658 research outputs found

    Existence of positive solutions in the superlinear case via coincidence degree: the Neumann and the periodic boundary value problems

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    We prove the existence of positive periodic solutions for the second order nonlinear equation u"+a(x)g(u)=0u" + a(x) g(u) = 0, where g(u)g(u) has superlinear growth at zero and at infinity. The weight function a(x)a(x) is allowed to change its sign. Necessary and sufficient conditions for the existence of nontrivial solutions are obtained. The proof is based on Mawhin's coincidence degree and applies also to Neumann boundary conditions. Applications are given to the search of positive solutions for a nonlinear PDE in annular domains and for a periodic problem associated to a non-Hamiltonian equation.Comment: 41 page

    Pairs of positive periodic solutions of nonlinear ODEs with indefinite weight: a topological degree approach for the super-sublinear case

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    We study the periodic and the Neumann boundary value problems associated with the second order nonlinear differential equation \begin{equation*} u'' + c u' + \lambda a(t) g(u) = 0, \end{equation*} where g ⁣:[0,+[[0,+[g \colon \mathopen{[}0,+\infty\mathclose{[}\to \mathopen{[}0,+\infty\mathclose{[} is a sublinear function at infinity having superlinear growth at zero. We prove the existence of two positive solutions when 0Ta(t) ⁣dt<0\int_{0}^{T} a(t) \!dt < 0 and λ>0\lambda > 0 is sufficiently large. Our approach is based on Mawhin's coincidence degree theory and index computations.Comment: 26 page

    A constructive approach to regularity of Lagrangian trajectories for incompressible Euler flow in a bounded domain

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    The 3D incompressible Euler equation is an important research topic in the mathematical study of fluid dynamics. Not only is the global regularity for smooth initial data an open issue, but the behaviour may also depend on the presence or absence of boundaries. For a good understanding, it is crucial to carry out, besides mathematical studies, high-accuracy and well-resolved numerical exploration. Such studies can be very demanding in computational resources, but recently it has been shown that very substantial gains can be achieved first, by using Cauchy's Lagrangian formulation of the Euler equations and second, by taking advantages of analyticity results of the Lagrangian trajectories for flows whose initial vorticity is H\"older-continuous. The latter has been known for about twenty years (Serfati, 1995), but the combination of the two, which makes use of recursion relations among time-Taylor coefficients to obtain constructively the time-Taylor series of the Lagrangian map, has been achieved only recently (Frisch and Zheligovsky, 2014; Podvigina {\em et al.}, 2016 and references therein). Here we extend this methodology to incompressible Euler flow in an impermeable bounded domain whose boundary may be either analytic or have a regularity between indefinite differentiability and analyticity. Non-constructive regularity results for these cases have already been obtained by Glass {\em et al.} (2012). Using the invariance of the boundary under the Lagrangian flow, we establish novel recursion relations that include contributions from the boundary. This leads to a constructive proof of time-analyticity of the Lagrangian trajectories with analytic boundaries, which can then be used subsequently for the design of a very high-order Cauchy--Lagrangian method.Comment: 18 pages, no figure

    Second-order ordinary differential equations with indefinite weight: the Neumann boundary value problem

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    We study the second-order nonlinear differential equation u\u2032\u2032+a(t)g(u)=0 , where g is a continuously differentiable function of constant sign defined on an open interval I 86R and a(t) is a sign-changing weight function. We look for solutions u(t) of the differential equation such that u(t) 08I, satisfying the Neumann boundary conditions. Special examples, considered in our model, are the equations with singularity, for I=R+0 and g(u) 3c 12u 12\u3c3, as well as the case of exponential nonlinearities, for I=R and g(u) 3cexp(u) . The proofs are obtained by passing to an equivalent equation of the form x\u2032\u2032=f(x)(x\u2032)2+a(t)

    Periodic solutions for critical fractional problems

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    We deal with the existence of 2π2\pi-periodic solutions to the following non-local critical problem \begin{equation*} \left\{\begin{array}{ll} [(-\Delta_{x}+m^{2})^{s}-m^{2s}]u=W(x)|u|^{2^{*}_{s}-2}u+ f(x, u) &\mbox{in} (-\pi,\pi)^{N} \\ u(x+2\pi e_{i})=u(x) &\mbox{for all} x \in \mathbb{R}^{N}, \quad i=1, \dots, N, \end{array} \right. \end{equation*} where s(0,1)s\in (0,1), N4sN \geq 4s, m0m\geq 0, 2s=2NN2s2^{*}_{s}=\frac{2N}{N-2s} is the fractional critical Sobolev exponent, W(x)W(x) is a positive continuous function, and f(x,u)f(x, u) is a superlinear 2π2\pi-periodic (in xx) continuous function with subcritical growth. When m>0m>0, the existence of a nonconstant periodic solution is obtained by applying the Linking Theorem, after transforming the above non-local problem into a degenerate elliptic problem in the half-cylinder (π,π)N×(0,)(-\pi,\pi)^{N}\times (0, \infty), with a nonlinear Neumann boundary condition, through a suitable variant of the extension method in periodic setting. We also consider the case m=0m=0 by using a careful procedure of limit. As far as we know, all these results are new.Comment: Calculus of Variations and Partial Differential Equations (2018

    Periodic solutions to planar Hamiltonian systems: high multiplicity and chaotic dynamics

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