2015
DOI: 10.1007/s10509-015-2574-2
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Bifurcations of nonlinear ion-acoustic travelling waves in a multicomponent magnetoplasma with superthermal electrons

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Cited by 65 publications
(17 citation statements)
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“…The potential function W ( ) has two points of extreme for , which are defined at ∂ W/∂ = 0; these are 1,2 and can be given as direction perpendicular to the magnetic field, the nonlinear periodic traveling wave disappears where the increase in θ causes the increase in the dispersion term coefficient in the nonlinear KdV equation and the periodic traveling wave becomes fatter. Also, the obtained periodic waves are affected by the obliqueness and species densities similarly as presented by Selim et al [56]. It is noticed that the used plasma system is entirely contained by the magnetic force, an arrangement referred to as magnetic confinement (i.e., the magnetic field makes the nonlinear periodic traveling wave structures in the field direction spikier as demonstrated in Ref.…”
Section: (A) (B)supporting
confidence: 62%
“…The potential function W ( ) has two points of extreme for , which are defined at ∂ W/∂ = 0; these are 1,2 and can be given as direction perpendicular to the magnetic field, the nonlinear periodic traveling wave disappears where the increase in θ causes the increase in the dispersion term coefficient in the nonlinear KdV equation and the periodic traveling wave becomes fatter. Also, the obtained periodic waves are affected by the obliqueness and species densities similarly as presented by Selim et al [56]. It is noticed that the used plasma system is entirely contained by the magnetic force, an arrangement referred to as magnetic confinement (i.e., the magnetic field makes the nonlinear periodic traveling wave structures in the field direction spikier as demonstrated in Ref.…”
Section: (A) (B)supporting
confidence: 62%
“…Therefore, due to its important applications in various plasma environments, bifurcation theory has been extensively applied to examine the physical features of non‐linear waves in different plasma models. [ 37,42,51 ] As mentioned in the last part, we introduced the transformation, χ=ζλτ to obtain Equation (14). After integration and simplifying Equation (14), assuming ϕ(1)false(ζ,τfalse)=ϕfalse(χfalse), we obtain the following equation: d2ϕ(1)dχ2=λBϕ+2A3B(goodbreak−ϕ)3/2. …”
Section: Bifurcation Analysismentioning
confidence: 99%
“…In addition, many investigators have applied bifurcation analysis [ 35 ] extensively to examine non‐linear waves' physical behaviour in different plasma models due to its significant applications in various plasma cases. [ 36–45 ] In particular, they discussed the probability of the existence and characteristics of periodic travelling waves. For instance, by applying the bifurcation theory, Abdelwahed et al [ 38 ] discussed the non‐linear propagation of dust‐ion acoustic periodic travelling waves in a dusty plasma consisting of cold ions, stationary charged dust grains, and two temperature superthermal electrons.…”
Section: Introductionmentioning
confidence: 99%
“…A lunar orbiter SELENE revealed the existence of electrostatic waves which are generated due to the electrostatic instability driven by energetic solar wind particles in the lunar wake [5]. e particles of astrophysical plasmas such as solar wind plasma were generally found to follow non-Maxwellian distribution containing suprathermal particles with highenergy tails [6]. e kappa distribution appropriately defines the influence of suprathermal particles [7].…”
Section: Introductionmentioning
confidence: 99%