1998
DOI: 10.1016/s0375-9601(98)00616-1
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Effect of adiabatic variation of dust charges on dust-acoustic solitary waves

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Cited by 132 publications
(56 citation statements)
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“…Therefore, the current balance equation becomes, at equilibrium (adiabatic dust charge variations), I e + I il + I ih ≈ 0 (Xie et al 1998;Ghosh et al 2001). With the aid of equations (1k)-(1m), one can write (1j) at equilibrium as…”
Section: Basic Equations and Interaction Between Two Daswsmentioning
confidence: 99%
“…Therefore, the current balance equation becomes, at equilibrium (adiabatic dust charge variations), I e + I il + I ih ≈ 0 (Xie et al 1998;Ghosh et al 2001). With the aid of equations (1k)-(1m), one can write (1j) at equilibrium as…”
Section: Basic Equations and Interaction Between Two Daswsmentioning
confidence: 99%
“…Therefore, the current balance equation becomes, at equilibrium (adiabatic dust charge variations), I el + I eh + I i ≈ 0 (Xie et al 1998;Ghosh et al 2001). With the aid of (1j)-(1l), one can write (1i) at equilibrium as…”
Section: Basic Equations and Formulation Of The Problemmentioning
confidence: 99%
“…Nonlinear evolution of dust acoustic and dust ion acoustic waves in presence of adiabatic and non adiabatic dust charge variation were studied earlier by several authors considering grain charging by the flow of plasma current [14]- [23]. Effect of both weak (negative equilibrium dust charge) and strong (positive equilibrium dust charge) secondary electron emission in this nonlinear evolution process were later investigated with Boltzmann distributed electrons and ions [12] [13].…”
Section: Introductionmentioning
confidence: 99%