Comment on the Model of Gormanet al.for Plasma Confinement Time in Stellarators

1969 ◽  
Vol 22 (18) ◽  
pp. 922-923
Author(s):  
T. Ohkawa ◽  
T. H. Jensen
Keyword(s):  
Confinement Time ◽  
Plasma Confinement

Radial Plasma Confinement Time in the Central Cell of GAMMA 6 Determined from Measurements with a Charge Collector

1981 ◽  
Vol 20 (8) ◽  
pp. L601-L604 ◽  
Author(s):  
Kiyoshi Yatsu ◽  
Ikuo Wakaida ◽  
Yoichi Kiyohara ◽  
Akira Sakasai ◽  
Syoichi Miyoshi
Keyword(s):  
Central Cell ◽  
Confinement Time ◽  
Plasma Confinement ◽  
A Charge

Plasma confinement time in trimix-M galatea multipole magnetic trap

2010 ◽  
Vol 36 (5) ◽  
pp. 487-488 ◽  
Author(s):  
A. M. Bishaev ◽  
A. I. Bugrova ◽  
M. V. Kozintseva ◽  
A. S. Lipatov ◽  
A. S. Sigov ◽  
...  
Keyword(s):  
Magnetic Trap ◽  
Confinement Time ◽  
Plasma Confinement

The effect of asymmetries on non‐neutral plasma confinement time

1994 ◽  
Vol 1 (5) ◽  
pp. 1123-1127 ◽  
Author(s):  
J. Notte ◽  
J. Fajans
Keyword(s):  
Confinement Time ◽  
Plasma Confinement ◽  
Neutral Plasma

Modifications of plasma edge electric field and confinement properties by limiter biasing on the KT-5C tokamak

1995 ◽  
Vol 54 (3) ◽  
pp. 393-400 ◽  
Author(s):  
Hui Gao ◽  
Kan Zhai ◽  
Yi-Zhi Wen ◽  
Shu-De Wan ◽  
Gui-Ding Wang ◽  
...  
Keyword(s):  
Magnetic Field ◽  
Electric Field ◽  
Electron Temperature ◽  
Particle Flux ◽  
Plasma Potential ◽  
Edge Plasma ◽  
Plasma Edge ◽  
Confinement Time ◽  
Plasma Confinement ◽  
Particle Confinement

Experiments using a biased multiblock limiter in the KT-5C tokamak show that positive biasing is more effective than negative biasing in modifying the edge electric field, suppressing fluctuations and improving plasma confinement. The biasing effect varies with the limiter area, the toroidal magnetic field and the biasing voltage. By positive biasing, the edge profiles of the plasma potential, the electron temperature and the density become steeper, resulting in a reduced edge particle flux, an increased global particle confinement time and lower fluctuation levels of the edge plasma.

JETTO simulations ofTe/Tieffects on plasma confinement

2005 ◽  
Vol 47 (3) ◽  
pp. 505-519 ◽  
Author(s):  
E Asp ◽  
J Weiland ◽  
X Garbet ◽  
P Mantica ◽  
V Parail ◽  
...  
Keyword(s):  
Plasma Confinement

scholarly journals Enhanced X-ray emission arising from laser-plasma confinement by a strong transverse magnetic field

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Evgeny D. Filippov ◽  
Sergey S. Makarov ◽  
Konstantin F. Burdonov ◽  
Weipeng Yao ◽  
Guilhem Revet ◽  
...  
Keyword(s):  
Magnetic Field ◽  
Transverse Magnetic ◽  
Radiative Properties ◽  
Magnetic Field Direction ◽  
Solid Target ◽  
Total Plasma ◽  
Plasma Confinement ◽  
X Ray ◽  
Magnetic Compression ◽  
The Magnetic Field

AbstractWe analyze, using experiments and 3D MHD numerical simulations, the dynamic and radiative properties of a plasma ablated by a laser (1 ns, 10$$^{12}$$ 12 –10$$^{13}$$ 13 W/cm$$^2$$ 2 ) from a solid target as it expands into a homogeneous, strong magnetic field (up to 30 T) that is transverse to its main expansion axis. We find that as early as 2 ns after the start of the expansion, the plasma becomes constrained by the magnetic field. As the magnetic field strength is increased, more plasma is confined close to the target and is heated by magnetic compression. We also observe that after $$\sim 8$$ ∼ 8  ns, the plasma is being overall shaped in a slab, with the plasma being compressed perpendicularly to the magnetic field, and being extended along the magnetic field direction. This dense slab rapidly expands into vacuum; however, it contains only $$\sim 2\%$$ ∼ 2 % of the total plasma. As a result of the higher density and increased heating of the plasma confined against the laser-irradiated solid target, there is a net enhancement of the total X-ray emissivity induced by the magnetization.

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