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1.
叶国菊  安天庆 《数学进展》2005,34(6):741-745
本文证明了如果X是不含c0的Banach空间,f是定义在区间I0包含R^m上取值于Panach空间X的函数,并且,在I0上Henstock可积,则总存在I0的一个非退化子区间J,使得f在J上McShane可积,从而对Kartak的一个问题作出了肯定的回答.  相似文献   

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本文通过几个典型物理习题,着重说明在应用微积分原理和方法计算物理问题时应注意的一些问题.  相似文献   

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本文举例说明 ,如何通过构造递推序列的方法 ,对被积函数是与自然数 n有关的一些定积分进行计算 .读者从中可以看出此方法的简捷和优越 ,用以抛砖引玉 .1 计算问题上的应用在某些定积分计算问题中 ,若被积函数是与自然数 n有关 ,则可把整个积分看成一个序列的一般项 ,然后根据其积分的结构特点 ,恰当地找出它的递推公式 .通常首先考虑 In± In- 1,In± In- 2 ,In/In- 1等型 ,这样再经过递推 ,问题往往就可简捷而巧妙地得到解决 .例 1 计算著名的狄利克莱 (Dirichlet)积分∫π0sin(n 12 ) xsin x2dx,n =0 ,1 ,2 ,…解 令 In =∫π0s…  相似文献   

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本文给出了将部分重积分问题转化为定积分求解的一些推论,讨论了应用中运用“微元法”解决实际问题的方法。  相似文献   

5.
含有积分的一些极限问题的解法   总被引:1,自引:1,他引:0  
在处理积分极限问题时 ,若将积分计算出来再求极限 ,有时候难以办到 ,如 ex2 、sinxx 、 cosx2等函数的原函数不能用初等函数表示 ,所以无法先积分再求极限 .实际上 ,往往也不需要如此 ,本文介绍几种处理此类问题的方法 .一、利用积分中值定理利用积分中值定理将积分号去掉 ,然后再求极限 ,这是一种常用方法 .例 1 求 limn→∞∫n ansinxx dx  (a >0 ) .解 因 sinxx 在 [n,n a]连续 ,故依积分中值定理 ,存在ξn ∈ [n,n a],使得limn→∞∫n ansinxx dx =limn→∞ (a .sinξnξn) =limξn→∞ (a .sinξnξn) =0 .  例 2 设函数 …  相似文献   

6.
叶国菊  李秉彝 《数学研究》2004,37(3):250-258
在本文中,我们定义和研究了I0Rm到Banach空间X中函数的强McShane积分,直接证明了强Mcshane积分与Bochner积分是等价的,McShane积分与强Mcshane积分等价当且仅当Banach空间X有限维. 从而部分地回答了R.A.Gordon的一个公开问题.  相似文献   

7.
复积分的概念起源于计算实定积分的问题,根据历史上原有的简单方法解释柯西积分定理和留数定理可以使学生更加深刻地理解其基本内涵.  相似文献   

8.
利用变分法证明平面调和函数的外问题的确切形式;在此基础上,建立外问题的具有间接变量的等价边界积分方程;传统的外问题及边界积分方程不具有普遍适用性,本文对此进行了详细的讨论.  相似文献   

9.
评广义积分定义肖良渠,杨紫彦(辽宁本溪本钢工学院117000)(辽宁本溪本钢技校)本文所谈的是无穷区间上的广义积分的定义.为了说明问题,先看几个例子.例1limcosxdx=lim[sinx]=limsinb它不存在.b一十∞例2lim2xdx=li...  相似文献   

10.
王娟 《工科数学》2008,(5):194-197
计算极限是极限理论的重要内容,大多数函数的极限运算问题可用常规的算法及运算法则解决.而无限多项的和式的极限是极限论当中很难求解的,具有一定难度.本文给出了积分在和式极限求解中的若干命题及计算方法.  相似文献   

11.
In this paper, the authors cosider the derivation of the exact distributions of the ratios of the extreme roots to the trace of the Wishart matrix. Also, exact percentage points of these distributions are given and their applications are discussed.  相似文献   

12.
The valuation of levered investment in the practice is made with the WACC approach, even if the superior technique of the APV is available. The paper shows that the APV can be interpreted as the arbitrage free value of the portfolio made by an investment and a supporting loan. Therefore the WACC evaluation, generally different from the APV, allows for arbitrage. We provide various conditions which completely characterize the sign of the error as a functions of all the variables entering the model.  相似文献   

13.
通过建立常微分方程模型 ,分析了预防和隔离措施对 SARS发病率的影响 ,并把计算结果与实际统计数据进行了比较 ,结果表明 ,及时高效的预防和隔离措施能够有效地控制 SARS的传播 .  相似文献   

14.
Two recent findings necessitate a closer look at the existing standard models of particle physics and cosmology. These are the discovery of neutrino oscillation, and hence a non-zero mass on the one hand and, on the other, observations of distant supernovae which indicate that contrary to popular belief, the universe would continue to expand for ever, possibly accelerating in the process. In this paper it is pointed out that relatively recent studies which indicate a stochastic, quantum vacuum underpinning and a fractal structure for space time, reconcile both of the recent observations, harmoniously.  相似文献   

15.
The spectrum of the translations in local quantum field theory will be analyzed in order to show that in a positive energy representation without vacuum vector and with lowest mass m1 there is no gap in the spectrum which is larger than 2m1. In particular in a zero mass representation there is no hole at all. These results are obtained with methods of analytic functions of several complex variables.  相似文献   

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For a Riesz operator T on a reflexive Banach space X with nonzero eigenvalues denote by Ei; T) the eigen-projection corresponding to an eigenvalue λi. In this paper we will show that if the operator sequence is uniformly bounded, then the Riesz operator T can be decomposed into the sum of two operators Tp and Tr: T = Tp + Tr, where Tp is the weak limit of Tn and Tr is quasi-nilpotent. The result is used to obtain an expansion of a Riesz semigroup T(t) for t ≥ τ. As an application, we consider the solution of transport equation on a bounded convex body.  相似文献   

19.
Let $\mathcal{G}(z):=\sum_{n\geqslant0} z^{2^{n}}(1-z^{2^{n}})^{-1}$ denote the generating function of the ruler function, and $\mathcal {F}(z):=\sum_{n\geqslant} z^{2^{n}}(1+z^{2^{n}})^{-1}$ ; note that the special value $\mathcal{F}(1/2)$ is the sum of the reciprocals of the Fermat numbers $F_{n}:=2^{2^{n}}+1$ . The functions $\mathcal{F}(z)$ and $\mathcal{G}(z)$ as well as their special values have been studied by Mahler, Golomb, Schwarz, and Duverney; it is known that the numbers $\mathcal {F}(\alpha)$ and $\mathcal{G}(\alpha)$ are transcendental for all algebraic numbers α which satisfy 0<α<1. For a sequence u, denote the Hankel matrix $H_{n}^{p}(\mathbf {u}):=(u({p+i+j-2}))_{1\leqslant i,j\leqslant n}$ . Let α be a real number. The irrationality exponent μ(α) is defined as the supremum of the set of real numbers μ such that the inequality |α?p/q|<q ?μ has infinitely many solutions (p,q)∈?×?. In this paper, we first prove that the determinants of $H_{n}^{1}(\mathbf {g})$ and $H_{n}^{1}(\mathbf{f})$ are nonzero for every n?1. We then use this result to prove that for b?2 the irrationality exponents $\mu(\mathcal{F}(1/b))$ and $\mu(\mathcal{G}(1/b))$ are equal to 2; in particular, the irrationality exponent of the sum of the reciprocals of the Fermat numbers is 2.  相似文献   

20.
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