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© 2024 MJH Life Sciences^{™} and Pharmaceutical Technology. All rights reserved.

*Quantitative data from the literature show strong relationships among average particle size, powder densification, tensile strength, and hardness.*

The indentation-size effect forms the basis of the relationships connecting average particle size (*r ^{0.5}* ) with densification, tensile strength, and hardness of one-component tableting systems. Those structure–property relationships also have been verified by quantitative data presented in the literature, and they may serve as a predictive tool for crystal engineers and formulators to design particles with the right average size for tableting at the beginning of product development. In general, densification, tensile strength, and hardness increase as the average particle size decreases, and a significant amount of compaction pressure is required for densification to occur. These effects present a potential problem when compacting particles that are very small.

Producing pharmaceutical tablets involves combining the active pharmaceutical ingredient (API) and excipients. When a high API drug-load is desired, selection or manipulation of the excipients or process alone may not be sufficient to compact the tablet. The average particle size of an API influences compactability, but how particle size affects compactability remains unclear. Correlations between average particle size and tablet properties such as densification, tensile strength, and hardness are important because those correlations can generate predictions, which facilitate the selection and design of appropriately sized particles.

Loose powders have a very low initial relative density (ρ_{0}). Relative density (*ρ _{r}*) is defined as the density of the compact (mass of a compact divided by its volume) divided by the true density, which is determined by helium pycnometry (1). The cold isostatic compaction of powders by the application of macroscopic compaction pressure (

In stage one, weak interparticle attractive forces counteract gravitational forces and produce dangling bonds (2), which form low-density aggregates of particles. In stage two, mechanical compaction begins to take place. The fractional packing density *ρ _{0}* increases from 0.35 to 0.74 (2). At this stage, each particle averages 4.75 contacts and begins to experience "jamming." The onset of general particle deformation starts around

The densification phenomenon usually is described as the first-order kinetics of applied macroscopic pressure *P* by the Heckel equation (4):

in which *k* and *A* are constants obtained from the slope and intercept of the plot ln (1/(1*- ρ _{r}*))

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in which ε, *b*, and ln σ_{0} in Equation 2 are porosity and constants obtained from the slope and intercept of the plot ln *σversus* (1 - *ρ _{r}*), respectively.

Interestingly, empirical studies suggest that densification (Equation 1), tensile strength (Equation 2), and hardness (Equation 3) of tablets are not affected only by packing structures e and *ρ _{r}* and pressure, but that those properties are also affected by initial average particle size. (1, 6, 7). Although the effects of initial average particle size are implicitly included in the material characteristic constants of

**Modeling**

Helle *et al.* derived a simple relationship that assumes all powders are monosized spheres and the number of contacts per particle resembles microindentation and increases during stage-two compaction (2, 8):

in which *H* is the indentation hardness of the particle material. Helle *et al*. also derived a semiempirical relationship between the contact size, *L,* and the average particle radius, ** r,** for a given level of density that is reached

Effects of initial average particle size on powder compaction that involve interparticle contacts is conceptualized as the indentation-size effect (ISE) among particles. Hardness increases with decreasing indentation size. The phenomenon of ISE is explained by the strain-gradient plasticity. Under the influence of strain-gradient plasticity, plastic strengthening becomes important when a material in question is plastically deformed in very small volumes (*e.g*., at the tips of cracks or microindentations). The semiempirical ISE equation has the form (2, 9):

in which *H _{0}* is the large-size hardness lower limit,

**Particle-size dependence of densification. **If one combines Equations 4, 5, and 6 and assumes *L* << *L _{0}* , the average particle size

in which C is a constant:

**Particle-size dependence of tensile strength. **By substituting Equation 2 into Equation 7, the average particle size *r* dependence of tensile strength becomes:

**Particle-size dependence of hardness. **By linking Equation 3 with Equation 7 and assuming that *H/H _{max}* << 1 and that

**Results and discussion**

To test the validity of Equations 7, 9, and 10, those equations were plotted against some useful quantitative data from the literature using Microsoft Excel (Microsoft Corp., Redmond, WA). The cold compaction data of pure paracetamol powders (*P*, ln(1/(1 *- ρ _{r}*)), and 2

Figure 1: Effects of average particle size on densification of pure paracetamol powders.

Apparently, linearity in Figures 1, 3, and 4 seems to verify the validity of Equations 7, 9, and 10 and suggests that the initial particle-size effects of *r ^{0.5}* on densification, tensile strength, and hardness, which are different from the average number of interparticle contacts and the contact force, for they scale with

Table I: Calculation of the relative density rr and particle-size dependence of densification (the right-hand side parameter of Equation 7) from the Heckel plots of paracetamol powders of two different sizes under compression (Reference 6).

Different slopes and different *y*-intercepts of straight lines in each figure could imply that factors other than average particle size also have profound effects on densification, tensile strength, and hardness. These factors include and are not limited to morphology (12), water content in the particle (12), crystallinity (13), lattice defects (13), impurities (13), and cracks (14), which are all strongly process dependent. Isolation of the effects of average particle size from other factors requires a consistent processing route, powders of various sizes sorted by careful sieving, and plotting a curve for each specific average particle size instead of a curve for each compaction pressure.

Table II: Calculation of the particle-size dependence of densification (the right-hand side parameter of Equation 7) from the effect of particle size on the compressibility of ([(2S)-2-mercapto-1-oxo-4-(3,4,4-trimethyl-2,5-dioxo-1-imidazolidinyl) butyl]-L-leucyl-N,3-dimethyl-L-valinamide (Reference 10).

Equations 7, 9, and 10 further suggest that at a constant compaction pressure *P*, densification *ρ _{r}*, hardness

Table III: Calculation of the particle-size dependence of tensile strength (the right-hand side parameter of Equation 9) from the relationship between tensile strength Ï of the tablets and compaction pressure P for different fractions of L-lysine monohydrochloride dihydrate powders (Reference 1).

Future work requires systematic experiments and direct measurements in powder compaction. Further refinements in the modeling of the effects of initial average particle size on tableting should include the elastic flattening of the contacts (17). Equations 7, 9, and 10 can be used to link Hiestand indices (18) and the effect of average particle size.

Table IV: Calculation of the particle-size dependence of hardness (the right-hand side parameter of Equation 10) from compact strength versus mean original particle diameter for tablets compressed from sieve fractions of Î±âlactose monohydrate at different compaction levels (Reference 7).

The latest developments in crystal engineering and particle nanotechnology, which both allow for the design and control of particle size at the submicron and nanosize levels, reinforce the importance of studies that describe the effects of initial average particle size on tableting. Structure–property relationships that relate the average particle size with densification, tensile strength, and hardness on tableting serve as predictive tools for crystal engineers and formulators to choose and design particles of the appropriate size for tableting, thereby decreasing the development time for API and tablet production.

Figure 2: Effects of average particle size on densification of 80% ([(2S)-2-mercapto-1-oxo-4-(3,4,4-trimethyl-2,5-dioxo-1-imidazolidinyl)butyl]-L-leucyl-N,3-dimethyl-L-valinamide), 19.5% microcrystalline cellulose and 0.5% magnesium stearate.

**Conclusion**

Quantitative data from the literature show strong relationships among average particle size *r ^{0.5}* with powder densification, tensile strength, and hardness. The inverse proportionality between compaction pressure and initial average particle size indicates potential difficulties in compaction if particles are made too fine. The linearity of those relationships allows a rapid evaluation of tablet performance for any powder with a minimum of two data points. Upon further refinements and more powder compaction experiments, structure–property relationships similar to Equations 7, 9, and 10 could be useful predictive tools for crystal engineers and formulators involved in tablet manufacture.

Figure 3: Effects of average particle size on tensile strength of pure L-lysine monohydrochloride dihydrate powders.

**Acknowledgments**

This work was supported by a research grant from the National Science Council of Taiwan, Republic of China (NSC 93-2119-M-008-003 and NSC 94-2119-M-008-001).

Figure 4: Effects of average particle size on hardness (crushing strength) of pure Î±-lactose monohydrate powders.

**References**

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2. J. Gil Sevillano, "Size Effects in Powder Compaction," *J. Mat. Res*. **16 **(5), 1238–1240 (2001).

3. C. Sun and D.J.W. Grant, "Influence of Elastic Deformation of Particles on Heckel Analysis," *Pharm. Dev. Technol*.** 6** (2), 193–200 (2001).

4. R.W. Heckel, "Density–Pressure Relationships in Powder Compaction," Tr*ans. Metal. Soc. AIME*. 221, 671–675 (1961).

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7. H. Vromans *et al.*, "Studies on Tableting Properties of Lactose: The Effect of Initial Particle Size on Binding Properties and Dehydration Characteristics of (α–Lactose Monohydrate," *Drug Dev. Ind. Pharm*. **12** (11–13), 1715–1730 (1986).

8. A.S. Helle, K.E. Easterling, and M.F. Ashby, "Hot-Isostatic Pressing Diagrams: New Developments," *Acta Metall*. **33** (12), 2163–2174 (1985).

9. W.D. Nix and H. Gao, "Indentation Size Effects in Crystalline Materials: A Law for Strain-Gradient Plasticity," *J. Mech. Phys. Solids ***46** (3), 411–425 (1998).

10. O.L. Sprockel *et al*., "Control of Compactability through Crystalliztion in Tablet Formation," (Bristol-Myers Squibb Company, USA) PCT Int. Appl. WO 02088664 A2, 2002.

11. N. Ouchiyama and T. Tanaka, "Estimation of the Average Number of Contacts between Randomly Mixed Solid Particles," *Ind. Eng. Chem. Fundam.***19 **(4), 338–340 (1980).

12. M. Radeka *et al*., "Compaction Mechanism as the Function of Atomized Powder Particle Size," *Ceramics Int*. **21 **(4), 249–255 (1995).

13. R. Hüttenrauch, "Modification of Starting Materials to Improve Tableting Properties," *Pharm. Ind*. **45 **(4), 435–440 (1983).

14. T. S. Srivatsan *et al.*, "An Investigation of the Influence of Powder Particle Size on Microstructure and Hardness of Bulk Samples of Tungsten Carbide," *Powder Technol*. **122 **(1), 54–60 (2002).

15. E. Merisko-Liversidge, G.G. Liversidge, and E.R. Cooper, "Nanosizing: A Formulation Approach for Poorly Water-Soluble Compounds," *Eur. J. Pharm*. *Sci.***18 **(2), 113–120 (2003).

16. A. Hasnaoui, H. Van Swygenhoven, and P. M. Derlet, "Dimples on Nanocrystalline Fracture Surfaces as Evidence for Shear Plane Formation," *Science***300 **(5625**)**, 1550–1552 (2003).

17. *Mechanical Behavior of Materials*, F.A. McClintock and A.S. Argon, Eds. (Addison-Wesley, Reading, MA, 1966).

18. H.E.N. Hiestand and D.P. Smith, "Indices of Tableting Performance," *Powder Technol*. **38 **(2), 145–159 (1984).

**Tu Lee, PhD,*** is an assistant professor at the Department of Chemical and Materials Engineering and at the Institute of Materials Science and Engineering, at the National Central University, Chung-Li, Taoyuan, Taiwan 320, Republic of China, tel. +886 3 422 7151, ext. 34204, fax +886 3 425 2296, tulee@cc.ncu.edu.tw**Chung Shin Kuo** is a graduate student in the Department of Chemical and Materials Engineering at the National Central University.

*To whom all correspondence should be adressed.

Submitted: Oct. 20, 2005. Accepted: Nov. 22, 2005.

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