关于复合函数的一个错误命题

文[1]称:若已知f[g(x)]的定义域为A,则f(x)的定义域就是函数g(x)(x∈A)的值域.错误!例1设函数f(x)=2x,函数g(x)=x2,则复合函数f[g(x)]=2x2.显然,复合函数f[g(x)]的定义域是R,函数g(x)(x∈R)的值域[0,+∞),但函数f(x)的定义域是R,而不是函数g(x)(x∈R)的值     

平均值函数的性质及应用

设函数 f (x)在 (-∞ , ∞ )上连续 ,当 x≠ 0时 ,我们称 F(x) =1x∫x0 f (t) dt为 f (x)在 [0 ,x]上的平均值函数 ,本文将介绍平均值函数 F(x)的若干性质并举例说明其应用 .一、F(x)的性质性质 1　 f(x)是 [0 ,x](或 [x,0 ])上的有界函数 ,F(x)也是 [0 ,x]或 [x,0 ]上的有界函数 .性质 2　若 f (x)为奇 (偶 )函数 ,则 F(x)也为奇 (偶 )函数 .性质 3　若 f(x)是周期为 T(T>0 )的周期函数 ,则limx→ ∞1x∫x0f (t) dt=1T∫T0f (t) dt (1 )　　　性质 4　若 f(x)为单调递增 (减 )函数 ,则 F(x)也为单调递增 (减 )函数 .性质 5　若对任意…     

多元函数的微分法则

我们知道 ,若函数 x =φ( s,t) ,y =ψ( s,t)在点 ( s,t)有连续导数 ,函数 z =f ( x,y)在相应点 ( x,y) =(φ( s,t) ,ψ( s,t) )有连续偏导数 ,则复合函数 z=f (φ( s,t) ,ψ( s,t) )在点 ( x,t)可微 ,且dz =( z x x s+ z y y s) ds+( z x x t+ z y y t) dt同样有 ,若函数 x =φ( t) ,y =ψ( t)在点 t可微 ,函数 z =f ( x,y)在相应点 ( x,y) =(φ( t) ,ψ( t) )有连续偏导数 ,则复合函数 z =f (φ( t) ,ψ( t) )在点 t可微 ,且 dz =( z x+ z ydydt) dt;若函数 x =φ( s,t)在点 ( s,t)有连续偏导数 ,函数 z =f ( x)在相应点 x =φ( s,t)有…     

函数单调性与最值问题的探究

<正>1引言函数的单调性和奇偶性是函数的基本性质.常见的函数单调性的求法有:(1)定义法;(2)图象法;(3)导数法.还有一些与函数单调性有关的结论:若函数f(x),g(x)均为增(减)函数,则f(x)+g(x)为增(减)函数;若f(x)为增(减)函数,则-f(x)为增(减)函数;若函数f(x)为增(减)函数且f(x)>0,     

一道课本例题的探究

人民教育出版社出版的高中数学第三册 (选修Ⅱ )《函数的极限》一节有这样一道例题 :limx→ 1x2 - 1x - 1=2 .此例很好地说明了函数f(x) 在点x =x0 处的极限是a ,仅与函数f(x) 在点x0 附近的函数值的变化有关而与函数f(x) 在点x0 的值无关 .笔者认为 ,它不仅对此类不连续函数求     

约化为三对角矩阵的改进Newton算法

一、引言 本文用g(x)表示目标函数的梯度,G(x)表示目标函数f(x)在x点的Hessain矩阵,p(x)表示在x点进行一维搜索的方向。用Newton法求目标函数f(x)极小时是通过所谓求解方程组     

对一道稳派联考题的解法思考

题目已知函数f(x)=x2+2x+alnx(a∈R).(Ⅰ)当a=-4时,求f(x)的最小值;(Ⅱ)若函数f(x)在区间(0,1)上为单调函数,求实数a的取值范围;     

在全实轴上的一个特殊的二阶微分方程反问题(英文)

为了解轴对称的KDV方程要考虑以下问题 曾考虑以上二端奇型反问题,他指出函数Q(x)可由2×2的谱矩阵来确定。本文指出当Q(x)=x q(x),而q(x)满足以下条件时则函数q(x)可由一个谱函数来确定,在§1我们引进黎曼函数证明了函数φ(x,λ)和φ(x,λ)间变换的存在性,其中是方程(0.1)当Q(x)=x时的解,φ(x,λ)是方程(0.1)当Q(x)=x q(x)时的解。在§2中,根据Titchmarsh-Kodaira理论给出对一个谱函数的完备性。最后推导出类似于Gel’fand-Levitan方程。     

我为高考设计题目

题67已知函数f(x)=ax3+x2-ax,a,x∈R.(1)若函数f(x)在区间(1,2)上不是单调函数,试求a的取值范围;(2)直接写出(不需给出演算步骤)函数g(x)     

函数的周期性与图像对称性的相互关系

全文约定:函数y=f(x)的定义域为R．结论1 若函数y=f(x)的图像关于x=a 和x=b(a≠b)对称,则函数y=f(x)为周期函数．证明∵函数y=f(x)的图像关于x= a和x=b对称, ∴ f(-x)-f(x 2a), 且 f(-x)-f(x 2b)．∴ f(x 2a)=f(x 2b)．∴ f(x)=f[x (2a-2b)]．∴函数y=f(x)是周期函数,2a-2b是     

Study of the blow-up of solutions of systems of equations of hydrodynamic type

Mathematical Notes - We study the initial boundary-value problem for three-dimensional systems of equations of pseudoparabolic type. The system is similar to the Oskolkov system, but differs from...     

Characterization of types of asymptotic discernibility of families of hypotheses

We give a characterization of the types of asymptotic discernibility of families of hypotheses in the case of hypothetical measures that are not, in general, mutually absolutely continuous. The case when the logarithm of the likelihood ratio admits an asymptotic expansion of the type of an expansion with local asymptotic normality is examined in detail. Examples are studied.Translated fromTeoriya Sluchainykh Protsessov, Vol. 15, pp. 64–71, 1987.     

Distribution of types of symmetry of tensors of high degree

The asymptotic distribution of tensors of degree N in symmetry types is studied in this paper.Translated from Zapiski Nauchnykh Seminarov Leningradskogo Otdeleniya Matematicheskogo Instituta im. V. A. Steklova AN SSSR, Vol. 155, pp. 181–186, 1986.     

Singularities of Solutions of One Class of Equations of Continuum Mechanics

We analyze one class of families of integral equations and describe the dependence of the singularities of solutions of integral equations on the dimensions of the families of kernels of equations. On the basis of these results, we propose procedures for the construction of approximate solutions for a small parameter.     

Determination of asymptotic solutions of problems of nonlinear theories of thermoviscoelasticity

It is shown that the asymptotic solution of a problem of the nonlinear theory of thermoviscoelasticity, if it exists, can be found directly from the solution of the asymptotic boundary-value problem without completely solving the starting problem.M. V. Lomonosov Moscow State University. Translated from Mekhanika Polimerov, No. 3, pp. 395–400, May–June, 1976.     

Emptiness of set of points of lower semicontinuity of Lyapunov exponents

We consider parametric families of differential systems with coefficients that are bounded and continuous on the half-line and uniformly in time continuously depend on a real parameter. For each Lyapunov exponent, we construct a family such that the Lyapunov exponent of its systems treated as a function of the parameter is not a lower semicontinuous function for any value of the parameter.