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A selfadjoint second order hyperbolic system

机译:自伴二阶双曲系统

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We consider a second order hyperbolic system of the type Lu=utt-Buxx=f(x,t), (x,t)∈Tm (1) where matrix B is a nonsingular constant matrix with positive eigenvalues, (x,t)R2 and u,fRn. The set Tm is defined to be Tm={(x,t)|0≤t≤1/m,|x|≤1-mt} (2) where m=min{μk} and is any eigenvalue of the matrix B. We will show that, under the condition u(x,0)=0, |x|1, a symmetric Green's function Gn×n can be constructed [K. Kreith, A selfadjoint problem for the wave equation in higher dimensions, Comput. Math. Appl. 21 (5) (1991) 12–132] so that u(x,t)=∫∫Tm Gnxn(x,t;ξ,τ)f(ξ,τ) dξ dτ (3)for any function fL2(Tm). This will imply that the operator L in (1) over the set L2(Tm) of functions given by Eq. (3) and u(x,0)=0, |x|1, is selfadjoint. We also note that the same result holds for u in (1), under the condition that ut(x,0)=0, |x|1. We further note that when B has only one eigenvalue μ2, the function u in Eq. (3) satisfies a boundary condition similar to that of Kalmenov [T. Kalmenov, On the spectrum of a selfadjoint problem for the wave equation, Akad. Nauk. Kazakh SSR Vestnik 1 (1983) 63–66] on the characteristic boundaries of Tμ.
机译:我们考虑类型为Lu = utt-Buxx = f(x,t),(x,t)∈Tm(1)的二阶双曲系统,其中矩阵B是具有正特征值(x,t)的非奇异常数矩阵R2和u,fRn。集合Tm定义为Tm = {(x,t)|0≤t≤1/ m,| x |≤1-mt}(2)其中m = min {μk},并且是矩阵B的任何特征值我们将证明,在u(x,0)= 0,| x | 1的条件下,可以构造对称的格林函数Gn×n。 Kreith,高维波动方程的自伴问题,计算。数学。应用21(5)(1991)12–132],因此对于任何函数fL2(Tm),u(x,t)=∫∫TmGnxn(x,t;ξ,τ)f(ξ,τ)dξdτ(3) )。这将意味着,式(1)中的算子L在方程(2)给出的函数集合L2(Tm)上。 (3)和u(x,0)= 0,| x | 1是自伴的。我们还注意到,在条件ut(x,0)= 0,| x | 1的情况下,对于(1)中的u也具有相同的结果。我们进一步注意到,当B仅具有一个特征值μ2时,方程中的函数u。 (3)满足与卡尔梅诺夫[T。 Kalmenov,关于波动方程的自伴问题的频谱,Akad。娜克哈萨克斯坦SSR Vestnik 1(1983)63-66]。

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