
TAE Technologies Neutron Diagnsotics
November 2010 | E. Ruskov | APS-DPP | Poster
The plasma is not in thermal equilibrium.
November 2010 | E. Ruskov | APS-DPP | Poster
The plasma is not in thermal equilibrium.
November 2010 | X. Sun | APS-DPP | Poster
November 2010 | M. Thompson | APS-DPP | Poster
Diamagnetic measurements of field-reversed configuration (FRC) plasmas produced in the C-2 experiment are obtained with a linear array of 19 magnetic probes positioned along the length of the stainless steel confinement vessel.
November 2010 | M. Wyman | APS-DPP | Poster
In C-2, two high-beta plasmas are merged to produce a field-reversed configuration (FRC) plasma.
November 2010 | H. Guo | APS-DPP | Presentation
October 2010 | D. Gupta | Review of Scientific Instruments | Paper
Two Doppler spectroscopy diagnostics with complementary capabilities are developed to measure the ion temperatures and velocities of FRC plasmas in the C-2 device.
October 2010 | D. Gupta | Review of Scientific Instruments | Paper
One aim of the flux-coil generated field reversed configuration at TAE Technologies TAE is to establish the plasma where the ion rotational energy is greater than the ion thermal energy.
October 2010 | O. Gornostaeva | Review of Scientific Instruments | Paper
A six-channel two-color interferometer has been developed for plasma electron density measurements in the C-2 field reversed configuration experiment.
October 2010 | H. Gota |Review of Scientific Instruments | Paper
A two-chord IR3.39 m He–Ne laser interferometer system was developed for a flux-coil-generated field-reversed configuration to estimate the electron density and the total temperature of the field-reversed configuration FRC plasma.
October 2010 | F. Glass | Review of Scientific Instruments | Paper
A Thomson scattering diagnostic has been developed for the C-2 field-reversed configuration device. Based on a multipulse ruby laser, the system measures the electron temperature at nine spatial points.