求解双曲方程正反问题的非标准方法

Tabita Treilande, I. Iltiņš
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摘要

我们考虑了一种非标准的方法,该方法已用于求解抛物热方程,但从未用于求解描述振荡过程的双曲方程。这项技术是由亚伯拉罕·特姆金(1919-2007)在20世纪60年代发展起来的,概念总结在A.特姆金的专著中描述,“热传导的逆方法”,莫斯科:Energija出版社,1973;464页(俄文)。该方法是基于非稳态边界条件下的非稳态热传导,初始条件对温度分布的影响减小。过了一会儿,我们就可以假设温度分布只取决于边界条件随时间的变化。双曲型方程具有相同的性质,因此检验该方法是否适用于双曲型方程是有用的。当应用Temkin方法时,我们寻求一个级数形式的解,其中每一项是给定边界条件的导数与空间变量的未知函数P的乘积。把这个级数代入给定的微分方程得到一个常微分方程组。在求解时,我们找到了空间函数p,并将经典解与该方法得到的解进行了比较。空间函数要么是多项式,要么是包含一个多项式作为加数的表达式,这取决于域的几何形状和边界条件的类型。这样的解使我们能够制定反问题来找到传播速度,知道在域的中间点的振荡幅度。本文提出的方法使我们能够得到反问题近似解的简单公式。
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Non-standard method of solving direct and inverse problems for hyperbolic equations
We consider a non-standard method that has been used for solving parabolic heat equations, but never to solve hyperbolic equations describing oscillatory processes. This technique was developed by Abraham Temkin (1919-2007) in the 1960s and the concept summary is described in the monograph by A. Temkin, “Inverse Methods of Heat Conduction”, Moscow: Energija Press, 1973; 464 p. (in Russian). The method is based on the fact that for non-stationary heat conduction with non-stationary boundary conditions, the influence of initial conditions on the temperature distribution decreases. And after a while, one can assume that the temperature distribution is determined only by a change of boundary conditions over time. Hyperbolic equations have the same property, so it is useful to check whether this method applies to hyperbolic equations. When applying Temkin’s method, we seek a solution in the form of a series where each term is a product of a derivative of the given boundary condition and an unknown function P of a space variable. Plugging the series into the given differential equation yields a system of ordinary differential equations. When solving this, we find the spatial functions P. Further, we compare the classical solution with the solution obtained by this method. The spatial functions are either polynomials or expressions that contain a polynomial as an addend, depending on the geometry of the domain and the type of the boundary conditions. Such a solution allows us to formulate the inverse problem to find the speed of propagation, knowing amplitudes of oscillations at an intermediate point of the domain. The method proposed here allows us to obtain simple formulas for approximate solution of the inverse problem.
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