Variation in particle pumping due to changes in topology in high performance DIII-D plasmas

Recent experiments on DIII-D point to the importance of two factors in determining the rate at which deuterium particles can be pumped at the divertor target(s): (1) the divertor magnetic balance, i.e., the degree to which the divertor topology is single-null (SN) or double-null (DN), and (2) the di...

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Veröffentlicht in:Journal of nuclear materials 2005-03, Vol.337-339, p.216-220
Hauptverfasser: Petrie, T.W., Brooks, N.H., Fenstermacher, M.E., Greenfield, C.M., Groth, M., Hyatt, A.W., Leonard, A.W., Mahdavi, M.A., Porter, G.D., Rensink, M.E., Schaffer, M.J., Wade, M.R., Watkins, J.G., Wolf, N.S., The DIII–D Team
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container_end_page 220
container_issue
container_start_page 216
container_title Journal of nuclear materials
container_volume 337-339
creator Petrie, T.W.
Brooks, N.H.
Fenstermacher, M.E.
Greenfield, C.M.
Groth, M.
Hyatt, A.W.
Leonard, A.W.
Mahdavi, M.A.
Porter, G.D.
Rensink, M.E.
Schaffer, M.J.
Wade, M.R.
Watkins, J.G.
Wolf, N.S.
The DIII–D Team
description Recent experiments on DIII-D point to the importance of two factors in determining the rate at which deuterium particles can be pumped at the divertor target(s): (1) the divertor magnetic balance, i.e., the degree to which the divertor topology is single-null (SN) or double-null (DN), and (2) the direction of the of B×∇B ion drift with respect to the X-point(s). Changes in divertor magnetic balance near the DN shape have a much stronger effect on the pumping rate at the inner divertor target(s) than on the pumping rate at the outer divertor target(s). The behavior in the particle pumping observed at the inner and outer divertor target(s) in the DN and near-DN shapes suggests a redistribution of particles that would be expected in the presence of B×∇B and E×B ion particle drifts in the scrapeoff layer (SOL) and divertor(s).
doi_str_mv 10.1016/j.jnucmat.2004.10.063
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subjects Divertor asymmetry
Divertor pumping
Magnetic topology
Particle drifts
Recycling
title Variation in particle pumping due to changes in topology in high performance DIII-D plasmas
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