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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Main Authors: Kernbichler Winfried, Kapper Gernot, Kasilov Sergei V., Marushchenko Nikolai B.
Format: Article
Language:English
Published: EDP Sciences 2015-01-01
Series:EPJ Web of Conferences
Online Access:http://dx.doi.org/10.1051/epjconf/20158701006
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spelling 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.
url http://dx.doi.org/10.1051/epjconf/20158701006
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AT kappergernot computationofthespitzerfunctioninstellaratorsandtokamakswithfinitecollisionality
AT kasilovsergeiv computationofthespitzerfunctioninstellaratorsandtokamakswithfinitecollisionality
AT marushchenkonikolaib computationofthespitzerfunctioninstellaratorsandtokamakswithfinitecollisionality
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