The kinetics of drug release from hydrocolloid embeddings can largely
be described by the semi-empirical equation Q/Q(infinity) = k . t(n) b. Drug release ranges from diffusion control (highly viscous polymer
matrices) according to Higuchi's root t-law (n = 0.5) over anomalous
transport to zero order kinetics (erosion control, n = 1, plane surfac
e in both cases). The chain length of the hydrocolloid, the polymer co
ncentration and the nature of the added excipients also play a part in
the predomination of one mechanism. In general, dehydration leads to
a decrease in retardation. In order to explain the constant drug relea
se (erosion), one of three models can be consulted dependent on the so
lubility of the drug and the properties of the applied polymer. These
three models are the diffusion layer, the polymer dissolution and the
recently developed particle erosion model. In contrast to the matrix r
elease, all three erosion models have in common that the release is fa
irly independent of the properties of the drug. Low susceptibility of
the release to hydrodynamic stress is generally given with matrix rele
ase, or in the case of erosion control with particle erosion. Real Cas
e II (relaxation control) or Super Case II release seems unlikely with
hydrocolloid embeddings. For the differentiation and confirmation of
the release mechanism, swelling numbers (Deborah number, swelling inte
rface number, swelling area number) and the time dependence of the dif
fusion coefficients can additionally be consulted.