November 2013 | M. Thompson | APS-DPP | Poster
The C-2 experiment seeks to study the evolution, heating and sustainment effects of neutral beam injection on field-reversed configuration (FRC) plasmas.
November 2013 | T. Roche | APS-DPP | Poster
The divertor magnetic field configuration is varied to investigate its influence on the C-2 FRC and its jet.
November 2013 | N. Rath | APS-DPP | Poster
FRC Equilibria are calculated with the LR_eq Grad-Shafranov solver.
September 2013 | H. Gota | US-Japan CT Workshop | Presentation
Demonstration of a High Performance FRC (HPF) regime by combining effects of edge-biasing from end-on plasma guns and of neutral-beam injection.
September 2013 | M. Tuszewski | US-Japan CT Workshop | Presentation
Ideal FRC pressure balance.
August 2013 | H. Guo | GA Seminar | Presentation
Simple geometry for ease of construction & maintenance. C-2 achieved new High Confinement Field-Reversed Configuration (FRC) regime with dramatically improved stability & confinement.
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.