scholarly journals Adhesion of rubbers to metals and its alloy. Part 1. Cure-adhesion of rubbers to electroless Pd-P alloy deposit.

1990 ◽  
Vol 63 (8) ◽  
pp. 503-508 ◽  
Author(s):  
Yoshiyuki IKEDA ◽  
Hidemi NAWAFUNE ◽  
Shozo MIZUMOTO ◽  
Kazushige KADOTA ◽  
Koichi YAMAGUCHI ◽  
...  
1991 ◽  
Vol 64 (6) ◽  
pp. 372-377 ◽  
Author(s):  
Yoshiyuki IKEDA ◽  
Hidemi NAWAFUNE ◽  
Shozo MIZUMOTO ◽  
Koichi YAMAGUCHI ◽  
Kazushige KADOTA ◽  
...  

1994 ◽  
Vol 67 (5) ◽  
pp. 376-382 ◽  
Author(s):  
Yoshiyuki IKEDA ◽  
Hidemi NAWAFUNE ◽  
Shozo MIZUMOTO ◽  
Kiyoshi IKEDA ◽  
Koichi YAMAGUCHI

2019 ◽  
Vol 754 ◽  
pp. 161-177 ◽  
Author(s):  
Waqas Muhammad ◽  
Abhijit P. Brahme ◽  
Usman Ali ◽  
Jürgen Hirsch ◽  
Olaf Engler ◽  
...  

2008 ◽  
Vol 49 (5) ◽  
pp. 898-902 ◽  
Author(s):  
Akira Takara ◽  
Li-Fu Chian ◽  
Sung Wook Chung ◽  
Hidetoshi Somekawa ◽  
Hiroyuki Watanabe ◽  
...  
Keyword(s):  

2011 ◽  
Vol 462-463 ◽  
pp. 1355-1360
Author(s):  
Omar Suliman Zaroog ◽  
Aidy Ali ◽  
Sahari B. Barkawi

It is important to account for residual stress relaxation phenomenon in the design of the component. Specimens of 2024-T351 aluminium alloy were used in this study. The specimens were shot peened under three different shot peening intensities. Cyclic tests for two load magnitudes were performed for 1, 2, 10, 1000 and 10000 cycles. Residual stresses, microhardness and the cold work percentage were measured at initial state and after each loading cycle for the three shot peening intensities and for the two loads. The study revealed that most of the drop in the residual stress, microhardness and cold work happened in the first cycle are dependent on the applied load.


2011 ◽  
Vol 43 (1) ◽  
pp. 327-339 ◽  
Author(s):  
Yuhong Xiong ◽  
Dongming Liu ◽  
Ying Li ◽  
Baolong Zheng ◽  
Chris Haines ◽  
...  

1996 ◽  
Vol 10 (20) ◽  
pp. 2469-2529 ◽  
Author(s):  
A.O. ANOKHIN ◽  
M.I. KATSNELSON

A model of alloy is considered which includes both quenched disorder in the electron subsystem (“alloy” subsystem) and electron-phonon interaction. For given approximate solution for the alloy part of the problem, which is assumed to be conserving in Baym’s sense, we construct the generating functional and derive the Eliashberg-type equations which are valid to the lowest order in the adiabatic parameter. The renormalization of bare electron–phonon interaction vertices by disorder is taken into account consistently with the approximation for the alloy self-energy. For the case of exact configurational averaging the same set of equations is established within the usual T-matrix approach. We demonstrate that for any conserving approximation for the alloy part of the self-energy the Anderson’s theorem holds in the case of isotropic singlet pairing provided disorder renormalizations of the electron-phonon interaction vertices are neglected. Taking account of the disorder renormalization of the electron-phonon interaction we analyze general equations qualitatively and present the expressions for Tc for the case of weak and intermediate electron-phonon coupling. Disorder renormalizations of the logarithmic corrections to the effective coupling, which arise when the effective interaction kernel for the Cooper channel has the second energy scale, as well as the renormalization of the dilute paramagnetic impurity suppression are discussed.


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