Two aspects of the nucleon electromagnetic polarizabilities, alpha(N)
and beta(N), are discussed. The first one is the interrelation between
static and Compton polarizabilities. Relativistically consistent trea
tment of the polarization effects based on effective Lagrangians resul
ts in the conclusion that the Compton polarizabilities, rather than th
e static ones, drive the energy shift of the nucleon in external field
s. The cluster substructure of the static polarizabilities. is shown t
o be crucial for consistent calculations of the polarizabilities. The
second aspect concerns the dominant role of pion degrees of freedom in
alpha(N) as seen through dispersion relations, chiral perturbation th
eory, and constituent models. The reported calculations of alpha(N) wi
thin soliton models are shown to be inconsistent with gauge invariance
. The difficulties in explaining the observed large diamagnetic compon
ent of beta(N) are emphasized.