scholarly journals Characterization of untransformed ferrite in 10Cr and 12Cr ODS steels

Materialia ◽  
2021 ◽  
Vol 16 ◽  
pp. 101066
Author(s):  
Anthony Durand ◽  
Denis Sornin ◽  
Yann de Carlan ◽  
Gabriel Spartacus ◽  
François Brisset ◽  
...  
Keyword(s):  
2018 ◽  
Vol 81 (5) ◽  
pp. 502-508 ◽  
Author(s):  
Iwona Jóźwik ◽  
Agata Strojny-Nędza ◽  
Marcin Chmielewski ◽  
Katarzyna Pietrzak ◽  
Łukasz Kurpaska ◽  
...  
Keyword(s):  

2011 ◽  
Vol 417 (1-3) ◽  
pp. 201-204 ◽  
Author(s):  
Kimihiro Nogiwa ◽  
Akihiko Nishimura ◽  
Atsushi Yokoyama ◽  
Satoshi Ohtsuka ◽  
Takaji Kaito ◽  
...  
Keyword(s):  

Author(s):  
Masatoshi Sakairi ◽  
Sublime Ningshen ◽  
Keita Suzuki ◽  
Shigeharu Ukai

2017 ◽  
Vol 373 ◽  
pp. 96-99 ◽  
Author(s):  
Lu Hui Han ◽  
Tao Fa ◽  
Ya Wen Zhao

The purpose of this study is to evaluate the irradiation defects of 12Cr-ODS steels induced by He/H ions, to provide basic understanding concerning development of fusion reactor components. Firstly, single He、H ion implantation and He/H ion co-implantation of 12Cr-ODS steels were performed at room temperature; and then SIMS were used to determine the He/H ion depth; finally, the irradiation induced defects were investigated by PALS and TEM. Characterization of the implanted samples with SIMS shows that He/H ions are mainly distributed at 4-6μm depth, consistent with the SRIM simulation. The PALS results show that the positron lifetime of H ions implanted samples increases slightly with increasing incident ions fluence, while for He and He/H ion implantation it is reversed. In addition, TEM results demonstrate that after irradiation, cavities are created in all samples, and He ion irradiation produce seriously larger damage compared to H ion. The positron lifetime results can be mainly ascribed to the difference of He and H ion interaction with defects.


2014 ◽  
Vol 444 (1-3) ◽  
pp. 43-48 ◽  
Author(s):  
Chansun Shin ◽  
Sangyeob Lim ◽  
Hyung-ha Jin ◽  
Peter Hosemann ◽  
Junhyun Kwon
Keyword(s):  

2017 ◽  
Vol 131 (4) ◽  
pp. 1090-1092 ◽  
Author(s):  
V. Slugeň ◽  
I. Bartošová ◽  
J. Dekan
Keyword(s):  

2015 ◽  
Vol 465 ◽  
pp. 236-244 ◽  
Author(s):  
Daniel Brimbal ◽  
Lucile Beck ◽  
Oliver Troeber ◽  
Ermile Gaganidze ◽  
Patrick Trocellier ◽  
...  

Author(s):  
B. L. Soloff ◽  
T. A. Rado

Mycobacteriophage R1 was originally isolated from a lysogenic culture of M. butyricum. The virus was propagated on a leucine-requiring derivative of M. smegmatis, 607 leu−, isolated by nitrosoguanidine mutagenesis of typestrain ATCC 607. Growth was accomplished in a minimal medium containing glycerol and glucose as carbon source and enriched by the addition of 80 μg/ ml L-leucine. Bacteria in early logarithmic growth phase were infected with virus at a multiplicity of 5, and incubated with aeration for 8 hours. The partially lysed suspension was diluted 1:10 in growth medium and incubated for a further 8 hours. This permitted stationary phase cells to re-enter logarithmic growth and resulted in complete lysis of the culture.


Author(s):  
A.R. Pelton ◽  
A.F. Marshall ◽  
Y.S. Lee

Amorphous materials are of current interest due to their desirable mechanical, electrical and magnetic properties. Furthermore, crystallizing amorphous alloys provides an avenue for discerning sequential and competitive phases thus allowing access to otherwise inaccessible crystalline structures. Previous studies have shown the benefits of using AEM to determine crystal structures and compositions of partially crystallized alloys. The present paper will discuss the AEM characterization of crystallized Cu-Ti and Ni-Ti amorphous films.Cu60Ti40: The amorphous alloy Cu60Ti40, when continuously heated, forms a simple intermediate, macrocrystalline phase which then transforms to the ordered, equilibrium Cu3Ti2 phase. However, contrary to what one would expect from kinetic considerations, isothermal annealing below the isochronal crystallization temperature results in direct nucleation and growth of Cu3Ti2 from the amorphous matrix.


Author(s):  
B. H. Kear ◽  
J. M. Oblak

A nickel-base superalloy is essentially a Ni/Cr solid solution hardened by additions of Al (Ti, Nb, etc.) to precipitate a coherent, ordered phase. In most commercial alloy systems, e.g. B-1900, IN-100 and Mar-M200, the stable precipitate is Ni3 (Al,Ti) γ′, with an LI2structure. In A lloy 901 the normal precipitate is metastable Nis Ti3 γ′ ; the stable phase is a hexagonal Do2 4 structure. In Alloy 718 the strengthening precipitate is metastable γ″, which has a body-centered tetragonal D022 structure.Precipitate MorphologyIn most systems the ordered γ′ phase forms by a continuous precipitation re-action, which gives rise to a uniform intragranular dispersion of precipitate particles. For zero γ/γ′ misfit, the γ′ precipitates assume a spheroidal.


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