Shock compaction of AlMgSi0.5 was realized by using a LEXAN projectile
with a velocity of 1655 m s(-1). The dynamic pressure in the zone of
impact was 8 GPa in the sample in the target at room temperature. The
sample consisted of spheres of two particle size fractions (100-200 mu
m and 200-315 mu m) separated in layers th rough wh ich the same shoc
k wave was passing. The appearance of non-porous interparticle contact
s in the impact zone, with the content of melted areas up to 10% was d
etected in the case of the larger particle fraction only. Smaller part
icles had no tendency to form the strong interparticle contacts, not e
ven in the first layers in the direction of the shock wave. TEM analys
is showed the presence of an intensively deformed structure in the zon
e of the planar shock wave, as well as the structures with very poor s
igns of recovery and recrystallization in particle contact areas. The
hardening effect of the shock wave was obvious, so that microhardness
in the zone of the planar wave in larger particles had reached the val
ue of 120 Hv, much higher than the microhardness of the initial powder
(70 Hv).