Abstract
| Original language | English |
|---|---|
| Article number | 083007 |
| Journal | Nuclear Fusion |
| Volume | 52 |
| Issue number | 8 |
| DOIs | |
| Publication status | Published - 2012 |
| MoE publication type | A1 Journal article-refereed |
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Non-resonant magnetic braking on JET and TEXTOR. / Sun, Y.; Liang, Y.; Shaing, K.C.; Liu, Y.Q.; Koslowski, H.R.; Jachmich, S.; Alper, B.; Alfier, A.; Asunta, O.; Buratti, P.; Corrigan, G.; Delabie, E.; Giroud, C.; Gryaznevich, M.P.; Harting, D.; Hender, T.; Nardon, E.; Naulin, V.; Parail, V.; Tala, Tuomas; Wiegmann, C.; Wiesen, S.; Zhang, T.; contributors, JET-EFDA.
In: Nuclear Fusion, Vol. 52, No. 8, 083007, 2012.Research output: Contribution to journal › Article › Scientific › peer-review
TY - JOUR
T1 - Non-resonant magnetic braking on JET and TEXTOR
AU - Sun, Y.
AU - Liang, Y.
AU - Shaing, K.C.
AU - Liu, Y.Q.
AU - Koslowski, H.R.
AU - Jachmich, S.
AU - Alper, B.
AU - Alfier, A.
AU - Asunta, O.
AU - Buratti, P.
AU - Corrigan, G.
AU - Delabie, E.
AU - Giroud, C.
AU - Gryaznevich, M.P.
AU - Harting, D.
AU - Hender, T.
AU - Nardon, E.
AU - Naulin, V.
AU - Parail, V.
AU - Tala, Tuomas
AU - Wiegmann, C.
AU - Wiesen, S.
AU - Zhang, T.
AU - contributors, JET-EFDA
PY - 2012
Y1 - 2012
N2 - The non-resonant magnetic braking effect induced by a non-axisymmetric magnetic perturbation is investigated on JET and TEXTOR. The collisionality dependence of the torque induced by the n = 1, where n is the toroidal mode number, magnetic perturbation generated by the error field correction coils on JET is observed. The observed torque is located mainly in the plasma core (normalized radius ρ < 0.4) and increases with decreasing collisionality. The neoclassical toroidal plasma viscosity (NTV) torque in the collisionless regime is modelled using the numerical solution of the bounce-averaged drift kinetic equation. The calculated collisionality dependence of the NTV torque is in good agreement with the experimental observation on JET. The reason for this collisionality dependence is that the torque in the plasma core on JET mainly comes from the flux of the trapped electrons, which are still mainly in the 1/ν regime. The strongest NTV torque on JET is also located near the plasma core. The magnitude of the NTV torque strongly depends on the plasma response, which is also discussed in this paper. There is no obvious braking effect with n = 2 magnetic perturbation generated by the dynamic ergodic divertor on TEXTOR, which is consistent with the NTV modelling.
AB - The non-resonant magnetic braking effect induced by a non-axisymmetric magnetic perturbation is investigated on JET and TEXTOR. The collisionality dependence of the torque induced by the n = 1, where n is the toroidal mode number, magnetic perturbation generated by the error field correction coils on JET is observed. The observed torque is located mainly in the plasma core (normalized radius ρ < 0.4) and increases with decreasing collisionality. The neoclassical toroidal plasma viscosity (NTV) torque in the collisionless regime is modelled using the numerical solution of the bounce-averaged drift kinetic equation. The calculated collisionality dependence of the NTV torque is in good agreement with the experimental observation on JET. The reason for this collisionality dependence is that the torque in the plasma core on JET mainly comes from the flux of the trapped electrons, which are still mainly in the 1/ν regime. The strongest NTV torque on JET is also located near the plasma core. The magnitude of the NTV torque strongly depends on the plasma response, which is also discussed in this paper. There is no obvious braking effect with n = 2 magnetic perturbation generated by the dynamic ergodic divertor on TEXTOR, which is consistent with the NTV modelling.
U2 - 10.1088/0029-5515/52/8/083007
DO - 10.1088/0029-5515/52/8/083007
M3 - Article
VL - 52
JO - Nuclear Fusion
JF - Nuclear Fusion
SN - 0029-5515
IS - 8
M1 - 083007
ER -