Second order kinetic theory of parallel momentum transport in collisionless drift wave turbulence
Abstract
A second order kinetic model for turbulent ion parallel momentum transport is presented. A new nonresonant second order parallel momentum flux term is calculated. The resonant component of the ion parallel electrostatic force is the momentum source, while the nonresonant component of the ion parallel electrostatic force compensates for that of the nonresonant second order parallel momentum flux. The resonant component of the kinetic momentum flux can be divided into three parts, including the pinch term, the diffusive term, and the residual stress. By reassembling the pinch term and the residual stress, the residual stress can be considered as a pinch term of parallel waveparticle resonant velocity, and, therefore, may be called as “resonant velocity pinch” term. Considering the resonant component of the ion parallel electrostatic force is the transfer rate between resonant ions and waves (or, equivalently, nonresonant ions), a conservation equation of the parallel momentum of resonant ions and waves is obtained.
 Authors:
 Department of Engineering Physics, Tsinghua University, Beijing 100084 (China)
 (China)
 Institute of Plasma Physics, Chinese Academy of Sciences, Hefei 230031 (China)
 Publication Date:
 OSTI Identifier:
 22599913
 Resource Type:
 Journal Article
 Resource Relation:
 Journal Name: Physics of Plasmas; Journal Volume: 23; Journal Issue: 8; Other Information: (c) 2016 Author(s); Country of input: International Atomic Energy Agency (IAEA)
 Country of Publication:
 United States
 Language:
 English
 Subject:
 70 PLASMA PHYSICS AND FUSION TECHNOLOGY; EQUATIONS; IONS; PARTICLES; RESIDUAL STRESSES; TRANSPORT THEORY; TURBULENCE; VELOCITY; WAVE PROPAGATION
Citation Formats
Li, Yang, Email: lyang13@mails.tsinghua.edu.cn, Southwestern Institute of Physics, Chengdu 610041, Gao, Zhe, Chen, Jiale, and Center for Magnetic Fusion Theory, Chinese Academy of Sciences, Hefei. Second order kinetic theory of parallel momentum transport in collisionless drift wave turbulence. United States: N. p., 2016.
Web. doi:10.1063/1.4960827.
Li, Yang, Email: lyang13@mails.tsinghua.edu.cn, Southwestern Institute of Physics, Chengdu 610041, Gao, Zhe, Chen, Jiale, & Center for Magnetic Fusion Theory, Chinese Academy of Sciences, Hefei. Second order kinetic theory of parallel momentum transport in collisionless drift wave turbulence. United States. doi:10.1063/1.4960827.
Li, Yang, Email: lyang13@mails.tsinghua.edu.cn, Southwestern Institute of Physics, Chengdu 610041, Gao, Zhe, Chen, Jiale, and Center for Magnetic Fusion Theory, Chinese Academy of Sciences, Hefei. 2016.
"Second order kinetic theory of parallel momentum transport in collisionless drift wave turbulence". United States.
doi:10.1063/1.4960827.
@article{osti_22599913,
title = {Second order kinetic theory of parallel momentum transport in collisionless drift wave turbulence},
author = {Li, Yang, Email: lyang13@mails.tsinghua.edu.cn and Southwestern Institute of Physics, Chengdu 610041 and Gao, Zhe and Chen, Jiale and Center for Magnetic Fusion Theory, Chinese Academy of Sciences, Hefei},
abstractNote = {A second order kinetic model for turbulent ion parallel momentum transport is presented. A new nonresonant second order parallel momentum flux term is calculated. The resonant component of the ion parallel electrostatic force is the momentum source, while the nonresonant component of the ion parallel electrostatic force compensates for that of the nonresonant second order parallel momentum flux. The resonant component of the kinetic momentum flux can be divided into three parts, including the pinch term, the diffusive term, and the residual stress. By reassembling the pinch term and the residual stress, the residual stress can be considered as a pinch term of parallel waveparticle resonant velocity, and, therefore, may be called as “resonant velocity pinch” term. Considering the resonant component of the ion parallel electrostatic force is the transfer rate between resonant ions and waves (or, equivalently, nonresonant ions), a conservation equation of the parallel momentum of resonant ions and waves is obtained.},
doi = {10.1063/1.4960827},
journal = {Physics of Plasmas},
number = 8,
volume = 23,
place = {United States},
year = 2016,
month = 8
}

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