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@ARTICLE{Wenninger:827699,
author = {Wenninger, R. and Albanese, R. and Ambrosino, R. and
Arbeiter, F. and Aubert, J. and Barbato, L. and Barrett, T.
and Beckers, M. and Biel, W. and Boccaccini, L. and
Carralero, D. and Coster, D. and Eich, T. and Fasoli, A. and
Federici, G. and Firdaouss, M. and Graves, J. and Horacek,
J. and Kovari, M. and Lanthaler, S. and Loschiavo, V. and
Lowry, C. and Lux, H. and Maddaluno, G. and Maviglia, F. and
Mitteau, R. and Neu, R. and Pfefferle, D. and Schmid, K. and
Siccinio, M. and Sieglin, B. and Silva, C. and Snicker, A.
and Subba, F. and Varje, J. and Zohm, H. and Bachmann, C.},
title = {{T}he {DEMO} wall load challenge},
journal = {Nuclear fusion},
volume = {57},
number = {4},
issn = {1741-4326},
address = {Vienna},
publisher = {IAEA},
reportid = {FZJ-2017-01812},
pages = {046002 -},
year = {2017},
abstract = {For several reasons the challenge to keep the loads to the
first wall within engineering limits is substantially higher
in DEMO compared to ITER. Therefore the pre-conceptual
design development for DEMO that is currently ongoing in
Europe needs to be based on load estimates that are derived
employing the most recent plasma edge physics knowledge.An
initial assessment of the static wall heat load limit in
DEMO infers that the steady state peak heat flux limit on
the majority of the DEMO first wall should not be assumed to
be higher than 1.0 MW m−2. This compares to an average
wall heat load of 0.29 MW m−2 for the design ${\tt
{EU}}{\tt {~}}{\tt {DEMO1}}{\tt {~2015}}$ assuming a perfect
homogeneous distribution. The main part of this publication
concentrates on the development of first DEMO estimates for
charged particle, radiation, fast particle (all static) and
disruption heat loads. Employing an initial engineering wall
design with clear optimization potential in combination with
parameters for the flat-top phase (x-point configuration),
loads up to 7 MW m−2 (penalty factor for tolerances etc
not applied) have been calculated. Assuming a fraction of
power radiated from the x-point region between 1/5 and 1/3,
peaks of the total power flux density due to radiation of
0.6–0.8 MW m−2 are found in the outer baffle region.This
first review of wall loads, and the associated limits in
DEMO clearly underlines a significant challenge that
necessitates substantial engineering efforts as well as a
considerable consolidation of the associated physics basis.},
cin = {IEK-4},
ddc = {530},
cid = {I:(DE-Juel1)IEK-4-20101013},
pnm = {174 - Plasma-Wall-Interaction (POF3-174) / HITEC -
Helmholtz Interdisciplinary Doctoral Training in Energy and
Climate Research (HITEC) (HITEC-20170406)},
pid = {G:(DE-HGF)POF3-174 / G:(DE-Juel1)HITEC-20170406},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000405943600001},
doi = {10.1088/1741-4326/aa4fb4},
url = {https://juser.fz-juelich.de/record/827699},
}