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The Dirichlet Problem for the Fourth Order Nonlinear Ordinary Differential Equations at Resonance

机译:共振四阶非线性常微分方程的Dirichlet问题

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摘要

Landesman-Lazer's type efficient sufficient conditions are established for the solvability of the two-point boundary value problem u((4))(t) = p(t)u(t) + f(t, u(t)) + h(t) for a = t = b, u((i))(a) = 0, u((i))(b) = 0, (i = 0, 1), where h, p is an element of L([a, b]; R) and f is an element of K([a, b] x R; R), in the case where the linear problem w((4))(t) = p(t)w(t), w((i))(a) = 0, w((i))(b) = 0, (i = 0, 1) has nontrivial solutions. The results obtained in the paper are optimal in the sense that if f = 0, i.e. when nonlinear equation turns to the linear equation, from our results follows the first part of Fredholm's theorem.
机译:Landesman-Lazer的类型有效充分条件是为双点边值问题的可解性U((4))(t)= p(t)u(t)u(t)+ f(t,u(t))+ h (t)对于<= t <= b,u((i))(a)= 0,u((i))(b)= 0,(i = 0,1),其中h,p是一个L([a,b]; r)和f的元素是k([a,b] x r; r)的元素,在线性问题w((4))(t)= p( t)w(t),w((i))(a)= 0,w((i))(b)= 0,(i = 0,1)具有非竞争解决方案。本文中获得的结果是最佳的,如果F = 0,即非线性方程转向线性方程,我们的结果遵循Fredholm定理的第一部分。

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