1973
DOI: 10.1143/jpsj.34.1093
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Interactions of Solitary Waves –A Perturbation Approach to Nonlinear Systems–

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Cited by 86 publications
(47 citation statements)
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“…To evaluate the dynamics of this collision, we use asymptotic expansion of plasma variables around thermodynamics equilibrium state in an appropriate strained coordinate which contains the phase records of each wave. The technique is the so-called extended Poincaré-Lighthill-Kuo (PLK) method [39,40]. The reductive perturbation method in nonlinear wave propagation has been put forward by Taniuti and Wei [41], where it was shown that the stretching of ξ = ε a (x − ct), τ = ε a+1 and a = ( p − 1) −1 with p = 2, p = 3 admit reductions to Burgers and KdV equations, respectively.…”
Section: Qhd Description Of Plasmamentioning
confidence: 99%
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“…To evaluate the dynamics of this collision, we use asymptotic expansion of plasma variables around thermodynamics equilibrium state in an appropriate strained coordinate which contains the phase records of each wave. The technique is the so-called extended Poincaré-Lighthill-Kuo (PLK) method [39,40]. The reductive perturbation method in nonlinear wave propagation has been put forward by Taniuti and Wei [41], where it was shown that the stretching of ξ = ε a (x − ct), τ = ε a+1 and a = ( p − 1) −1 with p = 2, p = 3 admit reductions to Burgers and KdV equations, respectively.…”
Section: Qhd Description Of Plasmamentioning
confidence: 99%
“…It has been shown [44] that, the method of multiple scales combined with the reductive perturbation technique, not only eliminates the secularities arising in the second-order correction but also modifies the phase factor of the lowest KdV soliton proportional to its amplitude. A fuller discussion of the elimination of secularities in higher-order amplitude approximation is given in [40]. From the latter requirement the phase-shifts introduced in eqs (8) are derived.…”
Section: Solitary Collision Dynamicsmentioning
confidence: 99%
“…The phase shift is computed at an instant of time much larger than t d to consider a wave travelling unaffected by the presence of the wall. Oikawa and Yajima (1973) explicitly computed the spatial phase shift x incurred after reflection from the wall, namely: …”
Section: Phase Shiftmentioning
confidence: 99%
“…This loss of amplitude is due to the presence of the third-order dispersive tail. Oikawa and Yajima (1973) used a singular perturbation method developed to secondorder to study the interaction between two solitary waves which propagate in opposite directions. They provided an estimate of the phase shifts in the collision process of the two solitary waves.…”
Section: Introductionmentioning
confidence: 99%
“…Several different approaches are known at present. These include a method based on the inverse-scattering transform (IST) [12 -16], a direct method using multiple-time-scale expansion [17 -20], a mixture of the above two methods [21 -24], a technique using the variational principle [25], and a generalized reductive perturbation method [5,6,26]. These methods are reviewed critically in the literature [27,28] and hence their advantages are not discussed here.…”
Section: Introductionmentioning
confidence: 99%