n阶常系数非齐次线性微分方程的降阶解法

给出一阶线性非齐次微分方程的积分因子解法,避免了常数变易法带来的不便和不自然;给出,n阶常系数非齐次线性微分方程的降阶解法,可以看出,高阶常系数线性非齐次微分方程最终都可以归结为求解一阶线性微分方程,从而避免了待定系数法求非齐次方程特解的繁琐,并最终说明了一般微积分教材中只给出两种类型常系数非齐次线性微分方程的待定系数解法的原因．     

用逆微分算子法求n阶常系数线性一般非齐次微分方程特解公式

本文利用逆微分算子及其线性性质 ,给出了求 n阶常系数线性一般非齐次项微分方程特解公式 ,     

常系数非齐次线性微分方程组的初等解法

利用初等变换将常系数非齐次线性微分方程组化为由若干个相互独立的高阶常系数非齐次线性微分方程组成的方程组,再利用高阶常系数齐次线性微分方程的特征根法和非齐次方程的待定系数法求该方程组的基本解组及特解,最后通过初等变换求原方程组的基本解组及特解,从而可求出其通解.     

求常系数线性非齐次微分方程特解的矩阵方法

求常系数线性非齐次微分方程特解的矩阵方法秦宗慈（镇江高等专科学校，镇江２１２００３）对于常系数线性非齐次微分方程，如何简化求特解的运算，是高等数学教学中值得探讨的一个课题．本文给出一种方法，它仍属于待定系数法，但省去了把所谓“形式特解”代入线性微分算...     

常系数非齐次线性微分方程特解的另一种求法

将常系数线性微分方程转化为一阶常系数线性微分方程组,并利用线性微分方程组的基解矩阵的性质和矩阵指数的性质以及非齐次线性微分方程组的常数变易公式,得到了常系数非齐次线性微分方程的积分形式的特解公式,并通过实例说明所得结论的有用性.     

求高阶常系数非齐次线性微分方程特解的新方法

求高阶常系数非齐次线性微分方程:y(n)+P1y(n-1)+…+Pny=f(x)(P1,P2,…,Pn是实数)的特解的一种新方法.首先将该方程降为n个一阶非齐次线性微分方程组:其中w1,w2,…,wn是对应的齐次方程的特征方程:tn+P1tn-1+…+Pn=0的n个根.然后得出了求原方程一个特解的迭代公式.     

求二阶和三阶常系数非齐次线性微分方程特解的一个公式

基于微分算子分裂的思想,受到一阶线性方程求解公式的启发,运用多重积分交换积分顺序的技巧,得到求二阶和三阶常系数非齐次线性微分方程特解的一般性公式.     

应用特征多项式简化求常系数非齐次线性微分方程特解的方法

应用特征多项式简化求常系数非齐次线性微分方程特解的方法杨琪瑜（南京林业大学．南京２１００３７）目前国内外的高等数学教材在常系数非齐次线性微分方程的章节中，在求自由项为，（ｄ一Ｐ。（。）。“等形式的特解９“时，几乎全采取待定系数法，即先定出特解ｇ”形式...     

常微分方程通解、特解、所有解的区别与联系

通过具体实例分析、讨论了高等数学中常微分方程的通解、特解和微分方程的所有解之间的区别与联系,并对高等数学教材中二阶线性微分方程的降阶法与二阶常系数非齐次线性微分方程特解求解过程中的作法进行了说明.     

求高阶非齐次微分方程(组)特解的矩阵解法

给出了求一类高阶非齐次线性微分方程(组)特解的矩阵解法.即由对应齐次微分方程(组)的n个特解以及非齐次微分方程(组)的自由项构成某线性方程组的增广矩阵,并对该增广矩阵进行初等行变换,即可求得非齐次微分方程(组)特解的一种简便方法.     

Riccati微分方程特解新求法的研究

通过对一般Riccati方程进行初等变换,使之变为特殊的Riccati方程,然后利用公式、观察实验,或利用二阶微分方程的特解,或利用一阶微分方程组的特解等方法,求得这些Riccati方程的特解.     

线性微分方程的微分算子级数解法

介绍了微分算子级数法及其求解线性常微分方程通解、特解的原理、方法和实例.这个方法和其它解法的差别,在于不借助其它学科知识的启示,直接通过方程中微分算子的运算求出方程的特解或通解.     

A research into the numerical method of Dirichlet's problem of complex Monge-Ampère equation on Cartan-Hartogs domain of the third type

Monge-Ampère equation is a nonlinear equation with high degree, therefore its numerical solution is very important and very difficult. In present paper the numerical method of Dirichlet's problem of Monge-Ampère equation on Cartan-Hartogs domain of the third type is discussed by using the analytic method. Firstly, the Monge-Ampère equation is reduced to the nonlinear ordinary differential equation, then the numerical method of the Dirichlet problem of Monge-Ampère equation becomes the numerical method of two point boundary value problem of the nonlinear ordinary differential equation. Secondly, the solution of the Dirichlet problem is given in explicit formula under the special case, which can be used to check the numerical solution of the Dirichlet problem.     

常微分方程中的反问题

研究某函数或函数组是什么常微分方程的通解或特解,这可以称为常微分方程中的反问题.这类问题,可以用"微分法"来解决.研究这类问题的意义在于通过利用"微分法"及"逆向思维方法"解决反问题的过程来加强对常微分方程理论内涵的深刻理解.     

Exact Solutions and Integrability of the Duffing – Van der Pol Equation

The force-free Duffing–Van der Pol oscillator is considered. The truncated expansions for finding the solutions are used to look for exact solutions of this nonlinear ordinary differential equation. Conditions on parameter values of the equation are found to have the linearization of the Duffing–Van der Pol equation. The Painlevé test for this equation is used to study the integrability of the model. Exact solutions of this differential equation are found. In the special case the approach is simplified to demonstrate that some well-known methods can be used for finding exact solutions of nonlinear differential equations. The first integral of the Duffing–Van der Pol equation is found and the general solution of the equation is given in the special case for parameters of the equation. We also demonstrate the efficiency of the method for finding the first integral and the general solution for one of nonlinear second-order ordinary differential equations.     

用“升阶法”求解一类一阶线性微分方程——兼谈逆向思维能力的培养

"升阶法"能够把一类特殊的一阶线性微分方程化为二阶常系数齐次线性微分方程求解,而一般的一阶线性微分方程的求解问题可以转化为二元函数全微分的求积问题.利用"升阶法"和"全微分法"对学生进行逆向思维训练,培养学生的创新思维能力.     

On the asymptotic stability of discontinuous systems analysed via the averaging method

The averaging method is one of the most powerful methods used to analyse differential equations appearing in the study of nonlinear problems. The idea behind the averaging method is to replace the original equation by an averaged equation with simple structure and close solutions. A large number of practical problems lead to differential equations with discontinuous right-hand sides. In a rigorous theory of such systems, developed by Filippov, solutions of a differential equation with discontinuous right-hand side are regarded as being solutions to a special differential inclusion with upper semi-continuous right-hand side. The averaging method was studied for such inclusions by many authors using different and rather restrictive conditions on the regularity of the averaged inclusion. In this paper we prove natural extensions of Bogolyubov’s first theorem and the Samoilenko-Stanzhitskii theorem to differential inclusions with an upper semi-continuous right-hand side. We prove that the solution set of the original differential inclusion is contained in a neighbourhood of the solution set of the averaged one. The extension of Bogolyubov’s theorem concerns finite time intervals, while the extension of the Samoilenko-Stanzhitskii theorem deals with solutions defined on the infinite interval. The averaged inclusion is defined as a special upper limit and no additional condition on its regularity is required.     

非齐次“Euler方程组”的解

本文研究一类特殊的非齐次变系数微分方程组——Euler方程组的解法.首先,建立特征方程求出齐次Euler方程组的通解;其次,针对一类特殊的非齐次项利用待定系数法给出了非齐次Euler方程组的特解.