Poloidal rotation velocity measurement with an MIR system on KSTAR

被引:10
|
作者
Lee, W. [1 ]
Leem, J. [1 ]
Yun, G. S. [1 ]
Park, H. K. [1 ]
Lee, J. A. [1 ]
Nam, Y. B. [1 ]
Nam, Y. U. [2 ]
Ko, W. H. [2 ]
Jeong, J. H. [2 ]
Bae, Y. S. [2 ]
Park, H. [3 ]
Kim, K. W. [3 ]
Domier, C. W. [4 ]
Luhmann, N. C., Jr. [4 ]
机构
[1] POSTECH, Dept Phys, Pohang 790784, Gyeongbuk, South Korea
[2] Natl Fus Res Inst, Taejon 305333, South Korea
[3] Kyungpook Natl Univ, Sch Elect Engn, Taegu 702701, South Korea
[4] Univ Calif Davis, Dept Elect & Comp Engn, Davis, CA 95616 USA
来源
关键词
Nuclear instruments and methods for hot plasma diagnostics; Plasma diagnostics - interferometry; spectroscopy and imaging; FLUCTUATION MEASUREMENTS; MICROWAVE; REFLECTOMETRY; DENSITY; PLASMA;
D O I
10.1088/1748-0221/8/10/C10018
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
A multi-channel microwave imaging reflectometry (MIR) system has been commissioned in the 2012 and 2013 KSTAR campaigns for the measurement of semi 2D (16 poloidal and 2 radial channels) electron density fluctuations for transport study on KSTAR. A time delayed cross correlation analysis among 16 poloidal channels has been applied to obtain the poloidal rotation velocities of the measured turbulent density fluctuations. The measured poloidal rotation directions for an 170 GHz ECH assisted ohmic plasma was in opposite direction to that of a neutral beam (NB) heated L-mode plasma. This is due to the fact that the intrinsic toroidal rotation in ohmic plasma (counter-clockwise) is in opposite direction to the NB heated plasma (clockwise) with respect to the plasma current direction.
引用
收藏
页数:10
相关论文
共 50 条
  • [1] IMPURITY POLOIDAL ROTATION VELOCITY IN TOKAMAKS
    MEIGS, AG
    ROWAN, WL
    PHYSICS OF PLASMAS, 1994, 1 (04) : 960 - 967
  • [2] KSTAR poloidal and toroidal field design
    Lee, BJ
    Pomphrey, N
    Chang, CS
    Cho, SY
    Jardin, SC
    Lee, GS
    Neilson, GH
    Park, H
    Reierson, W
    17TH IEEE/NPSS SYMPOSIUM ON FUSION ENGINEERING, VOLS 1 AND 2, 1998, : 641 - 644
  • [3] Predictions of the poloidal asymmetries and transport frequencies in KSTAR
    Bae, C.
    Stacey, W. M.
    Lee, S. G.
    Terzolo, L.
    PHYSICS OF PLASMAS, 2014, 21 (01)
  • [4] Design and analysis of poloidal field magnet structures for KSTAR
    Ahn, HJ
    Kwon, TH
    Lee, YW
    Lee, CD
    Choi, CH
    Sa, JW
    Oh, YK
    IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, 2004, 14 (02) : 1423 - 1426
  • [5] Measurement of poloidal velocity on the National Spherical Torus Experiment (invited)
    Bell, Ronald E.
    Feder, Russell
    REVIEW OF SCIENTIFIC INSTRUMENTS, 2010, 81 (10):
  • [6] POLOIDAL ROTATION IN TOKAMAKS
    HASSAM, AB
    KULSRUD, RM
    BULLETIN OF THE AMERICAN PHYSICAL SOCIETY, 1976, 21 (09): : 1089 - 1089
  • [7] A method for determining poloidal rotation from poloidal asymmetry in toroidal rotation (invited)
    Chrystal, C.
    Burrell, K. H.
    Grierson, B. A.
    Lao, L. L.
    Pace, D. C.
    REVIEW OF SCIENTIFIC INSTRUMENTS, 2014, 85 (11):
  • [8] Measurement of angular velocity in the perception of rotation
    Barraza, JF
    Grzywacz, NM
    VISION RESEARCH, 2002, 42 (21) : 2457 - 2462
  • [9] Demonstration of real-time control for poloidal beta in KSTAR
    Han, Hyunsun
    Hahn, S. H.
    Bak, J. G.
    Hyatt, A.
    Johnson, R.
    Woo, M. H.
    Kim, J. S.
    Bae, Y. S.
    FUSION ENGINEERING AND DESIGN, 2015, 95 : 44 - 49
  • [10] Measurements of poloidal rotation velocity using charge exchange spectroscopy in a large helical device
    Ida, K
    Kado, S
    Liang, Y
    REVIEW OF SCIENTIFIC INSTRUMENTS, 2000, 71 (06): : 2360 - 2366