Global modes of flute instability of a rotating cylindrical plasma

2009 ◽  
Vol 35 (5) ◽  
pp. 426-435 ◽  
Author(s):  
E. A. Sorokina
Keyword(s):  
Cylindrical Plasma ◽  
Flute Instability ◽  
Global Modes

Discussion following the presentation by F. Deubner

1977 ◽  
Vol 36 ◽  
pp. 69-74
Keyword(s):  
List Type ◽  
The Sun ◽  
Type Number ◽  
Harmonic Motion ◽  
Locally Excited ◽  
Long Period ◽  
Coherent Wave ◽  
Short Period ◽  
Global Modes

The discussion was separated into 3 different topics according to the separation made by the reviewer between the different periods of waves observed in the sun :1) global modes (long period oscillations) with predominantly radial harmonic motion.2) modes with large coherent - wave systems but not necessarily global excitation (300 s oscillation).3) locally excited - short period waves.

Vortex Breakdown Types and Global Modes in Swirling Combustor Flows with Axial Injection

2015 ◽  
Vol 31 (1) ◽  
pp. 219-229 ◽  
Author(s):  
Steffen Terhaar ◽  
Thoralf G. Reichel ◽  
Christina Schrödinger ◽  
Lothar Rukes ◽  
Christian Oliver Paschereit ◽  
...  
Keyword(s):  
Vortex Breakdown ◽  
Axial Injection ◽  
Global Modes

Comparison of probe and narrow-band imaging measurements in a magnetized cylindrical plasma

2019 ◽  
Vol 26 (2) ◽  
pp. 023502
Author(s):  
A. D. Light ◽  
S. Chakraborty Thakur ◽  
G. R. Tynan
Keyword(s):  
Narrow Band ◽  
Narrow Band Imaging ◽  
Cylindrical Plasma

Helicon waves in a cylindrical plasma

1999 ◽  
Vol 77 (5) ◽  
pp. 385-391
Author(s):  
M Shoucri
Keyword(s):  
Dispersion Relation ◽  
Coupling Mechanism ◽  
Electron Mass ◽  
Cylindrical Plasma ◽  
Bounded Plasma ◽  
Helicon Waves

The dispersion relation for helicon waves in a uniform bounded plasma is derived by including the finite electron mass. The eigenmodes are identified and the coupling mechanism between the Ez and Bz modes is discussed. This is important since an essential part of the physics associated with the application of helicon waves for the generation and heating of plasmas consists in coupling the whistler branch with the Ez mode, which can interact directly with the electrons.PACS No.: 52.35-g

Experimental study of curvature‐driven flute instability in the gas‐dynamic trap*

1994 ◽  
Vol 1 (5) ◽  
pp. 1529-1535 ◽  
Author(s):  
A. A. Ivanov ◽  
A. V. Anikeev ◽  
P. A. Bagryansky ◽  
V. N. Bocharov ◽  
P. P. Deichuli ◽  
...  
Keyword(s):  
Experimental Study ◽  
Flute Instability ◽  
Gas Dynamic ◽  
Curvature Driven
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