| dc.contributor.author | Burrell, K. H. | |
| dc.contributor.author | Rost, Jon C. | |
| dc.contributor.author | Porkolab, Miklos | |
| dc.contributor.author | Dorris, James | |
| dc.date.accessioned | 2015-09-01T14:29:37Z | |
| dc.date.available | 2015-09-01T14:29:37Z | |
| dc.date.issued | 2014-06 | |
| dc.date.submitted | 2013-11 | |
| dc.identifier.issn | 1070-664X | |
| dc.identifier.issn | 1089-7674 | |
| dc.identifier.uri | http://hdl.handle.net/1721.1/98285 | |
| dc.description.abstract | A region of turbulence with large radial wavenumber (k[subscript r]ρ[subscript s] > 1) is found in the high-shear portion of the plasma edge in Quiescent H-mode (QH-mode) on DIII–D using the Phase Contrast Imaging (PCI) diagnostic. At its peak outside the minimum of the Er well, the turbulence exhibits large amplitude [~ over n]/n ~ 40%, with large radial wavenumber ∣[¯over k][subscript r]/[¯ over k][subscript θ]∣ ~ 11 and short radial correlation length L[subscript r]/ρ[subscript i] ~ 0.2. The turbulence inside the E[subscript r] well minimum is characterized by the opposite sign in radial wavenumber from that of turbulence outside the minimum, consistent with the expected effects of velocity shear. The PCI diagnostic provides a line-integrated measurement of density fluctuations, so data are taken during a scan of plasma position at constant parameters to allow the PCI to sample a range in k[subscript r]/k[subscript θ]. Analysis of the Doppler shift and plasma geometry allows the turbulence to be localized to a narrow region 3 mm inside the last closed flux surface, outside the minimum of the E[subscript r] well. The turbulence amplitude and radial wavenumber and correlation length are determined by fitting the PCI results with a simple non-isotropic turbulence model with two regions of turbulence. These PCI observations, made in QH-mode, are qualitatively similar to those made in standard edge localized modes (ELM)-free H-mode and between ELMs, suggesting a similar role for large k[subscript r] turbulence there. | en_US |
| dc.description.sponsorship | United States. Dept. of Energy (DE-FG02-94ER54235) | en_US |
| dc.description.sponsorship | United States. Dept. of Energy (DE-FC02-04ER54698) | en_US |
| dc.language.iso | en_US | |
| dc.publisher | American Institute of Physics (AIP) | en_US |
| dc.relation.isversionof | http://dx.doi.org/10.1063/1.4883135 | en_US |
| dc.rights | Creative Commons Attribution-Noncommercial-Share Alike | en_US |
| dc.rights.uri | http://creativecommons.org/licenses/by-nc-sa/4.0/ | en_US |
| dc.source | MIT web domain | en_US |
| dc.title | Short wavelength turbulence generated by shear in the QH-mode edge on DIII–D | en_US |
| dc.title.alternative | Short wavelength turbulence generated by shear in the quiescent H-mode edge on DIII–D | en_US |
| dc.type | Article | en_US |
| dc.identifier.citation | Rost, J. C., M. Porkolab, J. Dorris, and K. H. Burrell. “Short Wavelength Turbulence Generated by Shear in the Quiescent H-Mode Edge on DIII–D.” Phys. Plasmas 21, no. 6 (June 2014): 062306. | en_US |
| dc.contributor.department | Massachusetts Institute of Technology. Department of Physics | en_US |
| dc.contributor.department | Massachusetts Institute of Technology. Plasma Science and Fusion Center | en_US |
| dc.contributor.mitauthor | Rost, Jon C. | en_US |
| dc.contributor.mitauthor | Porkolab, Miklos | en_US |
| dc.contributor.mitauthor | Dorris, James | en_US |
| dc.relation.journal | Physics of Plasmas | en_US |
| dc.eprint.version | Author's final manuscript | en_US |
| dc.type.uri | http://purl.org/eprint/type/JournalArticle | en_US |
| eprint.status | http://purl.org/eprint/status/PeerReviewed | en_US |
| dspace.orderedauthors | Rost, J. C.; Porkolab, M.; Dorris, J.; Burrell, K. H. | en_US |
| dc.identifier.orcid | https://orcid.org/0000-0002-9518-4097 | |
| mit.license | OPEN_ACCESS_POLICY | en_US |
| mit.metadata.status | Complete | |