| Symbols used | |
| a | Average frequency of drug particle compressions, Hz |
| c | Bead loading or fractional volumetric concentration of the beads, – |
| d | Particle diameter (size), m |
| e | Restitution coefficient, – |
| F b n | Average maximum normal force during collision of two identical elastic beads, N |
| g 0 | Radial distribution function, – |
| i | Observation (run) index, – |
| I | Maximum # of observations, – |
| j | Predictor index, – |
| J | Maximum # of allowed predictors, – |
| k | Breakage rate constant in Equations.(2) and (3), min–1 and µm1–n∙min–1, respectively |
| k(t) | Time-dependent breakage rate parameter in Equation (4), min–1 |
| k 0 | Breakage rate constant in Equation (6), min–n |
| K | Coefficient obtained from an empirical correlation, – |
| n | Exponent in the kinetic models, – |
| p | Probability for a single drug particle to be caught between the beads, – |
| PSD | Particle size distribution |
| P w | Average stirrer power per unit volume, W/m3 |
| Q | Volumetric flow rate, m3/s |
| R | Radius, m |
| R diss | Dissipation coefficient of the bead, – |
| R diss0 | Dissipation coefficient when relative motion of the bead/liquid is absent, – |
| t | Milling time, s |
| T | Available # of predictors for a given MLRM approach, – |
| V | Volume, m3 |
| u b | Average bead oscillation velocity, m/s |
| V m | Volume of the milling chamber, m3 |
| Y | Young’s modulus, Pa |
| Y* | Reduced elastic modulus for the bead–drug contact, Pa |
| Greek letters | |
| α b | Radius of the contact circle formed at the contact of two beads, m |
| ε coll | Energy dissipation rate due to partially inelastic bead–bead collisions, W/m3 |
| ε ht | Power spent on shear of milled suspension of the slurry at the same shear rate, but calculated (measured) when no beads were present in the flow, W/m3 |
| ε m | Non-dimensional bead–bead gap thickness at which the lubrication force stops increasing and becomes a constant, – |
| ε tot | Total energy dissipation rate, W/m3 |
| ε visc | Energy dissipation rate due to both the liquid–beads viscous friction and lubrication, W/m3 |
| Φ | Warped time, minn |
| η | Poisson’s ratio, – |
| θ | Granular temperature, m2/s2 |
| µ L | Apparent shear viscosity, Pa·s |
| ν | Frequency of single-bead oscillations, Hz |
| Π | Energy dissipation rate attributed to the deformation of drug particles per unit volume, W/m3 |
| Πσ y | Pseudo energy dissipation rate, J2/m6s |
| ρ | Density, kg/m3 |
| σ b max | Maximum bead contact pressure at the center of the contact circle, Pa |
| σ y | Contact pressure in drug particle when the fully plastic condition is obtained, Pa |
| Mean residence time, s | |
| ω | Stirrer (rotational) speed, rpm |
| Ψ | Volumetric fraction of drug particles in the drug suspension, – |
| Indices | |
| b | Bead |
| cm | Chamber of the mill |
| L | Equivalent liquid (milled drug suspension) |
| m | Mill |
| p | Drug particle |
| sm | Suspension in the mill |
| T | Holding tank |
| 50 | Median (50% passing) particle size |
| 90 | 90% passing particle size |