Nov 2018 | Research Library, Posters, Diagnostics, Experiment, Fusion Energy, Fusion Research, Fusion Science, Fusion Technology, Plasma Research
October 2018 | M. Nations | APS-DPP | Poster
One of the key advantages of using two different spectral regions (VIS and NIR) to measure bremsstrahlung continuum is that they have different pollutant sensitivities
Nov 2018 | Research Library, Posters, Diagnostics, Experiment, Fusion Energy, Fusion Research, Fusion Science, Fusion Technology, Plasma Research
October 2018 | M. E. Griswold | APS-DPP | Poster
In an hypothetical isolated mirror (with no net current flow), an ambipolar electric potential modifies the loss cone so electrons are lost at the same rate as ions.
Nov 2018 | Research Library, Posters, Diagnostics, Experiment, Fusion Energy, Fusion Research, Fusion Science, Fusion Technology, Plasma Research
October 2018 | M. Beall | APS-DPP | Poster
The purpose of the C-2W experiment is to demonstrate control, stability and heating of a Field-Reversed Configuration (FRC) plasma via magnetic controls …
Nov 2018 | Research Library, Posters, Equilibrium, Fusion Energy, Fusion Research, Fusion Science, Fusion Technology, Modeling, Plasma Profiles, Plasma Research, Theory
October 2018 | L. Steinhauer | APS-DPP | Poster
The magnetic structure of FRCs cannot be measured directly by existing diagnostics. A new tool “Grushenka” finds the structure based on magnetic measurements at the vessel wall.
Nov 2018 | Research Library, Posters, Fusion Energy, Fusion Research, Fusion Science, Fusion Technology, Plasma Research
October 2018 | L. Schmitz | APS-DPP | Poster
An advanced multi-channel combined Doppler Back-scattering (DBS)/Cross-Polarization (CPS)[1] diagnostic for the C-2W Field-Reversed Configuration (FRC) will be discussed
Nov 2018 | Research Library, Posters, Diagnostics, Experiment, Fusion Energy, Fusion Research, Fusion Science, Fusion Technology, Plasma Research
October 2018 | K. Zhai | APS-DPP | Poster
5-channel bandpass filter polychromators (in collaboration with GA) Four spectral channels are optimized for electron temperature measurement from 10eV to 2keV.