Plasma energy balance in the L-2M stellarator View Full Text


Ontology type: schema:ScholarlyArticle     


Article Info

DATE

2007-10

AUTHORS

O. I. Fedyanin, D. K. Akulina, G. M. Batanov, M. S. Berezhetskiĭ, D. G. Vasil’kov, I. Yu. Vafin, G. S. Voronov, E. V. Voronova, G. A. Gladkov, S. E. Grebenshchikov, L. M. Kovrizhnykh, N. F. Larionova, A. A. Letunov, V. P. Logvinenko, N. I. Malykh, A. I. Meshcheryakov, Yu. I. Nechaev, K. A. Sarksyan, N. N. Skvortsova, S. V. Shchepetov, N. K. Kharchev, Yu. V. Khol’nov

ABSTRACT

Results are presented from studies of the effect of the discharge parameters (in particular, plasma density and heating power) and the characteristics of the magnetic configuration (e.g., rotational transform) on the confinement of a low-pressure plasma during electron-cyclotron resonance heating in the L-2M stellarator. An analysis shows that the plasma energy in the steady-state phase of a discharge is fairly well described by the product of power functions of the plasma density, heating power, and rotational transform: \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $$W = W_0 n_e^{\alpha _n } P^{\alpha _p } \iota ^{\alpha _\iota } $$ \end{document}. The energy scalings constructed in terms of the parameters in the initial stage of free plasma decay and those in the steady-state phase are close to one another. The dynamic analysis of the plasma energy decay is now under way. More... »

PAGES

805-815

Identifiers

URI

http://scigraph.springernature.com/pub.10.1134/s1063780x07100029

DOI

http://dx.doi.org/10.1134/s1063780x07100029

DIMENSIONS

https://app.dimensions.ai/details/publication/pub.1015342704


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6 schema:description Results are presented from studies of the effect of the discharge parameters (in particular, plasma density and heating power) and the characteristics of the magnetic configuration (e.g., rotational transform) on the confinement of a low-pressure plasma during electron-cyclotron resonance heating in the L-2M stellarator. An analysis shows that the plasma energy in the steady-state phase of a discharge is fairly well described by the product of power functions of the plasma density, heating power, and rotational transform: \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} $$W = W_0 n_e^{\alpha _n } P^{\alpha _p } \iota ^{\alpha _\iota } $$ \end{document}. The energy scalings constructed in terms of the parameters in the initial stage of free plasma decay and those in the steady-state phase are close to one another. The dynamic analysis of the plasma energy decay is now under way.
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13 schema:keywords L-2M stellarator
14 M stellarator
15 analysis
16 balance
17 characteristics
18 configuration
19 confinement
20 decay
21 density
22 discharge
23 discharge parameters
24 dynamic analysis
25 effect
26 electron-cyclotron resonance heating
27 energy
28 energy balance
29 energy decay
30 energy scaling
31 free plasma decay
32 function
33 heating
34 heating power
35 initial stage
36 low-pressure plasma
37 magnetic configuration
38 parameters
39 phase
40 plasma
41 plasma decay
42 plasma density
43 plasma energy
44 plasma energy decay
45 power
46 power function
47 products
48 resonance heating
49 results
50 rotational transform
51 scaling
52 stage
53 steady-state phase
54 stellarator
55 study
56 terms
57 transform
58 way
59 schema:name Plasma energy balance in the L-2M stellarator
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