Development of hot-melt extrusion as a novel technique for the ...

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Fig. 8.5c: A plot of the cubic root of unreleased fraction of HCS from tablets as a function oftime according to the Hixson–Crowell model. Each result shows the mean±S.D. (n = 3).According to the Hixson–Crowell model plot which shows the relationship between thecubic root of the drug residual rate and time on the basis of Eq. (8.5) results are depicted inFig 8.5c. Hixson and Crowell showed that the law of cubic root is valid in uniform particles.This equation is based on the assumption that the release occurs only in the vertical directionrelative to the matrix surface, and that the release progresses with proportional decreases inall dimensions of the matrix, which maintains its shape [17] . Analyses were performed in theranges in which linearly was maintained with both tablets. The release from coated tabletswas not linear as the R 2 value was found to be (0.8829 - 0.8964). On the other hand, the HCSrelease from coated tablets according to the Hixson-Crowell model is quite linear throughoutthe whole test (R 2 = 0.9622 - 0.9838). According to the Hixson-Crowell theory of drugrelease it is presumed that the release progression has been maintained with the decreases inall dimensions of the matrix due to the applied coating on the tablet surfaces and thusmaintained the shapes of the tablets.165 | P a g e
Eq. (6) is a Korsmeyer–Peppas model equation concerning the diffusion mechanism,and it has been evaluated concerning pharmaceutical preparations of many matrix types.When both terms of Eq. (8.6) are converted to logarithms, the equation becomes ln F = lnK4+ n ln t, and the slope n can be determined by plotting the logarithm of the release rate againstthe logarithm of time (Fig. 8.5d).Fig. 8.5d: A plot of the logarithm of HCS released as a function of the logarithm of timeaccording to the Korsmeyer–Peppas model. Each result shows the mean±S.D. (n=3).The exponent (n) determined by this equation suggests that both the uncoated andcoated tablets show Fick‘s diffusion when n = 0.40-0.45 (for tablets). It has been reportedthat a non-Fickian type release which is also known as anomalous transport occurs only when0.45 < n < 0.89, case-II transport can be observed when n = 0.89, and super case-II transport166 | P a g e
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DECLARATION“I certify that this w
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taste masking effect of the process
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CHAPTER 2: DISSOLUTION ENHANCEMENT
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3.2 Powder and ODT characterization
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3.7 In vitro drug release profiles
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3.1 Solubility parameters and extru
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polymers.7.2 DSC findings of all AP
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2.4b Diffractograms of FMT formulat
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4.3 Schematic representation of the
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55 exrudates (b) DPD/L100-55 PM (c)
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8.5d A plot of the logarithm of HCS
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L100Eudragit L100L100-55 Eudragit L
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Maniruzzaman M, Rai D, Boateng JS.
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Maniruzzaman M, Boateng JS, Bonnefi
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CHAPTER 1: INTRODUCTION1.0 Backgrou
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Table 1.1: HME and other convention
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homogenize but also compress the ex
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properties of polymers and excipien
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particles‘ wettability [46] . A v
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Table 1.2: Different hot-melt extru
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1.8 Aims and objectivesThe purpose
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29. Zheng X, Yang R, Tang X and Zhe
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56. International Conference on Har
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CHAPTER 2: DISSOLUTION ENHANCEMENT
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Fdid ,Vi F2pip , p( Ehi/ ViVi )i =
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used. Each sample was scanned from
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Furthermore, by means of thermodyna
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3.2 Particle size morphology and pa
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Fig. 2.4a: Diffractograms of INM fo
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However, the DSC thermograms of the
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Fig. 2.5b: DSC thermograms of INM a
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Fig. 2.5e: DSC thermograms of FMT a
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Nevertheless, more than 80% FMT was
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6. Caron V, Tajber L, Corrigan OI,
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CHAPTER 3: DEVELOPMENT AND EVALUATI
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2.2 Hot-Melt extrusionHot-melt extr
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Committee of the University of Gree
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The PM of formulation II (40% IBU)
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Fig. 3.3: DSC thermograms of pure I
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As a general rule, the powder compr
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Fig. 3.4: Schematic diagram of ODT
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Fig. 3.5: Schematic diagram of ODTs
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Fig. 3.7: Schematic diagram of ODTs
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F2 0 0.5 0 1 0 1F6 0 0.5 0 1 0 2F7
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6. M.F. Al-Omran, S.A. Al-Suwayeh,
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30. L. Saerens, L. Dierickx, B. Len
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leading to significant variations w
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2.6. In vitro drug release studiesI
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v2d 2p(4.1)Table 4.1: Calculated so
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The observed melting peaks are shif
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Fig. 4.2a: Powder XRPD patterns of
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Interestingly, no difference was ob
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7 Astree sensors Taste masking effi
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The in vitro e-tongue evaluation wa
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3. K. Woertz, C. Tissen, P. Kleineb
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25. B.C. Hancock, P. York, R.C. Row
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CHAPTER 5: AN IN VIVO AND IN VITRO
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(dispersion forces and polarization
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Table 5.1: Sample preparation for t
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Table 5.2: Solubility parameters ca
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Physical mixtures (PM) and extruded
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Fig. 5.2c: Thermograms of CTZ and V
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masking effect for active concentra
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Fig. 5.5b: Distance and discriminat
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Table 5.4: Mean standard deviation
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Fig. 5.6b: Release profiles of VRP
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17. Woertz K,Tissen C, Kleinebudde
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scale or lower. XPS is more accurat
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patterns were identified after ener
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3.3 Differential scanning calorimet
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Fig. 6.3a: Diffractograms of PRP fo
Page 148 and 149: good agreement with the anticipated
Page 150 and 151: Since L100 contained higher proport
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Page 154 and 155: Finally, the XPS analysis confirmed
Page 156 and 157: Fig. 6.6b: 1 H NMR spectra of all P
Page 158 and 159: 6) Bonferoni, M.C.; Rossi, S.; Ferr
Page 160 and 161: 26) Vandencasteele, N.; Reniers, F.
Page 162 and 163: Gibbs free energy change before and
Page 164 and 165: 2.5 Hot-melt extrusion (HME) proces
Page 166 and 167: 2.11 X-ray photoelectron spectrosco
Page 168 and 169: Table 7.2: DSC findings of all APIs
Page 170 and 171: 3.4 In vivo and in vitro taste mask
Page 172 and 173: Fig. 7.3c: Normalised DI (%) of all
Page 174 and 175: Table 7.4: Binding energy calculati
Page 176 and 177: PRP/ polymers extruded in compariso
Page 178 and 179: atom as NH + 4 . This observed N 1s
Page 180 and 181: 8.0 ConclusionsThe presence of inte
Page 182 and 183: 20. Davies MC, Wilding IR, Short RD
Page 184 and 185: CHAPTER 8: SUSTAINED RELEASE HYDROC
Page 186 and 187: 2.3 Preparation of formulation blen
Page 188 and 189: medium pH was maintained as 1.2 by
Page 190 and 191: Fig. 8.1: SEM images of [(a), (b)]
Page 192 and 193: Fig. 8.2b: DSC transitions of HCS/E
Page 194 and 195: in the range of 10-12 kP. However,
Page 196 and 197: ate and time on the basis of Eq. (8
Page 200 and 201: when n > 0.89. From the results of
Page 202 and 203: 14. Lam PL, Lee KKH,Wong RSM, Cheng
Page 204 and 205: Furthermore, HME has successfully b
Page 206 and 207: Supp. Fig. 2: XPS O 1s peaks for PR
Page 208 and 209: Supp. Fig. 4: O 1s BE peaks for L10
Page 210 and 211: 8.2 s 6.2 s 3.8 s 1.8 s 200 msS
Page 212 and 213: 12.2 s 9.0 s 6.2 s 3.8 s 1.8 s
Page 214 and 215: Supplementary table 1: Solubility p
Page 216 and 217: N = 55000/ 219.2 = 250.912Density:
Page 218 and 219: (4) Eudragit L100, N = (125000/202
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