June 2013 | V. Bystritskii | ICOPS | Presentation
Based on several decades of experimental and theoretical research of Plasma Configuration with a Reversed magnetic Field (FRC) , it is presently considered as an alternative venue for steady state and/or pulsed CTF.
May 2013 | H. Gota | Transactions of Fusion Science and Technology | Paper
Field reversed configurations (FRCs) with high confinement are obtained in the C-2 device by combining plasma gun edge biasing and neutral beam injection.
April 2013 | D. Barnes | Sherwood Fusion Theory | Presentation
Mode is driven by rotation. Rotation provides fictitious outward gravity. Rayleigh-Taylor-like heavy-on-light instability.
April 2013 | F. Cecherini | Sherwood Fusion Theory | Presentation
The Field Reversed Configuration (FRC) exhibits very peculiar structures for both the plasma density and the magnetic field.
April 2013 | M. Onofri | Sherwood Fusion Theory | Presentation
A 2D transport code (Q2D) is used to study the evolution of C2 Field Reversed Configuration with neutral beam injection.
February 2013 | H. Gota | Nihon Symposium | Presentation
Demonstration of a High Performance FRC (HPF) operating regime by combining effects of edge-biasing from an end-plasma-gun and of neutral-beam injection.
February 2013 | M. Tuszewski | Nihon Symposium | Presentation
FRCs permit to use advanced fusion fuels.
February 2013 | L. Steinhauer | Nihon Symposium | Presentation
Five critical near-term issues.
February 2013 | H. Guo | EPR Workshop | Presentation
FRC offers an ideal configuration for an economic reactor and may allow use of aneutronic fuels.
January 2013 | S. Dettrick | 2013 Energetic Particles Workshop UCI | Presentation
Without magnetic perturbations, NB Ion energy confinement time is τE~ 500us. Most NB ion energy goes to heating electrons.