November 2013 | A. Necas | APS-DPP | Poster
Gyroviscous (GV) stress for weakly magnetized plasma has been implemented in the NIMROD code to study Hall and FLR effects on FRC stability with emphasis on the rotational modes.
November 2013 | S. Gupta | APS-DPP | Poster
The Neutral beam current drive mechanism, originally known as Ohkawa Current, is investigated for FRC plasmas using small amounts of high Z impurities.
November 2013 | D. Gupta | APS-DPP | Poster
To better understand and quantify the radial momentum balance in the C2 FRC plasma, experiments are performed with the mixture of Helium and Deuterium.
November 2013 | E. Garate | APS-DPP | Poster
Field reversed configurations (FRC) have closed field line regions in which the ratio of plasma to electron cyclotron frequency is greater than 1.
November 2013 | B. Deng | APS-DPP | Poster
Ideal FRC configuration has zero toroidal field.
November 2013 | F. Cecherini | APS-DPP | Poster
The generation and propagation of an ion cyclotron resonant wave is studied in a Field Reversed Configuration (FRC) plasma which includes at least two different ion species.
November 2013 | S. Aefsky | APS-DPP | Poster
The electron temperature of the plasma inside the C-2 Experiment is measured using a Thomson Scattering (TS) diagnostic.
November 2013 | R. Magee | APS-DPP | Poster
The C-2 field-reversed configuration (FRC) plasmas are created via the dynamic merging of two compact toroids and partially sustained through the injection of high power neutral beams.
November 2013 | K. Zhai | APS-DPP | Poster
C2 Thomson scattering system is upgraded with capability of electron density profile measurement.
November 2013 | H. Guo | APS-DPP | Poster
C-2 achieved new High Confinement FRC regime with dramatically improved stability & confinement.