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 UP11: Poster Session VIII: MST; DIII-D Tokamak; SPARC, C-Mod, and High Field Tokamaks; HBT-EP; Transport and LPI in ICF Plasmas, Hydrodynamic Instability; HEDP Posters; Space and Astrophysical Plasmas (2:00pm-5:00pm)
Thursday, November 8, 2018
OCC
Room: Exhibit Hall A1&A
Abstract ID: BAPS.2018.DPP.UP11.78
Abstract: UP11.00078 : Design and Implementation of a Gas Puff Imaging System on TCV*
Presenter:
Woonghee Han
(Massachusetts Inst of Tech-MIT)
Authors:
Woonghee Han
(Massachusetts Inst of Tech-MIT)
Nicola Offeddu
(EPFL - Lausanne)
Theodore Golfinopoulos
(Massachusetts Inst of Tech-MIT)
Christian Theiler
(EPFL - Lausanne)
James Layton Terry
(Massachusetts Inst of Tech-MIT)
Seung Gyou Baek
(Massachusetts Inst of Tech-MIT)
Basil Duval
(EPFL - Lausanne)
Brian LaBombard
(Massachusetts Inst of Tech-MIT)
Earl S Marmar
(Massachusetts Inst of Tech-MIT)
Gas Puff Imaging (GPI) diagnostics routinely measure the spatially-resolved edge fluctuations in tokamak plasmas. We plan to install a GPI system on TCV that will address multiple physics topics, such as turbulence characteristics during confinement transitions, and neutral density shadowing effect in GPI. The system’s 120 views comprise a 10x12 array (43x52 mm view), with light detection accomplished by APD arrays with a 1 MHz bandwidth. Parametric scans of the gas puff design parameters - including flow rate of the He or D2 gas puff (FR), spacing between the nozzle and the LCFS (Δ), nozzle design, and gas species - were performed using the DEGAS 2 neutral transport code to model and maximize the expected time-averaged emission within a practical design space. DEGAS 2 results predict that the system will give a brightness above a minimum usable level (2.0 mW/cm2/ster) with He puff and FR=6×1019 atoms/s, up to 2 mm inside the LCFS. The brightness and penetration are increased with higher FR or shorter Δ or collimated puffs, and the penetration will be deeper for D2 puffs. Installation of the system on TCV is planned for summer/fall 2018.
*This work is supported by USDoE awards DE-FC02-99ER54512 and DE-SC0014264.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DPP.UP11.78
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