Observation of spectrum effect on the measurement of intrinsic error field on EAST

HH Wang, YW Sun, JP Qian, TH Shi, B Shen… - Nuclear …, 2016 - iopscience.iop.org
HH Wang, YW Sun, JP Qian, TH Shi, B Shen, S Gu, YQ Liu, WF Guo, N Chu, KY He, MN Jia…
Nuclear Fusion, 2016iopscience.iop.org
Intrinsic error field on EAST is measured using the'compass scan'technique with different n=
1 magnetic perturbation coil configurations in ohmically heated discharges. The intrinsic
error field measured using a non-resonant dominated spectrum with even connection of the
upper and lower resonant magnetic perturbation coils is of the order ${{b} _ {r2, 1}}/{{B} _
{\text {T}}}\simeq {{10}^{-5}} $ and the toroidal phase of intrinsic error field is around
${{60}^{{}^\circ}} $. A clear difference between the results using the two coil configurations …
Abstract
Intrinsic error field on EAST is measured using the'compass scan'technique with different n= 1 magnetic perturbation coil configurations in ohmically heated discharges. The intrinsic error field measured using a non-resonant dominated spectrum with even connection of the upper and lower resonant magnetic perturbation coils is of the order and the toroidal phase of intrinsic error field is around . A clear difference between the results using the two coil configurations, resonant and non-resonant dominated spectra, is observed. The'resonant'and'non-resonant'terminology is based on vacuum modeling. The penetration thresholds of the non-resonant dominated cases are much smaller than that of the resonant cases. The difference of penetration thresholds between the resonant and non-resonant cases is reduced by plasma response modeling using the MARS-F code.
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