阻尼Mathieu方程WKB近似的收敛性

dwight nwaigwe
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引用次数: 1

摘要

考虑微分方程${ m\ddot{x} +\gamma \dot{x} -x\epsilon \cos(\omega t) =0}$, $0 \leq t \leq T$。基本解集的形式由Floquet理论决定。在极限为$m \to 0$的情况下,我们可以应用WKB理论得到这个基本集的一阶近似。WKB理论指出,这种近似在$m \to 0$时变得更好,因为对于给定的$T$, sup范数的差作为$m$的函数有界。然而,周期部分和指数部分的收敛性没有得到解决。我们证明了这些分量是收敛的。周期部分特征指数的渐近误差为$O(m^2)$和$O(m)$。
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On the convergence of WKB approximations of the damped Mathieu equation
Consider the differential equation ${ m\ddot{x} +\gamma \dot{x} -x\epsilon \cos(\omega t) =0}$, $0 \leq t \leq T$. The form of the fundamental set of solutions are determined by Floquet theory. In the limit as $m \to 0$ we can apply WKB theory to get first order approximations of this fundamental set. WKB theory states that this approximation gets better as $m \to 0$ in the sense that the difference in sup norm is bounded as function of $m$ for a given $T$. However, convergence of the periodic parts and exponential parts are not addressed. We show that there is convergence to these components. The asymptotic error for the characteristic exponents are $O(m^2)$ and $O(m)$ for the periodic parts.
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