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MECHANICAL ENGINEERING
Mechanistic Understanding of Microparticle Formation in
Respiratory Applications
Reinhard Vehring
Outline
Experimental model systems
Single droplet
Droplet chain
Monodisperse spray dryer
Research spray dryers with process model
Theoretical models
Analytical
Numerical
Particle Formation
Evaporation and condensation
Liquid phase diffusion
Precipitation
Particle Zoo
1
Single Particle Levitation
Electrodynamic Balance
Davies, J.F. Haddrell, A.E., Reid, J.P.: Time-resolved measurements of the evaporation of volatile components from single aerosol droplets. Aerosol Sci Technol, 46, 666-77, 2012
Highest level of idealization
Excellent control of parameters
Many analytical options
Difficult for fast processes and high temperatures
Dried particle not collected
2
Droplet Chain Technique
Gomez, M., Ordoubadi, M., McAllister, R. A., Melhem, O., Barona, D., Gracin, S., Ajmera, A., Lechuga-Ballesteros, D., Finlay, W. H., Vehring, R.: Monodisperse Droplet
Chain Technique to Support Development of Co-solvent Based Inhalation Products. Respiratory Drug Delivery 2018, Vol 2, pp 563–568, 2018.
Laminar gas flow,T,v,RH
Droplet Generator
SEM Sampler
Sensor
Laserz
3
Droplet Chain Model Particles
Vehring, R.: Expert Review: Pharmaceutical Particle Engineering via Spray Drying. Pharmaceutical Research, 25, 999-1022, 2008.
Production of monodisperse, monomorph particles
Good control of parameters
Allows sampling of dried particles
Realistic conditions for spray drying
Comprehensive analysis difficult for small particles
Small sample sizes (A few million particles)
Model ParticlesProduction Lot
4
Monodisperse Spray Drying
Azhdarzadeh, M., Shemirani, F. M., Ruzycki, C. A., Baldelli, A., Ivey, J., Barona, D., Church, T., Lewis, D., Olfert, J. S., Finlay, W. H.,
Vehring, R.: An Atomizer to Generate Monodisperse Droplets from High Vapor Pressure Liquids. Atomization & Sprays, 26, 121-134, 2016.
Replaces twin fluid atomizer with vibrating orifice droplet generator
in a spray dryer.
Most particles are monodisperse. Produces milligram quantities.
Works with propellants.
Not as well controlled as droplet chain
8 Orifice Plate
9 Spring Contact
10 Piezoceramic
11 Orifice Cup
12 Dispersion Cup Body
13 Dispersion Cup Top
5
Monodisperse Spray Drying Examples
Ivey, J.W., Bhambri, P., Church, T.K., Lewis, D.A., Vehring, R.: Experimental Investigations of Particle Formation from Propellant and Solvent Droplets Using a Monodisperse Spray
Dryer. Aerosol Science and Technology, 52 (6), 702-716, 2018.
BDP and Caffein particles from
HFA 134a + ethanol
Can function as a test bed for
pMDI aerosols
6
Research Spray Dryers
Ly, A., Carrigy, N.B., Wang, H., Harrison, M., Sauvageau, D., Martin, A. R., Vehring, R., Finlay, W. H.: Atmospheric Spray Freeze Drying of Sugar Solution with Phage D29.
Frontiers in Microbiology, submitted.
Atmospheric Spray Freeze DryingModular
Dryer
7
Model Based Particle Engineering
Vehring, R.: Theoretical Tools for Particle Engineers: Spray Drying Complex Formulations for Inhalation. Respiratory Drug Delivery Europe 2015, Vol 1, pp 187-196, 2015.8
Outline
Experimental model systems
Single droplet
Droplet chain
Monodisperse spray dryer
Research spray dryers with process model
Theoretical models
Analytical
Numerical
Particle Formation
Evaporation and condensation
Liquid phase diffusion
Precipitation
Particle Zoo
9
What part of particle formation can be modeled?
Just atomized:
Well mixed
solution
Saturated on
the surfaceNucleation
Crystal
growth
Shell
formation
Dry
particle
Example: Formation of a hollow crystalline particle from an evaporating solution droplet
Need to know the internal distribution of components at the onset of shell formation!
(Later stages of particle formation are very complex and material properties are missing)
10
Model Scope
Droplet: Gas Phase:
Isothermal, no convection No convection other than Stefan flow
Well mixed for solvents Spatially averaged material properties
Radial distribution of components Evaporation (condensation) rates
Time resolved
r
r0 a(t)
Tgas
11
Internal Distribution of Components
Based on Fick’s 2nd law: cDt
c
D: Diffusion coefficient, : evaporation rate,
: normalized time, c: normalized concentration,
R: normalized droplet radius
R
cR
R
c
RR
c
Pe
c
)1(2
2
)1(2
12
2
Fully normalized version for radial symmetry:
DPe
8
Boraey, M. A., Vehring, R.: Diffusion Controlled Formation of Microparticles. J. Aerosol Science, 67, 131-143, 2014.
is controlled by the Peclet number, Pe:
Analytical solution possible (VFL model)
- for constant evaporation rate and constant diffusion coefficient
Numerical model
- necessary for co-solvent systems, propellants, or variable material properties
12
Outline
Experimental model systems
Single droplet
Droplet chain
Monodisperse spray dryer
Research spray dryers with process model
Theoretical models
Analytical
Numerical
Particle Formation
Evaporation and condensation
Liquid phase diffusion
Precipitation
Particle Zoo
13
Single Solvent - Single Solute Constant Rate Evaporation
2
0d
Aqueous Solution Droplet
2
0D
d
tdtd 2
0
2
Measurement
Numerical model
Analytical model
14
Ethanol – Water Co-solvent System
Symbols: EDB data.
Solid line: Stefan-Fuchs model.
0 200 400 600 800 1000
0.0
0.5
1.0
20 °C
8 °C
0 °C
d2/d
2 0
t/d20 (s/mm2)
30 % water / 70 % ethanol
Different temperatures
0 200 400
0.0
0.5
1.0 0.4:0.6 w/w water/ethanol, EDB
0.4:0.6 w/w water/ethanol, Stefan-Fuchs
0.3:0.7 w/w water/ethanol, EDB
0.3:0.7 w/w water/ethanol, Stefan-Fuchs
0.2:0.8 w/w water/ethanol, EDB
0.2:0.8 w/w water/ethanol, Stefan-Fuchs
d2/d
2 0
t/d20 (s/mm2)
20 °C
Different co-solvent ratios
15
Solvent Composition Changes Over Time
0 200 400
0.0
0.5
1.0W
ater
Mas
s F
ract
ion
t/d20 (s/mm2)
0.4:0.6 w/w water/ethanol
0.3:0.7 w/w water/ethanol
0.2:0.8 w/w water/ethanol
20 °C
Different co-solvent ratios
co-solvent
water
ethanol
16
Impact on Particle Formation in Multi-Solvent Systems
In multi-solvent systems, the solubility of active or excipients can change with time due to the change in
solvent composition
17
Evaporation in Humid Air
100 % Ethanol, 20 °C, 91 % RH
Why does the evaporation rate
change?
Ordoubadi, M., Gregson, F., Finlay, W. H., Vehring, R., Reid, J. P.: Interaction of Evaporating Multicomponent Microdroplets with Humid Environments. Respiratory Drug
Delivery 2018, Vol 2, pp 569–572, 2018.18
Water Condensation Effect
100 % Ethanol, 20 °C, 91 % RH
Why does this matter?
Ordoubadi, M., Gregson, F., Finlay, W. H., Vehring, R., Reid, J. P.: Interaction of Evaporating Multicomponent Microdroplets with Humid Environments. Respiratory Drug
Delivery 2018, Vol 2, pp 569–572, 2018.
Ethanol droplet cools
Water condenses on
Ethanol evaporates
Water evaporates
19
Water or Ice Templated Porous Particles
Ivey, J. W., Bhambri, P., Church, T. K., Lewis, D. A., McDermott, M. T., Elbayomy, S., Finlay, W. H., Vehring, R.: Humidity Affects the Morphology of Particles Emitted from
Beclomethasone Dipropionate Pressurized Metered Dose Inhalers. International Journal of Pharmaceutics, 520 (1-2), 207-215, 2017.
Dry
Humid
20
Beclomethasone dipropionate
pMDI
Diffusion Controlled Particle Formation
Peclet Number:
Describes balance betweenvelocity of surface recession and diffusion
Predicts internal distribution of components
Example: Pe >> 1
Polystyrene nanoparticle suspension
500 nm5 µm
N. Tsapis et al. PNAS 99, 12001 (2002)
21
Low Peclet Number Particle Formation (Pe ~ 1)
100 % trehalose in water. Drying temperature 80 °C. Droplet chain (SEM and FIB-SEM)
Small molecule
excipients and
actives with high
solubility and low
propensity to
crystallize form solid
amorphous particles
22
Particle Density Changes with Peclet Number (non-crystallizing)
Pe = 2.7, 5.6, 12.5 Pe = 77
Glycoprotein
P = 0.5, 0.35, 0.15 kg/L
Cellulose acetate butyrate
P = 0.7 kg/L
Baldelli, A., Boraey, M. A., Nobes, D., Vehring, R.: Analysis of the Particle Formation Process of Structured Microparticles. Molecular Pharmaceutics, 12 (8),
2562-2573, 2015 23
Application Example: Stabilize Phage in a Flowable Powder
Campylobacter
Phage CP30A
Needs glass stabilization for
room temperature storage
add trehalose
Trehalose alone does not work, because
the phage (nanoparticle) enriches on the
surface where it is not protected
Approach: Add a high Pe number amorphous
shell former to replace the phage on the surface
while still allowing mixing with trehalose
Pullulan
24
Solid Phase Modeling to Achieve Storage Stability
Carrigy NB, Vehring R. Engineering stable spray dried biologic powder for inhalation. (Released February 2019). Chapter 12 in Pharmaceutical Inhalation Aerosol Technology, 3rd edition,
ed. Hickey AJ. New York: Marcel Dekker, Inc. 25
Particle Formation Model Predicts Radial Distributions
Carrigy NB, Ordoubadi M, Liu Y, Melhem O, Barona D, Wang H, Milburn L, Vehring R. Spray dried pullulan trehalose microparticle platform for pulmonary delivery of biologics.
In preparation.
0.00
0.25
0.50
0.75
1.00
0.7 0.8 0.9 1.0
Mass
Fra
ctio
n
r/R
40%P 60%T
10%P 90%T
Trehalose
Pullulan
120
150
180
210
0.7 0.8 0.9 1.0
Tg
,PT
,dry
(°C
)
r/R
40%P 60%T
10%P 90%T
Full numerical model simulation indicates
that pullulan enriches on the surface
Coupled with Fox equation:
Glass transition temperature increases
near the surface due to the high glass
transition temperature of pullulan
26
Use Droplet Chain to Study Shell Folding
5% pullulan, 95% trehalose
Carrigy NB, Liang L, Wang H, Kariuki S, Nagel TE, Connerton IF, Vehring R. Amorphous shell formers improve the biological stability of spray dried Campylobacter bacteriophage.
Frontiers in Microbiology. Submitted Oct 11, 2018.
Preliminary results:
Good dispersibility from DPI
100 fold better process loss and short term stability compared to trehalose alone
Perhaps a new platform for biologics
27
20% pullulan, 80% trehalose 40% pullulan, 60% trehalose
Outline
Experimental model systems
Single droplet
Droplet chain
Monodisperse spray dryer
Research spray dryers with process model
Theoretical models
Analytical
Numerical
Particle Formation
Evaporation and condensation
Liquid phase diffusion
Precipitation
Particle Zoo
28
Particle Formation in Crystallizing Systems
��,� =��
�
1 −
��,� �
����,�
��
Time to saturation:
j: component in multicomponent system
d0: Initial droplet diameter
C0: Initial solution concentration
: Evaporation rate
Csol : Solubility
E : Surface enrichment
Key parameters are related to kinetics not to formulation composition
Predicts which component, i, crystallizes first
29
Crystallization Window
Time available for crystal growth
��� =��
�
��
����
��
d0: Initial droplet diameter
: Evaporation rate
C0: Initial solution concentration
Csol: Solubility
E: Surface enrichment
Predicts crystal size and whether components may be amorphous
30
Particle Density Decreases With Increasing Crystallization Window
NaNO3Different T
Different feed
concentration
(Using critical supersaturation)
Baldelli, A., Power, R., Miles, R., Reid, J. P., Vehring, R.: Effect of Crystallization Kinetics on the Properties of Spray Dried
Microparticles. Aerosol Science and Technology, 50 (7), 693-704, 2016.
Low density is caused by shell
formation
Shell formation requires time for
nucleation and crystal growth
The earlier the shell formation
starts the more void space can be
created
31
Particle Density in Multicomponent Systems
Binary system:
NaNO3/KNO3
(For component that saturates first)
Baldelli, A. Vehring, R.: Control of the Radial Distribution of Chemical Components in Spray Dried Crystalline Microparticles. Aerosol Science and Technology, 50 (10),
1130-1142, 201632
How can we control crystal size?
5 mg/ml
75ºC
5 10-1 mg/ml
100ºC
5 10-2 mg/ml
75ºC5 10-3 mg/ml
75ºC
5 10-5 mg/ml
125ºC
�ts (ms): 221 6 119 18 117 2 101 3 18 2
Mostly
amorphous
NaNO3
Baldelli, A.: Experimental and Theoretical Studies on the Particle Formation Process of Particles for the Improvement of Pulmonary Drug
Delivery. PhD Thesis, University of Alberta, 2016.
The size of the crystals that form the shell decreases when less time is available for crystal growth (decreasing �ts)
The solid phase of the particles becomes increasingly disordered with decreasing �ts
Microcrystals nanocrystals amorphous
33
Crystal Size Determines Surface Roughness
Baldelli, A., Vehring, R.: Analysis of Cohesion Forces between Monodisperse Microparticles with Rough Surfaces. Coll. Surf. A, 506, 179, 2016
34
Colloidal Probe Microscopy on Monodisperse Particles
Baldelli, A., Vehring, R.: Analysis of Cohesion Forces between Monodisperse Microparticles with Rough Surfaces. Coll. Surf. A, 506, 179, 2016.
35
Effect of Different Rugosity on Cohesion
Baldelli, A., Vehring, R.: Analysis of Cohesion Forces between Monodisperse Microparticles with Rough Surfaces. Coll. Surf. A, 506, 179, 2016.
Cohesion measured by Colloidal Probe Microscopy
90 nN
Changes in crystal size cause large changes in roughness and cohesion.
Affected product parameters: Dispersibility, colloidal stability, MMAD.
45 nN 3 nN 10 nN 125 nN
9 nN
36
Surface Composition in Multi-components Particles Depends on Crystallization Sequence
Dilute,
Homogeneous,
binary
Radial profiles
develop
First component
crystallizesComposite
shell forms
Surface is enriched by the component which first reaches saturation (smallest ts)
j: component (NaNO3 or KNO3)
d0: Initial droplet diameter
C0: Initial solution concentration
(t) : Evaporation rate (function of gas temperature)
Csol (t) : Solubility
E (t) : Surface enrichment
Na K
��,� =��
�
1 −
��,� �
����,�
��
Boraey, M. A., Vehring, R.: Diffusion Controlled Formation of Microparticles. Journal of Aerosol Science, 67, 131-143, 2014.
37
Surface is enriched by the component which first reaches saturation
Baldelli, A. Vehring, R.: Control of the Radial Distribution of Chemical Components in Spray Dried Crystalline Microparticles. Aerosol Science and Technology, 50 (10), 1130-1142,
2016.
Time
to saturation
39
Shell Composition by STEM + X-ray Spectroscopy
Baldelli, A. Vehring, R.: Control of the Radial Distribution of Chemical Components in Spray Dried Crystalline Microparticles. Aerosol Science and Technology, 50 (10), 1130-1142, 2016.
40
Particle Zoo
unpublished
41
Multi-component nano-emulsion Low-density, nano-composite gel particles
Particle Zoo
unpublished
42
Multi-phase particles: Amorphous + nano-crystalline + oil nanodroplets
Particle Zoo
unpublished
43
Nano-crystal scaffolds
FIB -
HIM
HIM
Particle Zoo
unpublished
44
Ultralow-density particles via Atmospheric Spray Freeze Drying
Atomized solution droplet
Freeze
concentrate
Ice
Freezing
Freeze concentrate
desiccation
Ice sublimation
Summary and Conclusions
The morphology of spray dried, amorphous microparticles is determined by Peclet number and
shell buckling mechanisms.
The shell deformation (buckling) phase remains largely unexplored.
The morphology of spray dried, crystalline microparticles is strongly influenced by evaporation and
crystallization kinetics.
Material properties for many substances of interest are missing.
Experimental tools in combination with theoretical particle formation models are necessary for
advanced particle design.