chapter i: introduction

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advantages over oral drug delivery system such as avoiding first pass metabolism, ... Mostly the pouch is filled with liquid or semisolid type of drug formulation.
CHAPTER I: INTRODUCTION 1.1

Overview of Transdermal Drug Delivery System: Transdermal Drug Delivery System (TDDS) a novel drug delivery system is the dosage

form to deliver therapeutically active compound to the body through the skin. TDDS has a lot of advantages over oral drug delivery system such as avoiding first pass metabolism, increase therapeutic efficacy, self-administration, and controlled delivery of drug molecule over a longer period of time (such as 7 Days) to keep constant steady state plasma concentration. Due to its advantages over oral drug delivery, TDDS is becoming more promising choice of drug delivery system for new drug molecule. Currently, there are 35 approved products in the market for TDDS, which is producing $4.3 billion revenue. TDDS can provide controlled release of drug and also allowed continuous input and eliminate pulse entry in the systematic circulation.1 1.1.1

Advantages of TDDS:2,3

1. Avoid First Pass metabolism 2. Self-administration 3. Elude the fluctuation in drug plasma concentration level 4. Greater patient compliance due to elimination of multiple dosing regimen 5. Removal of patch at any time, due to side effects 6. Avoidance of GI incompatibility



1

7. Steady and optimum Plasma concentration obtained with reducing side effects 8. Enhance therapeutic efficacy and patient compliance. 1.1.2

Type of TDDS:4,5

1) Reservoir type of TDDS: The reservoir TDDS system has drug reservoir embedded in the pouch system. This pouch system has release liner on one side and backing membrane on the other side. Mostly the pouch is filled with liquid or semisolid type of drug formulation. The reservoir form of TDDS has an adhesive layer on peripheral of the patch system or the adhesive can be embedded in the patch system. (Fig.1.1) 2) Matrix type of TDDS: Matrix type of TDDS is further divided in two types a) Drug in Adhesive and b) Drug Matrix in Adhesive. Drug is suspended or solubilized in adhesive itself and coated on the backing layer, called Drug in Adhesive type TDDS. Here the polymer itself act as an adhesive, so there is no need for extra adhesive layer for affixing patch on to the skin. In Drug Matrix in adhesive type of TDDS, drug is solubilized or suspended in polymer. Here the polymer is not adhesive in nature and to affix the patch on the skin another layer of adhesive is applied on the polymer drug matrix patch. (Fig. 1.1) 1.1.3

Basic Components of TDDS:6

1. Polymer 2. Drug 3. Solubilizer/plasticizer 4. Permeability Enhancers

2

5. Pressure sensitive Adhesive 6. Backing laminate 7. Release liner

Fig. 1.1 Different Types of Transdermal Patches7

3

1.1.4

Diffusion Process in TDDS

TDDS is follow the passive diffusion process to transport drug molecules from TDDS system (Having high concentration of drug) to systematic circulation (low concentration of drug). There are two diffusion process is going on in the TDDS system. 1) Diffusion through the polymer and 2) Diffusion through the skin. 1) Diffusion through the polymer: Diffusion through polymer solutions and gels have been studied for decades by the use of various techniques such as gravimetry8, membrane permeation9, fluorescence10 and dynamic light scattering11. The studies have resulted in a better knowledge on polymer morphology and structure12, transport phenomena13 and recently the controlled release of drug from polymers. In addition, these studies have led to theoretical description of the diffusion of solvent and/or solutes in polymer solution and gels.14-16 There are numerous models have been proposed till now based on various theories such as the obstruction effects, the hydrodynamic interaction and the free volume theory17. (Fig.1.2)

Fig. 1.2: Polymer-Drug Interaction



4

2) Diffusion through Skin: It is a valid generalization to state that the stratum corneum allows no substance to penetrate easily and allows all substance to enter slightly. According to structure of the skin, the drugs are possibly traveled through the following pathway to reach the systemic circulation. 1) The appendages (Shunt Pathway): a) Hair follicles, b) Sebaceous gland and, 2) Transepidermal penetration: a) Transcellular route, b) Intercellular route. The penetration through appendages pathway mainly depends on following factors: 1) No. of horny cell layers available and b) Thickness of the horny layer. Lipid soluble compounds diffuse through the sebum filled follicles, in which sebum might be worked as a vehicle for lipophilic drugs which has high affinity, resulting in high partitioning coefficient for release into the skin. Sweat ducts comprise a tiny fraction of the surface and cannot play an important role in lipophilic drug flux profile but certain water soluble electrolytes and drugs can freely enter into the skin through water filled sweat channels. The transepidermal penetration is mainly achieved by either transcellular or intercellular pathway. Most of the lipophilic drugs travel through either of these routes. Fig.1.3 showed the different drug penetration pathway in the skin.18,19



5

Fig. 1.3: Stratum Corneum and Route of Penetration. 1.1.5

Thermodynamics of Skin Permeation The mechanism of skin permeation of water soluble and lipid soluble non-electrolytes are

demonstrated by means of thermodynamic parameters, such as, activation energy (Ea), preexposed factor (A-), enthalpy (H) and entropy (S). 20 1.1.5.1 Activation energy of Skin Permeation The skin permeation of non-electrolytes, such as alkanols was reported to be an energy requiring process and follow the Arrhenius relationship: )*

𝐽𝑠𝑠 = 𝐴𝑒 ((+,)



(1)

6

For hydrophilic alkanols (C5), the activation energy is constant and 16.5 ± 0.1 kcal/mol is required for their permeation through hydrated stratum corneum. On the other hand, for the lipophilic alkanols (G”, and both independent of frequency; lower tan d values (G”) to a dominant elastic solid-like behavior (G”>G’). This cross over point is also called the sol-gel point or the characteristics modulus and can be used in gel rheology to correspond to the change of behavior from a more solid-like to liquid-like. The cross over point may be related to the interaction between particles. All the formulations are same except permeability enhancers (carbon chain length in



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fatty acids), it means particle interaction is different for all formulation and give different sol-gel point for different permeability enhancers. Fig. 3.11 showed complex modulus (G*) vs. temperature profile for formulation; this can be used to predict the storage stability of different formulations. FO-25_T0 showed minimum changes in complex modulus and also phase angle remains high during storage period (Fig. 3.11-D). This indicates FO-25_T0 has a stable shelf life as observed. Other formulations are more sensitive to temperature change, which indicates a shorter shelf life than that of FO-25_T0. The higher the gelling temperature at a given formulation can be explained by the collision probability of polymer chains is higher even at high temperature thereby increasing the probability of polymer solvent interaction and thus network formation and gelation at higher temperature. Difference in gel points may be used to explain the relative rate of breaking. The gel point is the change from liquid to solid like behavior. The lower the gel point, the shorter the breaking time may be needed under the same conditions. For the different fatty acids, the temperature sweep test can be used to rank the time of breaking between different formulations and can be used as a consistency test. Table 3.12 shows an example of using the gel point to evaluate the breaking time of formulations having different permeability enhancers, storage time and homogenization speed. The temperature sweep test can be used as a predictive tool for a gel breaking.130



100

(A)

45

T0

T1

T2

Cross-Over Temperature (C)

40 35 30 25 20 15 10 5 0 FO-25

FL-25

FC-25

FT-25

FLAB-25

FLG90-25

F-25

Permeability Enhancers

(B)

70

25000

20000

15000

Cross-Over Temperatue (C)

60 50 40 30 20 10 0 FO

FL

FC

FT

FLAB

Permeability Enhancers



101

FLG90

F

(C)

50

T0

T1

T2

Cross-Over Temperature (C)

45 40 35 30 25 20 15 10 5 0 25000

20000

15000

Homoginization Speed (RPM)

F-25_T0 (D)

70 60

Modulsu (Pa)

50 40 30

G'

20

G"

10 0 0

10

20

30

40

50

60

70

80

90

Temperature (C)

Fig: 3.9: (A) Effect of Storage period and Permeability enhancers on the Cross-Over Temperature, (B) Effect of homogenization speed and Permeability enhancers on the CrossOver Temperature, (C) Effect of storage period and homogenization speed on the CrossOver Temperature, (D) Representative graph of Temperature Sweep.



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Table 3.12: Cross Over Temperature (Modulus) of Formulations

Formulation



Cross-Over Temperature (°C) (Modulus Pa) T0

T1

T2

FO-25

30.1 (13.8)

37.6 (18.8)

36.6 (19.4)

FL-25

32.7 (15.1)

36.5 (16.8)

35.4 (18.5)

FC-25

27.5 (13.6)

34.8 (19.7)

33.4 (19.0)

FT-25

40.1 (14.8)

32.5 (17.1)

34.3 (18.3)

FLAB-25

38.5 (15.7)

34.3 (17.0)

38.4 (18.2)

FLG90-25

30.2 (13.9)

41.3 (19.2)

37.9 (22.5)

F-25

37.9 (18.5)

37 (19.1)

35.9 (24.6)

FO-20

28.4 (13.6)

43.7 (19.1)

FL-20

54.7 (14.0)

29.7 (13.4)

36.1 (17.0)

FC-20

33.4 (13.9)

35.5 (15.8)

43.5 (20.3)

FT-20

49.9 (13.0)

25.9 (13.8)

60.6 (31)

FLAB-20

46.3 (18.5)

31.7 (14.6)

43.2 (20.9)

FLG90-20

24.7 (12.6)

34.8 (16.8)

39.3 (17.8)

F-20

29.4 (14.9)

41.6 (19.8)

46.0 (23.3)

FO-15

28.3 (12.8)

36.8 (16.6)

37.2 (18.2)

FL-15

39.8 (11.9)

30.1 (14.7)

38.8 (22.9)

FC-15

28.4 (13.1)

32.1 (15.7)

34.1 (17.3)

FT-15

59.5 (10.9)

23.1 (13.3)

33.6 (24.3)

FLAB-15

32.1 (12.9)

35.2 (14.7)

38.3 (21.2)

FLG90-15

27 (11.6)

32.3 (14)

26.9 (41.4)

F-15

40.8 (18.3)

39.6 (18.4)

41.3 (26.8)

103

(A)

T0

T1

T2

Temperature Loop Area (Pa/C)

600 500 400 300 200 100 0 FO-25

FL-25

FC-25

FT-25

FLAB-25

FLG90-25

F-25

Permeability Enhancers

(B)

25000

700

20000

15000

Temperature Loop Area (Pa/C)

600 500 400 300 200 100 0 FO

FL

FC

FT

FLAB

Permeability Enhancers



104

FLG90

F

(C)

25000

Temperature Loop Area (Pa/C)

450

20000

15000

400 350 300 250 200 150 100 50 0 T0

T1

T2

Storage Period (Days)

F-25_T0

90

Complex Modulus (Pa)

80 70 60 50 40 30 20 10 0 0

10

20

30

40

50

60

70

80

90

Temperature (C)

Fig: 3.10: (A) Effect of Storage period and Permeability enhancers on the Temperature Loop Area, (B) Effect of homogenization speed and Permeability enhancers on the Temperature Loop Area, (C) Effect of storage period and homogenization speed on the Temperature Loop Area, (D) Representative graph of Temperature Ramp.

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Table 3.13: Temperature Loop Area of Formulations

Temperature Loop Area (Pa/°C)

Formulation



T0

T1

T2

FO-25

215.91

194.61

147.66

FL-25

330.32

47.04

58.13

FC-25

337.6

194.51

153.84

FT-25

412.15

144.61

138.91

FLAB-25

480.65

228.06

31.31

FLG90-25

247.92

99.56

54.13

F-25

389.04

258.33

13.13

FO-20

204.99

117.18

1160.52

FL-20

316.85

197.93

711.69

FC-20

356.5

125.1

87.83

FT-20

418.84

196.99

517.49

FLAB-20

643.44

245.95

6.28

FLG90-20

222.87

130.16

459.66

F-20

428.04

215.08

62.33

FO-15

329.41

146.24

101.18

FL-15

344.49

124.94

248.5

FC-15

349.88

211.81

212.81

FT-15

455.47

96.33

60.81

FLAB-15

534.89

208.83

48.69

FLG90-15

271.80

164.93

152.38

F-15

424.22

206.28

139.28

106

(A) 80 FO-25_T0

Complex Modulus (G* Pa)

70 60

F-25_T0

50

FO-20_T0

40 F-20_T0

30

FO-15_T0

20 10

F-15_T0

0 0

10

20

30

40

50

60

70

80

90

Temperature (C)

(B) FO-20_T0

Complex Modulus (G* Pa)

80 70

FL-20_T0

60

FC-20_T0

50

FT-20_T0

40

FLAB-20_T0

30 FLG90-20_T0

20

F-20_T0

10 0 0

10

20

30

40

50

Temperature (C)



107

60

70

80

90

(C) 120

Complex Modulus (G* Pa)

100 80

FO-15_T0 F-15_T0

60

FO-15_T1 F-15_T1

40

FO-15_T2 20

F-15_T2

0 0

10

20

30

40

50

60

70

80

90

Temperature (C)

Fig. 3.11: Effect of Homogenization Speed (A), Permeability Enhancers (B) and Storage Period (C) on the complex modulus (G*) during Temperature sweep. 3.8

Diffusion study A modified Franz-diffusion cells were used in our studies, in which drug leaves an unstirred

donor compartment, crosses through a membrane of thickness h and cross sectional area A, and accumulates in a stirred receiver compartment for which sink conditions were maintained. For this type of steady-state diffusion, we can use Fick’s First law, which is as follows: 131,132 𝐽=

tG

(33)

u∗tw

Where, J = Flux (µg cm-2 hr-1)



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A= Cross sectional area of membrane (cm2) tG tw

=Amt of drug permeated vs. time (µg/hr.)

From, experimental point of view, the flux can be calculated by utilizing equation 34,

J=

Slope

(34)

Diffuison area

Where, Slope = resultant slope of

tG tw

vs. time

Diffusion area = A = 1.77 cm2 The movements of the diffusing particles are dependent on the concentration gradient i.e. tV tH

across the membrane. So, we can write above equation as follows. z{

J = −D( )

(35)

z|

Where D= Diffusion Coefficient of a penetrant (cm2/hr) tV tH

= concentration gradient.

If a cellulose membrane/Human cadaver skin separates the two compartments of a diffusion cell with cross section area A and thickness h, and if the concentration in the membrane on the donor and on the receptor sides are C1 and C2 respectively than equation 1 and 3 can be combined and re-written as follows:

J=



z} ~∗z•

= D

{P({W €

109

(36)

The concentrations C1 and C2 within the membrane ordinarily are not known but can be replaced by the partition coefficient multiplied by the concentration Cd on the donor side or Cr on the receiver side, which is given by as follows: {P

K =

=

{z

{W

(37)

{‚

So, we can write equation 36 and 37, z}

= DAK

z•

{z({‚

(38)



We maintain the sink conditions in receptor medium throughout the experiment, and so Cd>>>Cr, from that it was assuming Cr≈ 0 Hence, equation 38 is re-written to, tG tw

=

„u…V𝑑 †

= 𝑃𝐴𝐶𝑑

(39)

Where,

𝑃=

…„

(40)



So,

P=

dM

1

Adt

Cd

(41)

Form equation 33 and 39,

P=

Jss

(42)

Cd

110

The Diffusion Coefficient was calculated from the slope obtained by plotting amount of drug permeated as a function of square root of time. The formula used to calculate diffusion coefficient is as follows:132

D=Πx

Slope

2

(43)

2

4 x A x C02

Where, A = cross section area of membrane (1.77 cm2) C0 = concentration in donor compartment (µg/ml) Slope = resultant slope of amount permeated vs. square root of time Moreover, we calculated the lag time (tLag) by plotting the amt release vs. time graph. Here we calculated the tLag from the diffusion coefficient found from the equation 44,

tLag =

h2

(44)

6D

Also lag time can be calculated using the permeability coefficient according to equation 45,

tLag =

h

(45)

6P

Where, tLag = lag time (hr) h = Thickness of the membrane (cm) D = Diffusion coefficient (cm2/hr) P = Permeability coefficient (cm/hr)



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3.8.1

Diffusion through Human Cadaver skin Based on the previous experience, different fatty acids and other well-known permeability

enhancing agents were opted as permeability enhancers; these contain C10, C12, and C18 carbon chain in their structure. Such as Oleic acid (C18), Lauric acid (C12), Capric acid (C10), TranscutolP, Labrasol, Luroglycol-90. Earlier, the human cadaver skin was removed from the -80 °C of temperature and immediately put in phosphate buffer saline of pH 7.4. It was kept in the saline for about an hour to properly hydrate. The receptor compartment was filled with 100% phosphate buffer saline with 0.01% sodium azide and kept it for an hour to achieve 32 °C temperature of the receptor medium. In this case, samples were withdrawn at time interval of 1, 2, 4, 6, 8, 10, 12, 24, 36, 48, 60 and 72 hrs. Every time 0.5 ml of sample was withdrawn from the receptor medium and replaced by same amount of 100% PBS with 0.01% sodium azide solution. Samples were analyzed by HPLC at 230 nm wavelength. Every time the thickness of the skin was measured using vernule calepuse, and it was observed 0.30 ± 0.02 mm. In addition, by decreasing the carbon chain of enhancer the permeation of ECO was increased. This behavior can be due to more polar molecules of enhancers available to interact with the lipid of SC. All the data is the average of the three experiments. All physicochemical parameters such as Flux (J), permeability coefficient (P), diffusion coefficient (D), were calculated from equation 34, 40 and 43 respectively. 3.8.2

Effect of Enhancers: The data presented in Table 3.14 and Fig. 3.12, 3.13, with different permeation enhancers

in gel formulation (5% ECO + 1% Klucel-HF) were experimented with human cadaver skin, the best results were obtained with Capric acid (8%) and Lauric acid (8%). Capric acid is C10 saturated

112

fatty acid. As can be seen in Table 3.14 and Fig. 3.12, 3.13, the flux of ECO is increasing with decreasing the carbon chain length of fatty acids. This can be clarified by following mechanisms. Capric acid is hydrophilic as compare to other higher carbon chain containing fatty acids. Previous publication showed that capric acid is more soluble in polar solvents as compare to other hydrophobic fatty acids. Furthermore, PG with capric acid showed higher permeability as compare to other fatty acids.56,57 Capric acid is a hydrophilic fatty acid. Data illustrated that it has very small lag time as compare to the other permeability enhancers. During the uptake process, decanoic acid seems to increase transcellular permeability by perturbing membrane lipid, their disordering potency increasing with chain length. In addition, the sodium salt of fatty acids forms micelles in aqueous solution. The critical micelle concentration (CMC) of these systems decreases with increasing chain length. Above the CMC, increases in the absorption enhancing effect with increasing concentration of free enhancers. 133,134,135



113

(A)

250

T0

T1

T2

Flux (ug/cm2/Hr)

200

150

100

50

0 FO-25

FL-25

FC-25

FT-25

FLAB-25

FLG90-25

F-25

Permeability Enhancers

(B)

250

25000

20000

15000

FLux (ug/cm2/Hr)

200

150

100

50

0 FO

FL

FC

FT

FLAB

Permeability Enhancers



114

FLG90

F

(c)

6

25000

20000

15000

Flux (ug/cm2/Hr)

5 4 3 2 1 0 T0

T1

T2

Storage Period (Days)

Fig: 3.12: (A) Effect of Storage period and Permeability enhancers on the Flux Profile, (B) Effect of homogenization speed and Permeability enhancers on the Flux Profile, (C) Effect of storage period and homogenization speed on the Flux Profile,

(A)

Cumulative Amt of ECO/are (ug/cm2)

10000 9000 8000 7000

FC-25_T0

6000

FLAB-25_T0

5000

FL-25_T0

4000

FLG90-25_T0

3000

F-25_T0

2000

FO-25_T0

1000

FT-25_T0

0 0



10

20

30 40 Time (Hr)

115

50

60

70

Cumulative Amt of ECO/area (ug/cm2)

(B)

10000 9000 8000

FC-20_T0

7000

FLAB-20_T0

6000 5000

FL-20_T0

4000

FLG90-20_T0

3000

F-20_T0

2000

FO-20_T0

1000

FT-20_T0

0 0

10

20

30

40

50

60

70

Time (Hr)

(C)

Cumulative Amt of ECO/area (ug/cm2)

7000 6000

FC-15_T0

5000

FLAB-15_T0

4000

FL-15_T0 3000

FLG90-15_T0

2000

F-15_T0

1000

FO-15_T0 FT-15_T0

0 0

10

20

30

40

50

60

70

Time (Hr)

Fig: 3.13: Cumulative amount of ECO permeated through Human cadaver skin vs Time profile for formulations prepared at 25000 RPM (A), 20000 RPM (B) and 15000 RPM (C) for different enhancers.



116

Table 3.14: Flux Profile of Formulations (n=3) Flux (µg/cm2/hr) ± S.D. Formulation



T0

T1

T2

FO-25

23.17 ± 4.66

12.05 ± 3.79

11.44 ± 0.58

FL-25

185.6 ± 4.70

184.05 ± 5.51

167.87 ± 22.68

FC-25

205.58 ± 5.17

183.04 ± 4.23

181.76 ± 11.75

FT-25

34.57 ± 21.73

2.35 ± 2.95

1.97 ± 1.59

FLAB-25

4.19 ± 1.80

2.13 ± 0.5

0.52 ± 0.37

FLG90-25

59.16 ± 5.86

29.09 ± 20.06

25.77 ± 4.68

F-25

5.06 ± 2.27

2.29 ± 0.65

2.25 ± 0.60

FO-20

9.34 ± 3.59

6.86 ± 1.99

6.31 ± 2.17

FL-20

164.43 ± 25.0

161.52 ± 15.61

141.26 ± 16.81

FC-20

193.55 ± 7.28

188.2 ± 20.99

184.35 ± 16.62

FT-20

0.95 ± 1.06

0.45 ± 0.23

0.33 ± 0.09

FLAB-20

4.93 ± 4.51

0.5 ± 0.27

0.41 ± 0.25

FLG90-20

49.34 ± 26.09

29.03 ± 17.96

16.51 ± 4.70

F-20

1.91 ± 2.67

1.49 ± 0.76

0.84 ± 0.97

FO-15

8.18 ± 6.55

6.79 ± 3.0

4.02 ± 1.44

FL-15

132.05 ± 25.95

130.15 ± 34.95

92.12 ± 18.92

FC-15

179.66 ± 32.43

174.95 ± 23.30

131.55 ± 33.08

FT-15

0.25 ± 0.11

0.18 ± 0.19

0.12 ± 0.02

FLAB-15

1.4 ± 0.06

1.07 ± 1.27

0.49 ± 0.09

FLG90-15

38.13 ± 15.13

31.43 ± 6.99

8.2 ± 5.19

F-15

1.29 ± 0.94

1.12 ± 1.42

0.26 ± 0.11

117

CHAPTER IV 4.0

Conclusion Scale-up process for Transdermal formulations are very difficult. Rheological studies of

Transdermal formulations can help to solve some challenges during manufacturing scale-ups. During QbD principle application, homogenizations speed comes under critical process parameters (CPP), while diffusion and storage period is called critical quality attributes (CQA). Throughout the research, we had tried to see the effect of CPP and CQA on the rheological properties of the gel formulations. Furthermore, It is well-known that transdermal drug release is specially based on the diffusion process of drug molecules into the formulation components. And rheological properties affect the diffusion process of the drug molecules, Such as Viscosity inversely proportional to the diffusion co-efficient. Here, we tried to evaluate the mechanical properties of the transdermal gels in the presence of the permeability enhancers and also at different storage period and mixing speed. Rheological studies of the gels showed that permeability enhancers, processing parameters and storage period was affecting the microstructure systems organized in the gels. Moreover, the microstructure of the polymers also affected the diffusion process of the drug. During In-vitro study, ECO was diffusing from polymer entangled system and also from the skin membrane. As the cohesive energy of the gel system increased the diffusion of drug in polymer entangled system was decreased and the flux of ECO also decreased. Increase of cohesive energy demonstrated that the interaction of polymer-drug, or polymerenhancer was increased and it required higher amount of energy to break the bonds. Furthermore, temperature sweep data also validated this assumption by decreasing in loop area during temperature cycle and also increased the cross over point of G’ and G”. Oleic acids exhibited very stable microstructure as compare to other fatty acids. These rheological studies indicated that



118

knowledge of rheological properties during product development can be helpful during storage stability profiling and selecting processing parameters for manufacturing scale. Application of Time Temperature Superposition was helpful to evaluate the thermorhelogical properties of the transdermal gels. It was found that all the transdermal gels prepared at different mixing speed or with different permeability enhancers were thermorheologically simple and can apply TTS principle. TTS principle was useful to evaluate the thermal properties of final formulations such as glass transition temperature, thermal expansion co-efficient and fraction volume free volume of the formulations. It is very difficult to measure the glass transition temperature of formulation using DSC or any other techniques. Using frequency sweep, we can measure the modulus at different temperature and then by applying TTS principle, we can extend the frequency range using polymer free volume theory. Moreover, It can help us to evaluate the viscoelasticity of the formulation at different time periods.



119

CHAPTER V: REFRENCES 1.

Chhetri A., and Kumar Dey B., “An Overview on Transdermal Drug Delivery”, Indo American Journal of Pharmaceutical Research, 2016, 6(7), 6073-6091

2.

El-Kattan A., Asbill C., and Haidar S., “Transdermal Testing: Practical Aspects and Methods”, PSTT, 2000, 3(12), 426-430

3.

Yeoh T., “Master Class Designing Non-Invasive Skin Mediated Therapies II”, [2016], [August], [5], [Paramus], [NJ]

4.

Bathe R., Kapoor R., “Transdermal drug delivery system: formulation, development and evaluation- An overview”, International Journal of Biomedical and Advance Research, 2015, 6(1), 1-10

5.

Ashok kumar J., Pullakandam N., Prabu S. L., and Gopal V., “Transdermal Drug Delivery System: An Overview”, International Journal of Pharmaceutical Sceience Review and Research, 2010, 3(2), 49-54

6.

Kadam A.S., Ratanaparkhi M.P., and Chaudhary S.P., “Transdermal Drug Delivery: An Overview”, International Journal of Research and Development in Pharmacy and Life Sciences, 2014, 3(4), 1042-1053

7.

Padula C., Nicoli S., Aversa V., Colombo P., Falson F., Pirot F., Santi P., “Bioadhesive Film for Dermal and Transdermal Drug Delivery”, European Journal of Dermatology, 2007, 17(4), 309-312

8.

Hu G.S.W., Chou K.J.N., “Kinetics of water swelling and development of porous structure in ionic poly(acrylonitrile-acrylamide-acrylic acid) hydrogels”, Polymer, 1996, 37(6), 1019-1025



120

9.

Smith B.A.H., and Sefton M.V., “Permeability of a heparin-polyvinyl alcohol hydrogel to thrombin and antithrombin III”, Journal of Biomedical Material Research, 1988, 22(8), 673-685

10.

Wisnudel M.B., and Torkelson J.M., “Small-Molecule Probe Diffusion in polymer solutions:

Studies

by

Taylor

Dispersion

and

Phosphorescence

Quenching”,

Macromolecules, 1996, 29(19), 6193-6207 11.

Van Asten A.C., Kok W.T., Tilssen R., and Poppe H., “Characterization of thermal diffusion of polystyrene in binary mixture of THF/dioxane and THF/cyclohexane” Journal of Polymer science Part B: Polymer Physics, 1996, 34(2), 283-295

12.

Korsmeyer R.W., and Peppas N.A., “Effect of the morphology of hydrophilic polymeric matrices on the diffusion and release of water soluble drugs”, Journal of Membrane Science, 1981, 9(3), 211-227

13.

Hariharan D., and Peppas N.A., “Modeling of water transport and solute release in physiologically sensitive gels”, Journal of Controlled Release, 1993,23(2), 123-135

14.

Fricke H., “A mathematical Treatment of the Electric Conductivity and Capacity of Disperse Systems I. The Electric Conductivity of a Suspension of Homogeneous Spheroids”, Physical Reviews, 1924, 24 575

15.

Cukier R.I., “Diffusion of Brownian Spheres in semidilute polymer solutions”, Macromolecules, 1984, 17(2), 252-255

16.

Fujita H., “Diffusion in Polymer-Diluent Systems”, Advances Polymer Science, 1961, 3(1), 1-47

17.

Amsden B., “Solute Diffusion with Hydrogels: An Examination of the retardation effect”, Polymer Gels and Networks, 1998, 6(1), 13-43



121

18.

Klingman A.M., “A biological brief on percutaneous absorption”, Drug Development and Industrial Pharmacy, 1983, 9(4), 521-560

19.

Wiechers J.W., “The barrier function of the skin in relation to percutaneous absorption of drugs”, PhareceutischWeekblad Sceintific edition, 1989, 11(6), 185-198

20.

Scheuplein R.J., and Blank I.H., “Permeability of the Skin”, Physiology Rev., 1971, 51, 702-747

21.

Davis A.F., and Hadgraft J., “Supersaturated solution as topical drug delivery systems”, Pharmaceutical Skin Penetration Enhancement, New York: Marcel Dekker, 1993, 243-267

22.

Hinterstoisser B., and Salmen L., “Application of dynamic 2D FTIR to cellulose”, Vibrational Spectroscopy, 2000, 22, 111-118

23.

Bochek A.M., “Effect of hydrogen bonding on cellulose solubility in aqueous and nonaqueous solvents”, Russian Journal of Applied Chemistry, 2003, 76(11), 1761-1770

24.

Hon D.N.S., and Shiraishi N., “Wood and cellulosic chemistry”, Marcel Dekker, Inc. New York 2001

25.

Hirren M., Chevillard C., Desbrieres J., Axelos M.A.V., and Rinaudo M., “Theromogelation of methylcellulose: new evidence for understanding the gelation mechanism”, Polymer, 1998, 39(25), 6251-6259

26.

Bochek A.M., Zobivalova N.M., Lavren’ev V.K., Lebedeva M.F., Sukhanova T.E., and Petropavlovaskii G.A., “Formation of physical thermal reversible gel in solution of methyl cellulose in water and dimethylacetamide and properties of films thereof”, Russian Journal of Applied Chemistry, 1978, 74(8), 1358-1363



122

27.

Takahashi M., and Shimazaki M., “Formation of junction zones in thermoreversible methylcellulose gels”, Journal of Polymer Science: Part B: Polymer Physics, 2001, 39, 943-946

28.

Kobayashi K., Huang C., and Lodge T.P., “Thermoreversible gelation of aqueous methylcellulose solutions”, Macromolecules, 1999, 32, 7070-7077

29.

Li L., Thangamathesvaran P.M., Yue C.Y., Tam K.C., Hu X., and Lam Y.C., “Gel network structure of methylcellulose in water”, Langmuir, 2001, 17, 8062-8068

30.

Sarkar N., “Kinetics of thermal gelation of methyl cellulose and hydroxypropyl cellulose in aqueous solutions”, Carbohydrate Polymers, 1995, 26, 195-203

31.

Li L., “Thermal gelation of methylcellulose in water: scaling and thermoreversibility”, Macromolecules, 2002, 35, 5990-5998

32.

Takahashi M., Shimazaki M., and Yamamoto J., “Thermoreversible gelation and phase separation in aqueous methyl cellulose solutions”, Journal of Polymer Science: Part B: Polymer Physics, 2001, 39, 91-100

33.

Desbrieres J., Hirrien M., and Ross-Murphy S.B., “Thermogelation of methyl cellulose: Rheological considerations”, Polymer, 2000, 41, 2451-2461

34.

Hirsch S.G., and Spontak R.J., “Temperature-dependent property development in hydrogels derived from hydroxypropyl cellulose”, Polymer, 2002, 43, 123-129

35.

Sarkar N., “Thermal gelation properties of methyl and hydroxypropylmethyl cellulose”, Journal of Applied Polymer Science, 1979, 24, 1073-1087

36.

Roschinski C., and Kulicke W.M., “Rheological characterization of aqueous hydroxypropyl cellulose solution close to phase separation”, Macromolecular Chemistry and Physics, 2000, 201(15), 2031-2040



123

37.

Satishkumar S., Chen S., and Etzler F., “Rheological characterization of hydroxypropyl cellulose gels”, Drug Development and Industrial Pharmacy, 1999, 25(3), 153-161

38.

Iiyina E., and Daragan V., “Self-diffusion of dimethyl sulfoxide and dimethylformamide in solutions and gels of cellulose acetate by pulsed field gradient NMR”. Macromolecules, 1994, 27, 3759-3763

39.

Vaessen D.M., McCormick A.V., and Francis L.F., “Effect of Phase separation on stress development in polymeric coating”, Polymer, 2002, 43, 2267-2277

40.

Reuvers A.J., Altena F.W., and Smolders C.A., “Demixing and gelation behavior of ternary cellulose acetate solutions”, Journal of Polymer Science: Part B: Polymer Physics, 1986, 24, 793-804

41.

Matsuyama H., Nishiguchi M., and Kitamura Y., “Phase separation mechanism during membrane formation by dry-cast process”, Journal of Applied Polymer Science, 2000, 77, 776-782

42.

Gennes P.G., “Scaling concept in polymer physics”, Cornell University Press, Ithaca, 1979

43.

Hamley I.W., “Introduction to soft matter”, John Wiley & Sons Ltd. Chichester, 2000

44.

Antonietti M., Bremser W., and Schmidt M., “Microgels: model polymers for the crosslinked state”, Macromolecules, 1990, 23, 3796-3805

45.

Lin Y.H., “Polymer Viscoelasticity: Basics, Molecular Theories and Experiments”, World Scientific, New Jersey, 2003

46.

Doi M., and Edwards S.F., “The Theory of Polymer Dynamics”, Clarendon Press, Oxford, 1986

47.

Finnin B.C., and Morgan T.M., “Transdermal penetration enhancers: Application, Limitations and Potential”, Journal of Pharmaceutical Science, 1999, 88(10), 955-958



124

48.

Pathan I.B., and Setty C.M., “Chemical penetration enhancers for Transdermal drug delivery system”, Tropical Journal of Pharmaceutical Research, 2009, 8(2), 173-179

49.

Walker R.B., and Smith E.W., “The role of Percutaneous penetration enhancers”, Advanced drug delivery Reviews, 1996, 18, 295-301

50.

Aungst B.J., “Structure/Effect studies of fatty acid Isomers as skin penetration enhancers and skin irritants”, Pharmaceutical Research, 1989, 6 (3), 244-247

51.

Sinha V.R., and Kaur M.P., “Permeation Enhancers for Transdermal Drug Delivery”, Drug Development and Industrial Pharmacy, 2000, 26(11), 1131-1140

52.

Green P.G., Guy R.H., and Hadgraft J., “In vitro and In vivo enhancement of skin permeation with oleic and lauric acids”, International Journal of Pharmaceutics, 1988, 48(1-3), 103-111

53.

Roy S.D., Roos E., and Sharma K., “Transdermal delivery of buprenorphine through cadaver skin”, Journal of Pharmaceutical Sciences, 1994, 83(2), 126-130

54.

Green P.G., and Hadgraft J., “Facilitated transfer of cationic drugs across a lipoidal membrane by oleic acid and lauric acid”, International Journal of Pharmaceutics, 1987, 37(3), 251-255

55.

Stott P.W., Williams A.C., and Barry B.W., “Mechanistic study into the enhanced transdermal permeation of a model b-blocker, propanol, by fatty acids: A melting point depression effect”, International Journal of Pharmaceutics, 2001, 219(1-2), 161-176

56.

Smith E.W., and Maibach H.I., “Percutaneous penetration enhancers”, CRC press, Inc., Boca Raton, FL, 1995, PP. 277-288

57.

Oh H., Oh Y., and Kim C., “Effects of vehicle and enhancers on transdermal drug delivery of melatonin”, International Journal of Pharmaceutics, 2001, 212, 63-71



125

58.

Gattefosse, “Lipid Excipients for Topical drug delivery”, Pharmaceutical Performance Powered by Gattefosse, 1-16

59.

Carreau P.J., Kee D.C.R., Chhabra R.P., “Rheology of Polymeric Systems: Principle and Applications”, Hanser Gardner Publication Inc., Cincinnati, 1997

60.

Rohn C.L., “Analytical Polymer Rheology: Structure-Property Relationships”, Hanser Gardner Publications, Inc., Cincinnati, 1995

61.

Macosko C.W., “Rheology Principles, Measurements and Applications”, Wiley VCH Publishers, Inc., New York, 1994

62.

Pai V.B., “Tailoring Biopolymers Using Enzymes: Interactions in XanthanGalactomannan Blends”, PhD Thesis, Chemical Engineering Department, North Carolina State University, Raleigh, NC 2001

63.

Barnes H.A., Hutton J.F., and Walters K., “An Introduction to Rheology”, Elsevier, New York 1989

64.

Ferry J.D., “Viscoelastic Properties of Polymers”, John Wiley, New York, 1980

65.

Bird R.B., Armstrong R.C., and Hassager O., “Dynamics of Polymeric Liquids”, Wiley, New York, 1987

66.

Li L., “Thermal gelation of methylcellulose in water: scaling and thermoreversibility” Macromolecules, 2002, 35, 5990-5998

67.

Goodwin J.W., and Hughes R.W., “Rheology for Chemist: An Introduction”, RSC Publishing, Cambridge, UK, 2000

68.

Tamburic S., and Craig D.Q.M., “An Investigation into the Rheological, dielectric and mucoadhesive properties of poly(acrylic acid) gel System”, Journal of Controlled Release, 1995, 37, 59-68



126

69.

Ji. Y., Kang W., Liu S., Yang R., and Fan H., “The relationship between rheological rules and cohesive energy of amphiphilic polymers with different hydrophobic group”, Journal of Polymer Research,2015, 22(3), 26

70.

Capodagli J, Lakes R, “Isothermal viscoelastic properties of PMMA and LDPE over 11 decades of Frequency and Time: A Test of Time-Temperature Superposition”, Rheological Acta, 2008, 47, 777-786

71.

Muhammed Anwar H., and Plakogiannis F. M., “Transdermal controlled delivery of an atypical psychotropic agent, Aripiprazole”, Long Island University, The Brooklyn center, 2011; 125 pages

72.

Campbell K, Malcolm RK, Russell JA and Woolfson AD, “Rheological Behavior of Pharmaceutical Gels, Suspensions and Eutectic Emulsion of Ibuprofen and Methyl Nicotine”, Poster presented at the 18th Pharmaceutical Technology Conference and Exhibition, Netherland, Volume 2: 210-203, 1999

73.

Eccleston GM, “The Microstructure of Semisolid Creams”, Pharmacy International, 7, 6370, 1986a

74.

The Pharmaceutical Codex, Principles and Practice of Pharmaceutics, 1994, Chapter on Rheology, Ed. Lund W. 12th edition, London: The Pharmaceutical Press. 260-276

75.

Eccleston GM, Barry BW and Davis SS, “Correlation of viscoelastic function for Pharmaceutical Semisolids: Comparison of Creep and Oscillatory Test for Oil-in-Water Creams Stabilized by Mixed Emulsifiers”, Journal of Pharmaceutical Science, 1973, 62(12), 1954-1961

76.

Ceulemans J and Ludwig A, “Evaluation of the Rheological and Mucoadhesive Properties of Various Polymers (Ionic and Non-Ionic) Intended to Use in Viscous Eye Drops”, Poster



127

presented at the 18th Pharmaceutical Technology Conference and Exhibition, Netherland, 1999, Volume 2: 350-365 77.

Patton TF and Robinson JR, “Ocular Evaluation of Polyvinyl Alcohol in Rabbits”, Journal of Pharmaceutical Sciences, 1975, 64(8), 1312-1316

78.

Herh P, Tkachuk J, Wu S, Bernzen M and Rudolph B, “The Rheology of Pharmaceutical and Cosmetic Semisolids”, American Laboratory, 1998, 30(10), 12-14

79.

Adeyeye MC, Jain AC, Ghorab MKM and Reilly WJ. 2002, “Viscoelastic Evaluation of Topical Creams containing Microcrystalline Cellulose/ Sodium Craboxymethyl Cellulose Stabilizer”, AAPS Pharmascitech, 2003, 3(2)

80.

Davis SS, “Viscoelastic Properties of Pharmaceutical Semisolids II: Creams”, Journal of Pharmaceutical Sciences, 1969, 58(4), 418-421

81.

Eccleston GM, “Application of Emulsion Stability Theories of Mobile and Semisolid O/W Emulsion”, Cosmetic and Toiletries, 1986b, 101(11), 73-93

82.

Nash RA, “Validation of Disperse Systems. In Pharmaceutical Dosage Forms: Disperse Systems, Ed. Leiberman HA, Rieger MM and Banker GS. Volume 3, New York: Marcel Dekker Inc. 479-512

83.

Tan YTF, Peh KK and Al-Hanbali O, “Effect of Carbopol and Polyvinylpyrrolidone on the Mechanical, Rheological and Release Properties of Bioadhesive Polyethylene Glycol Gels”, AAPS PharmSciTech, 2000, 1(3),

84.

Lawlor MS, Jones DS and Woolfson AD, “Analysis of Mechanical and Rheological Properties of Tetracycline-Containing Gels Composed of Poly (Methyl Vinyl Ether-Maleic Anhydride) and Polyvinylpyroolidone”, Poster presented at the 18th Pharmaceutical Technology Conference and Exhibition, Netherland, 1999, 1, 306-309



128

85.

Goggin PL, He R, Craig DQM and Gregory DP, “An Investigation into the Supramolecular Structure of Ternary Gel Systems Using Oscillatory Rheometry, Microscopy, and Low Frequency Dielectric Spectroscopy”, Journal of Pharmaceutical Sciences, 1999, 88(7), 661-669

86.

Kutschmann E,"Rheological Analysis of the Stability of Pharmaceutical Suspensions”, Manufacturing Chemist, 2003, 2, 50-51

87.

Rieger MM, “Stability Testing of Macroemulsions”, Cosmetic and Toiletries, 1991, 106(5), 59-69

88.

Gasperlin M, Tusar L, Tusar M, Kristl J and Smid-Korbar J, “Lipophilic Semisolid Emulsion Systems: Viscoelastic Behavior and Predication of Physical Stability by Neural Network”, International Journal of Pharmaceutics, 1998, 168, 243-254

89.

Krajisnik D and Milic J, “Polymer-Stabilized Emulsion Systems: Structural Characteristics and Physical Stability Evaluation”, Drug Development and Industrial Pharmacy, 2003, 29(6), 701-711

90.

More Solutions to Sticky Problems, A Guide to Getting More from your Brookfield Viscometer, 1999, Paper by Brookfield Engineering Laboratories, Inc. Middleboro, MA, USA

91.

Holland D, “Measuring and Interpreting the Rheological Properties of Cosmetic Products”, Applied Rheology, 1991, 1(2), 198-213

92.

Boylan JC, “Rheological Estimation of the Spreading Characteristics of Pharmaceutical Semisolids”, Journal of Pharmaceutical Sciences, 1967, 56(9), 1164-1169



129

93.

Barry BW and Grace AJ, “Sensory Testing of Spreadability: Investigation of Rheological Conditions Operative During Application of Topical Preparations”, Journal of Pharmaceutical Sciences, 1972, 61(3), 335-341

94.

Henderson NL, Meer PM and Kostenbauder HB, “Approximate Rates of Shear Encountered in Some Pharmaceutical Processes”, Journal of Pharmaceutical Sciences, 1961, 50(9), 788-791

95.

Simon TH, Dekay HG and Banker GS, “Effect of Processing on the Rheology of Thixotropic Suspension”, Journal of Pharmaceutical Sciences, 1961, 50(10), 880-885

96.

Wood JH, “Pharmaceutical Rheology, In The Theory and Practice of Industrial Pharmacy, Ed. Lachman L, Lieberman HA and Kanig JL, 3rd Edition, Philadelphia: Lea and Febiger, 123-145

97.

Barnes HA, “Thixotropy- A Review”, Journal of Non-Newtonian Fluid Mech., 1997, 70, 1-33

98.

Dolz M, Gonzalez F, Delegido J, Hernandez MJ, Pellicer J, “A Time-Dependent Expression for Thixotropic Areas. Application of Aerosil 200 Hydrogels”, Journal of Pharmaceutical Sciences, 2000, 89(6), 790-797

99.

Lee CH, Moturi V, Lee Y, “Thixotropic Property in Pharmaceutical Formulations”, Journal of Controlled Release, 2009, 136, 88-98

100.

Mamdouh T, Ghannam M, Esmail MN, “Rheological Properties of Carboxymethyl Cellulose”, Journal of Applied Polymer Science, 1997,64(2), 289-301

101.

Islam MT, Hornedo NR, Ciotti S, Ackermann C, “Rheological Characterization of Topical Carbomer Gels Neutralized to Different pH”, Pharmaceutical Research, 2004, 21(7), 11921199.



130

102.

Ross-Murphy S.B., “Rheological Characterization of Gels”, Journal of Texture Studies, 1995, 26, 391-400

103.

Tung C.Y.M., and Dynes P.J., “Gelation in Thermosetting Systems”, Journal of Applied Polymer Science, 1982, 27, 569-574

104.

Ramachandran

S,

Chen

S

and

Etzler

F,

“Rheological

Characterization

of

Hydroxypropylcellulose Gels”, Drug Development and Industrial Pharmacy, 1999, 25(2), 153-161 105.

Stading M., and Hermansson A.M., “Viscoelastic behavior of b-lactoglobulin Gel Structures”, Food Hydrocolloids, 1990, 4, 121-135

106.

Egelandsdal B., Fretheim K., and Harbitz O.J., “Dynamic Rheological measurement of heat induced myosin gels I: An evaluation of the method’s suitability for the filamentous gels”, Journal of the Science of Food and Agriculture, 1986, 37, 944-954

107.

Dufy J., “Measuring the Rheology of Polymer Solutions”, Malvern Instruments White Paper, 1-12

108.

TA Instruments, “Thermal Analysis Application Brief: Application of Time-Temperature Superposition Principle to DMA”, Thermal analysis and Rheology, Application Note

109.

M.T. Nickerson, A.T. Paulson, and R.A. Speers, “A Time-Temperature rheological approach for examining food polymer gelation”, Trends in Food Science & Technology, 2004, 15, 569-574

110.

Heymans Nicole, “Constitutive equation for polymer viscoelasticity derived from hierarchical models in cases of failure of Time-Temperature superposition”, Signal Processing, 2003, 83, 2345-2357



131

111.

Han, C.D., Kim J., and Kim J.K., “Determination of the order-disorder transition temperature of block copolymers”, Macromolecules, 1989, 383-394

112.

Macaubas P.H.P., and Demarquete N. R., “Time-Temperature superposition principle applicability for Blends Formed of Immiscible polymers”, Polymer engineering and Science, 2002, 42(7), 1509-1519

113.

Beck D.M., and Han C.D., “Rheological behavior of binary mixture of polystyrene-blockpolyisoprene copolymers in the disorder state”, Polymer, 1995, 36, 4833-4839

114.

Han C.D., and Jhon M.S., “Correlation of the first normal stress difference with shear stress and of the storage modulus with loss modulus for homopolymers”, Journal of Applied polymer science, 1986, 32, 3809-3840

115.

Han C.D., and Kim J.K., “On the use of Time-Temperature superposition in multicomponent/multiphase polymer systems”, Polymer, 1993, 34, 2533-2539

116.

O’cornell P.A., and McKenna G.B., “Large deformation response of polycarbonate: TimeTemperature, Time-aging time, and time-strain superposition”, Polymer Engineering Science, 1997, 37, 1485-1495

117.

Palade L.I., Verney V., and Attane P., “Time-Temperature superposition and linear viscoelasticity of polybutadienes”, Macromolecules, 1995, 28, 7051-7057

118.

Peleg M., “On the use of the WLF model in polymers and foods”, Critical Reviews in Food Science and Nutrition, 1992, 32, 59-66

119.

Williams M.L., Landel R.F., and Ferry J.D., “The temperature dependence of relaxation mechanisms in amorphous polymers and other glass-forming liquids”, Journal of American Chemical Society, 1955, 77, 3701-3707



132

120.

Van Wazer J.R., Lyons J.W., Kim K.Y., and Colwell R.E., “Viscosity and Flow measurements- A laboratory handbook of rheology”, 1963, New York, NY: Interscience Publisher

121.

Al-Ruqaie I.M., Kasapis S., Richardson R.K., and Mitchell G., “The glass transition zone in high solid pectin and gellan preparations”, Polymer, 1997, 38, 5685-5694

122.

Evageliou V., Kasapis S., Hember M.W.N., “Vitrification of k-carrageenan in the presence of high level of glucose syrup”, Polymer, 1998, 39, 3909-3917

123.

Whittaker L.E., Al-Ruqaie I.M., Kasapis S., and Richardson R.K., “Development of composite structure in gellan polysaccharide/sugar system”, Carbohydrate Polymers, 1997, 33, 39-46

124.

Deszcynski

M.,

Ksapis

S.,

MacNaughton

W.,

and

Mitchell

J.R.,

“High

sugar/polysaccharide glasses: Resolving the role of water molecules in structure formation”, International Journal of Biological Macromolecules, 2002, 30, 279-282 125.

Deszczynski M., Ksapis S., MacNaughton W., and Mitchell J.R., “Effect of sugar on the mechanical and thermal properties of agarose gels”, Food Hydrocolloids, 2003, 17, 793799

126.

Kasapis S., Al-Marhoobi I.M.A., and Khan A.J., “Viscous Solutions, network and the glass transition in high sugar galactomannan and k-carrageenan mixture”, International Journal of Biological Macromolecules, 2000, 27, 13-20

127.

Barnes H.A., “An Introduction to Rheology”, Elsevier Science publisher 1993, 3rd Edition

128.

Bohdanecky, M. & Kovar, J., “Viscosity of polymer solutions”, In polymer Kience Library (Vol. 2). Amsterdam: Elsevier. (1982)



133

129.

Lapasin, R., & Prici, S., “Rheology of polysaccharide systems. Rheology of industrial polysaccharides: Theory and application”, Glasgow: Blackie Academic and Professional. (1995)

130.

Huachun Z, Salomon D and Miliron E, “Using Rheological Properties to Evaluate Storage stability and Setting Behaviors of Emulsified Asphalts”, Idaho Asphalt Supply, Inc. White Paper, Idaho (USA) (2006)

131.

Martin A., Chun A. H. C., and Bustamante P.,” Physical Pharmacy: Physical chemical principles in the pharmaceutical sciences”, 4th Ed., Lea and Febiger, PA, 1993, PP 325-330

132.

Khalafi S., and Plakogiannis F. M., “Comparative in vitro diffusion study of Lovastatin Transdermal Delivery system”, Long Island University, The Brooklyn center, 2010; 87 pages AAT 1459568

133.

Aungst B.J., Rogers N.J., Shefter E., “Enhancement of naloxone penetration through human cadaver skin in vitro using fatty acids, fatty alcohols, surfactant, sulfoxides and amines”, International Journal of Pharmaceutics 33 (1986) 225-234

134.

Komata Y., Inaoka M., Kaneko A., Fujie T., “In vitro percutaneous absorption of thiamine disulfide from a mixture of propylene glycol and fatty acids”, Journal of Pharmaceutical Science 81 (1992) 744-746

135.

Parisi N., Paz-Alvarez M., Matts P.J., Lever R., Hadgraft J., and Lane M.E., “Topical delivery of hexamidine”, International Journal of Pharmaceutics 506 (2016) 332-339



134