Dulcitol, known in a single crystalline form (hereafter called I), in
fact exhibits complex thermal behaviour. A second polymorph II appears
when the glassy material is allowed to crystallize at room temperatur
e. This form always coexists with I and cannot be well characterized.
The mixture I + II transforms very slowly to pure I when annealed at r
oom temperature for a week. When a melt of dulcitol is cooled very slo
wly vitrification does not occur and a new pure crystalline form III i
s obtained. Analysis of X-ray powder data leads to a possible monoclin
ic cell with a = 8.82 angstrom, b = 11.41 angstrom, c = 8.61 angstrom,
beta = 110.55-degrees, Dx = 1.49, Z = 4. These parameters are very cl
ose to those of I but the slightly smaller values for a and b could in
dicate a shrinking of some bonds in the molecular packing. Each of the
two forms II (mixed with I) and pure III are thermodynamically unstab
le. The ''normal'' form I is always obtained by evaporation from metha
nol/water solutions.