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. |
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Results 1-5 of 46
Page v
... component in the wave vector allows the introduction of the concept of interacting modes . The analogy to the Bubnov- Galerkin method and the approximate description of finite number level in quan- tum mechanics can also be shown . The ...
... component in the wave vector allows the introduction of the concept of interacting modes . The analogy to the Bubnov- Galerkin method and the approximate description of finite number level in quan- tum mechanics can also be shown . The ...
Page 6
... components of the vector , namely , v1 = { a , a } , _ = { a , -a } . Applying the operators P to ( 1.8 ) we have the system for right II = ( a - b ) / 2 and left A = ( a + b ) / 2 waves П ++ сПх = - I −Дt · = — — V ( + √ 2 ( II + A ) ...
... components of the vector , namely , v1 = { a , a } , _ = { a , -a } . Applying the operators P to ( 1.8 ) we have the system for right II = ( a - b ) / 2 and left A = ( a + b ) / 2 waves П ++ сПх = - I −Дt · = — — V ( + √ 2 ( II + A ) ...
Page 8
... component tends to zero [ 1.33 ] . The dissipation and dispersive effects in long internal wave propagation are discussed in connection with the hydrostatic approximation [ 1.68 ] . This approximation is equivalent to the NES with ...
... component tends to zero [ 1.33 ] . The dissipation and dispersive effects in long internal wave propagation are discussed in connection with the hydrostatic approximation [ 1.68 ] . This approximation is equivalent to the NES with ...
Page 9
... components of a magnetic field appears . The solution of the density matrix equation for the nuclear spin system ( which may be directly repeated for any n - level pseudospin system ) gives the nonlinear coupling constants as a function ...
... components of a magnetic field appears . The solution of the density matrix equation for the nuclear spin system ( which may be directly repeated for any n - level pseudospin system ) gives the nonlinear coupling constants as a function ...
Page 12
... components v1 = Vx = U , V2 = Vy = v , v3 = Vz = w . If the medium is complex and can be described by the Boltzmann equations , then The Discrimination and Interaction of Hydrodynamical Waves of Different Types 2 Hydrodynamic Wave ...
... components v1 = Vx = U , V2 = Vy = v , v3 = Vz = w . If the medium is complex and can be described by the Boltzmann equations , then The Discrimination and Interaction of Hydrodynamical Waves of Different Types 2 Hydrodynamic Wave ...
Contents
1 | |
12 | |
2223 | 19 |
5 | 30 |
6 | 37 |
7 | 45 |
88886 | 62 |
Nonlinear Waves in Stratified Plasma | 69 |
3 | 95 |
Waves in Gases Inhomogeneous in Knudsen Number | 106 |
Mean Field Generation by Waves in a Dissipative Medium | 114 |
5 | 134 |
Nonlinear Terms for Interacting Modes of Poincaré | 141 |
Basis Vectors Interaction Operator for Atomic Nuclei | 145 |
Subject Index 161 | 160 |
4 | 88 |
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Common terms and phrases
allows amplitude approximation atmosphere atmospheric waves B₁ basis functions boundary conditions calculation CKdV coefficients components contribution coordinate denote density density matrix dependence derivation described determined dielectric dimensionless dispersion branches dispersion relation dissipation distribution function dynamical variables effects electromagnetic evolution equations Fiz.Atm.Okean frequency given hydrodynamical inhomogeneity initial conditions integration internal waves ion-acoustic Ionosphere iteration KdV equation kinetic Langmuir Langmuir waves layer linear long waves magnetic field matrix mean field medium method mode interaction Moscow Nauka nonlinear constants nonlinear terms Nonlinear Waves nonlocal oscillations perturbation theory physical plasma waves problem projection operators quasisolitons region resonance Rossby waves S.B.Leble scale Sect small parameters soliton solution spectral subspaces substitution taking into account temperature thermoclyne thermoconductivity thermospheric three-wave transformed turbulence values vector velocity vertical w₁ wave propagation wave vector waveguide propagation wavelength пп