We present a theoretical study of the influence of solvent on ordered
block copolymer solutions. The phase behavior is examined as a functio
n of solvent selectivity, temperature, copolymer concentration, compos
ition, and molecular weight. Phase maps are constructed using self-con
sistent mean-field (SCMF) theory, via the relative stability of the ''
classical'' phases, lamellae (L), hexagonally packed cylinders (C), an
d a body-centered cubic array of spheres (S). Solvent selectivity and
polymer concentration strongly influence phase transitions in copolyme
r solutions. When a neutral good solvent is added to a symmetric block
copolymer, a direct (lyotropic) transition from L to disordered (D) i
s expected, analogous to the (thermotropic) L --> D transition in melt
s. Indeed for neutral good solvents the dilution approximation is foll
owed: the phase map is equivalent to that in the melt, once the intera
ction parameter is multiplied by the copolymer volume fraction. In con
trast, for a symmetric block copolymer in the presence of a slightly s
elective solvent, the progression L -->C -->S -->micelles -->D is expe
cted, although the micellar phase is not treated here. For asymmetric
copolymers more elaborate sequences are anticipated, such as the progr
ession C-B -->L -->C-A -->S-A --> micelles -->D. The stability limit o
f a homogeneous block copolymer solution is also examined via the rand
om phase approximation (RPA) method. The effect of polymer concentrati
on on the spinodal instability falls into two regimes. When the solven
t is not very selective, the stable microphase separation region is re
duced as polymer concentration decreases, whereas for very selective s
olvents, whereas for very selective solvents decreasing polymer concen
tration broadens the region of stable ordered microstructures.