Anatomy of a Field-Reversed Configuration
October 2019 | L. Steinhauer | APS-DPP | Poster
Tangibles” = inputs to Grushenka: what can be measured. Intangibles” = outputs from Grushenka: what can’t be directlymeasured
Overview of the C-2W Experimental Diagnostic Systems
October 2019 | T. Roche | APS-DPP | Poster
In TAE Technologies current experimental device, C-2W (also called Norman),1 record breaking, advanced beam-driven field-reversed configuration (FRC) plasmas are produced and sustained
Interpretation of the charge exchange neutral energy spectrum of C-2W
October 2019 | G. Player | APS-DPP | Poster
In TAE Technologies’ current experimental device, C-2W (also called “Norman”) [1], record breaking, advanced beam-driven field reversed configuration (FRC) plasmas are produced and sustained in steady state
Effect of electrode biasing on C-2W electron temperature
October 2019 | Manjit Kaur | APS-DPP | Poster
In TAE Technologies’ current experimental device, C-2W (also called “Norman”) [1], record-breaking,
advanced beam-driven field reversed configuration (FRC) plasmas are produced
Simulation of Fast Ion Effects on Global Stability of C-2W Equilibria: Early Results
October 2019 | Francesco Ceccherini | APS-DPP | Poster
In TAE Technologies’ current experimental device, C-2W, record breaking, advanced beam-driven FRC plasmas are produced and sustained in steady state…
0D Power Flow Analysis on the C-2W Device
October 2019 | R. Clary | APS-DPP | Poster
The C-2W device (aka “Norman”)[1] produces advanced beam-driven field re- versed configuration (FRC) plasmas. Variable energy neutral beam injection…