Physical stabilisation of amorphous ketoconazole in solid dispersions withpolyvinylpyrrolidone K25

Citation
G. Van Den Mooter et al., Physical stabilisation of amorphous ketoconazole in solid dispersions withpolyvinylpyrrolidone K25, EUR J PH SC, 12(3), 2001, pp. 261-269
Citations number
12
Categorie Soggetti
Pharmacology & Toxicology
Journal title
EUROPEAN JOURNAL OF PHARMACEUTICAL SCIENCES
ISSN journal
09280987 → ACNP
Volume
12
Issue
3
Year of publication
2001
Pages
261 - 269
Database
ISI
SICI code
0928-0987(200101)12:3<261:PSOAKI>2.0.ZU;2-V
Abstract
The glass forming properties of ketoconazole were investigated using differ ential scanning calorimetry (DSC), by quench cooling liquid ketoconazole fr om T-m+10 to 273.1 K, followed by subsequent heating at 5 K/min to T-m+10 K . It was shown that liquid ketoconazole forms a glass which did not recryst allise following reheating, indicating its stability; T-g was found to be 3 17.5+/-0.3 K. However, the presence of a small amount of crystalline ketoco nazole was able to convert the amorphous drug back to the crystalline state : the addition of only 4.1% (w/w) of crystalline material converted 77.1% o f the glass back to the crystalline state, and this value increased as the amount of added crystals increased. PVP K25 was found to be highly effectiv e in the prevention of such recrystallisation, but only if the amorphous dr ug was formulated in a solid dispersion, since physical mixing of amorphous ketoconazole with the polymer resulted in recrystallisation of the former compound. Storage of the solid dispersions for 30 days at 298.1 K (both 0 a nd 52% RH) in the presence or absence of crystals did not result in recryst allisation of the amorphous drug. Solid dispersions formed compatible blend s as one single T-g was observed, which gradually increased with increasing amounts of PVP K25, indicating the anti-plasticising property of the polym er. The values of T-g followed the Gordon-Taylor equation, indicating no si gnificant deviation from ideality and suggesting the absence of strong and specific drug-polymer interactions, which was further confirmed with C-13 N MR and FT-IR. It can be concluded therefore that the physical mechanism of the protective effect is not caused by drug-polymer interactions but due to the polymer anti-plasticising effect, thereby increasing the viscosity of the binary system and decreasing the diffusion of drug molecules necessary to form a lattice. (C) 2001 Elsevier Science B.V. All rights reserved.