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1.
二阶非线性中立型微分方程的振动和渐近性   总被引:9,自引:0,他引:9  
傅希林  俞元洪 《应用数学》1993,6(2):228-230
考虑二阶非线性中立型时滞微分方程[r(t)[y(t)+py(t—τ)]′]′+q(t)f[y(t—σ)]=0,(1)其中r,q:[t_0,∞)→(0,∞),f∈C(R,R),p,τ,σ是非负常数,p<1,对于y≠0有yf(y)>0和f′(y)≥0.本文研究方程(1)的振动和渐近性,所得结果不仅适用于非中立型情形,而且也推广了文[1]和[2]中的某些结果. 定理1 设  相似文献   

2.
设p和q是[a,∞)上的实连续函数,α>0,考虑四阶线性微分方程y~(4)+p(t)y″+q(t)y=0.(1)近年来,[1—3]在p≤0,q≤0时研究过方程(1)的解的振动性,但还没见到关于非负系数情况的工作,本文试图在这方面作些初步研究.我们所说的解都指非零解,其他概念也与[1—3]相同. 引理1 设p≥0,q>0,二阶线性微分方程u″+pu=0是非振动的,y(t)是方程(1)的非振动解,则存在c>a,在[c,∞)上或是y(t)y″(t)>0或是y(t)y″(t)<0. 证设y(t)是方程(1)确定在[a,∞)上的非振动解,不失一般性,设有b≥a,在[b,∞)上y(t)>0.  相似文献   

3.
设f(z)为一亚纯函数,其级p< ∞。re~(iω_1),re~(iω_2),…,re~(iω_q)(r≥0)为q条射线,其中0≤ω_1<ω_2<…<ω_q<2π,q≥1。本文证明了若方程:f(z)=0,f(z)=∞,f~((l))(z)=1(l≥0,f~((0))≡f)的根均分布在包含上述q条射线的q个窄形区域中,又δ(0,f) δ(∞,f) δ(1,f~((l))>0,则  相似文献   

4.
将空间曲线的一般式方程 F1(x,y,z) =0F2 (x,y,z) =0 化为参数方程x =x(t)y =y(t)z =z(t)是个难点 .而在计算两类曲线积分时 ,由于公式中曲线方程是由参数形式给出的 ,因此会遇到这个问题 .本文采用把曲线投影到坐标面上的方法 ,通过投影曲线标准方程的参数方程达到化空间曲线的一般式方程为参数方程的目的 .最后给出此问题的讨论在计算两类曲线积分时应用的例 .例 1 将曲线 L 的一般式方程x2 y2 z2 -x 3 y -z -4 =02 x -2 y -z 1 =0化为参数方程 .解 在方程中消去 z,得曲线 L 在 xoy平面上的投影曲线为L′:5 x2 -8xy 5 y2 …  相似文献   

5.
利用亚纯函数的Nevanlinna值分布理论,研究了一类二阶复微分方程f″+A(z)f′+B(z)f=0解的增长性,其中A(z)是方程ω″+P(z)ω=0的非平凡解,P(z)是n次多项式.证明了B(z)在适当条件的假设下,方程的每一个非平凡解为无穷级的结果,推广了以前一些文献的结论.  相似文献   

6.
超越型二阶周期线性微分方程复振荡的一个结果   总被引:1,自引:0,他引:1  
高仕安 《应用数学》2002,15(3):85-88
本文证明:设B(ζ)=g1(1/ζ) g2(ζ),其中g1(t)和g2(t)都是整数,且至少有一是级小于1的超越整函数。令A(z)=B(e^z)。对于方程ω″ A(z)ω=0的某解f(z)≠0,如果其零点较少,则f(z)和f(z 2πi)线性相关。并且上方程的任二线性无关解至少有一零点收敛指数为无穷。这一结论大大改进了作者先前的一个结果。  相似文献   

7.
利用Ho lder不等式研究一类非线性项具时滞的二阶中立型时滞微分方程{r(t)[y(t)+p(t)y(t-τ)]′2m+1}′+q(t)f[y(t-σ)]=0(t>t0)的振动性.给出了该方程的解振动的若干充分条件,所得结果推广了已有的相应结论.  相似文献   

8.
二阶奇异非线性边值条件的上下解方法   总被引:1,自引:1,他引:0  
郭彦平  葛渭高  朱玉峻 《数学学报》2003,46(5):1007-101
本文利用上下解方法,讨论奇性边值问题(py’)’+ p(t)q(t)f(t,y,py’)=0,0相似文献   

9.
本文在时间刻度T上定义新的L2(T)空间,利用Weyl圆理论研究了二阶动态方程Ly=-[p(t)y△]△+q(t)yσ=λyσ,(其中p(t)∈Cˊrd,q(t)∈Crd,q(t)>0,λ∈C0)的极限点型与极限圆型的分类问题.并在此基础上研究了方程Ly=λyσ的有界扰动问题,得到了扰动状态下极限圆型的不变性准则.  相似文献   

10.
一维奇异p-Laplace方程的上下解方法[英文]   总被引:1,自引:0,他引:1  
本文讨论了一维奇异 p Laplace方程( φp( y′) )′+ q(t) f(t,y) =0 ,0 相似文献   

11.
Summary The paper investigates the equation(1.1) in the two cases:i) p≡0,ii) p(≠0) is either bounded or satisfies |(p(t,x,y,z,u)|⩽(A0+|y|+|u|+|z| Ψ(t) where A0 is a constant. For the casei) the asymptotic stability (in the large) of the trivial solution x=0 is investigated and for the caseii) a general estimate and two boundedness results are obtained for solutions of(1.1). The results extend those obtained by Harrow[1] for the same equation(1.1). Entrata in Redazione il 18 novembre 1971.  相似文献   

12.
The Chebyshev polynomials have good approximation properties which are not affected by boundary values. They have higher resolution near the boundary than in the interior and are suitable for problems in which the solution changes rapidly near the boundary. Also, they can be calculated by FFT. Thus they are used mostly for initial-boundary value problems for P.D.E.'s (see [1, 3-4, 6, 8-11]). Maday and Quarterom discussed the convergence of Legendre and Chebyshev spectral approximations to the steady Burgers equation. In this paper we consider Burgers-like equations.$$\begin{cases}∂_iu+F(u)_x-vu_{zx}=0, & -1≤x≤1, 0<t≤T \\ u (-1,t) =u (1,t) =0, & 0≤t≤T & (0.1)\\ u (x,0) =u_0(x), & -1≤x≤1\end{cases}$$ where $F\in C(R)$ and there exists a positive function $A\in C(R)$ and a constant $p>1$ such that $$|F(z+y)-F(z)|\leq A(z)(|y|+|y|^p).$$ We develop a Chebyshev spectral scheme and a pseudospectral scheme for solving (0.1) and establish their generalized stability and convergence.  相似文献   

13.
莫德泽 《数学学报》1994,37(4):482-490
本文中,我们给出了丢番图方程的解x,y,z,w的上界,其中p,q是给定的互素的正整数,a,b,c,d是给定的适合abed≠0的整数,此外,我们将指出在具体情形下如何把上界降低到方程允许的实际的解.最后,我们将用这个方法来解方程19.5x·17y=12.5z+41.17w+14, 5. 3x· 13y + 20= 7. 3z + 14. 13w和 13· 2x+ 5· 3y= 25. 2z+ 11. 3w.  相似文献   

14.
We obtain exact solutions U(x, y, z, t) of the three-dimensional sine-Gordon equation in a form that Lamb previously proposed for integrating the two-dimensional sine-Gordon equation. The three-dimensional solutions depend on arbitrary functions F(α) and ϕ(α,β), whose arguments are some functions α(x, y, z, t) and β(x, y, z, t). The ansatzes must satisfy certain equations. These are an algebraic system of equations in the case of one ansatz. In the case of two ansatzes, the system of algebraic equations is supplemented by first-order ordinary differential equations. The resulting solutions U(x, y, z, t) have an important property, namely, the superposition principle holds for the function tan(U/4). The suggested approach can be used to solve the generalized sine-Gordon equation, which, in contrast to the classical equation, additionally involves first-order partial derivatives with respect to the variables x, y, z, and t, and also to integrate the sinh-Gordon equation. This approach admits a natural generalization to the case of integration of the abovementioned types of equations in a space with any number of dimensions. __________ Translated from Teoreticheskaya i Matematicheskaya Fizika, Vol. 158, No. 3, pp. 370–377, March, 2009.  相似文献   

15.
An alternative method of solving Lagrange's first-order partial differential equation of the form $$(a_1x+b_1y+c_1z)p+(a_2x+b_2y+c_2z)q=a_3x+b_3y+c_3z,$$ where p=∂z/∂x, q=∂z/∂y and a_i, b_i, c_i (i=1,2,3) are all real numbers has been presented here.  相似文献   

16.
在共振点附近的一类二阶泛函微分方程的解析解   总被引:3,自引:0,他引:3  
在复域C内研究一类包含未知函数迭代的二阶微分方程x″(z)=G(z,x(z),x~2(z),…,x~m(z))解析解的存在性.通过Schr(?)der变换,即x(z)=y(αy~(-1)(z)),把这类方程转化为一种不含未知函数迭代的泛函微分方程α~2y″(αz)y″(z)-αy′(αz)y″(z)= (y′(z))~3G(y(z),y(αz),…,y(α~mz)),并给出它的局部可逆解析解.本文不仅讨论了双曲型情形0<|α|<1和共振的情形(α是一个单位根),而且还在Brjuno条件下讨论了共振点附近的情形(即单位根附近).  相似文献   

17.
设b是大于3的正奇数.运用初等方法讨论了方程(bn)x+(2n)x+(2n)y=((b+2)n)y=((b+2)n)z适合(x,y,z)≠(1,1,1)的正整数解(x,y,z,n).证明了:i)对于任何给定的正整数N,存在无穷多个b可使该方程有满足min{x,y,z}≥N的正整数解(x,y,z,n);ii)对于任何给定的b,该方程仅有有限多组正整数解(x,y,z,n)满足y>z=x.  相似文献   

18.
稳定性理论中微分方程与微分差分方程的等价性问题   总被引:1,自引:0,他引:1  
秦元勋 《数学学报》1958,8(4):457-472
<正> §1.问题的提出任取一最简单的开式控制系统如图1.  相似文献   

19.
We consider the mixed problem for the hyperbolic partial differential-functional equation of the first order where is a function defined by z (x,y)(t, s) = z(x + t, y + s), (t, s) [–, 0] × [0, h]. Using the method of bicharacteristics and the method of successive approximations for a certain integral-functional system we prove, under suitable assumptions, a theorem of the local existence of generalized solutions of this problem.  相似文献   

20.
In the present paper we show that the integral functional is lower semicontinuous with respect to the joint convergence of yk to y in measure and the weak convergence of uk to u in L1. The integrand f: G × N × m , (x, z, p) f(x, z, p) is assumed to be measurable in x for all (z,p), continuous in z for almost all x and all p, convex in p for all (x,z), and to satisfy the condition f(x,z,p)(x) for all (x,z,p), where is some L1-function.The crucial idea of our paper is contained in the following simple  相似文献   

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