DIMENSIONALLY SCALED PENETRATION EXPERIMENTS - ALUMINUM TARGETS AND GLASS PROJECTILES 50 MU-M TO 3.2-MM IN DIAMETER

Spherical soda-lime glass projectiles 50, 150, 1000 and 3175 mum in diameter (D(p)) in aluminum targets (series 1100, ''annealed'') of variable thickness T were used to determine how the penetration-hole diameter (D(h)) varied as a function of D(p)/T at a constant impact velocity of 6 km/s. The target thickness ranged from infinite half-space geometries to 0.8 mum thick foils. Virtually identical morphologies characterize the penetration holes, no matter what projectile size, at equivalent D(p)/T conditions. The relative hole diameter (D(h)/D(p)) decreases systematically with increasing D(p)/T from D(h) congruent-to 4D(p) for massive targets, to D(h) = D(p) for very thin foils. A modest dependence on the absolute projectile size is observed; comparatively small cracters, yet relatively large penetration holes are produced by the smallest (50 mum) impactors. Nevertheless, linear dimensional scaling seems suitable for first-order estimates of D(p) from the measurement of D(h) and T on space-exposed surfaces. The projectile fragments and the debris dislodged from the target were intercepted by witness plates that were located behind the target. The dispersion angle of this debris cloud depends on the thickness of the target. In addition, millimeter-sized impactors are collisionally fragmented with greater ease than small impactors. Furthermore, we observe that systematic changes in the specific energy of dislodged projectile and target material occur as a function of D(p)/T. While linear scaling of target and projectile dimensions is a useful framework to explain many observations and associated shock processes, we suggest that consideration of the absolute and relative shock-pulse duration in the projectile (t(p)) and target (t(t)) may ultimately be the more useful approach. It implicitly accounts for all dimensions and, additionally, for specific impact velocities and pertinent material properties, via equations-of-state, for the impacting pair.