3aSPb2. Ray chaos and two-dimensional wave fields.

Session: Wednesday Morning, December 4

Time: 8:15


Author: Yoh-ichi Fujisaka
Location: Dept. of Information Eng., Kogakuin Univ., 2665-1 Nakano-machi, Hachioji-shi, Tokyo, 192 Japan
Author: Mikio Tohyama
Location: Dept. of Information Eng., Kogakuin Univ., 2665-1 Nakano-machi, Hachioji-shi, Tokyo, 192 Japan
Author: Akira Sugimura
Location: Konan Univ., Hyogo, 685 Japan

Abstract:

In a two-dimensional wave field under irregular shape boundary conditions, the trajectory of a sound ray is unstable because of chaotic motion [M. V. Berry, Eur. J. Phys. 2, 91 (1981)]. For wave theory, the spacing distribution of the neighboring eigenvalues is not degenerated in irregular systems because of the repulsion effects, but follows a Wigner distribution. [S. W. McDonald and A. N. Kaufman, Phys. Rev. Lett. 42, 1189 (1979); R. H. Lyon, J. Acoust. Soc. Am. 45, 545 (1969)]. This article discusses the sound fields in 2-D irregularly shaped boundaries, using both ray and wave theories. In ray theory, the reflection processes of billiard problems are considered to be like mapping processes on a logistic map, and the sensitivities to the initial conditions under several boundary conditions such as a stadium and an ellipse are investigated. It is shown that the reflection points at the boundary are sensitive to small changes in initial conditions, illustrating that changes in the reflection positions have a chaotic property in a 2-D field with mixed-shaped boundaries of curves and lines. In wave theory, the eigenvalues and eigenmodes are analyzed using the finite-element method (FEM), and the wave theoretic characteristics leftover in the ray-chaotic irregular systems by using (Delta)-statistics and dimensional analysis of the higher modes are shown.


ASA 132nd meeting - Hawaii, December 1996