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@ARTICLE{Chmielewski:904041,
author = {Chmielewski, P. and Zagórski, R. and Telesca, G. and Brix,
M. and Huber, Alexander and Ivanova-Stanik, I. and
Kowalska-Strzeciwilk, E. and Pereira, T. and Réfy, D. I.
and Tamain, P. and Vécsei, M. and Vianello, N.},
title = {{TECXY} simulations of {N}e seeding in {JET} high power
scenarios},
journal = {Nuclear materials and energy},
volume = {27},
issn = {2352-1791},
address = {Amsterdam [u.a.]},
publisher = {Elsevier},
reportid = {FZJ-2021-05611},
pages = {100962 -},
year = {2021},
abstract = {Preparation of D-T experiments on JET device raises a
question about the mitigation of assumed high power entering
the SOL. JET DT scenarios aim to achieve good plasma
confinement and the heat loads reduction to the divertor at
the same time. Therefore, the divertor corner magnetic field
geometry, strike point swiping and impurity seeding are
considered to reduce expected high heat fluxes to the
divertor plates. The aim of the paper is to analyse the
influence of the neon impurity seeding on the plasma
transport and its efficiency of the power mitigation in the
JET tokamak as well as to perform validation of applied edge
plasma model. In this contribution numerical simulations
have been performed for two high power (34 MW), neon seeded
DD JET discharges in the H-mode with different upstream
densities and the same corner divertor configuration
prepared as possible candidate for JET DT scenarios. The
edge plasma transport have been described by two-dimensional
multifluid TECXY code based on Braginskii plasma transport
equations with assumed classical parallel transport of the
plasma and anomalous perpendicular transport defined by ad
hoc heat and particle transport coefficients. TECXY results
show impact of the neon seeding on the reduction of the
power flowing to the divertor. Scan with the neon
concentration carried out for four different upstream
densities allow us to determine optimal plasma conditions
with the lowest target plate temperature and the lowest
effective charge. Performed studies with use of the TECXY
code and they comparison to experimental results give the
opportunity to perform validation of applied TECXY edge
plasma model and show the optimal range of plasma parameters
like the upstream density and neon concentration, for which
the radiation power in the SOL is the highest.},
cin = {IEK-4},
ddc = {624},
cid = {I:(DE-Juel1)IEK-4-20101013},
pnm = {134 - Plasma-Wand-Wechselwirkung (POF4-134)},
pid = {G:(DE-HGF)POF4-134},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000663579600004},
doi = {10.1016/j.nme.2021.100962},
url = {https://juser.fz-juelich.de/record/904041},
}