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1.
新题征展(3)     
题组新编1.(1)设M={x|f(x)=0}、N={x|g(x)=0},则{x|f(x)·g(x)=0}为(  );(A)M (B)N (C)M∪N (D)以上都不对(2)设f(x)=x-1x+3,g(x)=x+3x-1,则集合{x|f(x)·g(x)=0}=  ;(3)设函数f(x)、g(x)的定义域依次是F、G,且M={x|f(x)=0}、N={x|g(x)=0},则{x|f(x)·g(x)=0}=  .2.(1)设m、k∈N,则Cnn+Cnn+1+Cnn+2+…+Cnn+k=  ;(2)求…  相似文献   

2.
下列四种中学数学教学的权威文献都涉及到方程f1(x)·f2(x)=0的解集问题.(1)高级中学课本《代数》上册(必修)在引入并集的概念和解释其应用时写道:方程(x2-4)·(x2-1)=0的解集,可以从求方程x2-4=0的解集与方程x2-1=0的解集...  相似文献   

3.
复合函数的求导法则是求导运算的重要法则;对于y=f(u),u=g(x),复合函数y=f〔g(x)〕的求导法则的证明有一个很自然的想法:ΔyΔx=ΔyΔu·ΔuΔx,limΔx→0ΔyΔx=limΔu→0ΔyΔu·limΔx→0ΔuΔx;但是,当Δx→0时,Δu可能等于0,此时ΔyΔu没有意义,所以上面很直接的想法行不通;一般的证明采取另外的方法[1],[2];本文仍从上面直观的想法出发,加以改进,得到了又一个证明;定理 若y=f(u)在u可导,函数u=g(x)在x可导,则复合函数y=f〔g(x)…  相似文献   

4.
本文研究二阶线性常微分方程  d2 ydx2 + [λ2q1(x) + λq2(x,λ)]y = 0 ,其中  q1(x) = (x - μ1)(x - μ2)(x - μ3)f(x) ,  f(x) ≠0,μ1 < μ2 < μ3 ,λ为大参数,即具有三个转向点的方程· 而  q2(x,λ) = ∑∞i=0gi(x)λ- i  ( 此时g0(x) 0)· 本文使用JL函数得到方程在转向点附近形式一致有效渐近解的完全表达式·  相似文献   

5.
§1.IntroductionConsiderthefolowingddimensionalVlasovPoisonsystem,d=2,3,tf+v·xf-E·vf=0,f(0,x,v)=f0(x,v),E(t,x)=c(d)∫x-y|x...  相似文献   

6.
利用单调函数的性质证明一类不等式苏万春(吉林省永吉三中)由单调函数定义知:若函数f(x)在区间M上是增函数,则对于M上的任意两个不同的自变量的值x1和x2都有(x1-x2)·[f(x1)-f(x2)]>0(反之亦然);若函数f(x)在区间M上是减函数...  相似文献   

7.
关于f~n(x)=x的讨论张伟年(中国科学院成都计算所数理中心610041)首先从一简单的中学数学题谈起.问题x和c为实数,求:(a)满足f(f(x))=x的c值;(b)满足f(f(x))=x的x值.解由f(f(x))=x,x≠0得显然当2x-1=0?..  相似文献   

8.
重视常规方法解题——从今年一道高考题引发的思考桂元今年高考理科(24)题是这样的:“设二次函数f(x)=ax2+bx+c(a>0),方程f(x)-x=0的两个根x1,x2满足0<x1<x2<1a.(Ⅰ)当x∈(0,x1)时,证明x<f(x)<x1;(...  相似文献   

9.
读了《数学通讯》1999年第4期刊登的刘汉顶老师的《关于一类函数最小值问题的一种处理方法》一文后深受启发,本文特给出不能应用均值不等式处理“和一定,积最大”另一类函数的最大值问题的处理方法,以此作为前文的一个补充.定理 设初等函数f(x)在区间I上恒有0<f(x)<d,d为正常数,则当且仅当|2f(x)-d|取最小值时,函数g(x)=f(x)·[d-f(x)]取最大值.证 (1)若2f(x)=d在I上有解,则结论显然成立.(2)若2f(x)=d在I上无解,则由初等函数的连续性知:2f(x)>d或…  相似文献   

10.
陈绍仲 《数学学报》1997,40(3):333-344
本文用随机分析方法证明了拟线性抛物型方程ut+f(u)ux、uxx=0,u(0,x)=u0(x)在u0有界可测,f连续且f>0条件下,其解当→0时收敛于拟线性方程ut+f(u)ux=0,u(0,x)=u0(x)的熵解,即论证了“沾性消失法”解此方程的正确性,1957年Oleinik曾用差分方法解决了此问题。这里用概率方法重新获得此结果。  相似文献   

11.
求解微分方程初值问题的一种弧长法   总被引:1,自引:0,他引:1  
对于连续介质力学问题中导出的微分方程初值问题,常常具有解奇异性,如不连续、Stif性质或激波间断·本文通过在相应空间,引入一个或数个弧长参数变量,克服解的奇异性·对于常微分方程组引入弧长参数变量后,奇异性得以消除和削弱,应用一般的解常微分方程组的方法(如Runge_Kuta法)求解·对于偏微分方程引入弧长参数变量后,在相应的空间离散成常微分方程组,用解奇异性常微分方程组相同的方法即可求解·本文给出了两个算例  相似文献   

12.
解非线性方程的二阶敛速指数迭代法   总被引:21,自引:0,他引:21  
吴新元 《计算数学》1998,20(4):367-370
1.gi言文[1,2]中利用ODE方法[']给出解非线性方程在卜6I内的根x"的两个非线性迭代法其中'w由文[2]中(5)式确定.令h-1方法(2)具有M阶敛速,方法(3)是线性收敛的.它们是李雅普诺夫渐近稳定性和文[4]中Lambert提出的解Stiff方程的非线性方法相结合的结果.Lllbll't在每个小区间【Ln,Ln+1]上用一个有理函数月O一句(I十利来逼近微分方程的解z二"I,*。);*。Ek;q,使得对I_,J。)一J_,"乙十;,J。)=。_+i,l'(Ln,10)一人,而tim0(7;00)一0".那么我们能否在每个小区间【Ln,Ln+1]上用一个指…  相似文献   

13.
An effective characterization is given for a class of generalized nonlinear diffusion equations with power law dependent terms. Further, a new auxiliary equation ansatz is derived. Consequently, new exact traveling wave trigonometric function, solitary-like and Weierstrass elliptic solutions to a subclass are obtained by means of an auxiliary equation method and a generalized Riccati equation expansion method.  相似文献   

14.
In this paper, we combine the unified and the explicit exponential finite difference methods to obtain both analytical and numerical solutions for the Newell-Whitehead-Segel–type equations which are very important in mathematical biology. The unified method is utilized to obtain various solitary wave solutions for these equations. Numerical solutions of the specific case studies are investigated by using the explicit exponential finite difference method ensures the accuracy and reliability of the proposed scheme. After obtaining the approximate solutions, convergence analysis and error estimation (the error norms and absolute errors) are presented by comparing these results with the analytical obtained solutions and other methods in the literature through tables and graphs. The obtained analytical and numerical results are in good agreement.  相似文献   

15.
应用改进的简单方程法求得Cahn-Allen方程和Jimbo-Miwa方程的精确解,这些解包括双曲函数解、三角函数解.当对双曲函数解中的参数取特殊值时,可以得到了孤立波解.当对三角函数解中的参数取特殊值时,可以得到对应的周期波函数解.实践证明,简单方程法对于研究非线性数学物理方程具有非常广泛的应用意义.  相似文献   

16.
Discretisation of the integral equations of acoustic scattering yields a system of linear equations with full coefficient matrices. In recent years a number of fast algorithms for the solution of this system have been proposed. In this paper we present a complete analysis for a fast multipole method for the Helmholtz equation. A one-level diagonal form of the multipole method is applied to a hypersingular integral equation arising from 2d scattering theory. The error of the approximation is analysed and the results used to establish the complexity of the method.  相似文献   

17.
In this work, the variational iteration method (VIM) is used for analytic treatment of the linear and nonlinear ordinary differential equations, homogeneous or inhomogeneous. The method is capable of reducing the size of calculations and handles both linear and nonlinear equations, homogeneous or inhomogeneous, in a direct manner. However, for concrete problems, a huge number of iterations are needed for a reasonable level of accuracy.  相似文献   

18.
The Adomian decomposition method is used to obtain analytic and approximate solutions of the space-and time-fractional telegraph equations. The space- and time-fractional derivatives are considered in the Caputo sense. The analytic solutions are calculated in the form of series with easily computable terms. Some examples are given. The results reveal that the Adomian method is very effective and convenient.  相似文献   

19.
In this paper, using three distinct computational methods we obtain some new exact solutions for the generalized modified Degasperis-Procesi equation (mDP equation) ut-uxxt+(b+1)u2ux=buxuxx+uuxxx. We show the graph of some of the new solutions obtained here with the aim to illustrate their physical relevance. Mathematica is used. Finally some conclusions are given.  相似文献   

20.
In this article a numerical method for solving a two‐dimensional transport equation in the stationary case is presented. Using the techniques of the variational calculus, we find the approximate solution for a homogeneous boundary‐value problem that corresponds to a square domain D2. Then, using the method of the fictitious domain, we extend our algorithm to a boundary value problem for a set D that has an arbitrary shape. In this approach, the initial computation domain D (called physical domain) is immersed in a square domain D2. We prove that the solution obtained by this method is a good approximation of the exact solution. The theoretical results are verified with the help of a numerical example. © 2009 Wiley Periodicals, Inc. Numer Methods Partial Differential Eq 2010  相似文献   

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