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Non-linear electrostatic waves in pair-ion plasmas - National Centre ...

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6. Dissipative shocks and solitons <strong>in</strong> Pair-<strong>ion</strong> PlasmasKadomstev-Petviashvili-Burgers (KPB) Equat<strong>ion</strong> <strong>in</strong> PI PlasmasElectrostatic structures are studied <strong>in</strong> unmagnetized, weakly dissipative PI <strong>plasmas</strong> <strong>in</strong>the presence of weak transverse perturbat<strong>ion</strong>s.The dissipat<strong>ion</strong> <strong>in</strong> the system is <strong>in</strong>corporated by taken <strong>in</strong>to account the k<strong>in</strong>ematicviscosity of both the species.Normalized set of dynamic equat<strong>ion</strong>s are written as(Cont<strong>in</strong>uity equat<strong>ion</strong> for +ve<strong>ion</strong>s)(Momentum equat<strong>ion</strong>s for+ve <strong>ion</strong>s)(Cont<strong>in</strong>uity equat<strong>ion</strong> for -ve<strong>ion</strong>s)(Momentum equat<strong>ion</strong>s for-ve <strong>ion</strong>s)u∂n+∂t∂ ∂+ ( n+u+) + ( n+v+) = 0∂x∂y∂u∂uϕ 1 ∂n2∂+ ++ ∂+++ u++ v+= − − + η+ 2∂t∂x∂y∂xn+∂x∂x2∂ v+ ∂v+∂v+∂ϕ1 ∂n+∂ u++ u++ v+= − − + η+ 2∂t∂x∂y∂yn+∂y∂y∂u−∂t∂v∂t−∂n−∂t+ u+ u−−∂ ∂+ ( n−u−) + ( n−v−) = 0∂x∂y∂u−∂x∂v∂x−+ v+ v−−∂u−∂y∂v∂y−2∂ϕβ ∂n−∂ u−= − + η− 2∂xn−∂x∂x2∂ϕβ ∂n−∂ v= − + η−2∂yn ∂y∂y−∂u−27

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