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FERMAT'S AND HUYGENS' PRINCIPLES, AND HYPERBOLIC EQUATIONS AND THEIR EQUIVALENCE IN WAVEFRONT CONSTRUCTION

机译:费马原理和惠更斯原理,双曲型方程及其在波浪面构造中的等价性

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Consider propagation of a wavefront in a medium. According to Fermat's principle a ray, travelling from one point P_0 to another point P_1 in space, chooses a path such that the time of transit is stationary. Given initial position of a wavefront Ω_0, we can use rays to construct the wavefront Ω_t at any time t. Huygens' method states that all points of a wavefront Ω_0 at t = 0 can be considered as point sources of spherical secondary wavelets and after time t the new position Ω_t of the wavefront is an envelope of these secondary wavelets. The equivalence of the two methods of construction of a wavefront Ω_t in a medium governed by a general hyperbolic system of equations does not seem to have been proved. Hyperbolic equations have their own method of construction of a wavefront. We shall discuss this still open (as far as I know) problem for a general hyperbolic system and briefly sketch the relation between the three methods for a particular case when the medium is governed by Euler equations of a polytropic gas in free space.
机译:考虑波前在介质中的传播。根据费马原理,光线从空间中的一个点P_0传播到另一点P_1时,选择的路径应使传输时间固定。给定波前Ω_0的初始位置,我们可以在任何时间t使用射线构造波前Ω_t。惠更斯的方法指出,在t = 0时,波前Ω_0的所有点都可以视为球形次级子波的点源,并且在时间t之后,波前的新位置Ω_t是这些次级子波的包络。似乎尚未证明在由一般双曲方程组控制的介质中构造波前Ω_t的两种方法的等效性。双曲方程具有自己的波前构造方法。我们将讨论一般双曲系统的这个尚待解决的问题(据我所知),并简要概述当介质由自由空间中的多变气体的欧拉方程控制时,针对特定情况的三种方法之间的关系。

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