% 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”.
@PHDTHESIS{Spilker:829762,
author = {Spilker, Benjamin},
title = {{T}he {I}mpact of {T}ransient {T}hermal {L}oads on
{B}eryllium as {P}lasma {F}acing {M}aterial},
volume = {371},
school = {RWTH Aachen},
type = {Dr.},
address = {Jülich},
publisher = {Forschungszentrum Jülich GmbH Zentralbibliothek, Verlag},
reportid = {FZJ-2017-03396},
isbn = {978-3-95806-227-6},
series = {Schriften des Forschungszentrums Jülich Reihe Energie $\&$
Umwelt / Energy $\&$ Environment},
pages = {XII, 134 S.},
year = {2017},
note = {RWTH Aachen, Diss., 2017},
abstract = {The rising global energy consumption requires a broad
research and development approach in the field of energy
technology. Besides renewables, nuclear fusion promises an
efficient, CO$_{2}$ free, no long-term radioactive waste
producing, and safe energy source using only deuterium and
lithium as primary resources, which are widely abundant.
However, several technical challenges have to be overcome
before a nuclear fusion power plant can be built. For this
purpose, the experimental reactor ITER is currently under
construction in France. ITER is intended to demonstrate the
scientific and technological feasibility of net energy
generation via nuclear fusion. The most heavily loaded
components inside a fusion reactor, which are directly
facing the fusion plasma, have to be armoured with well
suited materials, which need to be able to withstand the
high thermal and particle loads for an economically
reasonable lifetime. For ITER, beryllium is chosen as plasma
facing material for the largest fraction of the inner vacuum
vessel, the so called first wall. Tungsten will be applied
in the bottom region of the vacuum vessel, the so called
divertor, which acts as the exhaust system of the machine.
The choice of beryllium as plasma facing material was driven
by its outstanding advantages, e.g. the low atomic number
assures that eroded wall material does not strongly decrease
the fusion plasma performance, while it combines a high
thermal conductivity with low chemical sputtering
characteristics. However, the relatively low melting
temperature of beryllium of 1287 °C comprises the risk of
amour damage by melting during transient plasma events, such
as edge localized modes or plasma disruptions. Even when
mitigated, these events put tremendous power densities in
the GW m$^{-2}$ range with durations in the ms scale onto
the plasma facing materials. Hence, the performance of the
ITER reference beryllium grade S-65 under transient thermal
loads was studied within this work. Thereby, the focus was
set on the understanding of the different damage mechanisms
and melting behaviour of beryllium in order to contribute to
more reliable performance and lifetime estimations under
ITER operational conditions. The transient thermal loads
were experimentally simulated in the electron beam
facilities JUDITH 1 and JUDITH 2. In the course of the
experiments, the absorbed power density, pulse duration,
base temperature, number of pulses, and the surface
qualities of beryllium specimens were varied to cover a
broad range of relevant loading scenarios. With the
generated data, a damage map was created showing the surface
damages to be expected originating from transient thermal
loads with varying absorbed power densities and base
temperatures. Furthermore, the damage, cracking, and melting
thresholds of beryllium were determined. These thresholds
mark the parameter range, in which ITER can be operated
without inducing the respective damage type to the first
wall. Furthermore, the performance of dierent surface
qualities under transient thermal loading was compared in
order to determine the optimal surface treatment for the
beryllium armour tiles. As a result, the polished and the as
received electric discharge machining cut surface qualities
exhibited the best performance, while all ground surfaces
were severely damaged after 1000 pulses. Hence, grinding of
the [...]},
cin = {IEK-2},
cid = {I:(DE-Juel1)IEK-2-20101013},
pnm = {899 - ohne Topic (POF3-899)},
pid = {G:(DE-HGF)POF3-899},
typ = {PUB:(DE-HGF)3 / PUB:(DE-HGF)11},
url = {https://juser.fz-juelich.de/record/829762},
}