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An upgrade of the magnetic diagnostic system of the DIII-D tokamak for non-axisymmetric measurements

dc.contributor.authorKing, J. D
dc.contributor.authorStrait, E. J
dc.contributor.authorBoivin, R. L
dc.contributor.authorTaussig, D.
dc.contributor.authorWatkins, M. G
dc.contributor.authorHanson, J. M
dc.contributor.authorLogan, N. C
dc.contributor.authorPaz-Soldan, C.
dc.contributor.authorPace, D. C
dc.contributor.authorShiraki, D.
dc.contributor.authorLanctot, M. J
dc.contributor.authorLa Haye, R. J
dc.contributor.authorLao, L. L
dc.contributor.authorBattaglia, D. J
dc.contributor.authorSontag, A. C
dc.contributor.authorHaskey, S. R
dc.contributor.authorBak, J. G
dc.date.accessioned2015-12-07T03:22:41Z
dc.date.available2015-12-07T03:22:41Z
dc.date.issued2014
dc.date.updated2015-12-08T10:41:46Z
dc.description.abstractThe DIII-D tokamak magnetic diagnostic system [E. J. Strait, Rev. Sci. Instrum. 77, 023502 (2006)] has been upgraded to significantly expand the measurement of the plasma response to intrinsic and applied non-axisymmetric "3D" fields. The placement and design of 101 additional sensors allow resolution of toroidal mode numbers 1 ≤ n ≤ 3, and poloidal wavelengths smaller than MARS-F, IPEC, and VMEC magnetohydrodynamic model predictions. Small 3D perturbations, relative to the equilibrium field (10(-5) < δB/B0 < 10(-4)), require sub-millimeter fabrication and installation tolerances. This high precision is achieved using electrical discharge machined components, and alignment techniques employing rotary laser levels and a coordinate measurement machine. A 16-bit data acquisition system is used in conjunction with analog signal-processing to recover non-axisymmetric perturbations. Co-located radial and poloidal field measurements allow up to 14.2 cm spatial resolution of poloidal structures (plasma poloidal circumference is ~500 cm). The function of the new system is verified by comparing the rotating tearing mode structure, measured by 14 BP fluctuation sensors, with that measured by the upgraded B(R) saddle loop sensors after the mode locks to the vessel wall. The result is a nearly identical 2/1 helical eigenstructure in both cases.
dc.description.sponsorshipS. R. Haskey wishes to thank AINSE Ltd. for providing financial assistance.en_AU
dc.format9 pages
dc.identifier.issn0034-6748en_AU
dc.identifier.urihttp://hdl.handle.net/1885/17061
dc.publisherAmerican Institute of Physics (AIP)
dc.rights© 2014 AIP Publishing. This article may be downloaded for personal use only. Any other use requires prior permission of the author and AIP Publishing. The following article appeared in Review of Scientific Instruments and may be found at http://doi.org/10.1063/1.4891817 http://publishing.aip.org/authors/copyright-reuse http://www.sherpa.ac.uk/romeo/issn/0034-6748
dc.sourceReview of Scientific Instruments
dc.subjectDIII-D tokamak magnetic diagnostic system
dc.subjectplasma response
dc.subjectintrinsic and applied non-axisymmetric "3D" fields
dc.subject101 additional sensors
dc.subjecttoroidal mode numbers 1 ≤ n ≤ 3
dc.subjectpoloidal wavelengths
dc.subjecthigh precision
dc.subjectelectrical discharge
dc.titleAn upgrade of the magnetic diagnostic system of the DIII-D tokamak for non-axisymmetric measurements
dc.typeJournal article
dcterms.dateAccepted2014-07-21
local.bibliographicCitation.issue8en_AU
local.bibliographicCitation.lastpage8
local.bibliographicCitation.startpage083503en_AU
local.contributor.affiliationKing, J.D, Oak Ridge Institute for Science and Education, United States of Americaen_AU
local.contributor.affiliationStrait, E.J., General Atomics, United States of Americaen_AU
local.contributor.affiliationBoivin, R.L, General Atomics, United States of Americaen_AU
local.contributor.affiliationTaussig, D., General Atomics, United States of Americaen_AU
local.contributor.affiliationWatkins, M.G., General Atomics, United States of Americaen_AU
local.contributor.affiliationHanson, J M, Columbia University, United States of Americaen_AU
local.contributor.affiliationLogan, N.C., Princeton Plasma Physics Laboratory, United States of Americaen_AU
local.contributor.affiliationPaz-Soldan, C., Oak Ridge Institute for Science and Education, United States of Americaen_AU
local.contributor.affiliationPace, D.C., General Atomics, United States of Americaen_AU
local.contributor.affiliationShiraki, D., Columbia University, United States of Americaen_AU
local.contributor.affiliationLanctot , M J, General Atomics, United States of Americaen_AU
local.contributor.affiliationLa Haye, R.J., General Atomics, United States of Americaen_AU
local.contributor.affiliationLao, L.L., General Atomics, United States of Americaen_AU
local.contributor.affiliationBattaglia, D.J., Princeton Plasma Physics Laboratory, United States of Americaen_AU
local.contributor.affiliationSontag, A.C., Oak Ridge Institute for Science and Education, United States of Americaen_AU
local.contributor.affiliationHaskey, Shaun, College of Physical and Mathematical Sciences, CPMS Research School of Physics and Engineering, Plasma Research Laboratory, The Australian National Universityen_AU
local.contributor.affiliationBak, J G, National Fusion Research Institute, Korea, Southen_AU
local.contributor.authoruidu4707372en_AU
local.description.notesImported from ARIES.en_AU
local.identifier.absfor020204en_AU
local.identifier.ariespublicationu4695161xPUB147en_AU
local.identifier.citationvolume85en_AU
local.identifier.doi10.1063/1.4891817en_AU
local.identifier.essn1089-7623en_AU
local.identifier.scopusID2-s2.0-84905833563
local.publisher.urlhttps://www.aip.org/en_AU
local.type.statusPublished Versionen_AU

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