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1.
时滞Logistic方程非振动解的存在性   总被引:3,自引:0,他引:3  
本文获得了时滞Logistic方程 x'(t)=r(t)x(t)[1-a_1x(g_1(t))-a_2x(g_2(t))]~a,t≥0关于其正平衡状态x=1/(a_1+a_2)存在非振动解的充分条件与充要条件,改进并推广了Aiello中的结果.  相似文献   

2.
一阶非线性偏差变元微分方程解的振动性   总被引:7,自引:0,他引:7  
关于偏差变元微分方程解的振动性问题已在实际应用中提了出来.如文献[1,2].也越来越引起人们的重视,且得到了一些很好的结果,如文献[3—8],综述文献[9]在“一些问题”中提出了进一步研究方程x′(t)+p(t)f(x(g(t)))=0(1)的解的振动性的充分条件的课题.本文首先给出了较一般的滞后型方程x′(t)+p(t)F(x(g_1(t)),x(g_2(t)),…,x(g_n(t)))+h(t,x(t),x(g_1(t)),…,x(g_n(t)))=0(2)的解的振动的充分条件.把所得结果应用于方程(1),从而在很大程度上改进了文献[3]的结果.然后,又在 g_i(t)超前情形下,给出了方程(2)解振动的充分条件,把所得结果应用于某些文献[3,4]称之为超线性方程,得到了与滞后型亚线性方程解振动的类似结果.假定 x(t)在[t_x,+∞)上存在.记 g(t)=(?){g_i(t)}.  相似文献   

3.
本文考虑下列二阶微分方程 (r(t)x′(t))′ q(t)x′(t) p(t)x(t)=0. (1) 和 (r(t)x′(t))′ q(t)x′(t) p(t)f(x(g(t)))=0 (2)解的振动性质。我们给出了方程(1)非振动解存在的充要条件和方程(2)存在振动解的充分判据。  相似文献   

4.
一类三阶泛函微分方程周期解的存在唯一性   总被引:2,自引:0,他引:2  
利用重合度理论研究了一类三阶泛函微分方程x′′′(t)+multiply from i=1 to 2[a_ix~((i))+b_ix~((i))(t-τ_i)]+ g_1(x(t))+g_2(x(t-τ))=p(t)的2π-周期解问题,获得了该方程2π-周期解存在唯一性的若干新结论.  相似文献   

5.
研究二阶非线性变时滞微分方程x″(t)+p(t)f(x(g(t)))=0,对振动因子p(t)变符号的情况讨论了方程的振动性,通过两个已有引理得到了方程振动的两个充分条件.所得结论推广了原有的二阶非线性微分方程与变时滞微分方程当系数不变号时的振动性结论,完善了具变符号振动因子的二阶非线性变时滞微分方程的研究.  相似文献   

6.
在α>1,且0<β<α情性下研究了高阶具非线性中立项不稳定型时滞微分方程[x(t)-pxα(t-τ)](n)=q(t)xβ(t-σ),(t≥t0)的振动和非振动性.利用一些新的技巧,获得了上述方程有界解振动的振动准则和至少存在一个非振动解的非振动准则,所得结果补充和推广了已有文献部分结果.  相似文献   

7.
廖六生 《数学杂志》1992,12(4):368-374
本文考虑二阶既具正系数又具负系数的时滞微分方程(x|¨)(t)+p(t)x(t-τ)-q(t)x(t-σ)=0 (*)(其中 p(t)、q(t)是[f_o,+∝)上的非负连续函数,τ、σ是正实数)的振动性。获得了方程(*)的所有有界解振动的充分性判据;以及在 p(t)、q(t)均为常数的情况下,获得了方程(1)的所有有界解振动的一些必要条件和充分必要条件。  相似文献   

8.
某类系数变号的二阶非线性变时滞微分方程的振动性   总被引:1,自引:1,他引:0  
研究了二阶非线性变时滞微分方程x″(t)+p(t)f(x(g(t)))=0的振动性,对振动因子p(t)变号的情况,给出了两个重要的引理,并得到方程振动的一个充分性定理.所得结论推广了二阶非线性变时滞微分方程当系数不变号时原有的振动性结论.  相似文献   

9.
研究一类二阶非线性变时滞微分方程x″(t)+p(t)f(x(g(t)))=0的振动性,对振动因子p(t)可变符号的情况,通过两个引理,得出了方程振动的两个充分性定理.所得结论推广了二阶非线性变时滞微分方程当系数不变号时的振动性结论.  相似文献   

10.
具有变系数的二阶中立型差分方程   总被引:1,自引:0,他引:1  
研究一类具有变系数的二阶中立型时滞差分方程 △τ^2[x(t)-c(t)x(t-τ)]=p(t)x(t-σ),t≥t0〉0 的解的振动性,给出了该类方程一切有界解振动的几个充分条件.  相似文献   

11.
By using some differential inequality, a second-order delay differential equation(r(t)x′(t))′ p(t)x(q(t)) = 0has been investigated and some necessary condition for this equation has a nonoscillatorysolution and some sufficient condition which ensures that all of the solutions of the aboveequation are oscillatory are obtained.  相似文献   

12.
An initial boundary-value problem for the Hirota equation on the half-line,0x∞, t0, is analysed by expressing the solution q(x, t) in terms of the solution of a matrix Riemann-Hilbert(RH) problem in the complex k-plane. This RH problem has explicit(x, t) dependence and it involves certain functions of k referred to as the spectral functions. Some of these functions are defined in terms of the initial condition q(x,0) = q_0(x), while the remaining spectral functions are defined in terms of the boundary values q(0, t) = g_0(t), q_x(0, t) = g_1(t) and q_(xx)(0, t) = g_2(t). The spectral functions satisfy an algebraic global relation which characterizes, say, g_2(t) in terms of {q_0(x), g_0(t), g_1(t)}.The spectral functions are not independent, but related by a compatibility condition, the so-called global relation.  相似文献   

13.
We establish asymptotic formulas for nonoscillatory solutions of a special conditionally oscillatory half-linear second order differential equation, which is seen as a perturbation of a general nonoscillatory half-linear differential equation
$ (r(t)\Phi (x'))' + c(t)\Phi (x) = 0,\Phi (x) = |x|^{p - 1} \operatorname{sgn} x,p > 1, $ (r(t)\Phi (x'))' + c(t)\Phi (x) = 0,\Phi (x) = |x|^{p - 1} \operatorname{sgn} x,p > 1,   相似文献   

14.
获得具连续变量差分方程x(t+τ)-x(t)+p(t)x(t-rτ)=0的非振动解在脉冲扰动x(tk+τ)-x(tk)=b_kx(tk), k∈N(1)下具有保持性的充分条件.  相似文献   

15.
A necessary and sufficient condition is established in order that (i) the retarded differential equation $$y''(t) = p_0 y(t) + f(y(t - \tau _1 ),...,y(t - \tau _N ))$$ has no bounded nonoscillatory solution and (ii) the advanced differential equation $$y''(t) = p_0 y(t) + f(y(t + \tau _1 ),...,y(t + \tau _N ))$$ has no unbounded nonoscillatory solution, wherep 0≥0 and τ j > 0,1 ?i ?N, are constants. Differential inequalities related to (*) and (**) are also studied. Finally, an oscillation criterion is given for a class of differential equations containing both retarded and advanced arguments.  相似文献   

16.
In this paper, we present oscillation criteria for the second-order nonlinear dynamic equation \({[a(t)\phi_{\gamma} (x^{\Delta}(t))]^{\Delta} + p(t)\phi_{\gamma}(x^{\Delta^{\sigma}}(t)) + q_{0}(t) \phi_{\gamma}(x(g_{0}(t)))+\sum_{i=1}^{2}\int_{a_{i}}^{b_{i}}q_{i}(t,s)\phi_{\alpha_{i}(s)}(x(g_{i}(t,s))) \Delta \zeta_{i}(s)=0}\) on a time scale \({\mathbb{T}}\) which is unbounded above. Our results generalize and improve some known results for oscillation of second-order nonlinear dynamic equation. Some examples are given to illustrate the main results.  相似文献   

17.
主要讨论的是一类三阶拟线性微分方程(p(t)|u″|~(α-1)u″)′+q(t)|u|~(β-1)u=0其中α0,β0,p(t)和q(t)是定义在区间[a,∞)上的连续函数,且满足当t≥a时p(t)0,q(t)0.当t→∞时此方程满足∫_a~∞1/((p(t))~(1/α))dt=∞的特殊非振动解存在的充分必要条件.  相似文献   

18.
The interest of this paper lies in the estimates of solutions of the three kinds of Gronwail-Bihari integral inequalities:(Ⅰ) y(x)≤f(x) sum from i=1 to n(g_i(x)integral from n=0 to x(h_i(d)y(s)ds)),(Ⅱ) y(x)≤f(x) g(x)φ(integral from n=0 to x(h(s)w(y(s))ds))(Ⅲ) y(x)≤f(x) sum from i=1 to n(g_i(x)integral from n=0 to a(h_i(s)y(s)ds g_(n 1)φ(integral from n=0 to x(h_(n 1)(s)w(y(t))ds)).The results include some modifications and generalizations of the results of D. Willett, U. D. Dhongade and Zhang Binggen. Furthermore, applying the conclusion on the above inequalities to a Volterra integral equation and a differential equation, the authors obtain some new better results.  相似文献   

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