Numerical analysis on the characteristics of particle orbits in quasi-axisymmetric stellarator

Based on the magnetic field configuration of the Chinese First Quasi-axisymmetric Stellarator (CFQS) device, three types of orbits such as the passing orbit, blocked trapped orbit, and localized trapped orbit are simulated using the Boris algorithm. Also, the orbital topology, orbit transition, and...

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Main Authors: C. Y. Su, S. Y. Chen, H. F. Liu, M. L. Mou, W. P. Guo, C. J. Tang
Format: Article
Language:English
Published: AIP Publishing LLC 2020-01-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.5124452
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spelling doaj-f4cb69a58e2c414a8df03276f23c9fb32020-11-25T00:17:11ZengAIP Publishing LLCAIP Advances2158-32262020-01-01101015004015004-710.1063/1.5124452Numerical analysis on the characteristics of particle orbits in quasi-axisymmetric stellaratorC. Y. Su0S. Y. Chen1H. F. Liu2M. L. Mou3W. P. Guo4C. J. Tang5College of Physics, Sichuan University, Chengdu 610065, ChinaCollege of Physics, Sichuan University, Chengdu 610065, ChinaCollege of Physics, Sichuan University, Chengdu 610065, ChinaCollege of Physics, Sichuan University, Chengdu 610065, ChinaCollege of Physics, Sichuan University, Chengdu 610065, ChinaCollege of Physics, Sichuan University, Chengdu 610065, ChinaBased on the magnetic field configuration of the Chinese First Quasi-axisymmetric Stellarator (CFQS) device, three types of orbits such as the passing orbit, blocked trapped orbit, and localized trapped orbit are simulated using the Boris algorithm. Also, the orbital topology, orbit transition, and loss characteristics of these particles under different initial conditions are studied in this paper. It is found that there exists a transition from blocked trapped orbits to localized trapped orbits due to small continuous helical ripples. This phenomenon is analyzed as follows: we define the angle between the particle drift velocity (v→D) and the radial direction (ρ^) as β. If the blocked-localized transition appears in the region where β>90○, the localized particles will return to the blocked particles and be constrained. However, if the blocked-localized transition happens in the region where β<90○, localized particles will drift out of the last closed flux surface and be lost. The simulation results show that the loss of localized particles in the CFQS is mainly located in some specific regions within the vicinity of the toroidal angle φ=0○,180○ and the poloidal angle θ=90○.http://dx.doi.org/10.1063/1.5124452
collection DOAJ
language English
format Article
sources DOAJ
author C. Y. Su
S. Y. Chen
H. F. Liu
M. L. Mou
W. P. Guo
C. J. Tang
spellingShingle C. Y. Su
S. Y. Chen
H. F. Liu
M. L. Mou
W. P. Guo
C. J. Tang
Numerical analysis on the characteristics of particle orbits in quasi-axisymmetric stellarator
AIP Advances
author_facet C. Y. Su
S. Y. Chen
H. F. Liu
M. L. Mou
W. P. Guo
C. J. Tang
author_sort C. Y. Su
title Numerical analysis on the characteristics of particle orbits in quasi-axisymmetric stellarator
title_short Numerical analysis on the characteristics of particle orbits in quasi-axisymmetric stellarator
title_full Numerical analysis on the characteristics of particle orbits in quasi-axisymmetric stellarator
title_fullStr Numerical analysis on the characteristics of particle orbits in quasi-axisymmetric stellarator
title_full_unstemmed Numerical analysis on the characteristics of particle orbits in quasi-axisymmetric stellarator
title_sort numerical analysis on the characteristics of particle orbits in quasi-axisymmetric stellarator
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2020-01-01
description Based on the magnetic field configuration of the Chinese First Quasi-axisymmetric Stellarator (CFQS) device, three types of orbits such as the passing orbit, blocked trapped orbit, and localized trapped orbit are simulated using the Boris algorithm. Also, the orbital topology, orbit transition, and loss characteristics of these particles under different initial conditions are studied in this paper. It is found that there exists a transition from blocked trapped orbits to localized trapped orbits due to small continuous helical ripples. This phenomenon is analyzed as follows: we define the angle between the particle drift velocity (v→D) and the radial direction (ρ^) as β. If the blocked-localized transition appears in the region where β>90○, the localized particles will return to the blocked particles and be constrained. However, if the blocked-localized transition happens in the region where β<90○, localized particles will drift out of the last closed flux surface and be lost. The simulation results show that the loss of localized particles in the CFQS is mainly located in some specific regions within the vicinity of the toroidal angle φ=0○,180○ and the poloidal angle θ=90○.
url http://dx.doi.org/10.1063/1.5124452
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