Anisotropic pressure and finite hot-electron Larmor radius effects on hot-electron ring stability

1983 ◽  
Vol 26 (10) ◽  
pp. 3079 ◽  
Author(s):  
K. T. Tsang
1984 ◽  
Vol 27 (4) ◽  
pp. 1019 ◽  
Author(s):  
S. Hiroe ◽  
J. B. Wilgen ◽  
F. W. Baity ◽  
L. A. Berry ◽  
R. J. Colchin ◽  
...  
Keyword(s):  

1983 ◽  
Vol 29 (1) ◽  
pp. 99-109 ◽  
Author(s):  
H. Sanuki

The dynamic stabilization of electrostatic flute modes by an RF electric field is studied on the basis of the relatively simple model of a smooth cylinder with artificial gravity and an ambipolar field. It is found that the electrostatic flute modes can be effectively stabilized by the RF electric field together with the hot electron ring.


1991 ◽  
Vol 30 (Part 1, No. 1) ◽  
pp. 152-160
Author(s):  
Minoru Hosokawa ◽  
Hideo Ikegami

2018 ◽  
Vol 84 (5) ◽  
Author(s):  
S. S. Cerri

We consider the one-dimensional equilibrium problem of a shear-flow boundary layer within an ‘extended-fluid model’ of a plasma that includes the Hall and the electron pressure terms in Ohm’s law, as well as dynamic equations for anisotropic pressure for each species and first-order finite-Larmor-radius (FLR) corrections to the ion dynamics. We provide a generalized version of the analytic expressions for the equilibrium configuration given in Cerri et al., (Phys. Plasmas, vol. 20 (11), 2013, 112112), highlighting their intrinsic asymmetry due to the relative orientation of the magnetic field $\boldsymbol{B}$, $\boldsymbol{b}=\boldsymbol{B}/|\boldsymbol{B}|$, and the fluid vorticity $\unicode[STIX]{x1D74E}=\unicode[STIX]{x1D735}\times \boldsymbol{u}$ (‘$\unicode[STIX]{x1D74E}\boldsymbol{b}$ asymmetry’). Finally, we show that FLR effects can modify the Chapman–Ferraro current layer at the flank magnetopause in a way that is consistent with the observed structure reported by Haaland et al., (J. Geophys. Res. (Space Phys.), vol. 119, 2014, pp. 9019–9037). In particular, we are able to qualitatively reproduce the following key features: (i) the dusk–dawn asymmetry of the current layer, (ii) a double-peak feature in the current profiles and (iii) adjacent current sheets having thicknesses of several ion Larmor radii and with different current directions.


1985 ◽  
Vol 25 (1) ◽  
pp. 71-84 ◽  
Author(s):  
E.F. Jaeger ◽  
L.A. Berry ◽  
C.L. Hedrick ◽  
R.K. Richards

1970 ◽  
Vol 4 (2) ◽  
pp. 403-424 ◽  
Author(s):  
Shigeki Morioka ◽  
John R. Spreiter

The Chew—Goldberger—Low theory of a collisionless plasma, modified to include the effect of finite Larmor radius of the ion and the electron, is applied to a linearized problem of two-dimensional steady flow. The zeroth-order terms in the Larmor radius expansions of the velocity distribution functions of the ion and the electron are assumed to be anisotropic Maxwellian. The spatial development of a given velocity profile is investigated for flows with either crossed or aligned magnetic fields, and for various values of Mach number, Alfvén Mach number, and anisotropic pressure ratios in the main flow.


1984 ◽  
Author(s):  
E. F. Jaeger ◽  
L. A. Berry ◽  
C. L. Hedrick ◽  
R. K. Richards

1986 ◽  
Author(s):  
D. L. Hillis ◽  
J. B. Wilgen ◽  
T. S. Bigelow ◽  
Jaeger, E/F. ◽  
D. W. Swain ◽  
...  

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