The main specific features of second-harmonic generation in biaxial cr
ystals (the presence of birefringence angles for all waves, the replac
ement of the terms ordinary and extraordinary waves by the terms fast
and slow waves, the presence of two phase-matching angles, the necessi
ty to specify the nonlinear tensor and field components in the same sy
stem of coordinates, and the difference of the crystal-physical system
from the crystal-optical system) are considered. It is demonstrated t
hat, in calculating the efficiency of second-harmonic generation, one
should precisely define the order of smallness for the accompanying ef
fects of approximately the same magnitude. We discuss the procedure fo
r choosing the optimal form of the differential operator in equations
for slowly varying amplitudes by means of the estimation of the dimens
ionless effective lengths of the relevant accompanying processes.