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Exponential decay of solutions of the wave equation in the exterior of a star‐shaped obstacle
Author(s) -
Lax P. D.,
Morawetz C. S.,
Phillips R. S.
Publication year - 1963
Publication title -
communications on pure and applied mathematics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 3.12
H-Index - 115
eISSN - 1097-0312
pISSN - 0010-3640
DOI - 10.1002/cpa.3160160407
Subject(s) - star (game theory) , citation , obstacle , exponential function , mathematics , computer science , calculus (dental) , mathematical physics , mathematical analysis , library science , law , medicine , political science , dentistry
In this paper we study the behavior for large time of solutions of the wave equation in three space dimensions in the exterior of some smooth, bounded reflecting obstacle which is assumed to be starshaped. We shall prove that , given an initial disturbance, the bulk of its energy is propagated to infinity. The precise statement of the result is Theorem IV; it has as its corollary the following result: Let u denote a smooth solution of the above exterior problem whose initial values have finite energy and are zero outside of some bounded re* gion. Then at a fixed point x> u(x> t) decays exponentially with time. When the scattering obstacle is a sphere, this result has been deduced by Wilcox [5 ] by analyzing the explicit expression for the solution obtained by separation of variables. In [4], C. S. Morawetz has proved that energy decays like the inverse square of time, and it follows that the solution decays like l/t. The sharper result of the present paper is obtained by combining her result with the techniques developed in [ l ] and [2], Theorem IV of this paper implies that the scattering matrix associated with the above problem can be continued analytically from the lower half-plane into a horizontal strip of the upper half-plane; a complete discussion of this can be found in [2]. Ho denotes the Hilbert space of Cauchy data 4>~{4>u $2) defined in the entire three-dimensional space, normed by the energy norm: