scholarly journals Preferred orientation formation in surface layer of aluminum sheet subjected to friction roll surface processing and temperature gradient annealing

2019 ◽  
Vol 1270 ◽  
pp. 012028 ◽  
Author(s):  
Yoshimasa Takayama ◽  
Ryuichi Hamano ◽  
Takuya Arakawa ◽  
Hideo Watanabe
2011 ◽  
Vol 702-703 ◽  
pp. 457-460 ◽  
Author(s):  
Yoshimasa Takayama ◽  
Mei Qin Shi ◽  
Yoshihiro Ougiya ◽  
Kenta Nonaka ◽  
Hideo Watanabe

Titanium and aluminum sheets were directionally strained by friction roll surface processing (FRSP). Severe shear strain was imposed into the surface layer and strain gradient was formed through the thickness of the sheet. The microstructure and texture in as-strained state were investigated by optical microscopy and X-ray diffraction technique. Ultra-fine grains in the surface layer of the titanium sheet were found to have a sharp texture with a preferred orientation strongly related to the FRSP direction. The evolution of microstructure and crystallographic texture of FRSPed samples during annealing were studied by electron back-scattered diffraction (EBSD) technique. Obvious preferred orientations of shear straining were obtained in the surface layer of both materials as a result from FRSP and subsequent annealing.


2015 ◽  
Vol 56 (3) ◽  
pp. 303-312 ◽  
Author(s):  
Yoshimasa Takayama ◽  
Ryuichi Hamano ◽  
Takuya Arakawa ◽  
Kenta Nonaka ◽  
Hideo Watanabe ◽  
...  

2015 ◽  
Vol 65 (6) ◽  
pp. 234-243
Author(s):  
Yoshimasa Takayama ◽  
Ryuichi Hamano ◽  
Takuya Arakawa ◽  
Kenta Nonaka ◽  
Hideo Watanabe ◽  
...  

2009 ◽  
Vol 50 (1) ◽  
pp. 210-214 ◽  
Author(s):  
Meiqin Shi ◽  
Yoshimasa Takayama ◽  
Tomohiro Umetsu ◽  
Hajime Kato ◽  
Hideo Watanabe ◽  
...  

2017 ◽  
Vol 110 (9) ◽  
pp. 093504 ◽  
Author(s):  
N. Zhao ◽  
Y. Zhong ◽  
W. Dong ◽  
M. L. Huang ◽  
H. T. Ma ◽  
...  

2012 ◽  
Vol 22 (11) ◽  
pp. 2616-2627 ◽  
Author(s):  
Mei-qin SHI ◽  
Yoshimasa TAKAYAMA ◽  
Chun-an MA ◽  
Hideo WATANABE ◽  
Hirofumi INOUE

2016 ◽  
Vol 73 (11) ◽  
pp. 4519-4529 ◽  
Author(s):  
Maithili Sharan ◽  
Piyush Srivastava

Abstract The behavior of the heat flux H with respect to the stability parameter (=z/L, where z is the height above the ground, and L is the Obukhov length) in the unstable atmospheric surface layer is analyzed within the framework of Monin–Obukhov similarity (MOS) theory. Using MOS equations, H is expressed as a function of and vertical surface-layer potential temperature gradient . A mathematical analysis is carried out to analyze the theoretical nature of heat flux with the stability parameter by considering the vertical potential temperature gradient as (i) a constant and (ii) a power-law function of heat flux. For a given value of H, two values of associated with different stability regimes are found to occur in both the conditions, suggesting the nonuniqueness of MOS equations. Turbulent data over three different sites—(i) Ranchi, India; (ii) the Met Office’s Cardington, United Kingdom, monitoring facility; and (iii) 1999 Cooperative Atmosphere–Surface Exchange Study (CASES-99; United States—are analyzed to compare the observed nature of H with that predicted by MOS. The analysis of observational data over these three sites reveals that the observed variation of H with is consistent with that obtained theoretically from MOS equations when considering the vertical temperature gradient as a power-law function of heat flux having the exponent larger than 2/3. The existence of two different values of the stability parameter for a given value of heat flux suggests that the application of heat flux as a boundary condition involves some intricacies, and it should be applied with caution in convective conditions.


1986 ◽  
Vol 20 (12) ◽  
pp. 2465-2471 ◽  
Author(s):  
F. Trombetti ◽  
M. Tagliazucca ◽  
F. Tampieri ◽  
T. Tirabassi

1952 ◽  
Vol 9 (7) ◽  
pp. 325-328 ◽  
Author(s):  
H. B. Hachey

On the basis of temperature observations made in the Great Lakes in the summer months it has been shown that: (a) the maximum depth of the thermocline does not exceed 50 feet, (b) the temperature gradient within the thermocline may be as much as 26 degrees Fahrenheit in 10 feet, (c) the thickness of the surface layer varies considerably with time and position, and can under certain circumstances be entirely removed from an area, and (d) the temperature of the deeper waters approximates to that of the maximum density of fresh water.


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