![Anatomy of a Field-Reversed Configuration](https://tae.com/wp-content/uploads/Anatomy-of-a-Field-Reversed-Configuration.jpg)
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
October 2019 | L. Steinhauer | APS-DPP | Poster
Tangibles” = inputs to Grushenka: what can be measured. Intangibles” = outputs from Grushenka: what can’t be directlymeasured
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
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…
October 2019 | P.C. Norgaard | APS-DPP | Poster
A holistic, high-fidelity plasma reconstruction based on Bayesian inference is applied to study the advanced beam-driven Field Reversed Configuration (FRC)
October 2019 | Richard Ignace | APS-DPP | Poster
Direct and local measurements of internal magnetic field are highly desirable in TAE’s fusion plasma experiments to characterize the magnetic field profile
October 2019 | B. S. Nicks | APS-DPP | Poster
C-2U experiment: beam-driven FRC. Proton beams injected into deuterium plasma. Fast proton injection greatly enhanced DD fusion rate