2025 AIChE Annual Meeting
(155b) How to Design a Pharmaceutical Drug Mixture with Prescribed Cohesive Properties Using Particle Scale Parameters
Author
Here is where a product development model can help. It turns out that the bulk cohesive flow property of powders depends on what causes the adhesion between two particles. It also turns out that the bulk unconfined yield strength (fc) for different types of adhesion forces between particles is a function of the reciprocal of the particle size raised to some power 1/Dpn where Dp is the particle size and (n) depends on what causes the adhesion between adjacent particles. Some of these adhesive forces are: capillary bond formation, Van der Waals attractive forces, crystal growth between particles, and/or elastic plastic sintering between particles. Any consistent material can be divided into variously sized class bins with a very narrow size distribution. The narrow size distribution is important because the models that exist relating unconfined yield strength to particle size assume a mono-dispersed particle size distribution (equation 1). The bulk unconfined yield strength of these narrow particles size bins can be measured and the strength plotted as a function of particle size.
fc=K1*1/Dp + K2*1/Dp2 + K3*1/Dp(1/2) + K4*1/Dpn (1)
Bulk strength is mechanistic in nature and is the combined effect of all the various adhesion effects that might act between particles in a mixture. This is expressed in equation 1. The measured strength for the various particle size data can then be curve-fit to equation 1 to find the K-values which include the effects of the multiple possible causes of adhesion between particles.
It is possible to identify the cause(s) of the bulk strength based on their different adhesive forces. This can be done with the API and all of the excipients in the drug product. The result is a model describing bulk unconfined yield strength as a function of particle size for each of the pure components that make up the mixture.
The bulk powder can be thought of as collection of unit cells where the corners of the unit cells consist of particles selected randomly from the coarse size particles in the bulk (greater than D50). The finer size particles (less than Dp50) can then fit in the space between the coarse size particles. The void size between the coarse particles has a certain volume and a certain number of fine particles can fit in this volume depending on the particle size.
As this unit cell shears the particles in the unit cell are pulled apart. The act of pulling adjacent particles apart results in a set of adhesion forces between particles that are in the shear plane. From a continuum point of view, bulk unconfined yield strength is defined as the major principal stress that causes the bulk material to yield in shear. But, from a particle point of view, unconfined yield strength is a function of the collection of all the adhesive and frictional forces formed in the all the possible unit cells where the particles move, on average, the distance of one unit cell. The bulk unconfined yield strength of the unit cell can be thought of as the combined effect of the strength of the pair-wise interaction of adjacent particles for both the fines and coarse particles in the unit cell.
This particle scale model, then, turns into a probabilistic problem where a set of coarse particles is preselected and placed at the corners of the unit cell. The fine particles are also randomly selected based on the fines particle size distribution to fit in the void space between the coarse particles. The strength functions, as a function of particle size for each component, are then used to compute the strength of the material in the unit cell. This random selection process is repeated many times using the probabilities of selecting the fine and coarse particles based on the size distributions that make up the bulk material. The bulk strength is the average strength of all these randomly selected unit cells. The beauty of this method is that, once the mechanistic model is created for the excipients and API relating strength to particle size, the model can be used with the probabilistic model described above to estimate the bulk unconfined yield strength of any vendor-supplied PSD as well as the bulk unconfined yield strength of any combination of excipients and API for any prescribed particle size distribution and prescribed drug loading or excipient concentrations.
This work shows how the model can be generated and then used to predict bulk unconfined yield strength using particle scale properties. It provides formulators and process engineers the means of optimizing product design to create a prescribed behavior without the guess-and-check approach.