Published May 3, 2018 | Version v1
Report

Experiments on Helicons in DIII-D: Investigation of the Physics of a Reactor-Relevant Noninductive Current Drive Technology

  • 1. General Atomics, San Diego, CA 92186 (United States)
  • 2. Massachusetts Institute of Technology (MIT), Cambridge, MA 02139 (United States)
  • 3. University of California San Diego, CA 92093 (United States)
  • 4. Oak Ridge National Laboratory (ORNL), Oak Ridge, TN 37831 (United States)
  • 5. Princeton Plasma Physics Laboratory (PPPL), Princeton, NJ 08540 (United States)
  • 6. Sandia National Laboratories (SNL), Albuquerque, NM 87185 (United States)
  • 7. University of California Los Angeles, CA 90095 (United States)

Description

Full text: Experiments have begun in DIII-D to evaluate noninductive current drive by the Landau absorption of a toroidally-directive spectrum of helicon waves (also known as very high harmonic fast waves, fast waves in the lower hybrid range of frequencies, or whistlers). Modelling has shown that noninductive current drive at midradius (p∼0:5) should be achievable in DIII-D with fast waves at 0.5 GHz, with an efficiency twice as high as with noninductive current drive tools currently available on DIII-D (neutral beams and electron cyclotron current drive) in high-β conditions. An innovative Travelling Wave Antenna (TWA) of the "comb-line" type with 12 radiating modules has been constructed, installed in DIII-D, and is currently being tested at very low power (< 1 kW) to evaluate the antenna coupling in the linear regime, and to prototype technological aspects of such structures in the tokamak environment. Preliminary results indicate strong antenna-plasma coupling, with detailed 3D modelling underway to quantitatively compare the measurements with theoretical expectations. A key input to this model is the edge and far SOL electron density profile, which is being measured with a microwave reflectometer and with fixed and movable Langmuir probes. An important issue for wave coupling in this regime is the degree to which (undesired) quasi-electrostatic slow waves are excited by the structure; evaluation of this is a point of emphasis in the ongoing work. A high-power system is presently being prepared for installation later in 2016 in which a single 1.2 MW klystron at 476 MHz will be used to power a TWA with ∼36 radiating elements in a structure 2 m wide. The goals of the high-power experiments include evaluation of nonlinear effects on excitation of the desired waves (ponderomotive effects, parametric decay) and measurements of the deposition profile and of the current drive efficiency. Ray-tracing predicts an RF-driven current of ∼60 kA per coupled MW of helicon power, which should result in an easily measurable driven current in DIII-D in high-β discharges. (author)

Part of:
26. IAEA Fusion Energy Conference. Programme, Abstracts and Conference Material

Additional details

Publishing Information

Imprint Title
26. IAEA Fusion Energy Conference. Programme, Abstracts and Conference Material
Imprint Pagination
935 p.
Journal Page Range
p. 225
Report number
IAEA-CN--234

Conference

Title
26. IAEA Fusion Energy Conference
Acronym
FEC 2016
Dates
17-22 Oct 2016
Place
Kyoto (Japan)