Stabilization of wave formation at the contact boundary of metal layers in an explosive welding regime

1989 ◽  
Vol 25 (5) ◽  
pp. 604-608
Author(s):  
O. B. Drennov ◽  
A. L. Mikhailov ◽  
R. S. Osipov ◽  
L. D. Rodigina
Author(s):  
V.G. Petushkov ◽  
M.I. Zotov ◽  
L.D. Dobrushin

Joining of metals in explosive welding takes place as a result of their plastic deformation during a high speed collision and is usually accompanied by typical formation of waves at the interface. In welding aluminium, the weld boundary can also be straight if the speed of the contact point is νc is ≤ 1900 m/s. These welding conditions make it possible to prevent melting of the metal at the interface and increase at the same time its corrosion resistance. In this article, the effect of the dynamic collision angle on the special features of plastic flow of the metal in the vicinity of the contact boundary in welding sheets of AS5 aluminium is described.


1989 ◽  
Vol 5 (2) ◽  
pp. 97-108 ◽  
Author(s):  
Cheng Chemin ◽  
Tan Qingming

1969 ◽  
Vol 3 (4) ◽  
pp. 344-348 ◽  
Author(s):  
A. A. Deribas ◽  
V. M. Kudinov ◽  
F. I. Matveenkov

Strong bonds can be produced by the explosive welding process and usually the weld interface has a characteristic wavy form. In this paper the mechanism of explosive welding is discussed, the present theories of wave formation are critically examined and a new mechanism of wave formation is proposed. According to this mechanism the materials of the impacting plates in the region of collision behave in a similar manner to liquids of low viscosity. As a result the impacting or flyer plate divides into a re-entrant jet and a salient jet. Very high pressure is produced at the stagnation point of the divided jet. The parent plate deforms under the stagnation point and consequently a hump is formed in the parent plate ahead of the point of collision. The hump builds up and eventually traps the re-entrant jet. The stagnation point then transfers to the top of the hump and then descends it and starts forming a new hump, and in this manner successive waves are formed. The proposed mechanism of wave formation seems to explain the experimentally observed behaviour reasonably well. Furthermore, experiments are reported in which one of the surfaces to be bonded was copper plated and the second surface was nickel plated and by this means the movements of the surfaces being bonded were traced. These experiments gave strong support to the proposed theory of wave formation.


1985 ◽  
Vol 21 (1) ◽  
pp. 124-130 ◽  
Author(s):  
S. V. Bazdenkov ◽  
V. F. Demichev ◽  
D. Kh. Morozov ◽  
O. P. Pogutse

1968 ◽  
Vol 17 (148) ◽  
pp. 669-680 ◽  
Author(s):  
J. N. Hunt

1973 ◽  
Vol 12 (3) ◽  
pp. 398-406 ◽  
Author(s):  
S. K. Godunov ◽  
A. A. Deribas ◽  
N. S. Kozin

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