January 2011 | M. Tuszewski | Transactions of Fusion Science and Technology | Paper
The Field Reversed Configuration (FRC) is a high-beta Compact Toroid that includes closed and open field line regions of poloidal magnetic field.
November 2010 | B. Deng | APS-DPP | Poster
Plasma electron density profiles in the C-2 field reversed configuration (FRC) experiment are investigated. Measured profiles of translated FRC plasmas agree with MHD simulation results from the MHD code LamyRidge.
November 2010 | J. Douglas | APS-DPP | Poster
November 2010 | L. Galeotti | APS-DPP | Poster
We describe a new formulation of the multi-ion species.
November 2010 | E. Garate | APS-DPP | Presentation
The TAE Technologies C-2 experimental system is a linear device consisting of two separate multi-coil theta-pinch formation sections and a central confinement vessel.
November 2010 | F. Glass | APS-DPP | Poster
Exploring electron temperature.
November 2010 | H. Gota | APS-DPP | Poster
Three-axis internal magnetic probes are being developed to measure simultaneously Bz, Bt and Br of a field-reversed configuration (FRC) plasma from the geometric axis (r=0) to outside of the separatrix in C-2.
November 2010 | A. Necas | APS-DPP | Poster
In this work we will present three computational tools to study the neutral particle transport in an FRC. Neutral particleʼs presence lead to CX losses, edge cooling.
November 2010 | Y. Mok | APS-DPP | Poster
A two-fluid code to measure FRC.
November 2010 | E. Ruskov | APS-DPP | Poster
The plasma is not in thermal equilibrium.