Details

Autor(en) / Beteiligte

• Rapp, Juergen
• Biewer, T. M.
• Bigelow, T. S.
• Caughman, J. B. O.
• Duckworth, R. C.
• Ellis, R. J.
• Giuliano, D. R.
• Goulding, R. H.
• Hillis, D. L.
• Howard, R. H.
• Lessard, T. L.
• Lore, J. D.
• Lumsdaine, A.
• Martin, E. J.
• McGinnis, W. D.
• Meitner, S. J.
• Owen, L. W.
• Ray, H. B.
• Shaw, G. C.
• Varma, V. K.

Titel

The Development of the Material Plasma Exposure Experiment

Ist Teil von

• IEEE transactions on plasma science, 2016-12, Vol.44 (12), p.3456-3464

Ort / Verlag

New York: IEEE

Erscheinungsjahr

2016

Quelle

IEEE Electronic Library (IEL)

Beschreibungen/Notizen

• The availability of future fusion devices, such as a fusion nuclear science facility or demonstration fusion power station, greatly depends on long operating lifetimes of plasma facing components in their divertors. ORNL is designing the Material Plasma Exposure eXperiment (MPEX), a superconducting magnet, steady-state device to address the plasma material interactions of fusion reactors. MPEX will utilize a new highintensity plasma source concept based on RF technology. This source concept will allow the experiment to cover the entire expected plasma conditions in the divertor of a future fusion reactor. It will be able to study erosion and redeposition for relevant geometries with relevant electric and magnetic fields in-front of the target. MPEX is being designed to allow for the exposure of a priori neutron-irradiated samples. The target exchange chamber has been designed to undock from the linear plasma generator such that it can be transferred to diagnostics stations for more detailed surface analysis. MPEX is being developed in a staged approach with successively increased capabilities. After the initial development step of the helicon source and electron cyclotron heating system, the source concept is being tested in the Proto-MPEX device. Proto-MPEX has achieved electron densities of more than 4×10 19 m -3 with a large diameter (13 cm) helicon antenna at 100 kW power. First heating with microwaves resulted in a higher ionization represented by higher electron densities on axis, when compared with the helicon plasma only without microwave heating.