Abstract

Based on the method of imagenary sources and imagenary scatterers is the solution of the problem of the sound diffraction by pulse signals at ideal (soft) prolate spheroid, put in the plane waveguide with the hard elastic bottom. In the work is proved that with such a formulation of problems eliminated possibility of using the method of normal waves because pulses are bundies of energy and can therefore only be distributed to the group velocity which is inherent in just the method of imaginary sources. Calculations made in the article shoved that imagenary sources with smail numbers experienci8ng the effect of total internal reflection, as the result of the reflection coefficient <i>V</i> by the hard elastic bottom is complex and the real part of <i>V</i> is close to 1,0 which corresponds <i>V</i> absolutely hard bottom. Found sequences of reflected pulses for the elastic hard bottom and the absolutely hard bottom floor confirmed this approach. In the final part of the arti8cle on the basis of the received results given by a solution (the method integral equations) is much more complex problem of the diffraction at the elastic non-analytical scatterer, put in the plane waveguide witch the hard elastic bottom.

Highlights

  • Will it is known [1] thay the sound signal as a bundle of energy propagates with the group velocity. This fact forces us to use method of imaginary sources in the study of the temporal characteristics of pulse signals scattered by various bodies put in plane wavegu-ide [2 – 7]

  • While spectral characteristics of dealing with continuous harmonic signals can be investigated using the method of normal waves [8]

  • We turn to a familiar problem of the diffraction of pulses on spheroial bodies I the pla-ne waveguide [2 – 4, 7], retairing the upper boundary condition Dirichlet, waveguide di-mensions and scatterer with respect to boundaries, replasing only ideal hard lower bounda-ry on the elastic isotropic bottom

Read more

Summary

American Journal of Modern Physics

Analytical and Non – analytical Scatterers in Plane Waveguide with Hard Elastic Bottom, Irradiated by Pulse Sound Signal

Alexander Kleshchev
Introduction
Conclusions

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.