2015
DOI: 10.1007/s10509-015-2479-0
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Nonlinear oscillatory and monotonic shocks in dense plasmas with ultra-relativistic degenerate electrons

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Cited by 6 publications
(2 citation statements)
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“…The expansions used are given as nc=1+ϵncfalse(1false)+ϵ2ncfalse(2false)+ ucx=ϵ2ucxfalse(1false)+ϵ3ucxfalse(2false)+ ucy=ϵ32ucyfalse(1false)+ϵ52ucyfalse(2false)+ ucz=ϵ1uczfalse(1false)+ϵ2uczfalse(2false)+ ϕ=ϵϕfalse(1false)+ϵ2ϕfalse(2false)+ ηcfalse‖=ϵ12ηcfalse‖o ηc=ϵ12ηco Due to anisotropy induced by external magnetic field, the parallel component of fluid electron u cz is stronger than the perpendicular components u cx and u cy . This effect is noticeable from the powers of the ϵ , that is, u cz , that contain lower power of ϵ as compared to u cx and u cy (Hussain et al, )...…”
Section: Derivation Of Kdv‐burgers Equationmentioning
confidence: 99%
“…The expansions used are given as nc=1+ϵncfalse(1false)+ϵ2ncfalse(2false)+ ucx=ϵ2ucxfalse(1false)+ϵ3ucxfalse(2false)+ ucy=ϵ32ucyfalse(1false)+ϵ52ucyfalse(2false)+ ucz=ϵ1uczfalse(1false)+ϵ2uczfalse(2false)+ ϕ=ϵϕfalse(1false)+ϵ2ϕfalse(2false)+ ηcfalse‖=ϵ12ηcfalse‖o ηc=ϵ12ηco Due to anisotropy induced by external magnetic field, the parallel component of fluid electron u cz is stronger than the perpendicular components u cx and u cy . This effect is noticeable from the powers of the ϵ , that is, u cz , that contain lower power of ϵ as compared to u cx and u cy (Hussain et al, )...…”
Section: Derivation Of Kdv‐burgers Equationmentioning
confidence: 99%
“…where 𝜖 is a small expansion parameter which characterizes the strength of nonlinearity, and 𝜆 is the phase velocity of the wave. We expand the perturbed quantities 𝑁 , 𝑛, 𝑉 i𝑥 , 𝑣 e𝑦 , 𝐵 𝑧 in terms of the smallness parameter 𝜖 as follows: (17) while for 𝑉 i𝑦 , 𝑣 e𝑦 , 𝐸 𝑥 , we have…”
mentioning
confidence: 99%