infinite boundary value problem
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2017 ◽  
Vol 8 (1) ◽  
pp. 517-532 ◽  
Author(s):  
Ahmed Mohammed ◽  
Giovanni Porru

Abstract Motivated by the work [9], in this paper we investigate the infinite boundary value problem associated with the semilinear PDE {Lu=f(u)+h(x)} on bounded smooth domains {\Omega\subseteq\mathbb{R}^{n}} , where L is a non-divergence structure uniformly elliptic operator with singular lower-order terms. In the equation, f is a continuous non-decreasing function that satisfies the Keller–Osserman condition, while h is a continuous function in Ω that may change sign, and which may be unbounded on Ω. Our purpose is two-fold. First we study some sufficient conditions on f and h that would ensure existence of boundary blow-up solutions of the above equation, in which we allow the lower-order coefficients to be singular on the boundary. The second objective is to provide sufficient conditions on f and h for the uniqueness of boundary blow-up solutions. However, to obtain uniqueness, we need the lower-order coefficients of L to be bounded in Ω, but we still allow h to be unbounded on Ω.


2011 ◽  
Vol 2011 ◽  
pp. 1-22
Author(s):  
Dajun Guo

The author discusses the multiple positive solutions for an infinite boundary value problem of first-order impulsive superlinear integrodifferential equations on the half line in a Banach space by means of the fixed point theorem of cone expansion and compression with norm type.


2000 ◽  
Vol 5 (2) ◽  
pp. 65-83 ◽  
Author(s):  
Cezar Avramescu ◽  
Cristian Vladimirescu

Using functional arguments, some existence results for the infinite boundary value problemx˙=F(t,x),x(−∞)=x(+∞)are given. A solution of this problem is frequently called, from Poincaré, homoclinic.


This work examines the stability of viscous, incompressible flow along a streamwise corner, often called the corner boundary-layer problem. The semi-infinite boundary value problem satisfied by small-amplitude disturbances in the ‘blending boundary layer’ region is obtained. The mean secondary flow induced by the corner exhibits a flow reversal in this region. Uniformly valid ‘first approximations’ to solutions of the governing differ­ential equations are derived. Uniformity at infinity is achieved by a suitable choice of the large parameter and use of an appropriate Langer variable. Approximations to solutions of balanced type have a phase shift across the critical layer which is associated with instabilities in the case of two-dimensional boundary layer profiles.


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