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.
November 2013 | E. Trask | APS-DPP | Poster
Ray propagation in the electron cyclotron range of frequencies (ECRF) has been studied for simulated two dimensional equilibria on the C-2 device.