Nonlinear Waves in Waveguides: with StratificationS.B. Leble's book deals with nonlinear waves and their propagation in metallic and dielectric waveguides and media with stratification. The underlying nonlinear evolution equations (NEEs) are derived giving also their solutions for specific situations. The reader will find new elements to the traditional approach. Various dispersion and relaxation laws for different guides are considered as well as the explicit form of projection operators, NEEs, quasi-solitons and of Darboux transforms. Special points relate to: 1. the development of a universal asymptotic method of deriving NEEs for guide propagation; 2. applications to the cases of stratified liquids, gases, solids and plasmas with various nonlinearities and dispersion laws; 3. connections between the basic problem and soliton- like solutions of the corresponding NEEs; 4. discussion of details of simple solutions in higher- order nonsingular perturbation theory. |
From inside the book
Results 1-3 of 35
Page 27
Hereafter the spherical coordinates (r, i9,y>) are introduced. Restricting ourselves
to the first term of the i9-expansion in the Coriolis acceleration near the point i9 =
tfrj and excluding 6 we get (A 1.3) where A = Ar + (1 /r2)A^. When Q = 0 the left ...
Hereafter the spherical coordinates (r, i9,y>) are introduced. Restricting ourselves
to the first term of the i9-expansion in the Coriolis acceleration near the point i9 =
tfrj and excluding 6 we get (A 1.3) where A = Ar + (1 /r2)A^. When Q = 0 the left ...
Page 34
with Stratification Sergei B. Leble. 8 16 21, 32 40 y Transverse coordinate y [Hm]
Fig. 2.1. Finite-gap genus 2 (Riemann 0-function) solution of the KP equation, (a)
Time dependence 9(f), 0,t). (b) Longitudinal coordinate dependence 0(x,O,O).
with Stratification Sergei B. Leble. 8 16 21, 32 40 y Transverse coordinate y [Hm]
Fig. 2.1. Finite-gap genus 2 (Riemann 0-function) solution of the KP equation, (a)
Time dependence 9(f), 0,t). (b) Longitudinal coordinate dependence 0(x,O,O).
Page 70
In the coordinate system oriented along the wave propagation axis the tensor has
two independent components e1 and ett and e*=(^-^y + ^. (4-8) The substitution
of (4.8) into (4.7) in this coordinate system leads to solvability condition of the ...
In the coordinate system oriented along the wave propagation axis the tensor has
two independent components e1 and ett and e*=(^-^y + ^. (4-8) The substitution
of (4.8) into (4.7) in this coordinate system leads to solvability condition of the ...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
Introduction | 1 |
The Discrimination and Interaction | 12 |
Interaction of Modes in an Electromagnetic Field Waveguide | 50 |
Copyright | |
6 other sections not shown
Other editions - View all
Common terms and phrases
allows amplitude approximation atmosphere atmospheric waveguide atmospheric waves basis functions boundary conditions calculation CKdV coefficients components considered contribution coordinate decrease denote density density matrix dependence derivation described determined dielectric dimensionless dispersion branches dispersion equation dispersion relation dissipation distribution function dynamical variables effects evolution equations exponential Fiz.Atm.Okean formulas Fourier frequency given hydrodynamical inhomogeneity initial conditions integration internal waves ion-acoustic ionospheric iteration Kaliningrad KdV equation kinetic Langmuir waves layer linear long waves magnetic field matrix mean field medium method mode interaction mode number Moscow nonlinear constants nonlinear terms Nonlinear Waves nonlocal ocean oscillations perturbation theory physical plasma waves problem projection operators quasi-waveguide quasisolitons region resonance Rossby waves S.B.Leble scale Sect small parameters soliton solution spectral SSSR stationary stratified subspaces substitution taking into account temperature thermoclyne thermoconductivity thermospheric three-wave transformed turbulence two-dimensional values velocity vertical wave interaction wave propagation wave vector waveguide propagation wavelength