A perturbative method for the spectral analysis of an acoustic multistratified strip
β Scribed by Elisabeth Croc; Yves Dermenjian
- Publisher
- John Wiley and Sons
- Year
- 1998
- Tongue
- English
- Weight
- 220 KB
- Volume
- 21
- Category
- Article
- ISSN
- 0170-4214
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β¦ Synopsis
We consider the acoustic propagator A"! ) c in the strip "+(x, z)31"0(z(H, with finite width H'0. The celerity c depends for large "x" only on the variable z and describes the stratification of : it is assumed to be in ΒΈ( ), bounded from below by c '0, such that there exists M'0 with c(x, z)"c (z) if x(!M and c(x, z)"c (z) if x'M. We look at the propagator A as a 'perturbation' of the free propagators A H in associated to the velocities c H , j"1, 2, and implement a 'perturbative' method, adapting ideas of Majda and Vainberg. The spectrum of A is defined in section 2, a limiting absorption principle is proved in section 3 outside of a countable set (A). The points of (A) can only accumulate at the left of the thresholds of the free propagators. The needed material about A H , j"1, 2, and some technical estimates for A are given in Appendix.
π SIMILAR VOLUMES
Let N( ) be the counting function of the eigenvalues associated with the self-adjoint operator !( (x, z) )) in the domain "1;]0, h[, h'0, with Neuman or Dirichlet conditions at z"0, h. If "1 in the exterior of a bounded rectangular region O, that is, for "x" large, then N( ) is known to be sublinear
## Abstract ChemInform is a weekly Abstracting Service, delivering concise information at a glance that was extracted from about 200 leading journals. To access a ChemInform Abstract, please click on HTML or PDF.
Based on a new global variational formulation, a spectral element approximation of the incompressible Navier-Stokes/Euler coupled problem gives rise to a global discrete saddle problem. The classical Uzawa algorithm decouples the original saddle problem into two positive definite symmetric systems.
beams in dynamic two-beam coupling with any intensity modulation depth and any constant light excitation efficiency. Such an exact solution can be distinguished for the straight Ε½ . formulation for unit light excitation p s 1 , the hidden formulation with an additional parameter for constant excita-