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dc.contributor.authorEdlund, Eric Matthias
dc.contributor.authorBonoli, Paul T
dc.contributor.authorPorkolab, Miklos
dc.contributor.authorWukitch, Stephen James
dc.date.accessioned2017-05-19T16:43:32Z
dc.date.available2017-05-19T16:43:32Z
dc.date.issued2015-12
dc.identifier.issn0094-243X
dc.identifier.issn1551-7616
dc.identifier.urihttp://hdl.handle.net/1721.1/109214
dc.description.abstractAccess to advanced operating regimes in the EAST tokamak will require a combination of electron-cyclotron resonance heating (ECRH), neutral beam injection (NBI) and ion cyclotron range frequency heating (ICRF), with the addition of lower-hybrid current drive (LHCD) for current profile control. Prior experiments at the EAST tokamak facility have shown relatively weak response of the plasma temperature to application of ICRF heating, with typical coupled power about 2 MW out of 12 MW source. The launched spectrum, at n[subscript φ] = 34 for 0-π -0-π phasing and 27 MHz, is largely inaccessible at line-averaged densities of approximately 2 × 10[superscript 19] m[superscript −3]. However, with variable antenna phasing and frequency, this system has considerable latitude to explore different heating schemes. To develop an ICRF actuator control model, we have used the full-wave code TORIC to explore the physics of ICRF wave propagation in EAST. The results presented from this study use a spectrum analysis using a superposition of nφ spanning −50 to +50. The low density regime typical of EAST plasmas results in a perpendicular wavelength comparable to the minor radius which results in global cavity resonance effects and eigenmode formation when the single-pass absorption is low. This behavior indicates that improved performance can be attained by lowering the peak of the k[subscript ||] spectrum by using π/3 phasing of the 4-strap antenna. Based on prior studies conducted at Alcator C-Mod, this phasing is also expected to have the advantage of nearly divergence-free box currents, which should result in reduced levels of impurity production. Significant enhancements of the loading resistance may be achieved by using low k|| phasing and a combination of magnetic field and frequency to vary the location of the resonance and mode conversion regions. TORIC calculations indicate that the significant power may be channeled to the electrons and deuterium majority. We expect that implementation of these recommendations in EAST will yield substantial improvements in the net absorbed power that will greatly assist in the attempt to access advanced tokamak operating regimes.en_US
dc.description.sponsorshipUnited States. Department of Energy (contract DE-FC02-01ER54648)en_US
dc.language.isoen_US
dc.publisherAmerican Institute of Physics (AIP)en_US
dc.relation.isversionofhttp://dx.doi.org/10.1063/1.4936500en_US
dc.rightsCreative Commons Attribution-Noncommercial-Share Alikeen_US
dc.rights.urihttp://creativecommons.org/licenses/by-nc-sa/4.0/en_US
dc.sourceMIT Web Domainen_US
dc.titleModeling of EAST ICRF antenna performance using the full-wave code TORICen_US
dc.typeArticleen_US
dc.identifier.citationEdlund, E. M., P. T. Bonoli, M. Porkolab, and S. J. Wukitch. “Modeling of EAST ICRF Antenna Performance Using the Full-Wave Code TORIC” AIP Conference Proceedings 1689, 060002 (2015)en_US
dc.contributor.departmentMassachusetts Institute of Technology. Plasma Science and Fusion Centeren_US
dc.contributor.mitauthorEdlund, Eric Matthias
dc.contributor.mitauthorBonoli, Paul T
dc.contributor.mitauthorPorkolab, Miklos
dc.contributor.mitauthorWukitch, Stephen James
dc.eprint.versionAuthor's final manuscripten_US
dc.type.urihttp://purl.org/eprint/type/ConferencePaperen_US
eprint.statushttp://purl.org/eprint/status/NonPeerRevieweden_US
dspace.orderedauthorsEdlund, E. M.; Bonoli, P. T.; Porkolab, M.; Wukitch, S. J.en_US
dspace.embargo.termsNen_US
dc.identifier.orcidhttps://orcid.org/0000-0002-1620-9680
dc.identifier.orcidhttps://orcid.org/0000-0002-9518-4097
mit.licenseOPEN_ACCESS_POLICYen_US
mit.metadata.statusComplete


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