When dissolved in aqueous solution, alpha -lactose, whether originally in t
he anhydrous or the monohydrated form, readily undergoes mutarotation to yi
eld the beta isomer. At equilibrium, which is reached in 6.5 h at 292 K and
more rapidly with increasing temperatures, the latter is present to the ex
tent of ca. 60% w/w. At saturation, alpha -lactose hydrate precipitates fro
m this solution being considerably less soluble than the beta form. The res
ulting crystals have a highly asymmetric, tomahawk shaped morphology charac
terized by large {0(1) over bar 1} in the {0(1) over bar 1} sectors of the
crystals coupled with a characteristic lack of growth in the [0(1) over bar
0] direction;. Growth under conditions that restrict the formation of the
beta isomer yields more symmetrically shaped, needlelike crystals. These sh
ow a gradual transition to the tomahawk shape as the concentration of the b
eta isomer in solution and hence in the crystal is increased. An assessment
is made of the degree of incorporation of the beta isomer into the crystal
, its distribution and its influence on the defect structure of the materia
l.