1983
DOI: 10.1088/0029-5515/23/10/005
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Determination of the plasma column shape in a tokamak from magnetic measurements

Abstract: On the basis of differential and integral methods of solving the boundary value problem and with the help of poloidal-magnetic-field or flux measurements by means of probes located outside the vacuum chamber, methods which are insensitive to measurement errors are developed for determining the position and shape of the boundary magnetic surface in a tokamak.

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Cited by 22 publications
(15 citation statements)
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“…The explicit expression for the internal multi-polar moments is evaluated as an integral of the current density J / ðh 0 ;x 0 Þ that flows inside the torus with coordinate h; The total plasma current is proportional to the sum of all the internal multi-polar moments as [12]; …”
Section: Internal and External Multi-polar Momentsmentioning
confidence: 99%
“…The explicit expression for the internal multi-polar moments is evaluated as an integral of the current density J / ðh 0 ;x 0 Þ that flows inside the torus with coordinate h; The total plasma current is proportional to the sum of all the internal multi-polar moments as [12]; …”
Section: Internal and External Multi-polar Momentsmentioning
confidence: 99%
“…A quantitative evaluation of the shape of the current distribution along the plasma radius on the basis of magnetic probe readings -or by means of saddle and Rogowsky coils with a particular winding densitycan be obtained by the multipole moment method [38,46] which was originally proposed for small deviations from cylindrical symmetry. By applying various numerical methods to the processing of the magnetic measurement results, it has been possible, with parametric representation of the current distribution in a plasma with non-circular cross-section, to evaluate a number of parameters quite rapidly, within less than 1 ms and to within 10% -parameters characterizing the position and shape of the plasma, as well as pressure, internal inductance and the current density profile [47][48][49].…”
Section: Electric and Magnetic Measurementsmentioning
confidence: 99%
“…For electron density measurements in the range from 6xlO 12 cm" 3 to 1.5xlO 14 cm" 3 , a frequency range of 22-110 GHz is required. Contemporary generators are incapable of providing such a broad range of scanning, and it has accordingly been proposed that the whole range should be divided into four sub-ranges: [22][23][24][25][26][27][28][29][30][31][32][33][34][35][33][34][35][36][37][38][39][40][41][42][43][44][45][46][47][48][49][50] In the experiments on TFR [78], a reflectometer with a backward-wave oscillator was used which scanned the frequency of the ordinary wave (the electric field of the wave being parallel to the toroidal magnetic field) in the range 75-110 GHz. The transmitting and receiving antennas were separate.…”
Section: Electron Density Measurementsmentioning
confidence: 99%
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“…This is done by least square fitting a truncated series of toroidal harmonic functions to the magnetic measurements. In principle this first step can be sufficient to determine the plasma boundary [2][3][4][5][6][7][8][9] (also see the review article 10 ). Indeed the toroidal harmonics expansion is valid anywhere in the vacuum surrounding the plasma.…”
Section: Introductionmentioning
confidence: 99%