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@PHDTHESIS{LopezBarrilao:828724,
author = {Lopez Barrilao, Jennifer Katharina},
title = {{M}icrostructure {E}volution of {L}aves {P}hase
{S}trengthened {F}erritic {S}teels for {H}igh {T}emperature
{A}pplications},
volume = {375},
school = {RWTH Aachen},
type = {Dr.},
address = {Jülich},
publisher = {Forschungszentrum Jülich GmbH Zentralbibliothek, Verlag},
reportid = {FZJ-2017-02590},
isbn = {978-3-95806-231-3},
series = {Schriften des Forschungszentrums Jülich Reihe Energie $\&$
Umwelt / Energy $\&$ Environment},
pages = {XVI, 134 S.},
year = {2017},
note = {RWTH Aachen, Diss., 2016},
abstract = {The present investigation focuses on a new concept of high
strength, high chromium (18 - 23 $wt.\%),$ fully ferritic
steels on the technical basis of Crofer$^{®}$ 22 H for the
application in high temperature energy conversion systems.
Fully ferritic means, that these steels possess a ferritic
matrix at any temperature below the melting point, i.e. no
martensitic transformation occurs. During Crofer$^{®}$ 22
APU and Crofer$^{®}$ 22 H development, over 50 trial alloys
with slight changes in chemical composition were designed.
Both steels are used as interconnect materials for solid
oxide fuel cells (SOFCs) and were developed by the Institute
for Microstructure and Properties of Materials (IEK- 2) at
Forschungszentrum Jülich GmbH in cooperation with VDM
Metals GmbH. Such steels possess potentially sufficient
steam oxidation resistance up to 650 $^{\circ}$C, because of
their high chromium content [1]. In contrast the steam
oxidation resistance of state of the art 9 - 12 \%Cr
advanced ferritic martensitic (AFM) steels is limited to
temperatures of approximately 620 $^{\circ}$C. To ensure
sufficient steam oxidation resistance of AFM steels above
620 $^{\circ}$C a higher chromium content is needed [2,3].
However, this promotes Z-phase formation on the expense of
the strengthening MX (M = V, Nb; X = C, N) particles [4],
what causes a drop in long-term creep strength.
Strengthening of the new fully ferritic steels is achieved
by solid-solution hardening and in case of Crofer$^{®}$ 22
H by supplemental intermetallic (Fe,Cr,Si)2(Nb,W) Laves
phase particles. The 22 H trial alloys possess superior
creep behaviour in the temperature range from 600
$^{\circ}$C to 650 $^{\circ}$C [1] and therefore may
potentially provide a basis for tackling the future
requirements of power plant operation, e.g. higher
operational flexibility, higher conversion efficiency and
thus lower CO$_{2}$ emission. In order to further
optimisation of these fully ferritic alloys the
investigation was performed on three various 22 H trial
alloys. The investigations aimed on the identification and
classification of Laves phase particles as well as on the
influence of chemical composition on the presence of
different Laves phases and particle size evolution in the
temperature range from 600 $^{\circ}$C to 650 $^{\circ}$C
after different annealing time utilising electron microscopy
techniques. Concurrently the suitability of a commercially
available thermodynamic modelling tool was checked and rated
as doubtful for further in detail alloy development of such
ferritic steels. Particle evolution results explain the
different creep behaviour of the trial alloys and show
promising thermodynamic stability of particle over the whole
covered time range (e.g. approximately 40,000 h at 600
$^{\circ}$C and approximately 10,000 h at 650 $^{\circ}$C).
Furthermore, investigation of microstructure evolution at
650 $^{\circ}$C focused on sub-grain formation, the
formation of particle free zones and associated dislocation
density in these. Due to missing particle strengthening in
these zones and consequently a drop in creep strength, the
particle free zones are suspected to be a reason of
premature material failure.},
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/828724},
}