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. 2021 Jul 10;13(7):1055. doi: 10.3390/pharmaceutics13071055
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