1993
DOI: 10.1063/1.860825
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Sub-Alfvénic plasma expansion

Abstract: A large ion Larmor radius plasma undergoes a particularly robust form of Rayleigh–Taylor instability when sub-Alfvénically expanding into a magnetic field. Results from an experimental study of this instability are reported and compared with theory, notably a magnetohydrodynamic (MHD) treatment that includes the Hall term, a generalized kinetic lower-hybrid drift theory, and with computer simulations. Many theoretical predictions are confirmed while several features remain unexplained. New and unusual features… Show more

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Cited by 103 publications
(87 citation statements)
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“…The growth of flute-like instabilities affecting the plasma dynamics at intermediate levels of magnetization was also demonstrated [25,26]. We should note however that all these studies were conducted in a regime where only the electrons in the plasma were magnetized, the ions being not or weakly magnetized.…”
Section: Historical Contextmentioning
confidence: 99%
“…The growth of flute-like instabilities affecting the plasma dynamics at intermediate levels of magnetization was also demonstrated [25,26]. We should note however that all these studies were conducted in a regime where only the electrons in the plasma were magnetized, the ions being not or weakly magnetized.…”
Section: Historical Contextmentioning
confidence: 99%
“…Similar phenomena can take place during Novae explosions (Zakharov 2003) and artificial magnetospheric releases, similar to the AMPTE magnetotail release (Bernhardt et al 1987;Ripin et al 1993).…”
Section: Introductionmentioning
confidence: 75%
“…During recent experiments on interaction of laser ablated plasma flows with the magnetic field created by the Zebra pulse power generator strong wave activity was detected in the region of plasma flow deceleration by the magnetic field (Presura et al, 2006). Similar phenomena can take place during Novae explosions (Zakharov, 2003) and artificial magnetospheric releases, similar to the AMPTE magnetotail release (Bernhardt et al, 1987;Ripin et al, 1993). To study its linear excitation and nonlinear evolution, a nonlinear set of equations for electrostatic potential, magnetic field, and density has been derived in the low frequency limit (ω ci ,where ω is the frequency of the excited mode and ci = ZeB 0z /M i c is the cyclotron frequency of the ion with charge Z and mass M i = μM p , M p being the proton mass) from two-fluid macroscopic equations which include gyroviscosity (Sotnikov et al, accepted by IEEE TPS, 2006).…”
mentioning
confidence: 82%