首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 31 毫秒
1.
We consider bilinear control systems of the form y(t)=Ay(t)+u(t)By(t) where A generates a strongly continuous semigroup of contraction (etA)t?0 on an infinite-dimensional Hilbert space Y whose scalar product is denoted by 〈.,.〉. We suppose that this system is unbounded in the sense that the linear operator B is unbounded from the state Y into itself. Tacking into account eventual control saturation, we study the problem of stabilization by (possibly nonquadratic) feedback of the form u(t)=−f(〈By(t),y(t)〉). Applications to the heat equation is considered.  相似文献   

2.
In this paper, we are concerned with the oscillation of second order superlinear differential equations of the form
(a(t)y(t))+p(t)y(t)+q(t)f(y(t))=0.  相似文献   

3.
In this paper, we are concerned with the oscillation of third order nonlinear delay differential equations of the form
(r2(t)(r1(t)y))+p(t)y+q(t)f(y(g(t)))=0.  相似文献   

4.
In this paper we will establish some oscillation criteria for the second-order nonlinear neutral delay dynamic equation
(r(t)((y(t)+p(t)y(tτ)Δ)γ)Δ)+f(t,y(tδ))=0  相似文献   

5.
Let (T, , P) be a probability space, a P-complete sub-δ-algebra of and X a Banach space. Let multifunction t → Γ(t), t T, have a (X)-measurable graph and closed convex subsets of X for values. If x(t) ε Γ(t) P-a.e. and y(·) ε Ep x(·), then y(t) ε Γ(t) P-a.e. Conversely, x(t) ε F(Γ(t), y(t)) P-a.e., where F(Γ(t), y(t)) is the face of point y(t) in Γ(t). If X = , then the same holds true if Γ(t) is Borel and convex, only. These results imply, in particular, extensions of Jensen's inequality for conditional expectations of random convex functions and provide a complete characterization of the cases when the equality holds in the extended Jensen inequality.  相似文献   

6.
As a simple model for lattice defects like grain boundaries in solid state physics we consider potentials which are obtained from a periodic potential V=V(x,y) on R2 with period lattice Z2 by setting Wt(x,y)=V(x+t,y) for x<0 and Wt(x,y)=V(x,y) for x?0, for t∈[0,1]. For Lipschitz-continuous V it is shown that the Schrödinger operators Ht=−Δ+Wt have spectrum (surface states) in the spectral gaps of H0, for suitable t∈(0,1). We also discuss the density of these surface states as compared to the density of the bulk. Our approach is variational and it is first applied to the well-known dislocation problem (Korotyaev (2000, 2005) [15] and [16]) on the real line. We then proceed to the dislocation problem for an infinite strip and for the plane. In Appendix A, we discuss regularity properties of the eigenvalue branches in the one-dimensional dislocation problem for suitable classes of potentials.  相似文献   

7.
New oscillation criteria of second-order nonlinear differential equations   总被引:1,自引:0,他引:1  
By employing a class of new functions Φ=Φ(t,s,l) and a generalized Riccati technique, some new oscillation and interval oscillation criteria are established for the second-order nonlinear differential equation
(r(t)y(t))+Q(t,y(t),y(t))=0.  相似文献   

8.
In this paper, a class of multiobjective control problems is considered, where the objective and constraint functions involved are f(tx(t), ?(t), y(t), z(t)) with x(t) ∈ Rn, y(t) ∈ Rn, and z(t) ∈ Rm, where x(t) and z(t) are the control variables and y(t) is the state variable. Under the assumption of invexity and its generalization, duality theorems are proved through a parametric approach to related properly efficient solutions of the primal and dual problems.  相似文献   

9.
In this paper, the authors study the existence of periodic solutions to a p-Laplacian Rayleigh differential equation with a delay as follows:
(φp(y(t)))+f(y(t))+g(y(tτ(t)))=e(t),  相似文献   

10.
Let (x(t),y(t))? be a solution of a Fuchsian system of order two with three singular points. The vector space of functions of the form P(t)x(t)+Q(t)y(t), where P,Q are real polynomials, has a natural filtration of vector spaces, according to the asymptotic behavior of the functions at infinity. We describe a two-parameter class of Fuchsian systems, for which the corresponding vector spaces obey the Chebyshev property (the maximal number of isolated zeros of each function is less than the dimension of the vector space). Up to now, only a few particular systems were known to possess such a non-oscillation property. It is remarkable that most of these systems are of the type studied in the present paper. We apply our results in estimating the number of limit cycles that appear after small polynomial perturbations of several quadratic or cubic Hamiltonian systems in the plane.  相似文献   

11.
Conditions on a(t), g(t), and f(t) have been found under which the bounded nonoscillatory solutions of the equation y(n)(t) ? a(t) y(g(t)) = f(t) approach zero. For the even order equation y(2n)(t) ? a(t) y(g(t)) = f(t) the delay is shown to be causing the oscillatory behavior.  相似文献   

12.
We look for conditions under which all solutions of the nonlinear ordinary differential equation y(n) + f(t, y) = 0, t ? 0, ?∞ < y < ∞, are oscillatory, as well as consider the asymptotic behaviour of the nonoscillatory solutions.  相似文献   

13.
We consider an inverse problem for identifying a leading coefficient α(x) in −(α(x)y′(x))′ + q(x)y(x) = H(x), which is known as an inverse coefficient problem for the Sturm-Liouville operator. We transform y(x) to u(xt) =  (1 + t)y(x) and derive a parabolic type PDE in a fictitious time domain of t. Then we develop a Lie-group adaptive method (LGAM) to find the coefficient function α(x). When α(x) is a continuous function of x, we can identify it very well, by giving boundary data of y, y′ and α. The efficiency of LGAM is confirmed by comparing the numerical results with exact solutions. Although the data used in the identification are limited, we can provide a rather accurate solution of α(x).  相似文献   

14.
In this paper we study centers of planar polynomial Hamiltonian systems and we are interested in the isochronous ones. We prove that every center of a polynomial Hamiltonian system of degree four (that is, with its homogeneous part of degree four not identically zero) is nonisochronous. The proof uses the geometric properties of the period annulus and it requires the study of the Hamiltonian systems associated to a Hamiltonian function of the form H(xy)=A(x)+B(xy+C(xy2+D(xy3.  相似文献   

15.
In this paper we consider the wave equation with nonlinear damping and source terms. We are interested in the interaction between the boundary damping −|yt(L,t)|m−1yt(L,t) and the interior source |y(t)|p−1y(t). We find a sufficient condition for obtaining the blow-up solution of the problem. Furthermore, we also obtain that the solution may blow up even if mp.  相似文献   

16.
This paper is concerned with the oscillation of second-order nonlinear neutral dynamic equations of the form
(r(t)((y(t)+p(t)y(τ(t)))Δ)γ)Δ+f(t,y(δ(t)))=0,  相似文献   

17.
We would like to investigate on the solution to the automatic control problem given by the differential equation y′(t) = f(ty(t), w(t)) for a given initial function x in the initial domain D(x, ω, Y) for almost all t in the interval I, with controls given by w(t) = g(ty(t), T(y)(t)), where T is a nonanticipating and Lipschitzian operator. The result will be generalized for a dynamical system y′(t) = f(ty(t), T(y), u(t)).  相似文献   

18.
Several oscillation criteria are given for the second-order damped nonlinear differential equation (a(t)[y′(t)]σi +p(t)[y′(t)]σ +q(t)f(y(t)) = 0, where σ > 0 is any quotient of odd integers, a ϵ C(R, (0, ∞)), p(t) and q(t) are allowed to change sign on [to, ∞), and f ϵ Cl (R, R) such that xf (x) > 0 for x≠0. Our results improve and extend some known oscillation criteria. Examples are inserted to illustrate our results.  相似文献   

19.
This paper deals with nonoscillatory behaviour of solutions of third-order nonlinear functional differential equations of the form y‴ + p(t)y′ + q(t)F(y(g(t))) = 0. It has been shown that under certain conditions on coefficient functions, the nonoscillatory solutions of this equation tends to either zero or ∓∞ as t → ∞.  相似文献   

20.
This paper is concerned with the linear ODE in the form y′(t) = λρ(t)y(t) + b(t), λ < 0 which represents a simplified storage model of the carbon in the soil. In the first part, we show that, for a periodic function ρ(t), a linear drift in the coefficient b(t) involves a linear drift for the solution of this ODE. In the second part, we extend the previous results to a classical heat non-homogeneous equation. The connection with an analytic semi-group associated to the ODE equation is considered in the third part. Numerical examples are given.  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号