June 2016 | Niko Rath | AIP Publishing | Paper
We show that in a field-reversed-configuration, the plasma is unstable to either transverse or axial rigid displacement, but never to both.
May 2016 | S. Gupta | Physics of Plasmas | Paper
A significant improvement of field reversed configuration (FRC) lifetime and plasma confinement times in the C-2 plasma, called High Performance FRC regime, has been observed with neutral beam injection (NBI), improved edge stability, and better wall conditioning.
May 2016 | Daniel Fulton | Physics of Plasmas | Paper
Following the recent remarkable progress in magnetohydrodynamic (MHD) stability control in the C-2U advanced beam driven field-reversed configuration (FRC), turbulent transport has become one of the foremost obstacles on the path towards an FRC-based fusion reactor.
April 2016 | Sean Dettrick | Sherwood | Presentation
The TAE research program has been successful due to the agility and close interaction between experiment, theory, and engineering groups.
April 2016 | Marco Onofri | Sherwood | Poster
The Q2D code is a 2D MHD code, which includes a neutral fluid and separate ion and electron temperatures, coupled with a 3D Monte Carlo code, which is used to calculate source terms due to neutral beams.
January 2016 | D. Fulton | Physics of Plasmas | Paper
Gyrokinetic particle simulation of the field-reversed configuration (FRC) has been developed using the gyrokinetic toroidal code (GTC). The magnetohydrodynamic equilibrium is mapped from cylindrical coordinates to Boozer coordinates for the FRC core and scrape-off layer (SOL), respectively.