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dc.contributor.authorLiu, Z. X.
dc.contributor.authorXu, X. Q.
dc.contributor.authorGao, X.
dc.contributor.authorXia, T. Y.
dc.contributor.authorZhang, T.
dc.contributor.authorLi, J. G.
dc.contributor.authorHubbard, Amanda E
dc.contributor.authorHughes Jr, Jerry
dc.contributor.authorWalk Jr, John R
dc.contributor.authorTheiler, Christian
dc.contributor.authorBaek, Seung Gyou
dc.contributor.authorGolfinopoulos, Theodore
dc.contributor.authorWhyte, Dennis G
dc.date.accessioned2018-07-25T18:12:59Z
dc.date.available2018-07-25T18:12:59Z
dc.date.issued2016-12
dc.date.submitted2016-08
dc.identifier.issn1070-664X
dc.identifier.issn1089-7674
dc.identifier.urihttp://hdl.handle.net/1721.1/117124
dc.description.abstractThe weakly coherent mode (WCM) in I-mode has been studied by a six-field two-fluid model based on the Braginskii equations under the BOUT++ framework for the first time. The calculations indicate that a tokamak pedestal exhibiting a WCM is linearly unstable to drift Alfven wave (DAW) instabilities and the resistive ballooning mode. The nonlinear simulation shows promising agreement with the experimental measurements of the WCM. The shape of the density spectral and location of the spectral peak of the dominant toroidal number mode n = 20 agrees with the experimental data from reflectometry. The simulated mode propagates in electron diamagnetic direction is consistent with the results from the magnetic probes in the laboratory frame, a large ratio of particle to heat diffusivity is consistent with the distinctive experimental feature of I-mode, and the value of the simulated χeat the edge is in the range of experimental errors of χefffrom the experiment. The prediction of the WCM shows that free energy is mainly provided by the electron pressure gradient, which gives guidance for pursuing future I-mode studies.en_US
dc.publisherAIP Publishingen_US
dc.relation.isversionofhttp://dx.doi.org/10.1063/1.4972088en_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.titleThe physics mechanisms of the weakly coherent mode in the Alcator C-Mod Tokamaken_US
dc.typeArticleen_US
dc.identifier.citationLiu, Z. X. et al. “The Physics Mechanisms of the Weakly Coherent Mode in the Alcator C-Mod Tokamak.” Physics of Plasmas 23, 12 (December 2016): 120703 © 2016 Author(s)en_US
dc.contributor.departmentMassachusetts Institute of Technology. Plasma Science and Fusion Centeren_US
dc.contributor.mitauthorHubbard, Amanda E
dc.contributor.mitauthorHughes Jr, Jerry
dc.contributor.mitauthorWalk Jr, John R
dc.contributor.mitauthorTheiler, Christian
dc.contributor.mitauthorBaek, Seung Gyou
dc.contributor.mitauthorGolfinopoulos, Theodore
dc.contributor.mitauthorWhyte, Dennis G
dc.relation.journalPhysics of Plasmasen_US
dc.eprint.versionOriginal manuscripten_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/NonPeerRevieweden_US
dc.date.updated2018-07-20T18:20:06Z
dspace.orderedauthorsLiu, Z. X.; Xu, X. Q.; Gao, X.; Hubbard, A. E.; Hughes, J. W.; Walk, J. R.; Theiler, C.; Xia, T. Y.; Baek, S. G.; Golfinopoulos, T.; Whyte, D.; Zhang, T.; Li, J. G.en_US
dspace.embargo.termsNen_US
dc.identifier.orcidhttps://orcid.org/0000-0003-4802-4944
dc.identifier.orcidhttps://orcid.org/0000-0001-8324-4227
dc.identifier.orcidhttps://orcid.org/0000-0001-8029-3525
dc.identifier.orcidhttps://orcid.org/0000-0002-0898-5217
dc.identifier.orcidhttps://orcid.org/0000-0002-9001-5606
mit.licenseOPEN_ACCESS_POLICYen_US


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