Bulletin of the American Physical Society
60th Annual Meeting of the APS Division of Plasma Physics
Volume 63, Number 11
Monday–Friday, November 5–9, 2018; Portland, Oregon
Session CP11: Poster Session II: Basic Plasma Physics; Boundary, PMI, Proto-MPEX; International Tokamaks; Turbulence and Transport; Other Configurations; Z-pinch, Dense Plasma Focus and MagLIF (2:00pm-5:00pm)
Monday, November 5, 2018
OCC
Room: Exhibit Hall A1&A
Abstract ID: BAPS.2018.DPP.CP11.69
Abstract: CP11.00069 : Investigating the effects of radial density gradient length scale on the nonlinear saturation of drift wave turbulence and zonal flow formation
Presenter:
Boda Yuan
(Univ of California - San Diego, University of Science and Technology of China)
Authors:
Boda Yuan
(Univ of California - San Diego, University of Science and Technology of China)
Eleonore Geulin
(Univ of California - San Diego)
Wenbin Liu
(Univ of California - San Diego, Tisnghua University)
Saikat Chakraborty Thakur
(Univ of California - San Diego)
George R Tynan
(Univ of California - San Diego)
Controlled Shear Decorrelation eXperimental (CSDX) is a linear magnetized plasma device for drift wave (DW) turbulence and zonal flow (ZF) formation research. In addition to experiments, we shall present numerical studies of the influence of the radial density gradient length (ρs/Ln) on saturated DW turbulence. The simulation was carried out with BOUT++ (BOUndary Turbulence 3D 2-fluid edge simulation) model of CSDX. The evolution of plasma is very sensitive to ρs/Ln. As ρs/Ln increases, there is a rapid turning on of the turbulence features along with the formation of a mean E×B shear flow (ZF). The DW turbulence enhances, gets saturated and then decreases rapidly when the ZF forms and grows. Meanwhile, the ZF behaves similarly: increases, gets saturated and then collapses, even changes sign. Experimentally, increasing the magnetic field (B) has a similar effect. Previous experiments have shown the growth, saturation and relaxation of mean E×B profiles with increasing B [1]. However, due to limited RF power, the relaxation of the profiles was also accompanied by axial detachment at high B, which is not included in the simulations. In the upgraded CDSX (with up to 20 kWatts) we can decouple the two phenomena and compare with the numerical results.
[1] S. C. Thakur, PSST (2014)
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DPP.CP11.69
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