟结果与精确解法和以前的工作进行了比较。此外,还对参数 c 进行了敏感性分析,并验证了所提算法的无条件稳定性。
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引用次数: 0
On the stability of θ-methods for DDEs and PDDEs 论 DDE 和 PDDE θ 方法的稳定性
IF 2.2 2区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-06-25 DOI: 10.1016/j.apnum.2024.06.018
Alejandro Rodríguez-Fernández , Jesús Martín-Vaquero

In this paper, the stability of θ-methods for delay differential equations is studied based on the test equation y(t)=Ay(t)+By(tτ), where τ is a constant delay and A is a positive definite matrix. It is mainly considered the case where the matrices A and B are not simultaneosly diagonalizable and the concept of field of values is used to prove a sufficient condition for unconditional stability of these methods and another condition which also guarantees their stability, but according to the step size. The results obtained are also simplified for the case where the matrices A and B are simultaneously diagonalizable and compared with other similar works for the general case. Several numerical examples in which the theory discussed here is applied to parabolic problems given by partial delay differential equations with a diffusion term and a delayed term are presented, too.

本文基于检验方程 y′(t)=-Ay(t)+By(t-τ)(其中 τ 为常数延迟,A 为正定矩阵)研究了延迟微分方程的 θ 方法的稳定性。主要考虑矩阵 A 和 B 不能同时对角化的情况,并利用值域概念证明了这些方法无条件稳定性的充分条件和另一个也能保证其稳定性的条件,但取决于步长。对于矩阵 A 和 B 同时可对角化的情况,所获得的结果也进行了简化,并与其他针对一般情况的类似著作进行了比较。此外,还介绍了几个数值示例,这些示例将本文讨论的理论应用于带有扩散项和延迟项的偏延迟微分方程给出的抛物问题。
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引用次数: 0
The sine and cosine diffusive representations for the Caputo fractional derivative 卡普托分数导数的正弦和余弦扩散表示法
IF 2.2 2区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-06-21 DOI: 10.1016/j.apnum.2024.06.017
Hassan Khosravian-Arab , Mehdi Dehghan

In recent years, various types of methods have been proposed to approximate the Caputo fractional derivative numerically. A common challenge of the methods is the non-local property of the Caputo fractional derivative which leads to the slow and memory consuming methods. Diffusive representation of fractional derivative is an efficient tool to overcome the mentioned challenge. This paper presents two new diffusive representations to approximate the Caputo fractional derivative of order 0<α<1. An error analysis of the newly presented methods together with some numerical examples is provided at the end.

近年来,人们提出了各种类型的卡普托分数导数数值近似方法。这些方法面临的一个共同挑战是卡普托分数导数的非局部特性,这导致了这些方法速度慢、内存消耗大。分数导数的扩散表示是克服上述难题的有效工具。本文提出了两种新的扩散表示法来近似阶数为 0<α<1 的卡普托分数导数,并在最后提供了新方法的误差分析和一些数值示例。
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引用次数: 0
Numerical threshold stability of a nonlinear age-structured reaction diffusion heroin transmission model 非线性年龄结构反应扩散海洛因传播模型的数值阈值稳定性
IF 2.2 2区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-06-19 DOI: 10.1016/j.apnum.2024.06.016
X. Liu , M. Zhang , Z.W. Yang

This paper deals with the numerical threshold stability of a nonlinear age-space structured heroin transmission model. A semi-discrete system is established by spatially domain discretization of the original nonlinear age-space structured model. A threshold value is proposed in stability analysis of the semi-discrete system and named as a numerical basic reproduction number. Besides the role it plays in numerical threshold stability analysis, the numerical basic reproduction number can preserve qualitative properties of the exact basic reproduction number and converge to the latter while stepsizes vanish. A fully discrete system is established via a time discretization of the semi-discrete system, in which an implicit-explicit technique is implemented to ensure the preservation of the biological meanings (such as positivity) without CFL restriction. Some numerical experiments are exhibited in the end to confirm the conclusions and explore the final state.

本文论述了非线性年龄-空间结构海洛因传播模型的数值阈值稳定性。通过对原始非线性年龄-空间结构模型进行空间域离散化,建立了一个半离散系统。在半离散系统的稳定性分析中提出了一个阈值,并将其命名为数值基本再现数。数值基本重现数除了在数值阈值稳定性分析中发挥作用外,还能保持精确基本重现数的定性特性,并在步长消失时收敛于精确基本重现数。通过对半离散系统进行时间离散化,建立了一个完全离散的系统,其中采用了隐式-显式技术,以确保在没有 CFL 限制的情况下保留生物学意义(如正性)。最后还展示了一些数值实验,以确认结论并探索最终状态。
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引用次数: 0
An efficient collocation technique based on operational matrix of fractional-order Lagrange polynomials for solving the space-time fractional-order partial differential equations 基于分数阶拉格朗日多项式运算矩阵的高效配位技术,用于求解时空分数阶偏微分方程
IF 2.2 2区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-06-19 DOI: 10.1016/j.apnum.2024.06.014
Saurabh Kumar , Vikas Gupta , Dia Zeidan

In this research, we propose a novel and fast computational technique for solving a class of space-time fractional-order linear and non-linear partial differential equations. Caputo-type fractional derivatives are considered. The proposed method is based on the operational and pseudo-operational matrices for the fractional-order Lagrange polynomials. To carry out the method, first, we find the integer and fractional-order operational and pseudo-operational matrix of integration. The collocation technique and obtained operational and pseudo-operational matrices are then used to generate a system of algebraic equations by reducing the given space-time fractional differential problem. The resultant algebraic system is then easily solved by Newton's iterative methods. The upper bound of the fractional-order operational matrix of integration is also provided, which confirms the convergence of fractional-order Lagrange polynomial's approximation. Finally, some numerical experiments are conducted to demonstrate the applicability and usefulness of the suggested numerical scheme.

在这项研究中,我们提出了一种新型快速计算技术,用于求解一类时空分数阶线性和非线性偏微分方程。我们考虑了卡普托类型的分数导数。提出的方法基于分数阶拉格朗日多项式的运算矩阵和伪运算矩阵。要实施该方法,首先要找到积分的整数阶和分数阶运算矩阵和伪运算矩阵。然后,利用配位技术和获得的运算矩阵和伪运算矩阵,通过还原给定的时空分数微分问题生成代数方程系统。由此产生的代数方程系可以用牛顿迭代法轻松求解。此外,还提供了分数阶积分运算矩阵的上界,证实了分数阶拉格朗日多项式近似的收敛性。最后,还进行了一些数值实验,以证明所建议的数值方案的适用性和实用性。
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引用次数: 0
A new class of quadrature rules for estimating the error in Gauss quadrature 用于估计高斯正交误差的一类新正交规则
IF 2.2 2区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-06-18 DOI: 10.1016/j.apnum.2024.06.011
Aleksandar V. Pejčev , Lothar Reichel , Miodrag M. Spalević , Stefan M. Spalević
<div><p>The need to evaluate Gauss quadrature rules arises in many applications in science and engineering. It often is important to be able to estimate the quadrature error when applying an <em>ℓ</em>-point Gauss rule, <span><math><msub><mrow><mi>G</mi></mrow><mrow><mi>ℓ</mi></mrow></msub><mo>(</mo><mi>f</mi><mo>)</mo></math></span>, where <em>f</em> is an integrand of interest. Such an estimate often is furnished by applying another quadrature rule, <span><math><msub><mrow><mi>Q</mi></mrow><mrow><mi>k</mi></mrow></msub><mo>(</mo><mi>f</mi><mo>)</mo></math></span>, with <span><math><mi>k</mi><mo>></mo><mi>ℓ</mi></math></span> nodes, and using the difference <span><math><msub><mrow><mi>Q</mi></mrow><mrow><mi>k</mi></mrow></msub><mo>(</mo><mi>f</mi><mo>)</mo><mo>−</mo><msub><mrow><mi>G</mi></mrow><mrow><mi>ℓ</mi></mrow></msub><mo>(</mo><mi>f</mi><mo>)</mo></math></span> or its magnitude as an estimate for the quadrature error in <span><math><msub><mrow><mi>G</mi></mrow><mrow><mi>ℓ</mi></mrow></msub><mo>(</mo><mi>f</mi><mo>)</mo></math></span> or its magnitude. The classical approach to estimate the error in <span><math><msub><mrow><mi>G</mi></mrow><mrow><mi>ℓ</mi></mrow></msub><mo>(</mo><mi>f</mi><mo>)</mo></math></span> is to let <span><math><msub><mrow><mi>Q</mi></mrow><mrow><mi>k</mi></mrow></msub><mo>(</mo><mi>f</mi><mo>)</mo></math></span>, with <span><math><mi>k</mi><mo>=</mo><mn>2</mn><mi>ℓ</mi><mo>+</mo><mn>1</mn></math></span>, be the Gauss-Kronrod quadrature rule associated with <span><math><msub><mrow><mi>G</mi></mrow><mrow><mi>ℓ</mi></mrow></msub><mo>(</mo><mi>f</mi><mo>)</mo></math></span>. However, it is well known that the Gauss-Kronrod rule associated with a Gauss rule <span><math><msub><mrow><mi>G</mi></mrow><mrow><mi>ℓ</mi></mrow></msub><mo>(</mo><mi>f</mi><mo>)</mo></math></span> might not exist for certain measures that determine the Gauss rule and for certain numbers of nodes. This prompted M. M. Spalević <span>[1]</span> to develop generalized averaged Gauss rules, <span><math><msub><mrow><mover><mrow><mi>G</mi></mrow><mrow><mo>ˆ</mo></mrow></mover></mrow><mrow><mn>2</mn><mi>ℓ</mi><mo>+</mo><mn>1</mn></mrow></msub></math></span>, with <span><math><mn>2</mn><mi>ℓ</mi><mo>+</mo><mn>1</mn></math></span> nodes for estimating the error in <span><math><msub><mrow><mi>G</mi></mrow><mrow><mi>ℓ</mi></mrow></msub><mo>(</mo><mi>f</mi><mo>)</mo></math></span>. Similarly as for <span><math><mo>(</mo><mn>2</mn><mi>ℓ</mi><mo>+</mo><mn>1</mn><mo>)</mo></math></span>-node Gauss-Kronrod rules, <em>ℓ</em> nodes of the rule <span><math><msub><mrow><mover><mrow><mi>G</mi></mrow><mrow><mo>ˆ</mo></mrow></mover></mrow><mrow><mn>2</mn><mi>ℓ</mi><mo>+</mo><mn>1</mn></mrow></msub></math></span> agree with the nodes of <span><math><msub><mrow><mi>G</mi></mrow><mrow><mi>ℓ</mi></mrow></msub></math></span>. However, generalized averaged Gauss rules are not internal for some measures. They therefore may not be applicable when the integrand only is define
在科学和工程学的许多应用中,都需要对高斯正交规则进行评估。在应用 ℓ 点高斯正交规则 Gℓ(f) 时,经常需要估计正交误差。这种估计通常是通过应用另一个具有 k>ℓ 节点的正交规则 Qk(f),并使用 Qk(f)-Gℓ(f) 的差值或其大小来估计 Gℓ(f) 的正交误差或其大小。估算 Gℓ(f) 中误差的经典方法是让 Qk(f) (k=2ℓ+1)成为与 Gℓ(f) 相关的高斯-克罗洛德正交规则。然而,众所周知,与高斯定则 Gℓ(f) 相关联的高斯-克朗罗德定则对于决定高斯定则的某些度量和某些节点数来说可能并不存在。这促使 M. M. Spalević [1] 开发了具有 2ℓ+1 节点的广义平均高斯规则 Gˆ2ℓ+1,用于估计 Gℓ(f) 的误差。与(2ℓ+1)节点高斯-克朗罗德规则类似,Gˆ2ℓ+1 规则的 ℓ 节点与 Gℓ 的节点一致。然而,广义平均高斯规则对于某些度量并不具有内部性。因此,当积分只定义在度量支持的凸壳上时,它们可能并不适用。本文介绍了一种新的正交规则,当广义平均正交规则不具有内部性时,它也可能具有内部性。新正交规则的构建基于 Peherstorfer [2] 提出的理论。当 Gˆ2ℓ+1 规则不是内部规则、积分无法在其所有节点上求值以及积分在正交点上求值成本较低时,它们的应用尤其具有吸引力。本文通过计算实例说明了新正交规则的性能。
{"title":"A new class of quadrature rules for estimating the error in Gauss quadrature","authors":"Aleksandar V. Pejčev ,&nbsp;Lothar Reichel ,&nbsp;Miodrag M. Spalević ,&nbsp;Stefan M. Spalević","doi":"10.1016/j.apnum.2024.06.011","DOIUrl":"https://doi.org/10.1016/j.apnum.2024.06.011","url":null,"abstract":"&lt;div&gt;&lt;p&gt;The need to evaluate Gauss quadrature rules arises in many applications in science and engineering. It often is important to be able to estimate the quadrature error when applying an &lt;em&gt;ℓ&lt;/em&gt;-point Gauss rule, &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;G&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;, where &lt;em&gt;f&lt;/em&gt; is an integrand of interest. Such an estimate often is furnished by applying another quadrature rule, &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;Q&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;, with &lt;span&gt;&lt;math&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; nodes, and using the difference &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;Q&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;G&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; or its magnitude as an estimate for the quadrature error in &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;G&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; or its magnitude. The classical approach to estimate the error in &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;G&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; is to let &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;Q&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;, with &lt;span&gt;&lt;math&gt;&lt;mi&gt;k&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;, be the Gauss-Kronrod quadrature rule associated with &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;G&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;. However, it is well known that the Gauss-Kronrod rule associated with a Gauss rule &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;G&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt; might not exist for certain measures that determine the Gauss rule and for certain numbers of nodes. This prompted M. M. Spalević &lt;span&gt;[1]&lt;/span&gt; to develop generalized averaged Gauss rules, &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mover&gt;&lt;mrow&gt;&lt;mi&gt;G&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;ˆ&lt;/mo&gt;&lt;/mrow&gt;&lt;/mover&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;, with &lt;span&gt;&lt;math&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt; nodes for estimating the error in &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;G&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;f&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;. Similarly as for &lt;span&gt;&lt;math&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/math&gt;&lt;/span&gt;-node Gauss-Kronrod rules, &lt;em&gt;ℓ&lt;/em&gt; nodes of the rule &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mover&gt;&lt;mrow&gt;&lt;mi&gt;G&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mo&gt;ˆ&lt;/mo&gt;&lt;/mrow&gt;&lt;/mover&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; agree with the nodes of &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;G&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;ℓ&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;. However, generalized averaged Gauss rules are not internal for some measures. They therefore may not be applicable when the integrand only is define","PeriodicalId":8199,"journal":{"name":"Applied Numerical Mathematics","volume":"204 ","pages":"Pages 206-221"},"PeriodicalIF":2.2,"publicationDate":"2024-06-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141434087","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"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
A phase field method for convective phase change problem preserving maximum bound principle 保留最大边界原则的对流相变问题相场方法
IF 2.2 2区 数学 Q1 MATHEMATICS, APPLIED Pub Date : 2024-06-17 DOI: 10.1016/j.apnum.2024.06.012
Hui Yao

Numerical simulations of convective solid-liquid phase change problems have long been a complex problem due to the movement of the solid-liquid interface layer, which leads to a free boundary problem. This work develops a convective phase change heat transfer model based on the phase field method. The governing equations consist of the incompressible Navier-Stokes-Boussinesq equations, the heat transfer equation, and the Allen-Cahn equation. The Navier-Stokes equations are penalised for imposing zero velocity within the solid region. For numerical methods, the mini finite element approach (P1b-P1) is used to solve the momentum equation spatially, the temperature and the phase field are approximated by the P1b elements. In the temporal discretization, the phase field and the temperature are decoupled from the momentum equation by using the finite difference method, forming a solvable linear system. A maximum bound principle for the phase field is derived, coming with an estimation of the tolerance of the time step size, which depends on the temperature range. This estimation guides the time step choice in the simulation. The program is developed within the FreeFem++ framework, drawing on our previous work on phase field methods [1] and a mushy-region method toolbox for heat transfer [2]. The accuracy and effectiveness of the proposed method have been validated through real-world cases of melting and solidification with linear or nonlinear buyangcy force, respectively. The simulation results are in agreement with experiments in references.

由于固液界面层的运动导致自由边界问题,对流固液相变问题的数值模拟一直是一个复杂的问题。本研究基于相场法建立了一个对流相变传热模型。控制方程包括不可压缩的 Navier-Stokes-Boussinesq 方程、传热方程和 Allen-Cahn 方程。纳维-斯托克斯方程因在固体区域内速度为零而受到惩罚。在数值方法方面,使用微型有限元方法(P1b-P1)求解空间动量方程,温度场和相场由 P1b 元素近似。在时间离散化中,使用有限差分法将相场和温度与动量方程解耦,形成一个可求解的线性系统。推导出了相场的最大约束原理,并对时间步长的容差进行了估计,这取决于温度范围。这一估算为模拟中的时间步长选择提供了指导。该程序是在 FreeFem++ 框架内开发的,借鉴了我们以前在相场方法[1]方面的研究成果以及用于热传递的蕈状区域方法工具箱[2]。通过分别使用线性或非线性买朗西力进行熔化和凝固的实际案例,验证了所提方法的准确性和有效性。模拟结果与参考文献中的实验结果一致。
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Applied Numerical Mathematics
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