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@ARTICLE{Loewenhoff:276434,
author = {Loewenhoff, Thorsten and Bardin, S. and Greuner, H. and
Linke, Jochen and Maier, H. and Morgan, T. W. and Pintsuk,
Gerald and Pitts, R. A. and Riccardi, B. and DeTemmermann,
G.},
title = {{I}mpact of {C}ombined {T}ransient {P}lasma/{H}eat {L}oads
on {T}ungsten {P}erformance {B}elow and {A}bove
{R}ecrystallization {T}emperature},
journal = {Nuclear fusion},
volume = {55},
number = {12},
issn = {0029-5515},
address = {Vienna},
publisher = {IAEA},
reportid = {FZJ-2015-06873},
pages = {123004},
year = {2015},
abstract = {The influence of recrystallization on thermal shock
resistance has been identified as an issue that may
influence the long term performance of ITER tungsten (W)
divertor components. To investigate this issue a unique
series of experiments has been performed on ITER divertor W
monoblock mock-ups in three EU high heat flux facilities:
GLADIS (neutral beam), JUDITH 2 (electron beam) and
Magnum-PSI (plasma beam). To simulate ITER mitigated edge
localised modes, heat fluxes between 0.11 and 0.6 GW m−2
were applied for Δt < 1 ms. Two different base
temperatures, Tbase = 1200 °C and 1500 °C, were
chosen on which ~18 000/100 000 transient events were
superimposed representing several full ITER burning plasma
discharges in terms of number of transients and particle
fluence. An increase in roughening for both e-beam and
plasma loaded surfaces was observed when loading during or
after recrystallization and when loading at higher
temperature. However, regarding the formation of cracks and
microstructural modifications the response was different for
e-beam and plasma loaded surfaces. The samples loaded in
Magnum-PSI did not crack nor show any sign of
recrystallization, even at Tbase = 1500 °C. This
could be a dynamic hydrogen flux effect, because pre-loading
of samples with hydrogen neutrals (GLADIS) or without
hydrogen (e-beam JUDITH 2) did not yield this result. These
results show clearly that the loading method used when
investigating and qualifying the thermal shock performance
of materials for ITER and future fusion reactors can play an
important role. This should be properly accounted for and in
fact should be the subject of further $R\&D.$},
cin = {IEK-2 / IEK-4},
ddc = {530},
cid = {I:(DE-Juel1)IEK-2-20101013 / 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:000366534500006},
doi = {10.1088/0029-5515/55/12/123004},
url = {https://juser.fz-juelich.de/record/276434},
}