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Compacon equaon and its use in the determinaon of compressibility of pharmaceucal materials REFERENCES 1. Hausner, H. H. Fricon condions in a mass of metal powder, Int. J. Powder Metall. 3, 7-13 (1967). 2. Řehula, M. and Rysl, T. Characterizaon of microcrystalline celluloses by means of the parameters of a three-exponenal compression equaon. Ces. Slov. Farm. 57, 165-169 (2008). 3. Ondrejček, P.; Řehula, M.; Svačinová, P.; Stoniš, J. and Rabišková, M. The effect of a new glidant Syloid on pressing of drug tablets. Chem. Listy. 108, 687-693 (2014). 4. Cooper, A. R. and Eaton, L. E., Compacon behavior of several ceramic powders. J. Am. Ceram. Soc. 45, 97-101 (1962). 5. Fell, J. T. and Newton, J. M. Determinaon of tablet strength by the diametral-compression test. J. Pharm. Sci. 59, 688-691 (1970). 6. Führer, C. Substance behaviour in direct compression. Labo-Pharma Probl. Tech. 46, 759-762 (1977). 7. Obae, K.; Iijima, H. and Imada, K. Morphological effect of microcrystalline cellulose parcles on tablet tensile strength. Int. J. Pharm. 182, 155-164 (1999). 8. Eriksson, M. and Alderborn, G. The effect of parcle fragmentaon and deformaon on the interparculate bond formaon process during powder compacon. Pharm. Res. 12, 1031-1039 (1995). P. Ondrejček, P. Svačinová, B. Vraníková, O. Holas, M. Rabišková, Z. Šklubalová Department of Pharmaceucal Technology, Charles University in Prague, Faculty of Pharmacy in Hradec Králové, Heyrovského 1203, 500 05 Hradec Králové, Czech Republic INTRODUCTION Tablets are dosage forms made by a compression of the same powdered mixture volumes of one or more acve ingredients and excipients. This work studies the flow and compressibility properes of three pharmaceucal excipients. The compressibility of used materials is evaluated using the three exponenal compacon equaon. MATERIALS Microcrystalline cellulose (MCC, Comprecel 102, Mingtai Chemical) lactose monohydrate (LAC, Spherolac 100, Meggle), and calcium phosphate anhydrate (DC, DI-CAFOS A150, Budenheim) were used as fillers. The parcle size of the used materials was esmated using the opcal microscope (Olympus BX51) at 10x magnificaon. The median parcle size (x 50 ) was expressed automacally. METHODS Flow properes measurement Moisture analyzer (Precisa XM60) was used for the evaluaon of loss on drying at 105 °C. According to the European Pharmacopoeia, the bulk density of used materials was determined using the Sco’s Volumeter (Copley Scienfic). Tapped density meter (Erweka SVM 102) was used for the evaluaon of Hausner rao (HR). 1 To determinate the angle of repose α (°) and the mass flow rate ṁ (g/s) of excipients, the granulate and powder flow tester (Erweka GT) with the 200 ml stainless steel conical hopper and a 10 mm outlet nozzle was used. The average of ten measurements with the standard deviaon (SD) is shown in Table 1. Tablet preparaon Material tesng instrument (Zwick/Roell T1 FRO 50; Fig 1) was used for the preparaon of tablets with the mass of 500 mg and 13 mm in diameter. Tablets used for the evaluaon of compacon process were made using the compacon force of 40 kN. The radial strength was evaluated in tablets compacted at the force of 10 kN. The compacon process was evaluated using the three-exponenal equaon (1). 2,3 Where V is the volume (mm 3 ) of the tested material at the current compacon pressure p (MPa) and V 0 is the volume of the compacted material (mm 3 ) at zero pressure (MPa). The parameter a i (d.u.) describes the theorecal maximal volume reducon of a tableng material at a parcular phase of the compression process, the parameter 1/t i describes the speed of the volume reducon at a parcular phase (MPa -1 ), and the parameter y 0 (d.u.) describes the maximal theorecal volume reducon at the infinite compacon pressure. In order to study the behavior of the excipients during the compacon process, the parameters a i and 1/t i are useful. In contrast to the oſten used Cooper and Eaton equaon 4 , the three parameters of the equaon (1) are esmated from the relaonship between the volume reducon of a compacted material and the applied compacon pressure. The equaon (1) divides the compacon process into three parcular phases. The first one describes the precompression that includes the parcle rearrangement, the interparculate fricon and the fricon between the material and the walls of the die. The second one characterizes the elasc deformaon of the parcles. In the third phase of the process, the plasc deformaon of the compacted material is described. The parameters of the compacon equaon (1) can be used for the calculaon of energy E i (J) needed for the compacon in a parcular phase of the process according to equaon (2). Used symbols have the same meaning as described above. Evaluaon of tablet properes Tablet hardness was esmated using the same instrument used for the compacon of tablets (Zwick/Roell T1 FRO 50). The tablet hardness was used to express the radial strength according to Fell and Newton. 5 CONCLUSIONS The results of this study proved that the used three exponenal compacon equaon is suitable for the compressibility evaluaon of pharmaceucal excipients. The parameters a 1 and E 1 directly relate to the material flowability while the parameter E 3 reflects the bonding mechanisms. Further study of the relaonship between the tablet strength and the parameters of the compacon equaon for other excipients is necessary in future. This study was supported by SVV 260 183 RESULTS AND DISCUSSION The most important parameters of the used compacon equaon are the parameters a i that describe the volume reducon and E i expressing the amount of energy used in the parcular phase of compacon process. In Table 2, the results of the theorecal volume reducon at each of three compacon phases are summarized. The values of parameter a 1 , i.e. the theorecal volume reducon caused by parcle rearrangement, depend greatly on the flow properes and the bulk density of the evaluated material. The beer the flowability and the lower the bulk density, the lower values of this parameter can be observed. In Table 1, the mass flow rate (ṁ), the angle of repose ( α) and Hausner rao (HR) are summarized. DC showed the best flow properes. The worst flow properes were measured in MCC. Differences are caused by the parcle size and the surface properes (Fig. 2 to 5). Parcles of MCC were acicular having the mean diameter of 77.66 μm and the lowest bulk density (0.32 g/ml). Parcles of LAC and DC were equant, larger (x 50 = 145.54 μm, and 209.12 μm, respecvely) and relavely smooth. Also the bulk density of LAC and DC was higher (0.60 g/ml and 0.68 g/ml). Worse flow properes of MCC can also by caused by the highest moisture content in comparison with LAC and DC (4.49%, 0.46 %, and 1.02 %, respecvely). In Table 2, parameter a 2 describes the volume reducon caused by elasc deformaons. Being related to the material elascity, the higher values are expected for the viscoelasc materials than for the brile ones. This was observed for MCC in comparison to LAC and DC. The parameter a 3 describes the volume reducon caused by the plasc deformaons. Values of this parameter depend on the material properes menoned above, moreover, the bonding mechanism is also important. 6 The results of energec parameters E i are summarized in Table 3. Parameter E 1 describes the amount of energy used during the parcle rearrangement. The values are influenced by the interparculate fricon that is connected with the parcle shape and the surface roughness. The rounder and the smoother the parcles the lower is the energy consumpon. However, such parcles are usually less compressible than the irregular and rougher ones. 7 The lowest value of the parameter E 1 was found in LAC with the regular, smooth parcles. The parameter E 2 describes the amount of energy used during the elasc deformaons. The viscoelasc MCC showed the highest values. Comparing the values for DC and LAC, the higher values for DC could result from removal of the air trapped inside the agglomerates of DC. The parameter E 3 describes the amount of energy used at plasc deformaon; it mostly depends on the bonding mechanism. The formaon of hydrogen bonds and the bridges are the main mechanisms for viscoelasc MCC while the creaon of van der Waals bonds is typical for brile materials (LAC and DC) that tend to fragment repeatedly during the compacon. The fragmentaon is connected with the creaon of the new bonds and surfaces which leads to higher energy consumpon. 8 This corresponds with the radial strength measurement; the highest values were detected for viscoelasc MCC (3.31 MPa) contrary to the significantly lower values for LAC and DC (0.24 MPa and 0.30 MPa, respecvely). Fig. 1 Material tesng machine Zwick/Roell Fig. 2 to 4 SEM Images of Comprecel 102, Spherolac and DI-CAFOS A150 parcles (mag. 550x, 250x and 1000x) Material ṁ (g/s) α (°) HR (d.u.) Material a 1 (d.u.) a 2 (d.u.) a 3 (d.u.) Material E 1 (J) E 2 (J) E 3 (J) MCC 9.75 (1.39) 47.33 (1.46) 1.39 (0.01) MCC 0.28 (0.01) 0.35 (0.01) 0.37 (0.01) MCC 0.12 (0.01) 2.80 (0.17) 39.8 (2.0) LAC 16.22 (2.18) 44.50 (1.04) 1.16 (0.02) LAC 0.19 (0.02) 0.26 (0.03) 0.55 (0.02) LAC 0.03 (0.05) 1.93 (0.42) 119.7 (10.2) DC 32.91 (0.16) 39.90 (0.30) 1.13 (0.01 DC 0.12 (0.01) 0.25 (0.01) 0.63 (0.02) DC 0.05 (0.01) 2.16 (0.13) 148.4 (11.1) Table 1 Mass flow rate, angle of repose and Hausner rao Table 2 Results of volume reducons Table 3 Results of energec parameters

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Page 1: Compaction equation and its use in the determination of ......In Table 2, parameter a2 describes the volume reduction caused by elastic deformations. eing related to the material elasticity,

Compaction equation and its use in the determination of compressibility

of pharmaceutical materials

REFERENCES

1. Hausner, H. H. Friction conditions in a mass of metal powder, Int. J. Powder Metall. 3, 7-13 (1967).

2. Řehula, M. and Rysl, T. Characterization of microcrystalline celluloses by means of the parameters of a three-exponential compression equation. Ces. Slov. Farm. 57, 165-169 (2008).

3. Ondrejček, P.; Řehula, M.; Svačinová, P.; Stoniš, J. and Rabišková, M. The effect of a new glidant Syloid on pressing of drug tablets. Chem. Listy. 108, 687-693 (2014).

4. Cooper, A. R. and Eaton, L. E., Compaction behavior of several ceramic powders. J. Am. Ceram. Soc. 45, 97-101 (1962).

5. Fell, J. T. and Newton, J. M. Determination of tablet strength by the diametral-compression test. J. Pharm. Sci. 59, 688-691 (1970).

6. Führer, C. Substance behaviour in direct compression. Labo-Pharma Probl. Tech. 46, 759-762 (1977).

7. Obae, K.; Iijima, H. and Imada, K. Morphological effect of microcrystalline cellulose particles on tablet tensile strength. Int. J. Pharm. 182, 155-164 (1999).

8. Eriksson, M. and Alderborn, G. The effect of particle fragmentation and deformation on the interparticulate bond formation process during powder compaction. Pharm. Res. 12, 1031-1039 (1995).

P. Ondrejček, P. Svačinová, B. Vraníková, O. Holas, M. Rabišková, Z. Šklubalová Department of Pharmaceutical Technology, Charles University in Prague,

Faculty of Pharmacy in Hradec Králové, Heyrovského 1203, 500 05 Hradec Králové, Czech Republic

INTRODUCTION

Tablets are dosage forms made by a compression of the same powdered mixture volumes of one or

more active ingredients and excipients. This work studies the flow and compressibility properties of

three pharmaceutical excipients. The compressibility of used materials is evaluated using the three

exponential compaction equation.

MATERIALS

Microcrystalline cellulose (MCC, Comprecel 102, Mingtai Chemical) lactose monohydrate (LAC,

Spherolac 100, Meggle), and calcium phosphate anhydrate (DC, DI-CAFOS A150, Budenheim) were used

as fillers. The particle size of the used materials was estimated using the optical microscope

(Olympus BX51) at 10x magnification. The median particle size (x50) was expressed automatically.

METHODS

Flow properties measurement

Moisture analyzer (Precisa XM60) was used for the evaluation of loss on drying at 105 °C. According to the European Pharmacopoeia, the bulk density of used materials was

determined using the Scott’s Volumeter (Copley Scientific). Tapped density meter (Erweka SVM 102) was used for the evaluation of Hausner ratio (HR).1 To determinate the angle of

repose α (°) and the mass flow rate ṁ (g/s) of excipients, the granulate and powder flow tester (Erweka GT) with the 200 ml stainless steel conical hopper and a 10 mm outlet nozzle was

used. The average of ten measurements with the standard deviation (SD) is shown in Table 1.

Tablet preparation

Material testing instrument (Zwick/Roell T1 FRO 50; Fig 1) was used for the preparation of tablets with the mass of 500 mg and 13 mm in diameter. Tablets used for the evaluation of

compaction process were made using the compaction force of 40 kN. The radial strength was evaluated in tablets compacted at the force of 10 kN.

The compaction process was evaluated using the three-exponential equation (1).2,3 Where V is the volume (mm3) of the tested material at the

current compaction pressure p (MPa) and V0 is the volume of the compacted material (mm3) at zero pressure (MPa). The parameter ai (d.u.)

describes the theoretical maximal volume reduction of a tableting material at a particular phase of the compression process, the parameter 1/ti

describes the speed of the volume reduction at a particular phase (MPa-1), and the parameter y0 (d.u.) describes the maximal theoretical volume

reduction at the infinite compaction pressure. In order to study the behavior of the excipients during the compaction process, the parameters ai

and 1/ti are useful. In contrast to the often used Cooper and Eaton equation4, the three parameters of the equation (1) are estimated from the

relationship between the volume reduction of a compacted material and the applied compaction pressure. The equation (1) divides the

compaction process into three particular phases. The first one describes the precompression that includes the particle rearrangement, the interparticulate friction and the friction between the material and the walls

of the die. The second one characterizes the elastic deformation of the particles. In the third phase of the process, the plastic deformation of the compacted material is described. The parameters of the compaction

equation (1) can be used for the calculation of energy Ei (J) needed for the compaction in a particular phase of the process according to equation (2). Used symbols have the same meaning as described above.

Evaluation of tablet properties

Tablet hardness was estimated using the same instrument used for the compaction of tablets (Zwick/Roell T1 FRO 50). The tablet hardness was used to express the radial strength according to Fell and Newton.5

CONCLUSIONS

The results of this study proved that the used three exponential compaction equation is suitable for the compressibility evaluation of pharmaceutical excipients. The parameters a1 and E1 directly relate to the material

flowability while the parameter E3 reflects the bonding mechanisms. Further study of the relationship between the tablet strength and the parameters of the compaction equation for other excipients is

necessary in future.

This study was supported by SVV 260 183

RESULTS AND DISCUSSION

The most important parameters of the used compaction equation are the parameters ai that describe the volume reduction and Ei expressing the amount of energy used in the particular phase of compaction

process. In Table 2, the results of the theoretical volume reduction at each of three compaction phases are summarized. The values of parameter a1, i.e. the theoretical volume reduction caused by particle

rearrangement, depend greatly on the flow properties and the bulk density of the evaluated material. The better the flowability and the lower the bulk density, the lower values of this parameter can be observed.

In Table 1, the mass flow rate (ṁ), the angle of repose (α) and Hausner ratio (HR) are summarized. DC showed the best flow properties. The worst flow properties were measured in MCC. Differences are caused by

the particle size and the surface properties (Fig. 2 to 5). Particles of MCC were acicular having the mean diameter of 77.66 μm and the lowest bulk density (0.32 g/ml). Particles of LAC and DC were equant, larger

(x50 = 145.54 μm, and 209.12 μm, respectively) and relatively smooth. Also the bulk density of LAC and DC was higher (0.60 g/ml and 0.68 g/ml). Worse flow properties of MCC can also by caused by the highest

moisture content in comparison with LAC and DC (4.49%, 0.46 %, and 1.02 %, respectively). In Table 2, parameter a2 describes the volume reduction caused by elastic deformations. Being related to the material

elasticity, the higher values are expected for the viscoelastic materials than for the brittle ones. This was observed for MCC in comparison to LAC and DC. The parameter a3 describes the volume reduction caused by

the plastic deformations. Values of this parameter depend on the material properties mentioned above, moreover, the bonding mechanism is also important.6

The results of energetic parameters Ei are summarized in Table 3. Parameter E1 describes the amount of energy used during the particle rearrangement. The values are influenced by the interparticulate friction that

is connected with the particle shape and the surface roughness. The rounder and the smoother the particles the lower is the energy consumption. However, such particles are usually less compressible than the

irregular and rougher ones.7 The lowest value of the parameter E1 was found in LAC

with the regular, smooth particles. The parameter E2 describes the amount of energy

used during the elastic deformations. The viscoelastic MCC showed the highest values.

Comparing the values for DC and LAC, the higher values for DC could result from

removal of the air trapped inside the agglomerates of DC. The parameter E3 describes

the amount of energy used at plastic deformation; it mostly depends on the bonding

mechanism. The formation of hydrogen bonds and the bridges are the main

mechanisms for viscoelastic MCC while the creation of van der Waals bonds is typical

for brittle materials (LAC and DC) that tend to fragment repeatedly during the

compaction. The fragmentation is connected with the creation of the new bonds and

surfaces which leads to higher energy consumption.8 This corresponds with the radial

strength measurement; the highest values were detected for viscoelastic MCC

(3.31 MPa) contrary to the significantly lower values for LAC and DC (0.24 MPa and

0.30 MPa, respectively).

Fig. 1 Material testing

machine Zwick/Roell

Fig. 2 to 4 SEM Images of Comprecel 102, Spherolac and DI-CAFOS A150 particles (mag. 550x, 250x and 1000x)

Material ṁ (g/s) α (°) HR (d.u.) Material a1 (d.u.) a2 (d.u.) a3 (d.u.) Material E1 (J) E2 (J) E3 (J)

MCC 9.75 (1.39) 47.33 (1.46) 1.39 (0.01) MCC 0.28 (0.01) 0.35 (0.01) 0.37 (0.01) MCC 0.12 (0.01) 2.80 (0.17) 39.8 (2.0)

LAC 16.22 (2.18) 44.50 (1.04) 1.16 (0.02) LAC 0.19 (0.02) 0.26 (0.03) 0.55 (0.02) LAC 0.03 (0.05) 1.93 (0.42) 119.7 (10.2)

DC 32.91 (0.16) 39.90 (0.30) 1.13 (0.01 DC 0.12 (0.01) 0.25 (0.01) 0.63 (0.02) DC 0.05 (0.01) 2.16 (0.13) 148.4 (11.1)

Table 1 Mass flow rate, angle of repose and Hausner ratio Table 2 Results of volume reductions Table 3 Results of energetic parameters