61st Annual Meeting of the APS Division of Plasma Physics
Volume 64, Number 11
Monday–Friday, October 21–25, 2019;
Fort Lauderdale, Florida
Session GI2: Invited MF: Stellarators and Computational Techniques
9:30 AM–12:30 PM,
Tuesday, October 22, 2019
Room: Floridian Ballroom AB
Chair: Benjamin Faber, University of Wisconsin
Abstract ID: BAPS.2019.DPP.GI2.1
Abstract: GI2.00001 : Observation of isotope separating and mixing states in isotope mixture plasmas in LHD
9:30 AM–10:00 AM
Preview Abstract
Abstract
Author:
Katsumi Ida
(National Institute for Fusion Science)
Ion and electron density profiles are identical due to quasi-neutrality in single isotope plasmas. However, in mixed isotope plasmas, individual isotope density profiles can differ. Measurements of radial hydrogen (H) and deuterium (D) density profiles, using bulk charge exchange recombination spectroscopy, reveal two states of isotope particle transport in H-D in LHD plasmas[1]. One is isotope-separating (IS), where the source location impacts the density ratio profile and the other is isotope-mixing (IM) where the density ratio profile is flat regardless of the location of the H and D source. Gyrokinetic simulations predict an IM state in ITG turbulence regimes and an IS state in TEM regimes[2].
The IS state is observed in the low-density plasmas ($n_e$ $\sim$ 1.5 $\times$ 10$^{19}$m$^{-3}$, $dn_e/dr$(0.8$\rho$) $<$ 0) where the beam fueling isotope species differ from the isotope species due to recycling. The H/(H+D) density profile is peaked for H beam fueling and D recycling wall conditions. A peaking of D/(H+D) density is observed for D beam fueling and H recycling wall conditions. When the wall recycling is equally mixed, (H/D $\sim$ 1), H/(H+D) dominates and D/(H+D) disappears. In contrast, the IM state is observed in higher density plasmas ($n_e$ $\sim$ 3$\times$ 10$^{19}$m$^{-3}$, $dn_e/dr$ (0.8$\rho$) $>$ 0) with shallow pellet injection. H and D pellets have been deposited at 0.9$\rho$ in the plasmas with peaked H/(H+D) density profile. This results in the H/(H+D) profile becoming flat after the H and D pellets are injected, which clearly results in the IM state.
These results demonstrate that either of two isotope states (IS or IM) can exist in mixed H and D plasmas depending on collisionality and density gradient and provides important insight into the control of isotope density ratio profiles needed for DT operations in tokamaks.
[1] K. Ida, et. al., Nucl. Fusion 59 (2019) 056029.
[2] C. Bourdelle et. al., Nucl. Fusion 58 (2018) 076028.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2019.DPP.GI2.1