Computation of the Spitzer function in stellarators and tokamaks with finite collisionality
The generalized Spitzer function, which determines the current drive efficiency in toka- maks and stellarators is modelled for finite plasma collisionality with help of the drift kinetic equation solver NEO-2 [1]. The effect of finite collisionality on the global ECCD efficiency in a tokamak is stu...
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Series: | EPJ Web of Conferences |
Online Access: | http://dx.doi.org/10.1051/epjconf/20158701006 |
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doaj-6f45cfa753bf4b858e46f7db6af3c9e72021-08-02T17:24:26ZengEDP SciencesEPJ Web of Conferences2100-014X2015-01-01870100610.1051/epjconf/20158701006epjconf_ec2015_01006Computation of the Spitzer function in stellarators and tokamaks with finite collisionalityKernbichler Winfried0Kapper Gernot1Kasilov Sergei V.Marushchenko Nikolai B.2Fusion@ӦAW, Institute for Theoretical and Computational PhysicsFusion@ӦAW, Institute for Theoretical and Computational PhysicsMax Planck Institute for Plasma Physics, EURATOM Association The generalized Spitzer function, which determines the current drive efficiency in toka- maks and stellarators is modelled for finite plasma collisionality with help of the drift kinetic equation solver NEO-2 [1]. The effect of finite collisionality on the global ECCD efficiency in a tokamak is studied using results of the code NEO-2 as input to the ray tracing code TRAVIS [2]. As it is known [3], specific features of the generalized Spitzer function, which are absent in asymptotic (collisionless or highly collisional) regimes result in current drive from a symmetric microwave spectrum with respect to parallel wave numbers. Due to this effect the direction of the current may become independent of the microwave beam launch angle in advanced ECCD scenarii (O2 and X3) where due to relatively low optical depth a significant amount of power is absorbed by trapped particles. http://dx.doi.org/10.1051/epjconf/20158701006 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Kernbichler Winfried Kapper Gernot Kasilov Sergei V. Marushchenko Nikolai B. |
spellingShingle |
Kernbichler Winfried Kapper Gernot Kasilov Sergei V. Marushchenko Nikolai B. Computation of the Spitzer function in stellarators and tokamaks with finite collisionality EPJ Web of Conferences |
author_facet |
Kernbichler Winfried Kapper Gernot Kasilov Sergei V. Marushchenko Nikolai B. |
author_sort |
Kernbichler Winfried |
title |
Computation of the Spitzer function in stellarators and tokamaks with finite collisionality |
title_short |
Computation of the Spitzer function in stellarators and tokamaks with finite collisionality |
title_full |
Computation of the Spitzer function in stellarators and tokamaks with finite collisionality |
title_fullStr |
Computation of the Spitzer function in stellarators and tokamaks with finite collisionality |
title_full_unstemmed |
Computation of the Spitzer function in stellarators and tokamaks with finite collisionality |
title_sort |
computation of the spitzer function in stellarators and tokamaks with finite collisionality |
publisher |
EDP Sciences |
series |
EPJ Web of Conferences |
issn |
2100-014X |
publishDate |
2015-01-01 |
description |
The generalized Spitzer function, which determines the current drive efficiency in toka- maks and stellarators is modelled for finite plasma collisionality with help of the drift kinetic equation solver NEO-2 [1]. The effect of finite collisionality on the global ECCD efficiency in a tokamak is studied using results of the code NEO-2 as input to the ray tracing code TRAVIS [2]. As it is known [3], specific features of the generalized Spitzer function, which are absent in asymptotic (collisionless or highly collisional) regimes result in current drive from a symmetric microwave spectrum with respect to parallel wave numbers. Due to this effect the direction of the current may become independent of the microwave beam launch angle in advanced ECCD scenarii (O2 and X3) where due to relatively low optical depth a significant amount of power is absorbed by trapped particles.
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url |
http://dx.doi.org/10.1051/epjconf/20158701006 |
work_keys_str_mv |
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