解高维广义对称正则长波方程的Fourier谱方法

１引言对称正则长波方程（ＳＲＬＷＥ）是正则化长波方程（ＲＬＷＥ）的一种对称叙述［１］用于描述弱非线性作用下空间变换的离子声波传播．［１］得到了方程组（１．１）的双曲正割平方孤立波解、四个不变量和数值结果、明显地,从（１．１）中消去ρ,得到一类正则长波方程（ＲＬＷＥ）代替（１．２）中第三项、第四项对ｔ的导数为对ｘ的导数,得到Ｂｏｕｓｓｉｎｅｓｑ方程．［２］对一类广义对称正则长波方程组提出了谱方法,证明了古典光滑解的存在性和唯一性,建立了近似解的收敛性和误差估计。［３］研究了高维对称正则长波方程整体…     

摩擦接触问题正则化方法的注记

1．问题及记号简化的具有库仑（Coulumb）摩擦的接触问题的变分形式如下（见［1］－［4］）：设fi，且＞0在上，其中为三维区域的边界，为固定位移边界，F为应力边界而rC为接触边界且mesC＞0．则问题题如下其等价的泛函极小问题为：Th：H‘（m－－＋H！（rD）的迹算子，o＝（。1，12，。扩为位移向量，／＝（人，h，h尸为体积力，土一（h，t。，tJ为rF上的边界应力向量；在r上，行为单位外法向，V。一本行，呵一i一V砰，而Eijki是弹性材料系数，满足通常的对称性及椭圆性条件：本文采用如下约定：凡每一项中出现重复指标，即意味着从1…     

铁磁链Landau-Lifshitz方程的显式差分法

正如在研究流体动力学时,Ｎａｖｉｅｒ－Ｓｔｏｋｅｓ方程起着十分重要的作用一样,在对于非平衡态磁学的研究中,描述连续铁磁体自旋场发展过程的 Ｌａｎｄａｎ－Ｌｉｆｓｈｉｔｚ方程［１］起着十分重要的作用［２］．一九九三年,美国和印度签署了一个大约 ２８０万美元的合作研究计划,在三年的时间里,对Ｌａｎｄａｕ－Ｌｉｆｓｈｉｔｚ铁磁链方程进行研究．在无阻尼的情况下,它为一完全可积的孤立子系统［３,４,５］。很多物理学家研究了它的孤立子解的存在性、逆散射方法以及相互碰撞［３,４,５］．关于解的存在性, Ａｌｏｎ…     

再议f（x）＝f~（－1）（x）与x＝f（x）是否同解

再议ｆ（ｘ）＝ｆ~（－１）（ｘ）与ｘ＝ｆ（ｘ）是否同解邬坤昌（上海宝山松浦中学）常绪珠（湖北钟祥一中）方程ｆ（ｘ）＝ｆ－１（Ｘ）与方程Ｘ＝ｆ（ｘ）［或Ｘ＝ｆ－１（Ｘ）］是否同解？文［１］以函数ｙ＝１－ｘ的反函数是它自己为反侧，说明了ｆ（ｘ）＝ｆ－１（?..     

连续同伦方法的点估计判据

本文证明了，当S·Smale［1］的点估计判据a（z0，f）＝||Df（z0）-1·f（z0）||sup||Df－1（z0）·时，求Banach空间解析映照f零点的连续同伦H（t，z）≡f（z）＋（t－1）f（z0）＝0有定义于［0，1］上的解z（t），且对t∈［0，1］，Hz（t，z（t））－1存在，进而F（Z（1））＝0，可以用连续同伦方法求得f的零点．     

一个刚性守恒律方程组的全隐式差分方法

１．引言本文研究如下非线性刚性守恒律方程组的全隐式差分逼近． 方程（1．１）中的源项ｇ（ｕ,ｖ）定义为 ｇ（ｕ,ｖ）＝ｖ－（１－μ）ｆ（ｕ）,（１．２）其中ｆ是ｕ的一个给定函数,δ是一个小正参数,称为松弛时间,μ是参数．方程组（１．１）频繁出现于粘弹性力学中． 在零松弛时间限（δ→０）下,从（１．１）可得到如下方程组该方程组通常称为“平衡”模型,而方程组（１．１）称为“非平衡”模型． 文中将假设μ满足 ０＜ μ＜ １,（１．４）以便保证拟稳定性条件［１９,２０］和次特征条件［１１,２,３］： λ１≤λ＊…     

复Schr(o)dinger场和实Klein-Gordon场相互作用下一类方程组守恒差分格式的收敛性和稳定性

１引言关于Ｚａｋｈａｒｏｖ方程各种定解问题的讨论,近年来已发表了许多的文献［１－５］,很明显,这是复非线性Schrod-inger（NLS）方程和实非线性波动方程耦合的一类方程组．文献［６］考察了复ＮＬＳ方程和实非线性Ｋｌｅｉｎ－Ｇｏｒｄｏｎ（Ｇ－Ｋ）方程耦合的一类方程组的各种定解问题,其中φ（ｘ,ｔ）是复值函数,ｕ（ｘ,ｔ）是实值函数,ｆ（ｓ）∈（－∞,∞）,μ,ｇ,ｍ均为正常数,ｉ２＝－１．文中证明了整体解的存在性、唯一性和存在如下两个守恒律其中Ｆ（ｓ）＝ｆ（ｚ）ｄｚ,Ｅ００,Ｅ０１均为仅与初始条件有关…     

一类一阶泛函微分方程解的存在性与分支

本文研究方程ｘ’（ｔ）＝（ｘ２（ｔ）－μ）ｘ（ｘ（ｔ））μ≤０（１）解的性态。当μ＜０时，我们得到与Ｅｄｅｒ［１］和ｗａｎｇ［２］相类似的结论，也得到一些新的性质；当μ＝０时，我们得到全新的结论，证明方程（１）存在两端均不可延拓到∞的严格单调饱和强解，μ＝０是方程（１）的分支值。     

离散速度动力学方程组的数值方法研究 Ⅰ.半隐式差分格式

１．引言文中考虑 Ｂｏｌｔｚｍａｎｎ方程的离散速度模型一两速度模型的数值方法的构造和分析．其中,ｃ为分子速度,Ｊ（ｕ,ｖ）为碰撞算子,具有如下一般形式式中ｋ（ｕ,ｖ）,和为非负实常数．模型（１．１）－（１．２０包含了一些著名的动力学模型,例如 Ｇｏｌｄｓｔｅｉｎ－Ｔａｙｌｏｒ模型［５,１４］, Ｒｕｉｊｇｒｏｏｋ－Ｗｕ模型［１２］,多孔介质方程［９,１１］等． 如果引进宏观变量产＝ｕ＋ｖ,ｊ＝（ｕ－ｖ）,则可得到宏观方程其中此外,方程（１．３）有两个自然渐近区．第一个是此时Ｊ（ｊ）＝０,如果该方程有…     

一类中立型微分方程的比较定理及应用

考虑中立型微分方程［ｘ（ｔ）－ｘ（ｔ－τ）］（ｎ）＋Ｑ（ｔ）ｘ（ｔ－σ）＝０，ｔｔ０，其中ｎ１为奇数，τ∈（０，∞），σ∈Ｒ＋＝［０，∞），Ｑ∈Ｃ（［ｔ０，∞），Ｒ＋）．本文获得了此方程存在最终正解以及所有解振动的新的比较定理．并据此获得了所有解振动的“ｓｈａｒｐ″条件以及存在最终正解的一般性结果，改进了文［４］的主要结果．     

一类广义KdV方程组的谱和拟谱方法

1.引 言在孤立子的研究中起着重要作用的典型方程-KdV方程已有不少作者[1-5]在数学分析上做了许多深入的研究,文[6]讨论了如下一类高阶广义KdV方程组     

Optimal error estimate of two linear and momentum-preserving Fourier pseudo-spectral schemes for the RLW equation

In this paper, two novel linear-implicit and momentum-preserving Fourier pseudo-spectral schemes are proposed and analyzed for the regularized long-wave equation. The numerical methods are based on the blend of the Fourier pseudo-spectral method in space and the linear-implicit Crank–Nicolson method or the leap-frog scheme in time. The two fully discrete linear schemes are shown to possess the discrete momentum conservation law, and the linear systems resulting from the schemes are proved uniquely solvable. Due to the momentum conservative property of the proposed schemes, the Fourier pseudo-spectral solution is proved to be bounded in the discrete L^∞ norm. Then by using the standard energy method, both the linear-implicit Crank–Nicolson momentum-preserving scheme and the linear-implicit leap-frog momentum-preserving scheme are shown to have the accuracy of in the discrete L^∞ norm without any restrictions on the grid ratio, where N is the number of nodes and τ is the time step size. Numerical examples are carried out to verify the correction of the theory analysis and the efficiency of the proposed schemes.     

Estudio comparativo de distintos modelos de condiciones de contorno de impedancia en problemas acústicos

In this paper, different implementations of numerical locally reacting boundary conditions are studied for acoustic problems. In this comparative study we analyze two types of equations, the Euler equations and the wave equation. We also analyze both finite-differences time-domain (FDTD) algorithms, and pseudo-spectral time domain (PSTD) numerical schemes. We compare different numerical implementations existing in the literature by means of exhaustive numerical experiments. These numerical experiments allow for the study of the absorbing properties of the different schemes as a function of the frequency and the angle of the incident sound waves. This novel comparative study will help the acoustic engineer in order to choose the proper numerical scheme for his/her simulations.     

Arbitrarily high-order accurate and energy-stable schemes for solving the conservative Allen–Cahn equation

In this paper, three high-order accurate and unconditionally energy-stable methods are proposed for solving the conservative Allen–Cahn equation with a space–time dependent Lagrange multiplier. One is developed based on an energy linearization Runge–Kutta (EL–RK) method which combines an energy linearization technique with a specific class of RK schemes, the other two are based on the Hamiltonian boundary value method (HBVM) including a Gauss collocation method, which is the particular instance of HBVM, and a general class of cases. The system is first discretized in time by these methods in which the property of unconditional energy stability is proved. Then the Fourier pseudo-spectral method is employed in space along with the proofs of mass conservation. To show the stability and validity of the obtained schemes, a number of 2D and 3D numerical simulations are presented for accurately calculating geometric features of the system. In addition, our numerical results are compared with other known structure-preserving methods in terms of numerical accuracy and conservation properties.     

A pseudo-spectral scheme for the approximate solution of a family of fractional differential equations

In this paper, the pseudo-spectral method is generalized for solving fractional differential equations with initial conditions. For this purpose, an appropriate representation of the solution is presented and the pseudo-spectral differentiation matrix of fractional order is derived. Then, by using pseudo-spectral scheme, the problem is reduced to the solution of a system of algebraic equations. Through several numerical examples, we evaluate the accuracy and performance of our proposed method.     

Kolmogorov-Spieqel-Siveshinky方程大时间问题的Fourier拟谱逼近

该文讨论了Kolmogorov-Spieqel-Siveshinky方程的周期初值问题, 研究了半离散Fourier拟谱解的长时间行为, 证明了半离散系统的收敛性和整体吸引子的存在性. 构造了全离散的三层显式Fourier拟谱格式, 并证明了该格式的收敛性, 最后通过数值计算验证了格式的可信性. 数值结果表明: 该格式是长时间稳定并可取时间大步长. 作者模拟了方程的解在相空间的轨线, 得到了一些有意义的结论.     

Error estimate of Fourier pseudo-spectral method for multidimensional nonlinear complex fractional Ginzburg–Landau equations

In this paper, we discuss the error estimate of Fourier pseudo-spectral method for multidimensional nonlinear complex space fractional Ginzburg-Landau equations. The continuous mass and energy inequalities as well as their discrete versions are presented. Moreover, by the discrete mass and energy inequalities, the error estimate of the Fourier pseudo-spectral scheme is established, and the scheme is proved to have the spectral accuracy.     

Linear second order in time energy stable schemes for hydrodynamic models of binary mixtures based on a spatially pseudospectral approximation

We develop two linear, second order energy stable schemes for solving the governing system of partial differential equations of a hydrodynamic phase field model of binary fluid mixtures. We first apply the Fourier pseudo-spectral approximation to the partial differential equations in space to obtain a semi-discrete, time-dependent, ordinary differential and algebraic equation (DAE) system, which preserves the energy dissipation law at the semi-discrete level. Then, we discretize the DAE system by the Crank-Nicolson (CN) and the second-order backward differentiation/extrapolation (BDF/EP) method in time, respectively, to obtain two fully discrete systems. We show that the CN method preserves the energy dissipation law while the BDF/EP method does not preserve it exactly but respects the energy dissipation property of the hydrodynamic model. The two new fully discrete schemes are linear, unconditional stable, second order accurate in time and high order in space, and uniquely solvable as linear systems. Numerical examples are presented to show the convergence property as well as the efficiency and accuracy of the new schemes in simulating mixing dynamics of binary polymeric solutions.     

高维广义Kuramoto-Sivashinsky型方程Fourier拟谱方法的大时间误差估计

在很多物理问题中出现如下方程:Kuramoto在研究反应扩散系统耗散结构时导出了上述方程,Sivashinsky在模拟火焰传播时也得到了它.此外,它还出现在粘性层流和Navier-Stokes方程的分枝解中.在[5-8]中,作者研究了一维情形下周期初值问题的整体吸引子和分枝解;[9]提出了广义KS型方程;[10-14]中研究了它的光滑解的存在性和t→+∞时的渐近性     

哮喘模型的谱方法与逆谱方法

哮喘模型的谱方法与逆谱方法鲁百年（陕西师范大学数学系）ＳＰＥＣＴＲＡＬＡＮＤＰＳＥＵＤＯＳＰＥＣＴＲＡＬＡＰＰＲＯＸＩＭＡＴＩＯＮＳＦＯＲＴＨＥＭＯＤＥＬＯＦＷＨＥＥＺＥＳ￥ＬｕＢａｉ－ｍｉａｎ（ＤｅｐａｒｔｍｅｎｔｏｆＭａｔｈｅｍａｔｉｃｓ，Ｓｈａ...