% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@ARTICLE{Corre:836226,
author = {Corre, Y. and Bunting, P. and Coenen, J. W. and Gaspar, J.
and Iglesias, D. and Matthews, G. F. and Balboa, I. and
Coffey, I. and Dejarnac, R. and Firdaouss, M. and Gauthier,
E. and Jachmich, S. and Krieger, K. and Pitts, R. A. and
Rack, M. and Silburn, S. A.},
title = {{T}hermal analysis of protruding surfaces in the {JET}
divertor},
journal = {Nuclear fusion},
volume = {57},
number = {6},
issn = {1741-4326},
address = {Vienna},
publisher = {IAEA},
reportid = {FZJ-2017-05347},
pages = {066009 -},
year = {2017},
abstract = {Tungsten (W) melting is a major concern for next step
fusion devices. Two ELM induced tungsten melting experiments
have been performed in JET by introducing two special target
plate lamellae designed to receive excessively high ELM
transient power loads. The first experiment was performed in
JET in 2013 using a special lamella with a sharp leading
edge gradually varying from h = 0.25 mm to
2.5 mm in order to maximise the temperature rise by
exposure to the full parallel heat flux. ELM-induced
transient melting has been successively achieved allowing
investigation of the melt motion. However, using the
available IR viewing geometry from the top, it was not
possible to directly discriminate between the top and
leading edge power loads. To improve the experimental
validation of heat load and melt motion modelling codes, a
new protruding W lamella with a 15° slope facing the
toroidal direction has been installed for the 2015–16
campaigns, allowing direct, spatially resolved observation
of the top surface and reduced sensitivity of the analysis
to the surface incidence angle of the magnetic field. This
paper reports on the results of these more recent
experiments, with specific focus on IR data analysis and
heat flux calculations during L-mode discharges in order to
investigate the behaviour of the W lamella with steady state
heat load, which is a prerequisite for the more complex
ELMing H-mode discharges (including both, steady and
transient heat loads). It shows that, at least in L-mode,
the assumption of optical heat flux projection is
justified.},
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:000399433800001},
doi = {10.1088/1741-4326/aa687e},
url = {https://juser.fz-juelich.de/record/836226},
}