Home > Publications database > Application of the elliptic approximation model for the edge turbulence rotation measurement via the poloidal correlation reflectometer in Wendelstein 7-X > print |
001 | 904049 | ||
005 | 20240711113818.0 | ||
024 | 7 | _ | |a 10.1088/1741-4326/abfb15 |2 doi |
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024 | 7 | _ | |a 1741-4326 |2 ISSN |
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037 | _ | _ | |a FZJ-2021-05619 |
082 | _ | _ | |a 620 |
100 | 1 | _ | |a Han, X. |0 P:(DE-Juel1)171363 |b 0 |e Corresponding author |
245 | _ | _ | |a Application of the elliptic approximation model for the edge turbulence rotation measurement via the poloidal correlation reflectometer in Wendelstein 7-X |
260 | _ | _ | |a Vienna |c 2021 |b IAEA |
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520 | _ | _ | |a The perpendicular velocity (v⊥) of turbulence is measured by means of a hopping poloidal correlation reflectometer diagnostic for the study of turbulence rotation in the plasma edge region in Wendelstein 7-X. An elliptic approximation (EA) model is applied for calculating the space-time correlation in the edge region. The v⊥ profile is compared in the high-ι (edge ι ≈ 1.2) and limiter (edge ι < 1) configurations. It is found that the v⊥ gradient is inversely proportional to the heating power in the high-ι configuration, which could be attributed to the turbulence activities in the plasma edge. In the limiter configuration, the v⊥ spike is observed near the island boundary, which is corresponded to the plasma current crash. In the standard configuration (edge ι ≈ 1), the v⊥ profile in the island region distributes as a function of the perpendicular separation. With increasing of the plasma current, the island enlarges the size as is referred from the v⊥ scope, accompanying with steepening of the v⊥ gradient at the boundary of the island. |
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700 | 1 | _ | |a Xiang, H. M. |0 P:(DE-Juel1)179595 |b 2 |u fzj |
700 | 1 | _ | |a Vécsei, M. |0 P:(DE-HGF)0 |b 3 |
700 | 1 | _ | |a Knieps, A. |0 P:(DE-Juel1)173792 |b 4 |
700 | 1 | _ | |a Windisch, T. |0 P:(DE-HGF)0 |b 5 |
700 | 1 | _ | |a Anda, G. |0 P:(DE-HGF)0 |b 6 |
700 | 1 | _ | |a Andreeva, T. |0 0000-0003-2390-4240 |b 7 |
700 | 1 | _ | |a Bozhenkov, S. A. |0 0000-0003-4289-3532 |b 8 |
700 | 1 | _ | |a Geiger, J. |0 0000-0003-4268-7480 |b 9 |
700 | 1 | _ | |a Dunai, D. |0 P:(DE-Juel1)130002 |b 10 |
700 | 1 | _ | |a Trier, E. |0 0000-0002-6901-8669 |b 11 |
700 | 1 | _ | |a Rahbarnia, K. |0 0000-0002-5550-1801 |b 12 |
700 | 1 | _ | |a Zoletnik, S. |0 0000-0002-7324-2647 |b 13 |
700 | 1 | _ | |a Liang, Y. |b 14 |
700 | 1 | _ | |a W7-X Team, the |0 P:(DE-HGF)0 |b 15 |
773 | _ | _ | |a 10.1088/1741-4326/abfb15 |g Vol. 61, no. 6, p. 066029 - |0 PERI:(DE-600)2037980-8 |n 6 |p 066029 - |t Nuclear fusion |v 61 |y 2021 |x 0029-5515 |
856 | 4 | _ | |u https://juser.fz-juelich.de/record/904049/files/Han_2021_Nucl._Fusion_61_066029.pdf |y Restricted |
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