TY - JOUR
T1 - Nth-nearest neighbor statistics for three-dimensional equilibrium arrays of monodisperse spheres
AU - Leggoe, Jeremy
AU - Riggs, J.B.
PY - 2006
Y1 - 2006
N2 - Measures based on mean Nth-nearest neighbor distances efficiently characterize particle clustering and deviation from the equilibrium random state (ERS) in microstructures. Mean center-to-center distances to the Nth-nearest neighbor particle have been determined for three-dimensional equilibrium ensembles of monodisperse spheres for N ≤ 200. Hard sphere distributions represent inhibited point processes, and for small N the inhibition effect was significant for volume fractions ranging from 0.01 to 0.40. Caution should therefore be exercised in comparing hard sphere distributions with point processes, even at low volume fractions. For volume fractions ≥ 0.20, a significant ordering-related oscillation arises in the inhibition ratio; the effect is sufficiently strong that at a volume fraction of 0.40 it extends over the entire range of N ≤ 200, and the inhibition ratio falls below unity for certain values of N. To enable calculation of the inhibition ratio for N ≤ 200, functions were fit to the data for the volume fractions considered in this investigation.
AB - Measures based on mean Nth-nearest neighbor distances efficiently characterize particle clustering and deviation from the equilibrium random state (ERS) in microstructures. Mean center-to-center distances to the Nth-nearest neighbor particle have been determined for three-dimensional equilibrium ensembles of monodisperse spheres for N ≤ 200. Hard sphere distributions represent inhibited point processes, and for small N the inhibition effect was significant for volume fractions ranging from 0.01 to 0.40. Caution should therefore be exercised in comparing hard sphere distributions with point processes, even at low volume fractions. For volume fractions ≥ 0.20, a significant ordering-related oscillation arises in the inhibition ratio; the effect is sufficiently strong that at a volume fraction of 0.40 it extends over the entire range of N ≤ 200, and the inhibition ratio falls below unity for certain values of N. To enable calculation of the inhibition ratio for N ≤ 200, functions were fit to the data for the volume fractions considered in this investigation.
U2 - 10.1016/j.msea.2006.04.017
DO - 10.1016/j.msea.2006.04.017
M3 - Article
VL - 426
SP - 289
EP - 297
JO - Materials Science and Engineering A
JF - Materials Science and Engineering A
SN - 0921-5093
IS - 1-2
ER -