Silicon carbide powders with three particle size distributions (averag
e sizes of 0.4, 3 and 50 mu m) were subjected to strain-controlled, hi
gh-strain-rate deformation ((epsilon) over dot approximate to 3 x 10(4
)/s) in a cylindrical geometry which imposed simultaneous compressive
stresses. The experiments involved two explosive stages to (a) densify
the powder and to (b) subject the densified granules to large deforma
tion. The powder, with initial density of 33-59% of theoretical densit
y, was densified to densities between 73 and 94% of theoretical densit
y in the first stage. The densified powders were subjected to a global
effective strain of approximate to-0.27 in the second stage. Their re
sponse to the imposed constraints occurred through both homogeneous de
formation (82-100%) and shear localization (0-18%), depending on the p
article size. In the coarse powder (50 mu m), the shear localization p
rocess was primarily due to particle break-up (comminution) and rearra
ngement of the comminuted particles, through a similar mechanism to th
e bulk and prefractured SIC (Shih, C. J., Nesterenko, V. F. and Meyers
, M. A., Journal of Applied Physics. 1998, 83, 4660). Comminution was
observed in the medium powder (3 mu m), but was never seen in the fine
powder (0.4 mu m). In medium and fine granular SiC, the shear localiz
ation at sufficiently high displacement (> 150 mu m) leads to the form
ation of a thin layer (5-20 mu m) of well-bonded material. Calculated
temperatures in the centers of the bands are up to 2300 degrees C (usi
ng an assumed shear strength of 2 GPa and linear thermal softening), w
hich explain the bonding. An analytical model is developed that correc
tly predicts break-up of large particles and plastic deformation of th
e smaller ones. It is based on the Griffith fracture criterion and Wei
bull distribution of strength, which quantitatively express the fact t
hat the fracture is generated by flaws the size of which is limited by
the particle size. (C) 1998 Acta Metallurgica Inc.