Dynamics of sheath evolution in magnetized charge-fluctuating dusty plasmas

On the Analytical and Numerical Solutions in the Quantum Magnetoplasmas: The Atangana Conformable Derivative (1+3)-ZK Equation with Power-Law Nonlinearity

“…(1) Applying the modified Khater method to the Atangana conformable derivative (1 + 3)-ZK equation with power-law nonlinearity has obtained sixty distinct traveling wave solutions 7 Advances in Mathematical Physics (2) The difference between our obtained solutions and that have been obtained in [41] by Aminikhah et al who had used the functional variable method; however, they have just found three solutions and accurate in their and our solutions, we can figure out the complete difference between these solutions that thing makes our solutions are novel (ii) Numerical solutions…”

“…In the existence of a magnetized e-p-i plasma [1], the ZK equation is one of the widely common methods to characterize the ion-acoustic solitary waves. The magnetized loadvarying dusty plasma is the best location to look for alternate placed dust ion acoustic waves of nonthermal electrons with a vortex-like spread of velocity [2]. In a comprehensive computational analysis, the ZK method was used to spread the dust-acoustic waves in a magnetized dusty plasma [3] and to excite the electrostatic ion-acoustic lone wave in two dimensions of negative ion magnetoplasmas of superthermal electrons [4].…”

Effects of a static and an magnetic field electron beam on the linear propagation of dust acoustic mode

“…Different dust grain charging procedures lead to intriguing modifications in the plasma structures, which have already been studied by a number of scientists [9][10][11][12][13][14]. The sheath structure in the magnetised dusty plasma can be dramatically changed by the dust charge variation, as Devi et al shown [12].…”