An effective method for calculating the sum of dipole magnetic fields of la
ttice sites is developed using the threefold axial symmetry and performing
summation over hexagonal planes. The values of fields in octahedral and tet
rahedral interstices of an hcp lattice are determined for spiral structures
of heavy RE metals and for samarium. It is shown that the absence of an ex
perimentally observed jump in the dipole field at the point of ferro-antife
rromagnetic transition in the disposition is due to the small angle of rota
tion of the spiral magnetic structure. The problem of interpretation of the
Lorentz macroscopic field is discussed on the basis of calculation of micr
oscopic fields in a homogeneous continuous medium. (C) 2000 MAIK "Nauka/Int
erperiodica".