Nonlinear Waves in Waveguides: With Stratification |
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Page 62
... ( 2 ) e12 = ( 2 ) = XỸ ( 1- 4iħ2T12 T23 Δρ e2 e3 - 17YZ ( A2 - 1 - α2 ) 013 ... field components into the linear part followed by the subsequent projection ... due to a nonlinear effect in which a slow propagating mode is excited , 62 ...
... ( 2 ) e12 = ( 2 ) = XỸ ( 1- 4iħ2T12 T23 Δρ e2 e3 - 17YZ ( A2 - 1 - α2 ) 013 ... field components into the linear part followed by the subsequent projection ... due to a nonlinear effect in which a slow propagating mode is excited , 62 ...
Page 80
... field allows one to find the particles velocity that determines a displacement current density j . The obtained mass ... due to the relatively small frequency and because the convective term is quadratic in amplitude . Moreover , in this ...
... field allows one to find the particles velocity that determines a displacement current density j . The obtained mass ... due to the relatively small frequency and because the convective term is quadratic in amplitude . Moreover , in this ...
Page 117
... ( 2 ) ( z ) dz . The coordinate system origin is placed in the middle of the channel depth . The indices “ 0 ” and “ v ... field with ko = woy = 0. Due to ( 6.2 ) approximately ∞ ην u == + cc . 27 , T = - Σ [ [ __ 4 ° rdz Atrekkers - wart ) ...
... ( 2 ) ( z ) dz . The coordinate system origin is placed in the middle of the channel depth . The indices “ 0 ” and “ v ... field with ko = woy = 0. Due to ( 6.2 ) approximately ∞ ην u == + cc . 27 , T = - Σ [ [ __ 4 ° rdz Atrekkers - wart ) ...
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