May 2012 | M. Thompson | HTPD | Poster
Magnetic measurements are a fundamental part of determining the size and shape of field reversed configuration (FRC) plasmas in the C-2 device.
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December 2011 | A. Ivanov | ICIS | Presentation
Based on several decades of experimental and theoretical research of Plasma Configuration with a Reversed magnetic Field (FRC) , it is presently considered as an alternative venue for steady state and/or pulsed CTF.
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November 2011 | R. Clary | APS-DPP | Poster
The TAE Technologies C-2 device [1,2] aims to explore confinement properties of colliding Field-Reversed Configuration (FRC) plasmas, augmented with neutral beam injection.
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November 2011 | B. Deng | APS-DPP | Poster
Plasma equilibrium profiles and fluctuations in the C-2 field reversed configuration (FRC) experiment [M. W. Binderbauer et al, Phys.Rev.Lett. 105, 045003 (2010)] are measured under various operation conditions.
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November 2011 | D. Gupta | APS-DPP | Poster
Although high rotation velocity in a FRC may lead to rotational instabilities, it is also believed that shear flow helps in improving FRC stability and transport.
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November 2011 | S. Korepanov | APS-DPP | Poster
One of the goals of the C-2 experiment [1,2] is to explore FRC sustainment and current drive from neutral beam injection. Studies of the relaxation and confinement of hot anisotropic ions created by the neutral beams are considered to be key elements of the experimental research program.
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November 2011 | T. Roche | APS-DPP | Poster
An optical tomography system has been developed and implemented in the Flux Coil Generated Field Reversed Configuration (FCG-FRC) at TAE Technologies.
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November 2011 | E. Ruskov | APS-DPP | Poster
High required time resolution resolves in high required modulation frequency and high IF: need very fast data acquisition.
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November 2011 | X. Sun | APS-DPP | Poster
Edge biasing has long been used in various fusion devices to actively control the plasma potential profile in order to suppress radial transport by decorrelating density and potential fluctuations through flow shear.
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November 2011 | M. Thompson | APS-DPP | Poster
In any magnetic plasma confinement device, it is advantageous to limit hot-ion loss through charge-exchange with cold neutral gas by minimizing the gas density near the plasma.
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