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Analysis on nonlinear differential equation with a deviating argument via Faedo–Galerkin method 通过 Faedo-Galerkin 方法分析带有偏离参数的非线性微分方程
IF 2 Q2 MATHEMATICS, APPLIED Pub Date : 2024-04-11 DOI: 10.1016/j.rinam.2024.100452
M. Manjula , E. Thilakraj , P. Sawangtong , K. Kaliraj

This article focuses on the impulsive fractional differential equation (FDE) of Sobolev type with a nonlocal condition. Existence and uniqueness of the approximations are determined via analytic semigroup and fixed point method. Convergence’s approximation is demonstrated by the idea of fractional power of a closed linear operator. Using an approximation procedure, a novel approach is reached. An illustration is used to clarify our key findings.

本文主要研究具有非局部条件的 Sobolev 型脉冲分微分方程(FDE)。通过解析半群和定点法确定了近似的存在性和唯一性。通过封闭线性算子的分数幂思想证明了收敛近似性。利用近似程序,我们得出了一种新方法。通过一个例子来阐明我们的主要发现。
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引用次数: 0
Global boundedness and asymptotic behavior of the chemotaxis system for alopecia areata with singular sensitivity 具有奇异敏感性的脱发症趋化系统的全局有界性和渐近行为
IF 2 Q2 MATHEMATICS, APPLIED Pub Date : 2024-04-06 DOI: 10.1016/j.rinam.2024.100450
Peng Gao , Lu Xu
<div><p>This paper is concerned with a three-component chemotaxis system for alopecia areata with singular sensitivity <span><span><span><math><mfenced><mrow><mtable><mtr><mtd><msub><mrow><mi>u</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mi>Δ</mi><mi>u</mi><mo>−</mo><msub><mrow><mi>χ</mi></mrow><mrow><mn>1</mn></mrow></msub><mo>∇</mo><mi>⋅</mi><mfenced><mrow><mfrac><mrow><mi>u</mi></mrow><mrow><mi>w</mi></mrow></mfrac><mo>∇</mo><mi>w</mi></mrow></mfenced><mo>+</mo><mi>w</mi><mo>−</mo><msub><mrow><mi>μ</mi></mrow><mrow><mn>1</mn></mrow></msub><msup><mrow><mi>u</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd><msub><mrow><mi>v</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mi>Δ</mi><mi>v</mi><mo>−</mo><msub><mrow><mi>χ</mi></mrow><mrow><mn>2</mn></mrow></msub><mo>∇</mo><mi>⋅</mi><mfenced><mrow><mfrac><mrow><mi>v</mi></mrow><mrow><mi>w</mi></mrow></mfrac><mo>∇</mo><mi>w</mi></mrow></mfenced><mo>+</mo><mi>w</mi><mo>+</mo><mi>r</mi><mi>u</mi><mi>v</mi><mo>−</mo><msub><mrow><mi>μ</mi></mrow><mrow><mn>2</mn></mrow></msub><msup><mrow><mi>v</mi></mrow><mrow><mn>2</mn></mrow></msup><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd><msub><mrow><mi>w</mi></mrow><mrow><mi>t</mi></mrow></msub><mo>=</mo><mi>Δ</mi><mi>w</mi><mo>+</mo><mi>u</mi><mo>+</mo><mi>v</mi><mo>−</mo><mi>w</mi><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi><mo>,</mo><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd><mfrac><mrow><mi>∂</mi><mi>u</mi></mrow><mrow><mi>∂</mi><mi>ν</mi></mrow></mfrac><mo>=</mo><mfrac><mrow><mi>∂</mi><mi>v</mi></mrow><mrow><mi>∂</mi><mi>ν</mi></mrow></mfrac><mo>=</mo><mfrac><mrow><mi>∂</mi><mi>w</mi></mrow><mrow><mi>∂</mi><mi>ν</mi></mrow></mfrac><mo>=</mo><mn>0</mn><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>∂</mi><mi>Ω</mi><mo>,</mo><mi>t</mi><mo>></mo><mn>0</mn><mo>,</mo></mtd></mtr><mtr><mtd><mi>u</mi><mrow><mo>(</mo><mi>x</mi><mo>,</mo><mn>0</mn><mo>)</mo></mrow><mo>=</mo><msub><mrow><mi>u</mi></mrow><mrow><mn>0</mn></mrow></msub><mrow><mo>(</mo><mi>x</mi><mo>)</mo></mrow><mo>,</mo><mi>v</mi><mrow><mo>(</mo><mi>x</mi><mo>,</mo><mn>0</mn><mo>)</mo></mrow><mo>=</mo><msub><mrow><mi>v</mi></mrow><mrow><mn>0</mn></mrow></msub><mrow><mo>(</mo><mi>x</mi><mo>)</mo></mrow><mo>,</mo><mi>w</mi><mrow><mo>(</mo><mi>x</mi><mo>,</mo><mn>0</mn><mo>)</mo></mrow><mo>=</mo><msub><mrow><mi>w</mi></mrow><mrow><mn>0</mn></mrow></msub><mrow><mo>(</mo><mi>x</mi><mo>)</mo></mrow><mo>,</mo><mspace></mspace></mtd><mtd><mi>x</mi><mo>∈</mo><mi>Ω</mi></mtd></mtr></mtable></mrow></mfenced></math></span></span></span>under the homogeneous Neumann boundary conditions in a smoothly bounded domain <span><math><mrow><mi>Ω</mi><mo>⊂</mo><msup><mrow><mi>R</mi></mrow><mrow><mn>2</mn></mrow></msup></mrow>
本文研究的是一种用于治疗斑秃的三组份趋化系统,其奇异敏感度为 ut=Δu-χ1∇⋅uw∇w+w-μ1u2,x∈Ω,t>;0,vt=Δv-χ2∇⋅vw∇w+w+ruv-μ2v2,x∈Ω,t>0,wt=Δw+u+v-w,x∈Ω,t>;0,∂u∂ν=∂v∂ν=∂w∂ν=0,x∈∂Ω,t>;0,u(x,0)=u0(x),v(x,0)=v0(x),w(x,0)=w0(x),x∈Ω在平滑有界域Ω⊂R2 中的均相 Neumann 边界条件下,其中参数 χi、μi(i=1,2)和 r 均为正值。研究表明,如果χ1,χ2<52,这个系统会有一个全局有界的经典解。此外,在μ1<μ2<3μ1和r=μ2-μ1的特定条件下,随着t→∞,全局有界解收敛到稳态(2μ1,2μ1,4μ1)。
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&lt;span&gt;&lt;span&gt;&lt;span&gt;&lt;math&gt;&lt;mfenced&gt;&lt;mrow&gt;&lt;mtable&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;Δ&lt;/mi&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;χ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;∇&lt;/mo&gt;&lt;mi&gt;⋅&lt;/mi&gt;&lt;mfenced&gt;&lt;mrow&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mo&gt;∇&lt;/mo&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;/mrow&gt;&lt;/mfenced&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;μ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;1&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;Δ&lt;/mi&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;χ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;∇&lt;/mo&gt;&lt;mi&gt;⋅&lt;/mi&gt;&lt;mfenced&gt;&lt;mrow&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mo&gt;∇&lt;/mo&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;/mrow&gt;&lt;/mfenced&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;r&lt;/mi&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;μ&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mi&gt;Δ&lt;/mi&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mo&gt;+&lt;/mo&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mo&gt;−&lt;/mo&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mi&gt;∂&lt;/mi&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;∂&lt;/mi&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mi&gt;∂&lt;/mi&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;∂&lt;/mi&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mfrac&gt;&lt;mrow&gt;&lt;mi&gt;∂&lt;/mi&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mi&gt;∂&lt;/mi&gt;&lt;mi&gt;ν&lt;/mi&gt;&lt;/mrow&gt;&lt;/mfrac&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mi&gt;∂&lt;/mi&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;t&lt;/mi&gt;&lt;mo&gt;&gt;&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;mtr&gt;&lt;mtd&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;u&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;v&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;msub&gt;&lt;mrow&gt;&lt;mi&gt;w&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;mrow&gt;&lt;mo&gt;(&lt;/mo&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;)&lt;/mo&gt;&lt;/mrow&gt;&lt;mo&gt;,&lt;/mo&gt;&lt;mspace&gt;&lt;/mspace&gt;&lt;/mtd&gt;&lt;mtd&gt;&lt;mi&gt;x&lt;/mi&gt;&lt;mo&gt;∈&lt;/mo&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;/mtd&gt;&lt;/mtr&gt;&lt;/mtable&gt;&lt;/mrow&gt;&lt;/mfenced&gt;&lt;/math&gt;&lt;/span&gt;&lt;/span&gt;&lt;/span&gt;under the homogeneous Neumann boundary conditions in a smoothly bounded domain &lt;span&gt;&lt;math&gt;&lt;mrow&gt;&lt;mi&gt;Ω&lt;/mi&gt;&lt;mo&gt;⊂&lt;/mo&gt;&lt;msup&gt;&lt;mrow&gt;&lt;mi&gt;R&lt;/mi&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/mrow&gt;","PeriodicalId":36918,"journal":{"name":"Results in Applied Mathematics","volume":"22 ","pages":"Article 100450"},"PeriodicalIF":2.0,"publicationDate":"2024-04-06","publicationTypes":"Journal 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引用次数: 0
Bernstein polynomials method for solving multi-order fractional neutral pantograph equations with error and stability analysis 伯恩斯坦多项式法求解多阶分数中性受电弓方程的误差和稳定性分析
IF 2 Q2 MATHEMATICS, APPLIED Pub Date : 2024-04-06 DOI: 10.1016/j.rinam.2024.100451
M.H.T. Alshbool

In this investigation, we present a new method for addressing fractional neutral pantograph problems, utilizing the Bernstein polynomials method. We obtain solutions for the fractional pantograph equations by employing operational matrices of differentiation, derived from fractional derivatives in the Caputo sense applied to Bernstein polynomials. Error analysis, along with Chebyshev algorithms and interpolation nodes, is employed for solution characterization. Both theoretical and practical stability analyses of the method are provided. Demonstrative examples indicate that our proposed techniques occasionally yield exact solutions. We compare the algorithms using several established analytical methods. Our results reveal that our algorithm, based on Bernstein series solution methods, outperforms others, exhibiting superior performance with higher accuracy orders compared to those obtained from Chebyshev spectral methods, Bernoulli wavelet method, and Spectral Tau method.

在这项研究中,我们提出了一种利用伯恩斯坦多项式方法解决分数中性受电弓问题的新方法。我们通过使用微分运算矩阵获得分数受电弓方程的解决方案,微分运算矩阵由应用于伯恩斯坦多项式的卡普托意义上的分数导数导出。误差分析以及切比雪夫算法和插值节点被用于求解特征。该方法提供了理论和实际稳定性分析。演示示例表明,我们提出的技术偶尔会产生精确解。我们使用几种成熟的分析方法对算法进行了比较。结果表明,我们基于伯恩斯坦数列求解方法的算法优于其他算法,与切比雪夫频谱法、伯努利小波法和频谱 Tau 法相比,我们的算法具有更高的精度等级,表现出卓越的性能。
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引用次数: 0
Decay analysis of bivariate Chebyshev coefficients for functions with limited regularity 有限正则函数的双变量切比雪夫系数的衰减分析
IF 2 Q2 MATHEMATICS, APPLIED Pub Date : 2024-04-01 DOI: 10.1016/j.rinam.2024.100449
Akansha

The Chebyshev polynomial approximation is a useful tool to approximate smooth and non-smooth functions. In fact, for a sufficiently smooth function, the partial sum of Chebyshev series expansion provides optimal polynomial approximation. Moreover, because the construction of these polynomial approximations is computational efficient, they are widely used in numerical schemes for solving partial deferential equations. Significant efforts have been devoted to establishing decay bounds for series coefficients, including Chebyshev, Jacobi, and Legendre series, for both smooth and non-smooth univariate functions. However, the literature lacks similar estimates for bivariate functions. This paper aims to address this gap by examining the decay estimates of bivariate Chebyshev coefficients, contributing both theoretically and practically to the understanding and application of Chebyshev series expansions, especially concerning functions with limited smoothness. Additionally, we derive L1-error estimates for the partial sum of Chebyshev series expansions of functions with bounded Vitali variation. Furthermore, we provide an estimate for the discrepancy between exact and approximated Chebyshev coefficients, leveraging a quadrature formula. This analysis leads to the deduction of an asymptotic L1-approximation error for finite partial sums of Chebyshev series with approximated coefficients.

切比雪夫多项式逼近法是逼近光滑和非光滑函数的有用工具。事实上,对于足够光滑的函数,切比雪夫级数展开的部分和提供了最佳多项式近似。此外,由于这些多项式近似的构造具有很高的计算效率,因此被广泛应用于求解偏微分方程的数值方案中。对于光滑和非光滑单变量函数,人们一直致力于为包括切比雪夫、雅可比和勒让德序列在内的序列系数建立衰减边界。然而,文献中缺乏对双变量函数的类似估计。本文旨在通过研究双变量切比雪夫系数的衰减估计值来填补这一空白,从理论和实践两方面促进对切比雪夫数列展开的理解和应用,尤其是对光滑度有限的函数的理解和应用。此外,我们还推导出了具有有界维塔利变化的函数的切比雪夫级数展开部分和的 L1 误差估计值。此外,我们还利用正交公式,提供了精确切比雪夫系数与近似切比雪夫系数之间差异的估计值。通过这一分析,我们推导出了具有近似系数的切比雪夫级数有限偏和的 L1 近似误差。
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引用次数: 0
Modeling flow and deformation in porous media from pore-scale to the Darcy-scale 从孔隙尺度到达西尺度的多孔介质流动和变形建模
IF 2 Q2 MATHEMATICS, APPLIED Pub Date : 2024-03-30 DOI: 10.1016/j.rinam.2024.100448
Zachary Hilliard , T. Matthew Evans , Malgorzata Peszynska

In this paper we address the connections between the computational models of coupled flow and mechanical deformation in soils at the Darcy-scale and pore-scale. At the Darcy scale the Biot model requires data including permeability which is traditionally provided by experiments and empirical measurements. At the pore-scale we consider the Discrete Element Method (DEM) to generate physically realistic assemblies of the particles, and we follow up with the Stokes flow model. Next we apply upscaling to obtain the permeabilities which we find dependent on the deformation. We outline the workflow with its challenges and methods, and present results which show, e.g., hysteretic dependence of the permeability and porosity on the load. We also show how to incorporate the deformation dependent permeability in a nonlinear Biot model, and illustrate with computational results.

在本文中,我们探讨了达西尺度和孔隙尺度土壤中流动和机械变形耦合计算模型之间的联系。在达西尺度上,Biot 模型需要包括渗透率在内的数据,这些数据传统上由实验和经验测量提供。在孔隙尺度上,我们考虑使用离散元素法(DEM)生成物理上真实的颗粒组合,并使用斯托克斯流模型进行跟进。接下来,我们采用放大法获得渗透率,并发现渗透率与变形有关。我们概述了工作流程及其挑战和方法,并展示了结果,例如,渗透率和孔隙率对载荷的滞后依赖性。我们还展示了如何将与变形有关的渗透率纳入非线性 Biot 模型,并用计算结果加以说明。
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引用次数: 0
Solving the general form of the fractional Black–Scholes with two assets through Reconstruction Variational Iteration Method 通过重构变式迭代法求解有两种资产的分数布莱克-斯科尔斯(Black-Scholes)一般形式
IF 2 Q2 MATHEMATICS, APPLIED Pub Date : 2024-03-04 DOI: 10.1016/j.rinam.2024.100444
Mohammad Hossein Akrami , Abbas Poya , Mohammad Ali Zirak

The objective of this study is to examine the dynamic components of option pricing in the European put option market by utilizing the two-dimensional time fractional-order Black–Scholes equation. To enhance the classical Black–Scholes equation, we utilize the Caputo type of the Katugampola fractional derivative. The Reconstruction of Variational Iteration Method is employed as a powerful tool for analyzing option price behavior in the European-style market. In our investigation, we utilize this method to obtain an exact solution for fractional Black–Scholes with two assets. Moreover, the findings demonstrate the impressive effectiveness of the Reconstruction of Variational Iteration Method in addressing two-dimensional fractional-order differential equations, thereby highlighting its potential as a valuable numerical solution technique.

本研究的目的是利用二维时间分数阶布莱克-斯科尔斯方程研究欧洲看跌期权市场中期权定价的动态成分。为了增强经典的 Black-Scholes 方程,我们使用了卡普托类型的 Katugampola 分数导数。重构变分迭代法是分析欧式市场期权价格行为的有力工具。在我们的研究中,我们利用该方法获得了两种资产的分数 Black-Scholes 精确解。此外,研究结果表明,重构变分迭代法在处理二维分数阶微分方程方面的有效性令人印象深刻,从而凸显了其作为一种有价值的数值求解技术的潜力。
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引用次数: 0
A truncated matrix variate gamma distribution 截断矩阵变异伽马分布
IF 2 Q2 MATHEMATICS, APPLIED Pub Date : 2024-03-04 DOI: 10.1016/j.rinam.2024.100446
Shokofeh Zinodiny , Saralees Nadarajah , Daya K. Nagar

A truncated form of a matrix variate gamma distribution is introduced and a number of properties of this distribution such as cumulative distribution function, orthogonal invariance, moment generating function, marginal distribution of block matrices, and moments are derived. Some results on distribution of random quadratic forms are also derived.

引入了矩阵变量伽马分布的截断形式,并推导出该分布的一些性质,如累积分布函数、正交不变性、矩产生函数、块矩阵的边际分布和矩。此外,还推导了一些关于随机二次型分布的结果。
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引用次数: 0
Error estimates of characteristic finite elements for bilinear convection–diffusion optimal control problems 双线性对流扩散优化控制问题的特征有限元误差估计
IF 2 Q2 MATHEMATICS, APPLIED Pub Date : 2024-03-02 DOI: 10.1016/j.rinam.2024.100445
Yuchun Hua, Yuelong Tang

This paper investigates a fully discrete characteristic finite element approximation of bilinear unsteady convection–diffusion optimal control problems. The characteristic line method is used to treat the convection term and the finite element method is adopted to treat the diffusion term. The state and adjoint state are discretized by piecewise linear functions, the control is approximated by piecewise constant functions. A priori error estimates are derived for the state, adjoint state and control variables. Some numerical examples are provided to confirm our theoretical findings.

本文研究了双线性非稳态对流-扩散最优控制问题的全离散特征有限元近似。特征线法用于处理对流项,有限元法用于处理扩散项。状态和邻接状态由分片线性函数离散化,控制由分片常数函数近似化。得出了状态、邻接状态和控制变量的先验误差估计值。还提供了一些数值示例来证实我们的理论发现。
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引用次数: 0
Difference interior penalty discontinuous Galerkin method for the 3D elliptic equation 三维椭圆方程的差分内部惩罚非连续伽勒金方法
IF 2 Q2 MATHEMATICS, APPLIED Pub Date : 2024-02-28 DOI: 10.1016/j.rinam.2024.100443
Jian Li, Wei Yuan, Luling Cao

This paper presents a difference interior penalty discontinuous Galerkin method for the 3D elliptic boundary-value problem. The main idea of this method is to combine the finite difference discretization in the z-direction with the interior penalty discontinuous Galerkin discretization in the (x,y)-plane. One of the advantages of this method is that the solution of 3D problem is transformed into a series of 2D problems, thereby overcoming the computational complexity of traditional interior penalty discontinuous Galerkin method for solving high-dimensional problems and allowing for code reuse. Additionally, we use the interior penalty discontinuous Galerkin method to solve each 2D problem, therefore, this method retains the advantage of the interior penalty discontinuous Galerkin method in dealing with non-matching grids and non-uniform, even anisotropic, polynomial approximation degrees. Then, the error estimates are given for difference interior penalty discontinuous Galerkin method. Finally, numerical experiments demonstrate the accuracy and effectiveness of the difference interior penalty discontinuous Galerkin method.

本文针对三维椭圆边界值问题提出了一种差分内部惩罚非连续 Galerkin 方法。该方法的主要思想是将 z 方向上的有限差分离散化与 (x,y) 平面上的内部惩罚非连续 Galerkin 离散化相结合。该方法的优点之一是将三维问题的求解转化为一系列二维问题,从而克服了传统内部惩罚非连续 Galerkin 方法求解高维问题的计算复杂性,并允许代码重用。此外,我们使用内部惩罚非连续伽勒金方法求解每个二维问题,因此,该方法保留了内部惩罚非连续伽勒金方法在处理非匹配网格和非均匀甚至各向异性多项式近似度时的优势。然后,给出了差分内部惩罚非连续伽勒金方法的误差估计值。最后,数值实验证明了差分内部惩罚非连续伽勒金方法的准确性和有效性。
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引用次数: 0
Graded mesh modified backward finite difference method for two parameters singularly perturbed second-order boundary value problems 两参数奇异扰动二阶边界值问题的分级网格修正后向有限差分法
IF 2 Q2 MATHEMATICS, APPLIED Pub Date : 2024-02-16 DOI: 10.1016/j.rinam.2024.100442
Fellek Sabir Andisso , Gemechis File Duressa

The existence of boundary layers in the solutions of two-parameter singularly perturbed boundary value problems makes classical numerical methods insufficient in providing accurate approximations. Consequently, the development of layer-adapted mesh methods that achieve parameter uniform convergence and are specifically designed to accurately handle these layers becomes highly significant. The aim of this paper is to construct and examine a numerical approach for obtaining approximate solutions to a specific class of two-parameter singularly perturbed second order boundary value problems whose solutions exhibit boundary layers at both ends of the domain. The problem is discretized by employing a modified backward finite difference method on a mesh that is graded. To validate the theoretical findings, well known test problems from the existing literature are utilized. Moreover, the efficiency of the proposed method is demonstrated by comparing it to other existing methods in the literature. The stability and uniform convergence with respect to the parameters of the proposed method have been verified, revealing that it attains second-order convergence in the maximum norm. The numerical outcomes illustrate that the proposed method offers remarkably accurate approximations of the solution. Theoretical findings are in agreement with the experimental results.

双参数奇异扰动边界值问题的解中存在边界层,这使得经典数值方法无法提供精确的近似值。因此,开发可实现参数均匀收敛并专门用于精确处理这些层的层适应网格方法变得非常重要。本文旨在构建和研究一种数值方法,以获得特定类别的两参数奇异扰动二阶边界值问题的近似解,该问题的解在域的两端都表现出边界层。该问题的离散化方法是在分级网格上采用改进的后向有限差分法。为了验证理论结论,利用了现有文献中已知的测试问题。此外,通过与文献中其他现有方法的比较,证明了所提方法的效率。验证了所提方法在参数方面的稳定性和均匀收敛性,发现它在最大规范上达到了二阶收敛。数值结果表明,提出的方法提供了非常精确的近似解。理论结论与实验结果一致。
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引用次数: 0
期刊
Results in Applied Mathematics
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