一维波方程随机均质化的时间范围

M. Schäffner, B. Schweizer
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引用次数: 0

摘要

具有随机快速振荡系数的波方程可以在有界时间间隔上进行经典同质化;解在同质化极限上收敛于具有常数系数的波方程的解。但在大时间尺度上,这种情况就不复存在了:即使在周期性为 ε 的情况下,经典同质化在时间为 ε - 2 阶时也会失效。我们考虑在尺度 ε 上具有随机快速振荡系数的一维波方程,并对临界时间尺度 ε - β 感兴趣,从这里开始经典均质化失效。在一般情况下,我们根据校正器的增长率推导出 β 的上界和下界。在具有匹配阻抗的 i.i.d. 系数的特定情况下,我们证明临界时间尺度为 ε - 1 。
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The time horizon for stochastic homogenization of the one-dimensional wave equation
The wave equation with stochastic rapidly oscillating coefficients can be classically homogenized on bounded time intervals; solutions converge in the homogenization limit to solutions of a wave equation with constant coefficients. This is no longer true on large time scales: Even in the periodic case with periodicity ε, classical homogenization fails for times of the order ε − 2 . We consider the one-dimensional wave equation with random rapidly oscillation coefficients on scale ε and are interested in the critical time scale ε − β from where on classical homogenization fails. In the general setting, we derive upper and lower bounds for β in terms of the growth rate of correctors. In the specific setting of i.i.d. coefficients with matched impedance, we show that the critical time scale is ε − 1 .
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