A phenomenological theory of the sequence of two second-order phase transit
ions with close temperatures is considered; such transitions occur in the N
i-Br boracite. The thermodynamic potential is written as a function of pola
rization P-i, magnetization M-i, and toroidal moment T-i vectors and fields
E-i and H-i; T-i is treated as an order parameter. It is assumed that only
one coefficient of T-i(2) passes through zero as T decreases. The possibil
ity of a sequence of two proper ferrotoroidal phase transitions alone, the
T-1 and T-2 components is demonstrated. Spontaneous Ti, Pi, and Mj vector v
alues and equations for susceptibility tensors (dielectric chi (ij) = dP(i)
/dE(j), magnetic k(ij) = dM(i)/dH(j), and magnetoelectric alpha (ij) = dP(i
)/dH(j) = dM(j)/dE(i)) were obtained for three phases. Some of these values
have well-defined anomalies in the vicinity of transitions. All possible s
equences of ferrotoroidal phase transitions in boracites are considered. De
pending on two potential coefficient values, these sequences may consist of
one, two, or three such transitions. (C) 2001 MAIK "Nauka/Interperiodica".