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@ARTICLE{Coenen:844287,
author = {Coenen, J. W. and Matthews, G. F. and Krieger, K. and
Iglesias, D. and Bunting, P. and Corre, Y. and Silburn, S.
and Balboa, I. and Bazylev, B. and Conway, N. and Coffey, I.
and Dejarnac, R. and Gauthier, E. and Gaspar, J. and
Jachmich, S. and Jepu, I. and Makepeace, C. and Scannell, R.
and Stamp, M. and Petersson, P. and Pitts, R. A. and Wiesen,
S. and Widdowson, A. and Heinola, K. and Baron-Wiechec, A.},
title = {{T}ransient induced tungsten melting at the {J}oint
{E}uropean {T}orus ({JET})174},
journal = {Physica scripta},
volume = {T170},
issn = {1402-4896},
address = {Bristol},
publisher = {IoP Publ.},
reportid = {FZJ-2018-01727},
pages = {014013 -},
year = {2017},
abstract = {Melting is one of the major risks associated with tungsten
(W) plasma-facing components (PFCs) in tokamaks like JET or
ITER. These components are designed such that leading edges
and hence excessive plasma heat loads deposited at near
normal incidence are avoided. Due to the high stored
energies in ITER discharges, shallow surface melting can
occur under insufficiently mitigated plasma disruption and
so-called edge localised modes—power load transients. A
dedicated program was carried out at the JET to study the
physics and consequences of W transient melting. Following
initial exposures in 2013 (ILW-1) of a W-lamella with
leading edge, new experiments have been performed on a
sloped surface (15${}^{\circ }$ slope) during the 2015/2016
(ILW-3) campaign. This new experiment allows significantly
improved infrared thermography measurements and thus
resolved important issue of power loading in the context of
the previous leading edge exposures. The new lamella was
monitored by local diagnostics: spectroscopy, thermography
and high-resolution photography in between discharges. No
impact on the main plasma was observed despite a strong
increase of the local W source consistent with evaporation.
In contrast to the earlier exposure, no droplet emission was
observed from the sloped surface. Topological modifications
resulting from the melting are clearly visible between
discharges on the photographic images. Melt damage can be
clearly linked to the infrared measurements: the emissivity
drops in zones where melting occurs. In comparison with the
previous leading edge experiment, no runaway melt motion is
observed, consistent with the hypothesis that the escape of
thermionic electrons emitted from the melt zone is largely
suppressed in this geometry, where the magnetic field
intersects the surface at lower angles than in the case of
perpendicular impact on a leading edge. Utilising both
exposures allows us to further test the model of the forces
driving melt motion that successfully reproduced the
findings from the original leading edge exposure. Since the
ILW-1 experiments, the exposed misaligned lamella has now
been retrieved from the JET machine and post mortem analysis
has been performed. No obvious mass loss is observed.
Profilometry of the ILW-1 lamella shows the structure of the
melt damage which is in line with the modell predictions
thus allowing further model validation. Nuclear reaction
analysis shows a tenfold reduction in surface deuterium
concentration in the molten surface in comparison to the
non-molten part of the lamella.},
cin = {IEK-4},
ddc = {530},
cid = {I:(DE-Juel1)IEK-4-20101013},
pnm = {174 - Plasma-Wall-Interaction (POF3-174)},
pid = {G:(DE-HGF)POF3-174},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000414120500013},
doi = {10.1088/1402-4896/aa8789},
url = {https://juser.fz-juelich.de/record/844287},
}