Existence and asymptotic expansion for a nonlinear wave equation associated with nonlinear boundary conditions
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文摘
Consider the initial–boundary value problem for the nonlinear wave equation

(1)

where p1, q1≥2, K1≥0 are given constants and μ, u0, u1, f, F are given functions, and the unknown function u(x,t) and the unknown boundary value P(t) satisfy the following nonlinear integral equation

(2)

where p0, q0≥2, K0≥0 are given constants and g, k are given functions.

In this paper, we consider three main parts. In Part 1, under the conditions , , μ(x,t)≥μ0>0, μtL1(0,T;L), μt(x,t)≤0, a.e. (x,t)QT; K0, K1≥0; p0, q0, p1, q1≥2, , the function f supposed to be continuous with respect to two variables and nondecreasing with respect to the second variable and some others, we prove that the problem (1) and (2) has a weak solution (u,P). If, in addition, 32b15b8871f473313da3824d75209733"" title=""Click to view the MathML source"">kW1,1(0,T), p0, p1{2}[3,+) and some other conditions, then the solution is unique. The proof is based on the Faedo–Galerkin method and the weak compact method associated with a monotone operator. For the case of q0=q1=2;p0,p1≥2, in Part 2 we prove that the unique solution (u,P) belongs to (L(0,T;H2)∩C0(0,T;H1)∩C1(0,T;L2))×H1(0,T), with utL(0,T;H1), uttL(0,T;L2), u(0,), u(1,)H2(0,T), if we assume , and some other conditions. Finally, in Part 3, with q0=q1=2; p0, p1N+1, , N≥2, we obtain an asymptotic expansion of the solution (u,P) of the problem (1) and (2) up to order N+1 in two small parameters K0, K1.

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