Microstructure of Oxide Layers Formed During Autoclave Testing of Zirconium Alloys

Author(s):  
B Wadman ◽  
Z Lai ◽  
H-O Andrén ◽  
A-L Nyström ◽  
P Rudling ◽  
...  
1998 ◽  
Vol 30 (3-4) ◽  
pp. 247-263 ◽  
Author(s):  
M. Parise ◽  
I. Touet ◽  
O. Sicardy

In order to have a better knowledge of the mechanical behaviour of the oxide layers growing on zirconium alloys in pressurized water reactors, the textures of different zirconium alloys and their oxide layers are studied. The results show that the texture of the oxide layers present a feature common to all the layers: the tilt angle of the maximum intensities of the pole figures obtained on the layers is almost quite identical for all the studied substrates. The azimuthal reinforcements depend on the metallurgical state of the substrate.The crystallographic direction of monoclinic zirconia common to all the oxide grains is identified. A computation based on mechanical issues is presented: considering the anisotropic elastic properties of the monoclinic monocrystal, it is shown that the particular crystallographic direction is linked to an isotropic state of strains in the plane of the metal–oxide interface.


2019 ◽  
Vol 526 ◽  
pp. 151779
Author(s):  
Brendan Ensor ◽  
David J. Spengler ◽  
John R. Seidensticker ◽  
Ram Bajaj ◽  
Zhonghou Cai ◽  
...  

2020 ◽  
Vol 55 (6) ◽  
pp. 460-470
Author(s):  
Pavel Sialini ◽  
Petr Sajdl ◽  
Krystof Dobrovolny

1996 ◽  
Vol 229 ◽  
pp. 79-92 ◽  
Author(s):  
A.J.G. Maroto ◽  
R. Bordoni ◽  
M. Villegas ◽  
A.M. Olmedo ◽  
M.A. Blesa ◽  
...  

10.14311/1002 ◽  
2007 ◽  
Vol 47 (6) ◽  
Author(s):  
H. Frank

Two batches of tubes of Zr1Nb and of Zry-4W were oxidized for 30 days at 425 °C in steam, and for 360 days at 500 °C in air, respectively. The analysis of the I-V characteristics at constant temperatures up to 220 °C of oxide layers of nearly equal thickness gave an activation energy of 1,3 eV for the grey homogeneous steam samples, and of 0.4 eV for the white surface layer, and of 1.3 eV at temperatures over 140 °C, for the grey bottom layer of the air samples, respectively. The I-V characteristics were sub-linear in the air samples, the current growing less at rising voltages, but staightening to super-linear space-charge limited currents at higher temperatures. The injection currents flowing when voltage was applied did not reach constant equilibrium, but at a bend, continued with a lesser slope. The resistivity was about one order of magnitude greater in air samples and greater in Zry-4W. The relative permittivity was greater in the steam samples and greater in Zr1Nb. The currents of the air samples were greater with Au electrodes than with Ag electrodes. 


2020 ◽  
Vol 86 (8) ◽  
pp. 32-37
Author(s):  
V. V. Larionov ◽  
Xu Shupeng ◽  
V. N. Kudiyarov

Nickel films formed on the surface of zirconium alloys are often used to protect materials against hydrogen penetration. Hydrogen adsorption on nickel is faster since the latter actively interacts with hydrogen, oxidizes and forms a protective film. The goal of the study is to develop a method providing control of hydrogen absorption by nickel films during vacuum-magnetron sputtering and hydrogenation via measuring thermoEMF. Zirconium alloy E110 was saturated from the gas phase with hydrogen at a temperature of 350°C and a pressure of 2 atm. A specialized Rainbow Spectrum unit was used for coating. It is shown that a nickel film present on the surface significantly affects the hydrogen penetration into the alloy. A coating with a thickness of more than 2 μm deposited by magnetron sputtering on the surface of a zirconium alloy with 1% Nb, almost completely protects the alloy against hydrogen penetration. The magnitude of thermoemf depends on the hydrogen concentration in the zirconium alloy and film thickness. An analysis of the hysteresis width of the thermoEMF temperature loop and a method for determining the effective activation energy of the conductivity of a hydrogenated material coated with a nickel film are presented. The results of the study can be used in assessing the hydrogen concentration and, hence, corrosion protection of the material.


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