The frequency and temperature dependence of the real (epsilon') and imagina
ry (epsilon ") parts of the dielectric constant of polycrystalline complex
beta-cyclodextrin-4-t-butylbenzyl alcohol [beta-CD.TERB.11.2H(2)O] and beta
-cyclodextrin [beta-CD 9.8H(2)O] and of the corresponding dried forms (beta
-CD. TERB.3.8H(2)O and beta-CD.2.4H(2)O, respectively) has been investigate
d, in the frequency range 0-100kHz and temperature range 130-350K. The diel
ectric behaviour is described well by Debye-type relaxation (alpha dispersi
on). All systems except for the beta-CD.TERB.3.8H(2)O, exhibit an additiona
l Omega dispersion at low frequencies, which usually is attributed to proto
n transport. In the non-dried samples the temperature dependence of epsilon
' and epsilon(max)(") exhibits two steps, whereas in the dried samples it e
xhibits only the low temperature step. The low temperature step is due to t
he tightly bound water molecules, whereas that at higher temperatures is du
e to easily removable water. The temperature dependence of epsilon " shows
a peak which has been attributed to a transition between ordered and disord
ered hydroxyl beta-CD groups, and water molecules. The relaxation time vari
es exponentially with temperature (in the range 8-12 mu sec), in a reverse
V like curve, with maximum values located at the corresponding: order-disor
der transition temperatures. Activation energies of the order of similar to
2.5 kJ mol(-1) are calculated for the transition in every sample. The diso
rder in the hydrogen bonding is equivalent to a system of two dipoles with
opposite directions, and the model of Frohlich can be applied to explain th
e order-disorder transition and the temperature dependence of the relaxatio
n time. An apparent negative activation energy before the transition temper
ature can be attributed to reorientation of the hydrogen bonding around the
cyclodextrin molecules, and it is related to endothermic drifts observed b
y calorimetric studies of beta-CD. The order-disorder transition can be pro
bed also from the phase shift component of the current passing through the
sample relative to the applied signal.