2005
DOI: 10.1016/j.jnucmat.2004.09.060
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Modeling of three-dimensional neutral transport in tandem mirror plasmas using a Monte-Carlo code

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Cited by 11 publications
(5 citation statements)
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“…5(a) shows the schematic view of the plasma mesh model used in the simulation. A fully 3-dimension mesh model of DEGAS ver.63 code has been developed for this purpose [16]. A particle source is defined at the position of gas puff exit as a secondary wall.…”
Section: Monte-carlo Simulation Of Gpimentioning
confidence: 99%
“…5(a) shows the schematic view of the plasma mesh model used in the simulation. A fully 3-dimension mesh model of DEGAS ver.63 code has been developed for this purpose [16]. A particle source is defined at the position of gas puff exit as a secondary wall.…”
Section: Monte-carlo Simulation Of Gpimentioning
confidence: 99%
“…The flowing out plasma from the central region intersects MLO in the periphery region (r cc 11 cm) and is neutralized there. In this simulation, MLO is modeled as the 'second wall' defined independently of the vacuum chamber wall, which has been successfully achieved by modifying the original code [5]. A particle source is given on MLO and is restricted in the area from r cc = −11 to −16 cm (shaded area in Fig.…”
Section: Modeling Of the Gamma 10 Anchor Cellmentioning
confidence: 99%
“…3-D Monte-Carlo simulation of the neutral transport is an indispensable method in order to solve this difficulty. Neutral transport studies in 3-D geometry by using DEGAS Monte-Carlo code [1,2] have been carried out in the GAM-MA 10 tandem mirror device [3,4], the helical device LHD [5] and Heliotron J [6,7].…”
Section: Introductionmentioning
confidence: 99%