非线性热传导方程的几类精确解

通过引入恰当的试探函数,将非线性热传导方程化为易于求解的常微分方程组并对其求解,进而得到非线性热传导方程的孤波解、奇异行波解、三角函数周期波解等一些不同形式的行波解.     

非线性热传方程的相似解

文[1]研究了非线性热传导方程的波动解,即相似变量ξ为波动变量(ξ=a+bx+ct)的情形,并规定热传导系数也只是ξ的函数。本文抛弃了这些限制条件,从更加普遍的角度去研究非线性热传导方程的相似性解。     

一类多维非线性Schrdinger方程及其方程组的数值计算问题

本文对一类多维非线性Schrdinger方程组提出了Galerkin有限元法,并由此证明了广义解的存在性.还对一类多维非线性Schrdinger方程采用有限差分法,证明了相应的四点隐式和六点隐式差分格式的收敛性和稳定性.我们对二维平面和一维球、柱对称非线性Schrdinger方程进行了数值计算,得到非线性Schrdinger方程多维孤立波坍塌(Collapse)的具体图象。     

用格子Boltzmann方法模拟非线性热传导方程

对具有非线性源项和非线性扩散项的热传导方程建立格子Boltzmann求解模型.在演化方程中增加了两个关于源项分布函数的微分算子,对演化方程实施Chapman-Enskog展开.通过对演化方程的进一步改进,恢复出具有高阶截断误差的宏观方程.对不同参数选取下的非线性热传导方程进行了数值模拟,数值解与精确解吻合得很好.该模型也可以用于同类型的其他偏微分方程的数值计算中.     

一类非线性热导方程的Cauchy问题

该文证明了一类非线性热传导方程Ｃａｕｃｈｙ问题在Ｃ（［０，＋∞），Ｈｓ（Ｒ））（ｓ≥ｉ）中解的存在位和唯一性，并讨论了在范数     

基于小波收缩求解时间反向热传导问题的正则化方法

时间反向热传导问题是一类典型的不适定问题.应用对偶最小二乘法给出了时间反向热传导问题的误差估计,同时用小波收缩方法给出了它的非线性近似解的误差估计,并证明了在高层上的收敛性.     

复变量热传导方程的动力系统

探讨一个复变量热方程的Cauchy问题,其中的非线性项是倒数型的.先提出一些全局解的存在性与不存在性的判定准则,然后采用解平面的不变子集的变换,证明了当初始值渐近于常数时,解是否会在无穷远处消失或在任意时间内全局存在,均依赖于初始值的渐近极限值.     

分数阶广义扰动热波方程

研究了一类分数阶广义非线性扰动热波方程.首先用奇异慑动方法,求出了分数阶广义非线性扰动热波方程初始边值问题的任意次近似解析解.然后利用泛函分析不动点定理证明了它的一致有效性,最后简述了它的物理意义.求得的近似解析解,弥补了单纯用数值方法求模拟解的不足.     

广义热传导方程有限元算法的计算准则

本文作者曾对经典的(抛物型)热传导方程提出了两种单调性的新概念,推导并证明了几组计算准则,可以使其有限元数值解消除很容易出现的振荡和超界现象.本文把上述成果用于广义(双曲型)热传导方程的有限元解中,推导出它的有限元解的计算准则,并获得了一些新结论.     

大挠度圆柱壳在温度场中的热弹耦合振动分析

对温度场与与应力场耦合时的圆柱壳的非线性热弹耦合的振动问题,推导得到了基本的振动方程,热传导方程和协调方程,对短圆柱壳运用伽辽金(Galerkin)法求解,得出振幅随时间变化的数值解,得到一些有价值的结论．即随着温度幅值和耦合系数的增大,振动衰减的速度变缓,热弹耦合效应减弱．随着长径比、长厚比的增大,振幅衰减的速度变快,同时热振动频率也随之增大,即热弹耦合效应增强．耦合系数越大,轴向应力、轴向力以及轴向弯矩越小．     

三维热传导型半导体问题的特征有限元方法和分析

本文研究三维热传导型半导体瞬态问题的特征有限元方法及其理论分析,其数学模型是一类非线性偏微分方程的初边值问题,对电子位势方程提出Ｇａｌｅｒｋｉｎ逼近;对电子,空穴浓度方程采用特征有限元逼近;对热传导方程采用对时间向后差分的Ｇａｌｅｒｋｉｎ逼近．应用微分方程先验估计理论和技巧得到了最优阶Ｌ＾２误差估计。     

Hybrid differential transform and finite difference method to solve the nonlinear heat conduction problem

In this paper, the differential transform is employed to discuss the behaviors of nonlinear heat conduction problem. A hybrid method of differential transform and finite difference approach is proposed to solve the transient responses of a nonlinear heat conduction problem. Different parameters of the equation and boundary conditions are considered to verify the feasibility of the proposed method to such problems. Simulation results are illustrated and discussed in comparison with the linear case. The results show that the hybrid method can achieve good results for such problems.     

Numerical solution of transient heat conduction equation with variable thermophysical properties by the Tau method

In this article, we proposed the operational approach to the Tau method for solving linear and nonlinear one‐dimensional transient heat conduction equations with variable thermophysical properties which can involve heat generation term. To solve heat conduction equation, first we recall the Tau method to obtain a matrix form of the governing differential equation. Then boundary and initial conditions are transformed into a matrix form. Finally the resulting systems of linear or nonlinear algebraic equations are given. Afterwards, efficient error estimation is also introduced for this method. Some numerical examples are given to illustrate the efficiency and high accuracy of the proposed method and also results are compared with solutions obtained by other methods. © 2013 Wiley Periodicals, Inc. Numer Methods Partial Differential Eq 30: 964–977, 2014     

Decay mode solution of nonlinear boundary–initial value problems for the cylindrical (spherical) Boussinesq–Burgers equations

The major target of this paper is to construct new nonlinear boundary–initial value problems for Boussinesq–Burgers Equations, and derive the solutions of these nonlinear boundary–initial value problems by the simplified homogeneous balance method. The nonlinear transformation and its inversion between the Boussinesq–Burgers Equations and the linear heat conduction equation are firstly derived; then a new nonlinear boundary–initial value problem for the Boussinesq–Burgers equations with variable damping on the half infinite straight line is put forward for the first time, and the solution of this nonlinear boundary–initial value problem is obtained, especially, the decay mode solution of nonlinear boundary–initial value problem for the cylindrical (spherical) Boussinesq–Burgers equations is obtained.     

Nonlinear heat equation for nonhomogeneous anisotropic materials: A dual‐reciprocity boundary element solution

A dual‐reciprocity boundary element method is presented for the numerical solution of initial‐boundary value problems governed by a nonlinear partial differential equation for heat conduction in nonhomogeneous anisotropic materials. To assess the validity and accuracy of the method, some specific problems are solved. © 2009 Wiley Periodicals, Inc. Numer Methods Partial Differential Eq, 2010     

On one boundary value problem for a nonlinear heat equation in the case of two space variables

The article addresses a boundary value problem with degeneration for a nonlinear heat equation in the case of two space variables. Solving this problem makes it possible to study heat conduction in a neighborhood of a closed cylindrical surface. The theorem of the existence and uniqueness of an analytic solution to the problem is proved.     

三维热传导型半导体问题的交替方向有限元方法

1　引　　言三维热传导型半导体器件瞬态问题的数学模型由四个非线性偏微分方程描述[1 ,2 ] ,记 Ω为 Ω=[0 ,1 ] 3的边界 ,三维问题-Δψ =α( p -e+ N( x) ) ,　　 ( x,t)∈Ω× [0 ,T] ,( 1 .1 ) e t= . ( De( x) e-μe( x) e ψ) -R( e,p,T) ,　 ( x,t)∈Ω× ( 0 ,T] ,( 1 .2 ) p t= . ( Dp( x) p +μp( x) p ψ) -R( e,p,T) ,　 ( x,t)∈Ω× ( 0 ,T] ,( 1 .3 )ρ( x) T t-ΔT =[( Dp( x) p +μp( x) p ψ) -( De( x) e-μe( x) e ψ) ] . ψ,　　　　　　 ( x,t)∈Ω× ( 0 ,T] . ( 1 .4 )ψ( x,t) =e( x,t) =p( …     

The relation between the Emden–Fowler equation and the nonlinear heat conduction problem with variable transfer coefficient

The main objective of this article is to analyze the RF-pair approach for the relation between the Emden–Fowler equation and the nonlinear heat conduction problem with variable transfer coefficient. The nonlinear heat conduction equation, by means of appropriate series of operators and transformations is transformed into the classical Emden–Fowler equation.     

A local iteration scheme for nonlinear two-dimensional steady-state heat conduction: a BEM approach

An efficient algorithm is proposed to solve the steady-state nonlinear heat conduction equation using the boundary element method (BEM). Nonlinearity of the heat conduction equation arises from nonlinear boundary conditions and temperature dependence of thermal conductivity. Using Kirchhoff's transformation, the case of temperature dependence of thermal conductivity can be transformed to the nonlinear boundary conditions case. Applying the BEM technique, the resulting matrix equation becomes nonlinear. The nonlinearity, however, only involves the boundary nodes that have nonlinearboundary conditions. The proposed local iterative scheme reduces the entire BEM matrix equation to a smaller matrix equation whose rank is the same as the number of boundary nodes with nonlinear boundary conditions. The Newton-Raphson iteration scheme is used to solve the reduced nonlinear matrix equation. The local iterative scheme is first applied to two one-dimensional problems (analytical solutions are possible) with different nonlinear boundary conditions. It is then applied to a two-region problem. Finally, the local iterative scheme is applied to two cavity problems in which radiation plays a role in the heat transfer.