An Averaging Theorem for Perturbed KdV Equation

preprint2013arXivOpen access

Abstract

We consider a perturbed KdV equation: [\dot{u}+u_{xxx} - 6uu_x = εf(x,u(\cdot)), \quad x\in \mathbb{T}, \quad\int_\mathbb{T} u dx=0.] For any periodic function u(x)u(x), let I(u)=(I1(u),I2(u),...)∈R+∞I(u)=(I_1(u),I_2(u),...)\in\mathbb{R}_+^{\infty} be the vector, formed by the KdV integrals of motion, calculated for the potential u(x)u(x). Assuming that the perturbation εf(x,u(⋅))εf(x,u(\cdot)) is a smoothing mapping (e.g. it is a smooth function εf(x)εf(x), independent from uu), and that solutions of the perturbed equation satisfy some mild a-priori assumptions, we prove that for solutions u(t,x)u(t,x) with typical initial data and for 0⩽t≲ε−10\leqslant t\lesssim ε^{-1}, the vector I(u(t))I(u(t)) may be well approximated by a solution of the averaged equation.

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