1960
DOI: 10.1103/revmodphys.32.898
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On Hydromagnetic Stability of Stationary Equilibria

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Cited by 435 publications
(415 citation statements)
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“…The advantages of using the Frieman and Rotenburg [16] for mode analysis are tremendous, especially for an investigation of electrostatic modes, where from the start specific forms of the displacement ξ can be chosen so that δJ = 0 and δB = 0. In particular, it will be shown below that GAMs and zonal flow continua in rotating plasmas can be derived intuitively, rigourously and briefly.…”
Section: B Gams and Zonal Flows In Isothermal Ideal Mhd Rotating Plamentioning
confidence: 99%
See 1 more Smart Citation
“…The advantages of using the Frieman and Rotenburg [16] for mode analysis are tremendous, especially for an investigation of electrostatic modes, where from the start specific forms of the displacement ξ can be chosen so that δJ = 0 and δB = 0. In particular, it will be shown below that GAMs and zonal flow continua in rotating plasmas can be derived intuitively, rigourously and briefly.…”
Section: B Gams and Zonal Flows In Isothermal Ideal Mhd Rotating Plamentioning
confidence: 99%
“…For a description of linear perturbed ideal MHD in a rotating plasma we follow the approach by Frieman and Rotenburg [16]. In this work, a Lagrangian displacement ξ is employed, which can be defined in terms of the Lagrangian perturbed fluid velocity as ∆U ≡ dξ dt = ∂ξ ∂t + U · ∇ξ where the perturbed Lagrangian flow ∆U is related to the Eulerian perturbed vectors X (including the fluid velocity) as ∆X = δX + ξ · ∇X so that Ohm's law…”
Section: B Gams and Zonal Flows In Isothermal Ideal Mhd Rotating Plamentioning
confidence: 99%
“…One of the earliest results on the effect of equilibrium flow on the spectrum is by Frieman and Rotenberg (1960). They showed that the eigenvalue problem becomes quadratic, which implies that the spectrum is no longer restricted to the axes in the complex plane.…”
Section: Introductionmentioning
confidence: 99%
“…By differentiating L with respect to , using the -flow analogue of (3.4) (after changing variables to x 0 , y 0 , z 0 , where, as in Frieman & Rotenberg (1960), superscript 0 refers to = 0) and integration by parts (Gauss' theorem) we find the convenient identity…”
Section: Holonomically Constrained and Free Variationsmentioning
confidence: 99%