Effect of Surface Micro-parameters on Contact Temperature of Sliding Electrical Contact

Author(s):  
Fengyi Guo ◽  
Xin Gu ◽  
Li Li ◽  
Zhiyong Wang ◽  
Tunan Wang ◽  
...  
2019 ◽  
pp. 101-109 ◽  
Author(s):  
M. I. Aleutdinova ◽  
V. V. Fadin ◽  
Yu. P. Mironov

The possibility of creating a wear-resistant dry sliding electrical contact tungsten/steel was studied. It was shown that tungsten caused severe wear of the quenched steel counterbody due to unlimited plastic flow of its surface layer at a current density up to 150 A/cm2 . This indicated the impossibility of achieving satisfactory characteristics of such a contact. Low electrical conductivity and wear resistance of the contact tungsten/steel were presented in comparison with the known high copper/steel contact characteristics under the same conditions. X-ray phase analysis data of the steel sliding surfaces made it possible to state that the cause of the unsatisfactory sliding of tungsten was the absence of the necessary concentration of FeO oxide on the sliding surface of the steel. 


2011 ◽  
Vol 18 (4) ◽  
pp. 1307-1313 ◽  
Author(s):  
Lee Li ◽  
Cai Li ◽  
Yu Feng ◽  
Nan Jing ◽  
Zhou Zheng-Yang ◽  
...  

2008 ◽  
Vol 131 (2) ◽  
Author(s):  
P. Rogeon ◽  
R. Raoelison ◽  
P. Carre ◽  
F. Dechalotte

This study deals with resistance spot welding process modeling. Particular attention must be paid to the interfacial conditions, which strongly influence the nugget growth. Imperfect contact conditions are usually used in the macroscopic model to account for the electrical and thermal volume phenomena, which occur near a metallic interface crossed by an electric current. One approach consists in representing microconstriction phenomena by surface contact parameters: The share coefficient and the thermal and electrical contact resistances, which depend on the contact temperature. The aim of this work is to determine the share coefficient and the contact temperature through a numerical model on a microscopic scale. This surface approach does not make it possible to correctly represent the temperature profiles, with the peak temperature, observed in the immediate vicinity of the interface and thus to define, in practice, the contact temperature correctly. That is why another approach is proposed with the introduction of a low thickness layer (third body) at the level of the interface the electric and thermal resistances of which are equivalent to the electrical and thermal contact resistance values. In this case, the parameters of the model are reduced to the thickness of the arbitrarily fixed layer and equivalent electric and thermal conductivities in the thin layer, the partition coefficient and the contact temperature becoming implicit. The two types of thermoelectric contact models are tested within the framework of the numerical simulation of a spot welding test. The nugget growth development is found to be much different with each model.


1992 ◽  
Vol 71 (8) ◽  
pp. 3713-3720 ◽  
Author(s):  
J. S. Walker ◽  
D. M. Audet ◽  
G. Talmage ◽  
S. H. Brown ◽  
N. A. Sondergaard

1999 ◽  
Vol 144-145 ◽  
pp. 287-291 ◽  
Author(s):  
A Senouci ◽  
H Zaidi ◽  
J Frene ◽  
A Bouchoucha ◽  
D Paulmier

2013 ◽  
Vol 41 (12) ◽  
pp. 3645-3650 ◽  
Author(s):  
Mintang Li ◽  
Guangdong Wang ◽  
Liang Wang ◽  
Ruzheng Pan ◽  
Dong Sun ◽  
...  

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