TY - JOUR

T1 - The large-time development of the solution to an initial-boundary value problem for the Korteweg-de Vries equation on the negative quarter-plane

AU - Leach, John

PY - 2009/8/1

Y1 - 2009/8/1

N2 - In this paper, we consider an initial-boundary value problem for the Korteweg-de Vries equation on the negative quarter-plane. The normalized Korteweg-de Vries equation considered is given by
u(tau) + uu(x) + u(xxx) = 0, x <0, tau > 0,
where x and tau represent dimensionless distance and time, respectively. In particular, we consider the case when the initial and boundary conditions are given by u(x, 0) = u(i) for x <0 and u(0, tau) = u(b), partial derivative/partial derivative xu(0, tau) = u(bx) for tau > 0. Here the initial value u(i) <0 and we restrict attention to boundary values u(b) and u(bx) in the ranges 0 <u(b) <-2u(i) and vertical bar u(bx)vertical bar <1/root 3 (u(b)-u(i))(-u(b)-2u(i))(1/2), respectively. The method of matched asymptotic coordinate expansions is used to obtain the large-tau asymptotic structure of the solution to this problem, which exhibits the formation of a steady state solution. A brief discussion is also given of the large-tau asymptotic structure to this problem when u(i) <0, u(i) <u(b) <0 and u(bx) = 0. (C) 2009 Elsevier Inc. All rights reserved.

AB - In this paper, we consider an initial-boundary value problem for the Korteweg-de Vries equation on the negative quarter-plane. The normalized Korteweg-de Vries equation considered is given by
u(tau) + uu(x) + u(xxx) = 0, x <0, tau > 0,
where x and tau represent dimensionless distance and time, respectively. In particular, we consider the case when the initial and boundary conditions are given by u(x, 0) = u(i) for x <0 and u(0, tau) = u(b), partial derivative/partial derivative xu(0, tau) = u(bx) for tau > 0. Here the initial value u(i) <0 and we restrict attention to boundary values u(b) and u(bx) in the ranges 0 <u(b) <-2u(i) and vertical bar u(bx)vertical bar <1/root 3 (u(b)-u(i))(-u(b)-2u(i))(1/2), respectively. The method of matched asymptotic coordinate expansions is used to obtain the large-tau asymptotic structure of the solution to this problem, which exhibits the formation of a steady state solution. A brief discussion is also given of the large-tau asymptotic structure to this problem when u(i) <0, u(i) <u(b) <0 and u(bx) = 0. (C) 2009 Elsevier Inc. All rights reserved.

U2 - 10.1016/j.jde.2009.03.019

DO - 10.1016/j.jde.2009.03.019

M3 - Article

SN - 1090-2732

VL - 247

SP - 1206

EP - 1228

JO - Journal of Differential Equations

JF - Journal of Differential Equations

IS - 4

ER -