Nonlinear Waves in Waveguides: With Stratification |
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Page 29
... conditions and two boundary conditions for every variable . We allow that at infinite x the solutions should decrease . Let us suppose that the initial conditions or sources working during a finite time are concentrated around the ...
... conditions and two boundary conditions for every variable . We allow that at infinite x the solutions should decrease . Let us suppose that the initial conditions or sources working during a finite time are concentrated around the ...
Page 50
... boundary conditions in metal or dielectric waveg- uides leads to the physically possible finite - mode case . The nonlocal dispersion operator may appear due to boundary matching of solutions for dielectric waveg- uides ( dielectric ...
... boundary conditions in metal or dielectric waveg- uides leads to the physically possible finite - mode case . The nonlocal dispersion operator may appear due to boundary matching of solutions for dielectric waveg- uides ( dielectric ...
Page 124
... boundary conditions for the electron density are determined by the known decrease of n in the lowest region of the ionospheric layer and by the presence of the plasma flux from the plasmasphere above : n ( 0 , t ) = 0 , n2 ( hi , t ) + ...
... boundary conditions for the electron density are determined by the known decrease of n in the lowest region of the ionospheric layer and by the presence of the plasma flux from the plasmasphere above : n ( 0 , t ) = 0 , n2 ( hi , t ) + ...
Contents
Introduction | 1 |
The Discrimination and Interaction | 12 |
3 | 27 |
Copyright | |
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amplitude approximation atmosphere B₁ boundary conditions calculation CKdV coefficients components contribution coordinate denote density density matrix dependence derivation described determined dielectric dispersion branches dispersion equation dispersion relation dissipation distribution function dynamical variables effects electromagnetic electron evolution equations Fiz.Atm.Okean frequency given H₂ hydrodynamical inhomogeneity initial conditions integration internal waves ion-acoustic waves Ionosphere iteration Kaliningrad KdV equation kinetic Langmuir wave layer linear longitudinal waves magnetic field matrix mean field medium method mode interaction Moscow Nauka nonlinear constants nonlinear terms Nonlinear Waves nonlocal oscillations particles 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 vector velocity vertical w₁ wave propagation wave vector waveguide propagation wavelength