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Analysis of Avalanche Runaway Generation after Disruptions with Low-Z and Noble Gas Species
https://repo.qst.go.jp/records/48346
https://repo.qst.go.jp/records/48346230d09ae-360f-49c6-88f5-ffa0557138db
Item type | 学術雑誌論文 / Journal Article(1) | |||||
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公開日 | 2017-10-05 | |||||
タイトル | ||||||
タイトル | Analysis of Avalanche Runaway Generation after Disruptions with Low-Z and Noble Gas Species | |||||
言語 | ||||||
言語 | eng | |||||
資源タイプ | ||||||
資源タイプ識別子 | http://purl.org/coar/resource_type/c_6501 | |||||
資源タイプ | journal article | |||||
アクセス権 | ||||||
アクセス権 | metadata only access | |||||
アクセス権URI | http://purl.org/coar/access_right/c_14cb | |||||
著者 |
松山, 顕之
× 松山, 顕之× 矢木, 雅敏× 松山 顕之× 矢木 雅敏 |
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抄録 | ||||||
内容記述タイプ | Abstract | |||||
内容記述 | The effects of impurities on runaway electron generation are studied using a zero-dimensional disruption simulation code. For describing collisions between fast electrons and partially stripped ions, a charge-resolved expression of the Coulomb logarithm is employed. Numerical analysis of the avalanche growth rate using the adjoint Fokker-Planck method is compared with two existing semi-analytic models, showing (i) the convergence of the growth rate to strong electric field limit of the Rosenbluth-Putvinski (R-P) model and (ii) the cancellation of the effect of second-order collisional diffusion for intermediate electric fields. Using the developed current quench (CQ) simulations, the parametric study is performed with the aid of the power balance analysis, which characterizes the onset of strong avalanche amplification in the presence of low-Z and noble gas species. Thermal quench (TQ) simulations are also developed for self-consistent evaluation of hot-tail seed electrons. The deposition timescale of impurity neutrals is shown to have significant impacts on hot-tail seeds, depending nonmonotonically on the pre-TQ temperature and the injected impurity density. |
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書誌情報 |
Plasma and Fusion Research 巻 12, p. 1403032-1-1403032-21, 発行日 2017-08 |
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DOI | ||||||
識別子タイプ | DOI | |||||
関連識別子 | 10.1585/pfr.12.1403032 |