Abstract:The propagation of electron acoustic solitary waves is investigated in magnetized two‐temperature electron plasma with supra‐thermal ion. By using the reductive perturbation technique, the Korteweg de‐Vries (KdV) equation is derived. Later solving this equation, a solitary wave solution has been derived. These are mainly in astrophysical plasmas where changes of local charge density, temperature, and energy of particles produce considerable effects on the plasma system. The effects of supra‐thermality, density… Show more
“…Thus, in order to find nontrivial solutions for the two inhomogeneous systems of Eqs. (13), it is imposed that the following determinants should also vanish:…”
Section: Application Of the Reductive Perturbation Methodsmentioning
confidence: 99%
“…In the context of plasma fluids, the NLS equations has been derived for the first times in the early '70s [8,9], and subsequently for a large variety of electrostatic plasma models. Recently, its localized solutions (envelope solitons, breathers) have in fact been associated with freak or rogue waves in plasmas [10,11,12,13]. Formally analogous NLS equations focusing on electromagnetic waves in plasmas modeled by fluid-Maxwell equations have been also derived [14,15,16].…”
The nonlinear dynamics of two co-propagating electrostatic wavepackets in a one-dimensional non-magnetized plasma fluid model is considered, from first principles. The coupled waves are characterized by different (carrier) wavenumbers and amplitudes. A plasma consisting of non-thermalized (κ−distributed) electrons evolving against a cold (stationary) ion background is considered. The original model is reduced, by means of a multiple-scale perturbation method, to a pair of coupled nonlinear Schr¨odinger (CNLS) equations for the dynamics of the wavepacket envelopes. For arbitrary wavenumbers, the resulting CNLS equations exhibit no known symmetry and thus intrinsically differ from the Manakov system, in general.
Exact analytical expressions have been derived for the dispersion, self-modulation (nonlinearity) and cross-modulation (coupling) coefficients involved in the CNLS equations, as functions of the wavenumbers (k1, k2) and of the spectral index κ characterizing the electron profile. An analytical investigation has thus been carried out of the modulational instability (MI) properties of this pair of wavepackets, focusing on the role of the intrinsic (variable) parameters. Modulational instability is shown to occur in most parts of the parameter space.
The instability window(s) and the corresponding growth rate are calculated numerically in a number of case studies. Two-wave interaction favors MI by extending its range of occurrence and by enhancing its growth rate. Growth rate patterns obtained for different κ index (values) suggest that deviation from thermal (Maxwellian) equilibrium, for low κ values, leads to enhances MI of the interacting wave pair.
Although we have focused on electrostatic wavepacket propagation in nonthermal (non-Maxwellian) plasma, the results of this study are generic and may be used as basis to model energy localization in nonlinear optics, in hydrodynamics or in dispersive media with Kerr-type nonlinearities where modulational instability is relevant.
“…Thus, in order to find nontrivial solutions for the two inhomogeneous systems of Eqs. (13), it is imposed that the following determinants should also vanish:…”
Section: Application Of the Reductive Perturbation Methodsmentioning
confidence: 99%
“…In the context of plasma fluids, the NLS equations has been derived for the first times in the early '70s [8,9], and subsequently for a large variety of electrostatic plasma models. Recently, its localized solutions (envelope solitons, breathers) have in fact been associated with freak or rogue waves in plasmas [10,11,12,13]. Formally analogous NLS equations focusing on electromagnetic waves in plasmas modeled by fluid-Maxwell equations have been also derived [14,15,16].…”
The nonlinear dynamics of two co-propagating electrostatic wavepackets in a one-dimensional non-magnetized plasma fluid model is considered, from first principles. The coupled waves are characterized by different (carrier) wavenumbers and amplitudes. A plasma consisting of non-thermalized (κ−distributed) electrons evolving against a cold (stationary) ion background is considered. The original model is reduced, by means of a multiple-scale perturbation method, to a pair of coupled nonlinear Schr¨odinger (CNLS) equations for the dynamics of the wavepacket envelopes. For arbitrary wavenumbers, the resulting CNLS equations exhibit no known symmetry and thus intrinsically differ from the Manakov system, in general.
Exact analytical expressions have been derived for the dispersion, self-modulation (nonlinearity) and cross-modulation (coupling) coefficients involved in the CNLS equations, as functions of the wavenumbers (k1, k2) and of the spectral index κ characterizing the electron profile. An analytical investigation has thus been carried out of the modulational instability (MI) properties of this pair of wavepackets, focusing on the role of the intrinsic (variable) parameters. Modulational instability is shown to occur in most parts of the parameter space.
The instability window(s) and the corresponding growth rate are calculated numerically in a number of case studies. Two-wave interaction favors MI by extending its range of occurrence and by enhancing its growth rate. Growth rate patterns obtained for different κ index (values) suggest that deviation from thermal (Maxwellian) equilibrium, for low κ values, leads to enhances MI of the interacting wave pair.
Although we have focused on electrostatic wavepacket propagation in nonthermal (non-Maxwellian) plasma, the results of this study are generic and may be used as basis to model energy localization in nonlinear optics, in hydrodynamics or in dispersive media with Kerr-type nonlinearities where modulational instability is relevant.
“…In the next part of our study we have focused on that regions where ion-loss occurs. Our study lies in that velocity regime on which two-stream instability leads to a strong acceleration of planetary ions which are very energetic in the range of suprathermal energies [27]. Some newer simulation studies based on homotopy [28][29][30][31][32] could provide some additional information.…”
In this work we investigate the possibility of two-stream instability in the Venusian atmosphere to lead to momentum transfer to subsequent escape of Hydrogen and Oxygen ions from the ionosphere. We employ the hydrodynamic model and obtain the linear dispersion relation from which the two-stream instability is studied. Further the interaction of solar wind with the ions of Venus ionosphere from which the instability sets in, has been studied with the data from ASPERA-4 of Venus Express (VEX). The data supports the fact that the two-stream instability can provide sufficient energy to accelerate ions to escape velocity of the planet.
“…Understanding the effect of the kappa index on solitary wave potentials is crucial for unraveling the underlying physics and predicting the behavior of waves in different plasma environments [23,24]. The kappa index has been found to influence diverse aspects of solitary waves, including their generation, propagation, and stability [25]. The nonlinear behavior of plasma waves and their interaction with the plasma medium can be better understood if the effect of the kappa index on solitary wave potentials is studied.…”
Nonlinear interactions between nonlinearity, dispersion, and other phenomena in a media give rise to solitons, which are self-reinforcing solitary waves that retain shape and velocity as they propagate across the medium. We investigate electrostatic ion-acoustic solitary waves in a homogeneous, unmagnetized, collision-less plasma environment at 200-500 km for a plasma system consists of three positive ions, whereas the electrons present as a super-thermal charge and follow kappa distribution function. The potential for electrostatic ion-acoustic solitary waves to form in the Martian ionosphere due to the movement of different ionic species was established using the one-dimensional Korteweg-de Vries (KdV) equation has been obtained using the reductive perturbation approach. Graphical representations of numerical studies that explain how super-thermal parameter affects nonlinear ion acoustic waves are shown. The kappa index influence on the soliton waves has been studied. Based on our model an increased kappa index can lead to modifications in soliton amplitude and width.
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