Abstract: Ferritic heat resistant steels are strongly desired to expand their maximum use temperature up to 650°C for application to the next highest temperature components of highly efficient, low emission ultra-supercritical (USC) power plant with maximum steam temperature of 700 °C. This minimizes the requirement of expensive nickel base superalloys. Critical issues for the development of ferritic steels for 650 °C USC boilers are the improvement of oxidation resistance as well as long-term creep rupture strength, including welded joints. The optimized combination of boron addition and dispersion of nanometer-sized vanadium nitrides significantly improves long-term creep strength of 9% Cr steel and also exhibits no degradation in welded joints at 650 °C. The protective Cr2O3-rich scale forms on the surface of 9% Cr steel by pre-oxidation treatment in Ar gas, which significantly improves the oxidation resistance in steam at 650°C.
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Abstract: Alloy-designing of high-strength ferritic heat resistant steels has been investigated for application to highly efficient, low emission ultra-supercritical power plant with maximum steam temperature of 700 oC. Ferritic heat resistant steels can be applied to the next highest temperature components and are strongly desired to expand their temperature range up to 650 oC in order to minimize the requirement of expensive nickel base superalloys. A dispersion of nanometer size MX nitrides along boundaries and the addition of boron significantly improve long-term creep strength. Newly alloy-designed 9Cr-3W-3Co-0.2V-0.05Nb steel with 160 ppm boron and 85 ppm nitrogen exhibits excellent creep strength of base metal and no degradation in welded joints at 650 oC. The protective Cr2O3-rich scale forms on the surface of 9Cr steel by pre-oxidation treatment in Ar gas, which significantly improves the oxidation resistance in steam at 650 oC.
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Authors: Noriyuki Y. Iwata, Ryuta Kasada, Akihiko Kimura, Takanari Okuda, Masaki Inoue, Fujio Abe, Shigeharu Ukai, Somei Ohnuki, Toshiharu Fujisawa
Abstract: Two types of oxide dispersion strengthened (ODS) ferritic steels have been produced by mechanical alloying (MA) either in argon or in hydrogen atmosphere, and vacuum hot pressing (VHP). A drastic reduction in the oxygen and nitrogen contents after VHP was strongly affected by hydrogen gas used as the MA atmosphere. MA in hydrogen was found to be effective for refining the steel matrix and enhancing the tensile ductility of the ODS ferritic steels.
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Abstract: The effect of fine precipitates, excess dislocations and sub-boundary hardening on creep strain behavior in the transient region has been investigated for tempered martensitic 9%Cr steel at 600 and 650oC. The fine precipitates that form during tempering or during creep decrease the creep rate in the transient region, while excess dislocations produced by cold rolling promote the recovery of dislocations during creep, resulting in higher creep rates. The sub-boundary hardening is enhanced by fine precipitates along lath and block boundaries, which retards the onset of acceleration creep. The movement and annihilation process of dislocations in the transient region is controlled by not only the movement of dislocations in the matrix but also the absorption of dislocations at boundaries. The minimum creep rate is basically determined by the time to minimum creep rate.
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Authors: Masaaki Igarashi, Koji Moriguchi, Seiichi Muneki, Fujio Abe, Yasuharu Shirai
Abstract: Creep deformation mechanism of the steels with a different matrix, α (ferrite), α’
(martensite) and γ (austenite), and precipitates such as MX and M23C6 has been analyzed using
positron annihilation lifetime measurement. The positron annihilation lifetime has been found to be a
very useful tool for evaluating the characteristic creep damage of the steels with different
microstructure and the corresponding microstructural evolution during creep deformation. The creep
deformation process of the α steel is heterogeneous, while the α’+M23C6 steel exhibits gradual
changes in the creep rate in both transient and acceleration creep regions with the largest off-set
strain, implying the homogeneous creep deformation. The α’+M23C6+ MX steel is in between the α
and α’+M23C6 steels. The homogeneous creep deformation takes place in the γ steel.
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Authors: Seiichi Muneki, Hiroshi Okubo, Fujio Abe
Abstract: In order to improve the creep strength of the heat resistant steels at elevated
temperatures over 700°C, a new attempt has been demonstrated using carbon and
nitrogen free Fe-Ni martensitic and austenitic alloys strengthened by Laves phase
such as Fe2W and Fe2Mo. It is important that these alloys are independent of any
carbides and any carbo-nitrides as strengthening factors. The high temperature
creep tests over 700°C exceed 36,000 hours and the test is continued. Creep
behavior of alloys is found to be completely different from that of the conventional
high-Cr ferritic steels. The alloys exhibit gradual change in the creep rate with
strain both in the transient and acceleration creep regions, and give a larger strain for
the minimum creep rate. Effect of Cr on the Fe-12Ni-9Co-10W alloys on the creep
properties more over 700°C was investigated. It became clear that the value for
100,000 hours was exceeded at 700°C and 100MPa calculated from the
Larson-Miller parameter at C=20. And surface appearance of crept specimen was
investigated in detail.
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Abstract: The effect of boron on microstructure evolution and creep deformation behavior has been
investigated for a tempered martensitic 9Cr-3W-3Co-0.2V-0.05Nb steel at 650oC. Creep tests were
carried out at 650oC for up to about 6 x 104 h. The addition of boron retards the onset of acceleration
creep at low stress and long time conditions, which results in lower minimum creep rate and longer
time to rupture. The addition of boron also retards the Ostwald ripening of M23C6 carbides near prior
austenite grain boundaries (PAGBs) during creep. The retardation of the onset of acceleration creep
results from the retardation of the recovery of martensitic microstructure near PAGBs by pinning
effects due to fine M23C6 carbides. The main effect due to boron is considered to occupy vacancies
near growing M23C6 carbides, which makes it difficult to accommodate local volume change around
the growing carbides. This reduces the rate of Ostwald ripening of M23C6 carbides.
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Authors: Seiichi Muneki, Hiroshi Okubo, Hirokazu Okada, Masaaki Igarashi, Fujio Abe
Abstract: The carbon and nitrogen free new alloys which were composed of the supersaturated
martensitic microstructure with high dislocation density before the creep test have been investigated
systematically. These alloys were produced from the new approach which raised creep strength
by the utilization of the reverse transformed austenite phase as a matrix and intermetallic
compounds such as Laves and μ-phases as precipitates during creep test. It is important that
these alloys are independent of any carbides and carbo-nitrides as strengthening factors. Creep
behavior of the alloys is found to be different from that of the conventional high-Cr ferritic heat
resistant steels. The minimum creep rates of the Fe-Ni alloys at 700°C are found to be much
lower than that of the conventional steel, which is due to fine dispersion strengthening useful even
at 700°C in these alloys. As a result carbon and nitrogen free alloys exhibited superior creep
properties at temperatures more over 700°C, and steam oxidation resistance.
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Authors: Yoshiaki Toda, Hideaki Kushima, Kazuhiro Kimura, Fujio Abe
Abstract: The effects of nickel content and heat treatment conditions on the creep strength of
precipitation-strengthened 15Cr ferritic steel were investigated. The creep strength of the 15Cr ferritic
steel was drastically improved by solution treatment and water quenching. However, over the long
term, the detrimental effect of nickel on the creep strength was pronounced for water-quenched steels.
The volume fraction of martensite phase increased with increased nickel content in both the
furnace-cooled and water-quenched steels. The volume fraction of martensite phase in the
water-quenched steel was smaller than that in the furnace-cooled type, even for the same nickel
content. Fine particles, smaller than 500 nm, were precipitated homogeneously within the ferrite
phase of the water-quenched steel. On the other hand, coarse block-like particles 1 $m in size were
precipitated sparsely within the martensite phase. The creep strength of the steels decreased with
increased volume fraction of the martensite phase caused by furnace cooling and nickel addition. The
lower creep strength and microstructural stability of the martensite phase is attributable to less
precipitation strengthening. To enable this steel to be put to practical use, it will be necessary to
suppress the formation of the martensite phase caused by addition of nickel by optimizing the
chemical composition and heat treatment conditions.
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Authors: Fujio Abe, H. Semba, T. Sakuraya
Abstract: The effect of boron on microstructure and creep deformation behavior has been
investigated for a tempered martensitic 9Cr-3WVNb steel with emphasis on the role of boron free
from boron nitrides. Creep tests were carried out at 650oC for up to about 3 x 104 h, using
specimens of 10 mm in gauge diameter and 50 mm in gauge length. The addition of boron in
combination with no nitrogen addition effectively reduces the coarsening rate of M23C6 carbides by
an enrichment of boron in M23C6 particles in the vicinity of prior austenite grain boundaries during
creep at 650oC. This stabilizes martensitic microstructure during creep and retards the onset of
acceleration creep, resulting in a decrease in minimum creep rate and an increase in creep life.
Excess addition of boron and nitrogen causes the formation of boron nitrides during normalizing at
1050-1150oC, which reduces dissolved boron and nitrogen. The dissolved boron enriches in
M23C6 carbides, while the dissolved nitrogen causes the precipitation of fine MX carbonitrides.
The variation of creep rates in transient region and of the onset time of acceleration creep with
various combinations of boron and nitrogen contents can be explained by the dissolved boron and
nitrogen concentrations after normalizing into account.
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