Feb 2018 | Research Library, Papers, Experiment, Featured Publications, Fusion Energy, Fusion Research, Fusion Science, Fusion Technology, Instabilities, Plasma Profiles, Plasma Research, Stability
February 2018 | J.A. Romero | Nature Communications | Paper
Active control of field reversed configuration (FRC) devices requires a method to determine the flux surface geometry and dynamic properties of the plasma during both transient and steady-state conditions.
Jul 2017 | Research Library, Papers, Experiment, Featured Publications, Fusion Energy, Fusion Research, Fusion Science, Fusion Technology, Instabilities, Plasma Research
July 2017 | E. A. Baltz | Scientific Reports | Paper
TAE and Google have partnered to combine human and machine interaction to further plasma science using their “Optometrist Algorithm.”
May 2017 | Research Library, Papers, Experiment, Fueling, Fusion Energy, Fusion Research, Fusion Science, Fusion Technology, Instabilities, Performance, Top Level
May 2017 | T. Asai | Nuclear Fusion | Paper
A repetitively driven compact toroid (CT) injector has been developed for the large eld- reversed con guration (FRC) facility of the C-2/C-2U, primarily for particle refueling. A CT is formed and injected by a magnetized coaxial plasma gun (MCPG) exclusively developed for the C-2/C-2U FRC.
May 2017 | Research Library, Posters, Diagnostics, Experiment, Fusion Energy, Fusion Research, Fusion Science, Fusion Technology, Plasma Research
May 2017 | A. Necas | The Sherwood Fusion Theory Conference | Poster
C-2U is a unique hybrid field-reversed configuration (FRC) where we successfully combine a high-beta (~1) FRC plasma with neutral beam injection (NBI), field line biasing, and mirror physics.
Oct 2016 | Research Library, Posters, Fusion Energy, Fusion Research, Fusion Science, Fusion Technology, Instabilities, Plasma Research, Simulation
October 2016 | Francesco Checcerini | APS-DPP | Poster
The goal of TAE’s experiments is to sustain through the of use of neutral beam heating and edge biasing an advanced beam-driven FRC for many milliseconds, i.e., well beyond the growth times of common instabilities.