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@ARTICLE{Guillemaut:845501,
author = {Guillemaut, C. and Drewelow, P. and Matthews, G. F. and
Kukushkin, A. S. and Pitts, R. A. and Abreu, P. and
Brezinsek, S. and Brix, M. and Carman, P. and Coelho, R. and
Devaux, S. and Flanagan, J. and Giroud, C. and Harting, D.
and Lowry, C. G. and Maggi, C. F. and Militello, F. and
Perez Von Thun, C. and Solano, E. R. and Widdowson, A. and
Wiesen, S. and Wischmeier, M. and Wood, D.},
title = {{M}ain chamber wall plasma loads in {JET}-{ITER}-like wall
at high radiated fraction},
journal = {Nuclear materials and energy},
volume = {12},
issn = {2352-1791},
address = {Amsterdam [u.a.]},
publisher = {Elsevier},
reportid = {FZJ-2018-02735},
pages = {234 - 240},
year = {2017},
abstract = {Future tokamak reactors of conventional design will require
high levels of exhaust power dissipation (more than $90\%$
of the input power) if power densities at the divertor
targets are to remain compatible with active cooling.
Impurity seeded H-mode discharges in JET-ITER-like Wall
(ILW) have reached a maximum radiative fraction (Frad) of
$∼75\%.$ Divertor Langmuir probe (LP) measurements in
these discharges indicate, however, that less than $∼3\%$
of the thermal plasma power reaches the targets, suggesting
a missing channel for power loss. This paper presents
experimental evidence from limiter LP for enhanced
cross-field particle fluxes on the main chamber walls at
high Frad. In H-mode nitrogen-seeded discharges with Frad
increasing from $∼30\%$ to up to $∼75\%,$ the main
chamber wall particle fluence rises by a factor ∼3 while
the divertor plasma fluence drops by one order of magnitude.
Contribution of main chamber wall particle losses to
detachment, as suggested by EDGE2D-EIRENE modeling, is not
sufficient to explain the magnitude of the observed divertor
fluence reduction. An intermediate detached case obtained at
Frad ∼ $60\%$ with neon seeding is also presented. Heat
loads were measured using the main chamber wall
thermocouples. Comparison between thermocouple and bolometry
measurements shows that the fraction of the input power
transported to the main chamber wall remains below $∼5\%,$
whatever the divertor detachment state is. Main chamber
sputtering of beryllium by deuterium is reduced in detached
conditions only on the low field side. If the fraction of
power exhaust dissipated to the main chamber wall by
cross-field transport in future reactors is similar to the
JET-ILW levels, wall plasma power loading should not be an
issue. However, other contributions such as charge exchange
may be a problem.},
cin = {IEK-4},
ddc = {333.7},
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:000417293300033},
doi = {10.1016/j.nme.2017.02.010},
url = {https://juser.fz-juelich.de/record/845501},
}