The magnetic properties of large Ising clusters with cube-octahedral,
icosahedral, body-centered cubic and simple cubic structures are studi
ed. The Ising Hamiltonian is solved in the mean field approximation an
d the magnetization and the Curie temperature are calculated for clust
ers consisting of as many as 2744 atoms. The dependence of Te with res
pect to the total number of atoms (N) follows a finite scaling behavio
r delta = 1 - T-C(N)/T-C(infinity) = alpha N--lambda. We find that for
all the structures studied and for the case in which the magnetic cou
pling constants between spins are assumed independent of their locatio
n in the cluster, 0.569 < lambda < 0.597 and 2.192 < alpha < 3.126. Th
ose quantities change considerably when the coupling constants between
surface spins are assumed to be different from the rest. These result
s clearly show the particular behavior of finite aggregates. We presen
t results for the magnetization profiles of sites lying on the central
plane and on one of the faces of a body-centered cubic cluster with 1
241 spins. We also studied the magnetization decay in the low temperat
ure limit and found that the amplitude and exponent are different from
the bulk values. We compare our calculations with other results in th
e literature.