The First Order Rogue Waves Via Solutions 24 With Download Download scientific diagram | the first order rogue waves via solutions (24) with d3(z)=0.01sinz\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym. Download scientific diagram | the first order rogue waves via solutions (24) with the parameters $\beta =0.5$ β = 0.5 > , $\alpha =0$ &agr; = 0 > , $\gamma =0$ γ = 0 > , $\delta =0.1$ δ = 0.1.
The First Order Rogue Waves Via Solutions 24 Downloadођ We create first , second , and third order rogue wave solutions via direct computation for various values of center controlled parameters and suitable choices of different constants in the said. The three extreme points of the first order rw solution (24) are obtained, which are maximum point (0, 0) and minimum points (− 113 3 17408, 3 425) and (113 3 17408, − 3 425), corresponding to the wave crest and two wave valleys of first order rw, respectively. taking (x, t) = (0, 0), we get the maximal amplitude | q [1] | m a x of first. The weak and strong interactions between the first , second order rogue waves, and spatial temporal period breather are studied. furthermore, variable coefficient δ (t) causes rogue waves to produce some interesting evolutionary phenomena, which have been systematically analyzed. in addition, the influences of parameters for the properties of. By virtue of hirota bilinear form of the coupled higgs field equation, some higher order rogue wave, the ma breather, the akhmediev breather and the general breather solutions are constructed through symbolic computation. with the help of the contour line method, we investigate the localization characters of the first order rogue wave, which is different from the case of its in nonlinear.
The First Order Rogue Waves Via Solutions 24 With The Para The weak and strong interactions between the first , second order rogue waves, and spatial temporal period breather are studied. furthermore, variable coefficient δ (t) causes rogue waves to produce some interesting evolutionary phenomena, which have been systematically analyzed. in addition, the influences of parameters for the properties of. By virtue of hirota bilinear form of the coupled higgs field equation, some higher order rogue wave, the ma breather, the akhmediev breather and the general breather solutions are constructed through symbolic computation. with the help of the contour line method, we investigate the localization characters of the first order rogue wave, which is different from the case of its in nonlinear. Higher order rogue waves have been a hot topic recently because actual wave dynamics are often generated as a nonlinear superposition of some lower order solutions [24], [25], [26]. via the darboux transformation and numerical simulations, even the 6th order rogue wave for the nls equation has been obtained, which is very complex when presented. Finally, to verify our analysis, via the taylor expansion, we have obtained the first order rogue wave solution at the critical wave number a = 1 (see fig. 3). it is worth while to compare our results with those in ref. [15], which also discussed the generation of rogue wave. for the case of eq.
3d Graphical Representations Of First Order Rogue Waves The Figures Higher order rogue waves have been a hot topic recently because actual wave dynamics are often generated as a nonlinear superposition of some lower order solutions [24], [25], [26]. via the darboux transformation and numerical simulations, even the 6th order rogue wave for the nls equation has been obtained, which is very complex when presented. Finally, to verify our analysis, via the taylor expansion, we have obtained the first order rogue wave solution at the critical wave number a = 1 (see fig. 3). it is worth while to compare our results with those in ref. [15], which also discussed the generation of rogue wave. for the case of eq.
The First Order Rogue Wave Solutions For Download Scientific Dia
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