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1.
当O〈a〈2时,积分∫^∞x sint/t^αdt收敛.本文研究在2≤a〈4时,反常积分∫^∞x sint/t^αdt当x→0^+时的估计式.  相似文献   

2.
<正> 大家知道在分析中已有多种方法计算概率积分 integral from 0 to ∞ e~(-x~2)dx 与 Fresnel 积分 integral from 0 to ∞ cosx~2dx,integral from 0 to ∞ sin x~2dx 的值,Yzeren,J.V.在美国数学月刊上曾发表了这两个积分的一个新求法.此外,Fresnel 积分也可以用复积分的方法求得,这可在任何一本复变函数的书中找到,但是这通常是在假定已知概率积分的条件下求得的.其实,概率积分也是可以用复积分法求得的.是谁最先用复变方法求得概率积分似乎有不同的说法,但不管怎样,我们可以从 Riemann 给出 Zeta 函数的函数方程的一个证明中得到这个积分值 (见[2] p.26或[3] p.198).现将 Yzeren 的分析方法作一点修改,与概率积分的复积分求法一并介绍给大家.  相似文献   

3.
根据无穷限反常积分∫a^+∞f(x)dx收敛的柯西准则和定积分的性质,讨论被积函数f(x)当x→∞时。的极限状态,并得出当无穷限反常积分∫a^+∞f(x)dx收敛且f(x)在[a,+∞)上连续,或者无穷限反常积分∫a^+∞f(x)dx绝对收敛时,存在数列{xn}∩[a,+∞]且xn→+∞(n→∞),使limn→∞xnf(xn)=0.  相似文献   

4.
+∞∫-∞e-x22dx=2π(1)式(1)是概率论中常用的积分,常见的证法是利用了极坐标变换[1],或利用Γ函数的性质[2].笔者给出一种利用旋转体体积公式的新证法.设I=+∞∫-∞12πe-x22dx,则(1)式等价于I=1.由于I2=(+∞∫-∞12πe-x22dx)2=+∞∫-∞12πe-x22dx+∞∫-∞12πe-y22dy=+∞∫-∞∫+∞-∞12πe-x2+2y2dxdy被积函数z=f(x,y)=12πe-x22+y2,-∞相似文献   

5.
本文借用几何直观和力学意义,在直角坐标系下用两种方法证明integral form n=-∞to ∞e~(-x~2)dx=π~(1/2)。方法一在有关的广义积分收敛的条件下,我们把旋转体积概念推广到积分限为无穷的情况。xoy面上的曲线y=e~(-x~2)绕y轴旋转一周,所得旋转体的体积为(如图)  相似文献   

6.
∫-∞^+∞e-(x2)/(2)dx=√2π(1)式(1)是概率论中常用的积分,常见的证法是利用了极坐标变换,或利用Γ函数的性质.笔者给出一种利用旋转体体积公式的新证法.  相似文献   

7.
+∞摘要将无穷限反常积分的敛散性与无穷级数的敛散性相联系,讨论反常积分∫a f (x)d x收敛的必要条+∞件。若被积函数 f (x)在[a ,+∞)上单调连续或其导函数有界,则limx→+∞ f (x)=0就是∫a f (x)d x收敛的必要条件。  相似文献   

8.
从无穷积分∫+∞ a f(x)dx收敛与无穷远极限lim x→+∞f(x)=0之间的关系展开论述,研究在广义积分∫+∞ a f(x)dx收敛的前提下,无穷远极限lim x→+∞f(x)=0的一个充分条件.在此基础上,适当减弱条件得到该条件的推广形式,为更好的解决无穷远极限lim x→+∞f(x)=0的问题提供更一般的方法.  相似文献   

9.
张宪 《高等数学研究》2000,3(4):34-35,37
讨论了当广义积分∫a ∞f(x)dx收敛时,极限linx→ ∞f(x)=0的各种条件。  相似文献   

10.
给出了在 Lp,2 p<∞ ,范意义下 ,核下自由项均属于 H函数类的多维 Fredholm积分方程类近似解的ε-计算复杂性估计 .  相似文献   

11.
利用函数的傅里叶展开式可求得级数∞∑n=11/n2+λ2及∞∑n=1(-1)m/n2+λ2的和,而通过引入复数并利用欧拉公式可求得级数∞∑n=1 1/n2+λ2及∞∑n=1(-1)m/n2+λ2的和.  相似文献   

12.
利用Euler公式求三角级∞∑m=1 sinmx/n与∞∑m=1 cosmx/m的和函数并讨论其一致收敛性.  相似文献   

13.
求出函数f(x)=xk的Fourier系数并将其代人Parseval等式,继而利用第二数学归纳法可证明:数项级数∞∑n=1 1/n2k的和能够表示为π2k/dk的形式.其中对于任意确定的k值.dk以为一常数.证明过程同时给出了求解dk的方法.  相似文献   

14.
Lp(Rm × Rn) boundedness is considered for the multiple Marcinkiewicz integral. Some size conditions implying the LP(Rm × Rn) boundedness of the multiple Marcinkiewicz integral for some fixed 1 < p <∞ are obtained.  相似文献   

15.
SOME REMARKS ABOUT THE R-BOUNDEDNESS   总被引:2,自引:0,他引:2       下载免费PDF全文
Let X,Y be UMD-spaces that have property (α), 1< p< ∞ and let M be anR-bounded subset in L(X, Y). It is shown that {T(M_k)_(k∈z): M_k, k(M_(k l)-M_k) ∈M for k∈Z} is an R-bounded subset of L(L~p (0,2π; X), L~p(0,2π; Y)), where T(M_m)_(k∈zdenotes the L~p-multiplier given by the sequence (M_k)_(k∈z), This generalizes a resultof Venni [10]. The author uses this result to study the strongly L~p-well-posedness ofevolution equations with periodic boundary condition. Analogous results for operator-valued L~p-multipliers on R are also given.  相似文献   

16.
In this paper, we study the inversion formula for recovering a function from its windowed Fourier transform. We give a rigorous proof for an inversion formula which is known in engineering. We show that the integral involved in the formula is convergent almost everywhere on $\mathbb {R}$ as well as in Lp for all 1 < p < ∞ if the function to be reconstructed is.  相似文献   

17.
设(X,d1,f1∞)与(Y ,d2,g1,∞)为两个非自治动力系统,h是从(X,d1,f.∞)到(Y,d2,g1∞)的拓扑半共轭.通过对自治动力系统中的h一极小覆盖的研究,本文得到了以下结论:1)对于任意的Y∈Y及X∈h-1(y),orb(x,f1∞)被h映射为orb(y,g1∞),w(x,f1∞)被h映射为w(y,g1∞);2)在(X,d1,f1∞)中引入关于拓扑半共轭的h-极小覆盖的定义,证明了h一极小覆盖的存在性;3)对于任意的XEX和Y∈Y,在(w(z,f1∞),f1∞。(x,f1,∞)与(w(y,g∞),g1,∞(y,g1∞))均构成原系统的子系统的前提下,R(f1∞)被h映射为R(g1∞).这些结论丰富了非自治动力系统的内容.  相似文献   

18.
Let X be a Banach space. We show that each m : ? \ {0} → L (X ) satisfying the Mikhlin condition supx ≠0(‖m (x )‖ + ‖xm ′(x )‖) < ∞ defines a Fourier multiplier on B s p,q (?; X ) if and only if 1 < p < ∞ and X is isomorphic to a Hilbert space; each bounded measurable function m : ? → L (X ) having a uniformly bounded variation on dyadic intervals defines a Fourier multiplier on B s p,q (?; X ) if and only if 1 < p < ∞ and X is a UMD space. (© 2005 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)  相似文献   

19.
The paper is concerned with certain kinds of random processes in infinite graphs. A finite trail of a graph which cannot be continued from either end is called terminated, and a finite trail is called terminable of it is a segment of a finite terminated trail; analogously for 1 - ∞ trails, finite paths, and 1 - ∞ paths.For k = 1,2,3,…, there exist graphs which contain 2 - ∞ paths and have node-connectivity k and in which no finite path and no 1 - ∞ path is terminable, and also such graphs in which every finite path and every 1 - ∞ path is terminable. In any graph with infinite node-connectivity every node of valency N0 is the end-node of terminated 1 - ∞ paths. There exist graphs with node-connectivity N0 in which every 1 - ∞ path is terminable. For λ = 1,2,3,…, there exist graphs which contain 2 - ∞ paths and have edge-connectivity λ and in which no finite trail and no 1 - ∞ trail is terminable, and also such graphs in which every finite trail and every 1 - ∞ trail is terminable. In contrast to the situation for 1 - ∞ paths, every connected infinite graph in which every 1 - ∞ trail is terminable contains at least one node of odd edge-degree and if in addition every finite trail is terminable, then there are at least two nodes of odd edge-degree.  相似文献   

20.
证明了傅立叶超函数和扩充傅立叶超函数可用爱米特热方程的解来表示,且用以表示的解有很良好的性质.  相似文献   

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