The widely used relation <(<alpha>)over tilde> = alpha (o) + Delta alpha fo
r the electric polarizability, where Delta alpha is proportional to the r.m
.s. charge radius of the system, is revisited within a simple model of two
spinless particles bound electromagnetically. A complete set of the relativ
istic corrections to ceo following from the Breit Hamiltonian is obtained.
It is shown that these corrections modify the result for a in comparison to
that obtained with ao taken in the nonrelativistic approximation. We propo
se that the same situation can take place in the more complicated case of h
adrons. Special attention is devoted to the correct definition of the cente
r-of-mass coordinates which are found to be very important.