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© 2018 HORIBA, Ltd. All rights reserved.
Introduction to Particle Size Analysis
Jeff Bodycomb, Ph.D.
jeff.bodycomb@horiba.com
www.horiba.com/us/particle
© 2018 HORIBA, Ltd. All rights reserved.
Why Particle Size?
Industry Industry
Ceramic Construction
Oil/rubber Chemical
Battery Pharmaceutical
Electricity Food/Drink
Automobile Paper/Pulp
Mining Ink/Toner
Size affects material behavior and processing across a
number of industries.
© 2018 HORIBA, Ltd. All rights reserved.
Application: Pigment Hiding Power
Operator dependent, need to
wait for drying.
Operator independent, no need
to wait for drying.
© 2018 HORIBA, Ltd. All rights reserved.
Size Terminology
The most common designation is micrometers or
microns. When very small, in colloid region,
measured in nanometers, with electron
microscopes or by dynamic light scattering.
10-10 10-810-9 10-610-7 10-410-5 10-210-3 10-1 10-0
meternanometer
Angstrom
(Å)
micrometer millimeter
micron or µm mnm mm
0.1µm 1.0µm 10µm 100µm
100 nm
Fun tip: Describing your work in terms of beard-seconds
make it much more interesting at parties.
“beard-second”
C-H bond
length
© 2018 HORIBA, Ltd. All rights reserved.
Poll!
Which size ranges do you measure?
© 2018 HORIBA, Ltd. All rights reserved.
Size: Particle Diameter (m)
0.01 0.1 1 10 100 1000
Colloidal
Suspensions and Slurries
DLS – SZ-100
Electron Microscope
Powders
Fine Coarse
Optical Microscopy PSA300, Camsizer
Laser Diffraction – LA-960
Acoustic Spectroscopy
Electrozone Sensing
Disc-Centrifuge
Light Obscuration
0.001
Macromolecules
Nano-Metric
MethodsAppsSizes
Sedimentation
Sieves
© 2018 HORIBA, Ltd. All rights reserved.
The Basics
Which is the most meaningful size?
different
size definitions
different
results
© 2018 HORIBA, Ltd. All rights reserved.
Same data, different size definitions
give different results!
different
size definitions
different
results
xcmin  xArea  xFemax
x [mm ]0 .2 0 .4 0 .6 1
0
10
20
30
40
50
60
70
80
Q3 [% ]
Samp leA_Bas ic_0 .2% _xc_m in_001 .rd f
Samp leA_Bas ic_0 .2% _x_area_001 .rd f
Samp leA_Bas ic_0 .2% _xFemax_001 .rd f
G raph o fmeasu remen t resu lts :
M :...rD is tribu toren-Mee ting CAMDAT Samp leA Samp leA_Bas ic_0 .2% _xc_m in_001 .rd f
Task file :Samp leA_Bas ic_0 .2% .a fg
x [mm ]0 .2 0 .4 0 .6 1
0
10
20
30
40
50
60
70
80
Q3 [% ]
Samp leA_Bas ic_0 .2% _xc_m in_001 .rd f
Samp leA_Bas ic_0 .2% _x_area_001 .rd f
Samp leA_Bas ic_0 .2% _xFemax_001 .rd f
G raph o fmeasu remen t resu lts :
M :...rD is tribu toren-Mee ting CAMDAT Samp leA Samp leA_Bas ic_0 .2% _xc_m in_001 .rd f
Task file :Samp leA_Bas ic_0 .2% .a fg
2 x[mm]
© 2018 HORIBA, Ltd. All rights reserved.
The Basics
What sizes can be measured?
© 2018 HORIBA, Ltd. All rights reserved.
Size Definitions
• Martins’s Diameter: The distance between opposite
sides of a particle measured on a line bisecting the
projected area. To ensure statistical significance all
measurements are made in the same direction
regardless of particle orientation.
• Feret’s Diameter: The distance between parallel
tangents on opposite sides of the particle profile.
Again to insure statistical significance, all
measurements are made in the same direction
regardless of particle orientation.
• Note: Both Martin’s and Feret’s diameters are
generally used for particle size analysis by optical and
electron microscopy.
• Equivalent Circle Diameter: The diameter of a circle
having an area equal to the projected area of the
particle in random orientation. This diameter is usually
determined subjectively and measured by oracular
micrometers called graticules.
• Equivalent Spherical Diameter: The diameter of a
sphere that has the same volume as the irregular
particle being examined.
Martin’s
Diameter
Feret’s Diameter
Equivalent Spherical
Diameter
© 2018 HORIBA, Ltd. All rights reserved.
Particle Orientation
• Martin’s and
Feret’s Diameter’s
will vary as
particles are
viewed in different
orientations. The
result will be a
DISTRIBUTION
from smallest to
largest.
Martin’s
Diameter
Feret’s Diameter
Equivalent Spherical
Diameter
Martin’s
Diameter
Feret’s Diameter
Equivalent Spherical
Diameter
© 2018 HORIBA, Ltd. All rights reserved.
The Basics
Particle Particle Distribution
© 2018 HORIBA, Ltd. All rights reserved.
The Basics
Particle Size Particle Size Distribution
4 µm
© 2018 HORIBA, Ltd. All rights reserved.
Poll!
What size(s) are reported by your PSA?
© 2018 HORIBA, Ltd. All rights reserved.
Monodisperse vs. Polydisperse
• Monodisperse Distribution:
– All particles are the same size
– Latex standards
• Wide Distribution:
– Particles of Many Sizes
– Everything else
VOLUME
VOLUME
Particle Size Particle Size
Monodisperse Polydisperse
© 2018 HORIBA, Ltd. All rights reserved.
Logarithmic vs. Linear Scale
• Logarithmic X-Axis
Distribution
• Linear X-Axis
Distribution
VOLUME
Particle Size
0 10 20 30 40 50 60 70 80 90 100
VOLUME
Particle Size
0 10 100
© 2018 HORIBA, Ltd. All rights reserved.
Distribution Display
– Represented by series of segments or channels known as
histogram.
– Number of channels based on design, practicality and
aesthetics
VOLUME
Particle Size
Cumulative Distribution
Differential
Distribution
Histogram
© 2018 HORIBA, Ltd. All rights reserved.
Frequency Frequency + cumulative (undersize)
Histogram Multiple frequency + cumulative (undersize)
Your Analyzer’s Displays
© 2018 HORIBA, Ltd. All rights reserved.
Central Values
Mean
Median
and
Mode
Size
Mean
Weighted Average
Center of Gravity
Median
50% Point
Mode
Peak of the distribution
Most common value
© 2018 HORIBA, Ltd. All rights reserved.
Three spheres of diameters 1,2,3 units
What is the average size of these spheres?
Average size = (1+2+3) ÷ 3 =2.00
This is called the D[1,0] - the number mean
1
2
3
What does “Mean” mean?
© 2018 HORIBA, Ltd. All rights reserved.
None of the answers
are wrong they have just
been calculated using
different techniques
X Dnl  
 
[ , ] .1 0
1 2 3
3
2 00
X Dns  
 
[ , ] .2 0
1 4 9
3
216
X Dnv  
 
[ , ] .3 0
1 8 27
3
2 293
X Dsv  
 
 
[ , ] .3 2
1 8 27
1 2 3
2 57
X Dvm  
 
 
[ , ] .4 3
1 16 81
1 8 27
2 72
Many possible Mean values
Number weighted mean Diameter (length)
Volume weighted mean diameter
Volume/surface mean,
Mean volume diameter
Mean surface diameter
© 2018 HORIBA, Ltd. All rights reserved.
Moment Ratios: ISO 9276-2
 qp
q
ii
p
ii
Dn
Dn
qpD












1
],[
qp 











q
ii
i
p
ii
Dn
DDn
qpD
ln
exp],[ qp 
For your reference
© 2018 HORIBA, Ltd. All rights reserved.
D[4,3] which is often referred to as the Volume Mean Diameter [ VMD ]
D [4,3] =


i i
i i
D n
D n
4
3
Monitoring the D[4,3] value in your specification
will emphasize the detection of large particles
Volume-based Mean diameter
© 2018 HORIBA, Ltd. All rights reserved.
Mode
Median
Mean
D[4,3]
Size
Remember: D[4,3] is sensitive to large particles
Central Values revisited
Mean
Weighted Average
Center of Gravity
Median
50% Point
Mode
Peak of the distribution
Most common value
© 2018 HORIBA, Ltd. All rights reserved.
D(v,0.9)D(v,0.1)
Size µm
D(4,3) sensitive to large particles
D(3,2)
D(v,0.5)
median
D(v,1.0)
Never use
the D100!
sensitive to small particles
10% of the particles lie
below this diameter
90% of the particles lie
below this diameter
half are larger than this diameterhalf are smaller than this diameter
Most Common Statistics
© 2018 HORIBA, Ltd. All rights reserved.
Standard Deviation
• Normal (Gaussian)
Distribution Curve
•  = distribution mean
•  = standard deviation
• Exp = base of natural
logarithms
Mean
+1 STD DEV-1 STD DEV
+2 STD DEV-2 STD DEV
68.27%
95.45%
 





 
 2
2
2
exp
2
1



x
Y
© 2018 HORIBA, Ltd. All rights reserved.
Distribution Width
• Polydispersity Index
(PI, PDI)
• Span
• Geometric Std. Dev.
• Variance
• Etc…
© 2018 HORIBA, Ltd. All rights reserved.
Note: Span typically = (d90 – d10)/ d50
For Your Reference
© 2018 HORIBA, Ltd. All rights reserved.
For Your Reference
© 2018 HORIBA, Ltd. All rights reserved.
Error Calculations in LA-960 only
For Your Reference
© 2018 HORIBA, Ltd. All rights reserved.
Skewness
© 2018 HORIBA, Ltd. All rights reserved.
From highest to lowest peak:
red, kurtosis 3
orange, kurtosis 2
green, kurtosis 1.2
black, kurtosis 0,
cyan, kurtosis −0.593762…
blue, kurtosis −1
magenta, kurtosis −1.2
Kurtosis (Peakedness)
© 2018 HORIBA, Ltd. All rights reserved.
r = 1 µm r =2 µm r = 3 µm
v = 4 = 32 = 108
V = 4  r3
3
V*3 = 12 96 324 Total = 12+96+324 = 432
12/432=2.8% 96/432=22.2% 324/432=75%
Number vs. Volume Distributions
© 2018 HORIBA, Ltd. All rights reserved.
Beans!
© 2018 HORIBA, Ltd. All rights reserved.
Equivalent Volume Distributions
© 2018 HORIBA, Ltd. All rights reserved.
Equivalent Volume Distributions
© 2018 HORIBA, Ltd. All rights reserved.
Equivalent Number Distributions
© 2018 HORIBA, Ltd. All rights reserved.
Equivalent Number Distributions
© 2018 HORIBA, Ltd. All rights reserved.
Comparing Distribution Bases
• Same material shown as volume, number and area
distribution
Volume
Area
Number
12
4
8
10
6
2
0
PercentinChannel
0.34
4.47
8.82
34.25
0.58
1.15
2.27
17.38Particle Size
Volume Distribution
Mean = 12.65µm
Median=11.58 µm
SA=13467 cm2/cm3
Std Dev.=8.29
Number Distribution
Mean = 0.38µm
Median=0.30 µm
SA=13467 cm2/cm3
Std Dev.=0.40
© 2018 HORIBA, Ltd. All rights reserved.
Statistical Issues with Distributions
• L Neumann, E T White, T Howes (Univ.
Queensland) “What does a mean size
mean?” 2003 AIChE presentation at Session
39 Characterization of Engineered particles
November 16 - 21 San Francisco
Other references:
• L Neumann, T Howes, E T White (2003) Breakage can cause mean
size to increase Dev. Chem. Eng. Mineral Proc. J.
• White E T, Lawrence J. (1970), Variation of volume surface mean for
growing particles, Powder Technology,4, 104 - 107
© 2018 HORIBA, Ltd. All rights reserved.
Does the Mean Match the Process?
• Particle size measurements often made to
monitor a process
– Size reduction (milling)
– Size growth (agglomeration)
• Does the measured/calculated mean diameter
describe the change due to the process?
• It depends on which mean used…
© 2018 HORIBA, Ltd. All rights reserved.
10 x1 m
100 m
breaks into two smaller particles
10 x 1 m
79.4 m
79.4 m
Size Reduction Scenario
© 2018 HORIBA, Ltd. All rights reserved.
Size Reduction: Number Mean
Ten particles of size 1; one of size 100 units
Number mean = D[1, 0] = (10*1 + 1*100)/11 = 10 units
..
Mean = (10*1+2*79.37)/12 = 14.06 units
Surprise, surprise a 40.6% increase!
Largest particle (100) breaks into two of 79.37
(conserves volume/mass: 2 @ 79.373 = 1 @ 1003)
Have broken one
What happens to the number mean?
© 2018 HORIBA, Ltd. All rights reserved.
Size Reduction: Volume Mean
Ten particles of size 1; one of size 100 units
Volume Moment Mean
D[4, 3] = (10*14 + 1*1004)/(10*13 + 1*1003) ~ 100 units
..
New D[4, 3] = (10*14+2*79.374)/(10*13 +2*79.373) ~ 79.37 units
This shows the expected behavior
Largest particle (100) breaks into two of 79.37
(conserves volume/mass: 2 @ 79.373 = 1 @ 1003)
Have broken one
What happens to the D[4, 3]?
© 2018 HORIBA, Ltd. All rights reserved.
Number mean = 10 Number mean = 14
Volume mean = 100 Volume mean = 79
Can You See the Problem?
© 2018 HORIBA, Ltd. All rights reserved.
10 1 m 10 1 m
10 46.4 m
1 100 m
Ten 46.4 m particles agglomerate into one 100 m particle
Size Growth Scenario
© 2018 HORIBA, Ltd. All rights reserved.
Growth: Number Mean
Ten particles of size 1; ten of size 46.42
D[1, 0] = (10*1 + 10*46.42)/20 = 23.71 units
.
Mean = (10*1+1*100)/11 = 10 units
Over a 50% decrease!
Ten of 46.42 agglomerate into one of 100
(conserves volume/mass: 10 @ 46.423 = 1 @ 1003)
Have agglomerated half; does mean increase?
© 2018 HORIBA, Ltd. All rights reserved.
Growth: Volume Mean
Ten particles of size 1; ten of size 46.42
D[4, 3] = (10*14 + 10*46.424)/(10*13 + 10*46.423)
~ 46.4 units
(Note again the volume moment mean is dominated by the large
particles)
.
D[4, 3] = (10*14+1*1004)/10*13 + 1*1003 ~ 100 units
This shows the expected behavior
Ten of 46.42 agglomerate into one of 100
(conserves volume/mass: 10 @ 46.423 = 1 @ 1003)
Have agglomerated half; does mean increase?
© 2018 HORIBA, Ltd. All rights reserved.
Number mean = 24 Number mean = 10
Volume mean = 46 Volume mean = 100
Can You See the Problem?
© 2018 HORIBA, Ltd. All rights reserved.
Practical Implications
• Not just a “party trick” topic!
“Do you know you can break particles and
the mean will increase?”
 Serious. “Did an experiment. I thought I
broke particles but the mean has increased”
(REAL experience)
 Should be aware it can happen!
 Analyse whole size distribution, not mean
alone.
© 2018 HORIBA, Ltd. All rights reserved.
METHODS OF ANALYSIS
PARTICLE MEASUREMENT
METHODS
© 2018 HORIBA, Ltd. All rights reserved.
• Why should one consider various
methods of particle size analysis?
– Material suppliers and users employ many
different types of instruments
– Use a different technique = get a different
answer
– It is important to understand how analysis
methods differ in order to know how to
compare data
PSA Method is Important
© 2018 HORIBA, Ltd. All rights reserved.
Size Range by Technique (m)
0.01 0.1 1 10 100 1000
Colloidal
Suspensions and Slurries
DLS – SZ-100
Electron Microscope
Powders
Fine Coarse
Optical Microscopy PSA300, Camsizer
Laser Diffraction – LA-960
Acoustic Spectroscopy
Electrozone Sensing
Disc-Centrifuge
Light Obscuration
0.001
Macromolecules
Nano-Metric
MethodsAppsSizes
Sedimentation
Sieves
© 2018 HORIBA, Ltd. All rights reserved.
Which Analyzer?
Size, desired resolution, and budget determine technology and
product. For a given problem the choice is often clear.
ViewSizer 3000
PSA-300
CAMSIZER X2
CAMSIZER
LA-350
LA-960
SZ-100
Size AND shape
© 2018 HORIBA, Ltd. All rights reserved.
What Size is Measured?
Laser Diffraction
Equivalent Spherical Diameter
Dynamic Light Scattering
Hydrodynamic Radius
Image Analysis
Lengths, Widths, Equivalent Spherical
Acoustic Spectroscopy
Equivalent Spherical Diameter
© 2018 HORIBA, Ltd. All rights reserved.
Particle Shape Definitions
Acicular: Needle-shaped, rigid
Angular: Edgy, hard angles
Fibrous: Thread-like, non-rigid
Granular/Blocky: Irregular-shaped, low aspect-ratio
Spherical: Regular-shaped, unity aspect ratio
Aspect ratio: Breadth / length OR Length / breadth
Sphericity: How spherical is the particle?
Roundness: How round is the particle?
© 2018 HORIBA, Ltd. All rights reserved.
Poll!
What are the shapes of your particles?
© 2018 HORIBA, Ltd. All rights reserved.
Hegman Gauge
• Used in paint and coatings industry
– Device has tapered center
channel
– Slurry is placed in
channel, then straight
edge is drawn across it
– “Hegman Number” is
where particles disturb
smooth surface of slurry
– Information from largest
particles only – no
distribution
© 2018 HORIBA, Ltd. All rights reserved.
Sieves
• Weigh % sample caught
on known screen sizes
• Solid particles 30 m – 30
mm (and larger)
Advantages:
Low equipment
cost
Direct
measurement
method
No practical upper
limit
Disadvantages:
Limited lower
range
Time
Consuming
High Labor Cost
Need Large
Sample
Available through www.retsch.com
© 2018 HORIBA, Ltd. All rights reserved.
Electrical Sensing Zone
• Coulter Principle
– Based on change in
conductivity of aperture
as particle traverses.
– Requires conducting
liquid.
– Directly measures
particle volume and
counts.
– High resolution
– Used for blood cell
counting more than
industrial applications
© 2018 HORIBA, Ltd. All rights reserved.
Light Obscuration
• Light Obscuration:
Advantages:
• Particle count available
• USP<788> testing
• High resolution histogram
Disadvantages:
• Dilution required for
particle size analysis
• Prone to cell clogging
Light Source
Liquid Flow
Sensing Zone
DetectorLight is blocked by single particles as
they traverse the light beam
© 2018 HORIBA, Ltd. All rights reserved.
Sedimentation
• Stokes Law
Time
Sedimentation of same density
material in a viscous medium
Vp = Settling velocity of discrete particle
g = Gravity constant
ρp = Density of Particle
ρl = Density of Carrier Fluid
µ = Viscosity of Carrier Fluid
Note: assumes settling of spherical particle
Under-sizes compared to other techniques if non-spherical
 g
V
D
lp
p




18
© 2018 HORIBA, Ltd. All rights reserved.
Sedimentation Issues
• Comparison of Brownian Motion and Gravitational
Settling
• Below 1 micrometer, Brownian motion becomes an appreciable factor in
particle dynamics. Gravity sedimentation may not be an appropriate
measurement technique for very small particles.
Particle Diameter
(In micrometers)
Movement due to
Brownian Motion
Movement due to
Gravitational Settling
0.01 2.36 >> 0.005
0.25 1.49 > 0.0346
0.50 1.052 > 0.1384
1.0 0.745 ~ 0.554
2.5 0.334 < 13.84
10.0 0.236 << 55.4
(Movement in 1 second; Particle density of 2.0 grams/cc)
© 2018 HORIBA, Ltd. All rights reserved.
Particles in suspension undergo Brownian
motion due to bombardment by solvent
molecules in random thermal motion.
Most common technique for sub-micron sizing
Range: 1 nm – 1 m*
* Density dependent, when does settling become prominent motion?
D6
kT
RH


Autocorrelation
Function
Signal
Stokes-Einstein
Dynamic Light Scattering
© 2018 HORIBA, Ltd. All rights reserved.
Manual Microscopy
• Count particles in a given
field of view
• Use graticule to obtain size
• Repeat this process for a
number of fields
• At least hundreds of particles
must be sized
Advantages:
Simple
Inexpensive
Can see shape
Disadvantages:
Slow
Measures very few particles
Very tedious
© 2018 HORIBA, Ltd. All rights reserved.
Dynamic:
Particles flow past camera(s)
Static:
Particles fixed on slide,
stage moves slide
Automated Microscopy
© 2018 HORIBA, Ltd. All rights reserved.
Image Acquisition
and enhancement
Thresholding
Image Processing
Measurements
Objective &
camera
Subjective or
automatic
Decisions or
black box
Advantages:
Quick size + shape info
Statistically valid
High resolution
Particle images
Disadvantages:
Expense
Knowing which
numbers are
important
Automated Microscopy
© 2018 HORIBA, Ltd. All rights reserved.
Acoustic Spectroscopy
• Acoustic signal sent into
concentrated sample
• Detector measure
attenuation f (frequency,
distance from source)
Advantages:
• Can accommodate high
sample concentrations
(no dilution)
• Rheological properties
• Also measure zeta potential
Disadvantages:
• Need at least 1 wt% particles
• Need to know wt%
• Minimum sample = 15 ml
Detector
Signal
source
Signal output
© 2018 HORIBA, Ltd. All rights reserved.
Laser Diffraction
•Converts scattered light to
particle size distribution
•Quick, repeatable
•Powders, suspensions
•Most common technique
© 2018 HORIBA, Ltd. All rights reserved.
Key Points
• Particle Analysis is about distributions
• Define terms (results) exactly
– Volume vs. Number
• Different techniques give different answers
since they measure different things
– All are correct…
• Discuss results in terms of technique.
© 2018 HORIBA, Ltd. All rights reserved.
© 2018 HORIBA, Ltd. All rights reserved. 71
© 2018 HORIBA, Ltd. All rights reserved.
Danke
Большое спасибо
Grazie
Σας ευχαριστούμε
감사합니다
Obrigado
谢谢
ขอบคุณครับ
ありがとうございました
धन्यवाद
நன்ற
Cảm ơn
Dziękuję
Tack ska ni ha
Thank you
Merci
Gracias

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Particle Classroom Series I: Introduction to Particle Analysis

  • 1. © 2018 HORIBA, Ltd. All rights reserved. Introduction to Particle Size Analysis Jeff Bodycomb, Ph.D. jeff.bodycomb@horiba.com www.horiba.com/us/particle
  • 2. © 2018 HORIBA, Ltd. All rights reserved. Why Particle Size? Industry Industry Ceramic Construction Oil/rubber Chemical Battery Pharmaceutical Electricity Food/Drink Automobile Paper/Pulp Mining Ink/Toner Size affects material behavior and processing across a number of industries.
  • 3. © 2018 HORIBA, Ltd. All rights reserved. Application: Pigment Hiding Power Operator dependent, need to wait for drying. Operator independent, no need to wait for drying.
  • 4. © 2018 HORIBA, Ltd. All rights reserved. Size Terminology The most common designation is micrometers or microns. When very small, in colloid region, measured in nanometers, with electron microscopes or by dynamic light scattering. 10-10 10-810-9 10-610-7 10-410-5 10-210-3 10-1 10-0 meternanometer Angstrom (Å) micrometer millimeter micron or µm mnm mm 0.1µm 1.0µm 10µm 100µm 100 nm Fun tip: Describing your work in terms of beard-seconds make it much more interesting at parties. “beard-second” C-H bond length
  • 5. © 2018 HORIBA, Ltd. All rights reserved. Poll! Which size ranges do you measure?
  • 6. © 2018 HORIBA, Ltd. All rights reserved. Size: Particle Diameter (m) 0.01 0.1 1 10 100 1000 Colloidal Suspensions and Slurries DLS – SZ-100 Electron Microscope Powders Fine Coarse Optical Microscopy PSA300, Camsizer Laser Diffraction – LA-960 Acoustic Spectroscopy Electrozone Sensing Disc-Centrifuge Light Obscuration 0.001 Macromolecules Nano-Metric MethodsAppsSizes Sedimentation Sieves
  • 7. © 2018 HORIBA, Ltd. All rights reserved. The Basics Which is the most meaningful size? different size definitions different results
  • 8. © 2018 HORIBA, Ltd. All rights reserved. Same data, different size definitions give different results! different size definitions different results xcmin  xArea  xFemax x [mm ]0 .2 0 .4 0 .6 1 0 10 20 30 40 50 60 70 80 Q3 [% ] Samp leA_Bas ic_0 .2% _xc_m in_001 .rd f Samp leA_Bas ic_0 .2% _x_area_001 .rd f Samp leA_Bas ic_0 .2% _xFemax_001 .rd f G raph o fmeasu remen t resu lts : M :...rD is tribu toren-Mee ting CAMDAT Samp leA Samp leA_Bas ic_0 .2% _xc_m in_001 .rd f Task file :Samp leA_Bas ic_0 .2% .a fg x [mm ]0 .2 0 .4 0 .6 1 0 10 20 30 40 50 60 70 80 Q3 [% ] Samp leA_Bas ic_0 .2% _xc_m in_001 .rd f Samp leA_Bas ic_0 .2% _x_area_001 .rd f Samp leA_Bas ic_0 .2% _xFemax_001 .rd f G raph o fmeasu remen t resu lts : M :...rD is tribu toren-Mee ting CAMDAT Samp leA Samp leA_Bas ic_0 .2% _xc_m in_001 .rd f Task file :Samp leA_Bas ic_0 .2% .a fg 2 x[mm]
  • 9. © 2018 HORIBA, Ltd. All rights reserved. The Basics What sizes can be measured?
  • 10. © 2018 HORIBA, Ltd. All rights reserved. Size Definitions • Martins’s Diameter: The distance between opposite sides of a particle measured on a line bisecting the projected area. To ensure statistical significance all measurements are made in the same direction regardless of particle orientation. • Feret’s Diameter: The distance between parallel tangents on opposite sides of the particle profile. Again to insure statistical significance, all measurements are made in the same direction regardless of particle orientation. • Note: Both Martin’s and Feret’s diameters are generally used for particle size analysis by optical and electron microscopy. • Equivalent Circle Diameter: The diameter of a circle having an area equal to the projected area of the particle in random orientation. This diameter is usually determined subjectively and measured by oracular micrometers called graticules. • Equivalent Spherical Diameter: The diameter of a sphere that has the same volume as the irregular particle being examined. Martin’s Diameter Feret’s Diameter Equivalent Spherical Diameter
  • 11. © 2018 HORIBA, Ltd. All rights reserved. Particle Orientation • Martin’s and Feret’s Diameter’s will vary as particles are viewed in different orientations. The result will be a DISTRIBUTION from smallest to largest. Martin’s Diameter Feret’s Diameter Equivalent Spherical Diameter Martin’s Diameter Feret’s Diameter Equivalent Spherical Diameter
  • 12. © 2018 HORIBA, Ltd. All rights reserved. The Basics Particle Particle Distribution
  • 13. © 2018 HORIBA, Ltd. All rights reserved. The Basics Particle Size Particle Size Distribution 4 µm
  • 14. © 2018 HORIBA, Ltd. All rights reserved. Poll! What size(s) are reported by your PSA?
  • 15. © 2018 HORIBA, Ltd. All rights reserved. Monodisperse vs. Polydisperse • Monodisperse Distribution: – All particles are the same size – Latex standards • Wide Distribution: – Particles of Many Sizes – Everything else VOLUME VOLUME Particle Size Particle Size Monodisperse Polydisperse
  • 16. © 2018 HORIBA, Ltd. All rights reserved. Logarithmic vs. Linear Scale • Logarithmic X-Axis Distribution • Linear X-Axis Distribution VOLUME Particle Size 0 10 20 30 40 50 60 70 80 90 100 VOLUME Particle Size 0 10 100
  • 17. © 2018 HORIBA, Ltd. All rights reserved. Distribution Display – Represented by series of segments or channels known as histogram. – Number of channels based on design, practicality and aesthetics VOLUME Particle Size Cumulative Distribution Differential Distribution Histogram
  • 18. © 2018 HORIBA, Ltd. All rights reserved. Frequency Frequency + cumulative (undersize) Histogram Multiple frequency + cumulative (undersize) Your Analyzer’s Displays
  • 19. © 2018 HORIBA, Ltd. All rights reserved. Central Values Mean Median and Mode Size Mean Weighted Average Center of Gravity Median 50% Point Mode Peak of the distribution Most common value
  • 20. © 2018 HORIBA, Ltd. All rights reserved. Three spheres of diameters 1,2,3 units What is the average size of these spheres? Average size = (1+2+3) ÷ 3 =2.00 This is called the D[1,0] - the number mean 1 2 3 What does “Mean” mean?
  • 21. © 2018 HORIBA, Ltd. All rights reserved. None of the answers are wrong they have just been calculated using different techniques X Dnl     [ , ] .1 0 1 2 3 3 2 00 X Dns     [ , ] .2 0 1 4 9 3 216 X Dnv     [ , ] .3 0 1 8 27 3 2 293 X Dsv       [ , ] .3 2 1 8 27 1 2 3 2 57 X Dvm       [ , ] .4 3 1 16 81 1 8 27 2 72 Many possible Mean values Number weighted mean Diameter (length) Volume weighted mean diameter Volume/surface mean, Mean volume diameter Mean surface diameter
  • 22. © 2018 HORIBA, Ltd. All rights reserved. Moment Ratios: ISO 9276-2  qp q ii p ii Dn Dn qpD             1 ],[ qp             q ii i p ii Dn DDn qpD ln exp],[ qp  For your reference
  • 23. © 2018 HORIBA, Ltd. All rights reserved. D[4,3] which is often referred to as the Volume Mean Diameter [ VMD ] D [4,3] =   i i i i D n D n 4 3 Monitoring the D[4,3] value in your specification will emphasize the detection of large particles Volume-based Mean diameter
  • 24. © 2018 HORIBA, Ltd. All rights reserved. Mode Median Mean D[4,3] Size Remember: D[4,3] is sensitive to large particles Central Values revisited Mean Weighted Average Center of Gravity Median 50% Point Mode Peak of the distribution Most common value
  • 25. © 2018 HORIBA, Ltd. All rights reserved. D(v,0.9)D(v,0.1) Size µm D(4,3) sensitive to large particles D(3,2) D(v,0.5) median D(v,1.0) Never use the D100! sensitive to small particles 10% of the particles lie below this diameter 90% of the particles lie below this diameter half are larger than this diameterhalf are smaller than this diameter Most Common Statistics
  • 26. © 2018 HORIBA, Ltd. All rights reserved. Standard Deviation • Normal (Gaussian) Distribution Curve •  = distribution mean •  = standard deviation • Exp = base of natural logarithms Mean +1 STD DEV-1 STD DEV +2 STD DEV-2 STD DEV 68.27% 95.45%           2 2 2 exp 2 1    x Y
  • 27. © 2018 HORIBA, Ltd. All rights reserved. Distribution Width • Polydispersity Index (PI, PDI) • Span • Geometric Std. Dev. • Variance • Etc…
  • 28. © 2018 HORIBA, Ltd. All rights reserved. Note: Span typically = (d90 – d10)/ d50 For Your Reference
  • 29. © 2018 HORIBA, Ltd. All rights reserved. For Your Reference
  • 30. © 2018 HORIBA, Ltd. All rights reserved. Error Calculations in LA-960 only For Your Reference
  • 31. © 2018 HORIBA, Ltd. All rights reserved. Skewness
  • 32. © 2018 HORIBA, Ltd. All rights reserved. From highest to lowest peak: red, kurtosis 3 orange, kurtosis 2 green, kurtosis 1.2 black, kurtosis 0, cyan, kurtosis −0.593762… blue, kurtosis −1 magenta, kurtosis −1.2 Kurtosis (Peakedness)
  • 33. © 2018 HORIBA, Ltd. All rights reserved. r = 1 µm r =2 µm r = 3 µm v = 4 = 32 = 108 V = 4  r3 3 V*3 = 12 96 324 Total = 12+96+324 = 432 12/432=2.8% 96/432=22.2% 324/432=75% Number vs. Volume Distributions
  • 34. © 2018 HORIBA, Ltd. All rights reserved. Beans!
  • 35. © 2018 HORIBA, Ltd. All rights reserved. Equivalent Volume Distributions
  • 36. © 2018 HORIBA, Ltd. All rights reserved. Equivalent Volume Distributions
  • 37. © 2018 HORIBA, Ltd. All rights reserved. Equivalent Number Distributions
  • 38. © 2018 HORIBA, Ltd. All rights reserved. Equivalent Number Distributions
  • 39. © 2018 HORIBA, Ltd. All rights reserved. Comparing Distribution Bases • Same material shown as volume, number and area distribution Volume Area Number 12 4 8 10 6 2 0 PercentinChannel 0.34 4.47 8.82 34.25 0.58 1.15 2.27 17.38Particle Size Volume Distribution Mean = 12.65µm Median=11.58 µm SA=13467 cm2/cm3 Std Dev.=8.29 Number Distribution Mean = 0.38µm Median=0.30 µm SA=13467 cm2/cm3 Std Dev.=0.40
  • 40. © 2018 HORIBA, Ltd. All rights reserved. Statistical Issues with Distributions • L Neumann, E T White, T Howes (Univ. Queensland) “What does a mean size mean?” 2003 AIChE presentation at Session 39 Characterization of Engineered particles November 16 - 21 San Francisco Other references: • L Neumann, T Howes, E T White (2003) Breakage can cause mean size to increase Dev. Chem. Eng. Mineral Proc. J. • White E T, Lawrence J. (1970), Variation of volume surface mean for growing particles, Powder Technology,4, 104 - 107
  • 41. © 2018 HORIBA, Ltd. All rights reserved. Does the Mean Match the Process? • Particle size measurements often made to monitor a process – Size reduction (milling) – Size growth (agglomeration) • Does the measured/calculated mean diameter describe the change due to the process? • It depends on which mean used…
  • 42. © 2018 HORIBA, Ltd. All rights reserved. 10 x1 m 100 m breaks into two smaller particles 10 x 1 m 79.4 m 79.4 m Size Reduction Scenario
  • 43. © 2018 HORIBA, Ltd. All rights reserved. Size Reduction: Number Mean Ten particles of size 1; one of size 100 units Number mean = D[1, 0] = (10*1 + 1*100)/11 = 10 units .. Mean = (10*1+2*79.37)/12 = 14.06 units Surprise, surprise a 40.6% increase! Largest particle (100) breaks into two of 79.37 (conserves volume/mass: 2 @ 79.373 = 1 @ 1003) Have broken one What happens to the number mean?
  • 44. © 2018 HORIBA, Ltd. All rights reserved. Size Reduction: Volume Mean Ten particles of size 1; one of size 100 units Volume Moment Mean D[4, 3] = (10*14 + 1*1004)/(10*13 + 1*1003) ~ 100 units .. New D[4, 3] = (10*14+2*79.374)/(10*13 +2*79.373) ~ 79.37 units This shows the expected behavior Largest particle (100) breaks into two of 79.37 (conserves volume/mass: 2 @ 79.373 = 1 @ 1003) Have broken one What happens to the D[4, 3]?
  • 45. © 2018 HORIBA, Ltd. All rights reserved. Number mean = 10 Number mean = 14 Volume mean = 100 Volume mean = 79 Can You See the Problem?
  • 46. © 2018 HORIBA, Ltd. All rights reserved. 10 1 m 10 1 m 10 46.4 m 1 100 m Ten 46.4 m particles agglomerate into one 100 m particle Size Growth Scenario
  • 47. © 2018 HORIBA, Ltd. All rights reserved. Growth: Number Mean Ten particles of size 1; ten of size 46.42 D[1, 0] = (10*1 + 10*46.42)/20 = 23.71 units . Mean = (10*1+1*100)/11 = 10 units Over a 50% decrease! Ten of 46.42 agglomerate into one of 100 (conserves volume/mass: 10 @ 46.423 = 1 @ 1003) Have agglomerated half; does mean increase?
  • 48. © 2018 HORIBA, Ltd. All rights reserved. Growth: Volume Mean Ten particles of size 1; ten of size 46.42 D[4, 3] = (10*14 + 10*46.424)/(10*13 + 10*46.423) ~ 46.4 units (Note again the volume moment mean is dominated by the large particles) . D[4, 3] = (10*14+1*1004)/10*13 + 1*1003 ~ 100 units This shows the expected behavior Ten of 46.42 agglomerate into one of 100 (conserves volume/mass: 10 @ 46.423 = 1 @ 1003) Have agglomerated half; does mean increase?
  • 49. © 2018 HORIBA, Ltd. All rights reserved. Number mean = 24 Number mean = 10 Volume mean = 46 Volume mean = 100 Can You See the Problem?
  • 50. © 2018 HORIBA, Ltd. All rights reserved. Practical Implications • Not just a “party trick” topic! “Do you know you can break particles and the mean will increase?”  Serious. “Did an experiment. I thought I broke particles but the mean has increased” (REAL experience)  Should be aware it can happen!  Analyse whole size distribution, not mean alone.
  • 51. © 2018 HORIBA, Ltd. All rights reserved. METHODS OF ANALYSIS PARTICLE MEASUREMENT METHODS
  • 52. © 2018 HORIBA, Ltd. All rights reserved. • Why should one consider various methods of particle size analysis? – Material suppliers and users employ many different types of instruments – Use a different technique = get a different answer – It is important to understand how analysis methods differ in order to know how to compare data PSA Method is Important
  • 53. © 2018 HORIBA, Ltd. All rights reserved. Size Range by Technique (m) 0.01 0.1 1 10 100 1000 Colloidal Suspensions and Slurries DLS – SZ-100 Electron Microscope Powders Fine Coarse Optical Microscopy PSA300, Camsizer Laser Diffraction – LA-960 Acoustic Spectroscopy Electrozone Sensing Disc-Centrifuge Light Obscuration 0.001 Macromolecules Nano-Metric MethodsAppsSizes Sedimentation Sieves
  • 54. © 2018 HORIBA, Ltd. All rights reserved. Which Analyzer? Size, desired resolution, and budget determine technology and product. For a given problem the choice is often clear. ViewSizer 3000 PSA-300 CAMSIZER X2 CAMSIZER LA-350 LA-960 SZ-100 Size AND shape
  • 55. © 2018 HORIBA, Ltd. All rights reserved. What Size is Measured? Laser Diffraction Equivalent Spherical Diameter Dynamic Light Scattering Hydrodynamic Radius Image Analysis Lengths, Widths, Equivalent Spherical Acoustic Spectroscopy Equivalent Spherical Diameter
  • 56. © 2018 HORIBA, Ltd. All rights reserved. Particle Shape Definitions Acicular: Needle-shaped, rigid Angular: Edgy, hard angles Fibrous: Thread-like, non-rigid Granular/Blocky: Irregular-shaped, low aspect-ratio Spherical: Regular-shaped, unity aspect ratio Aspect ratio: Breadth / length OR Length / breadth Sphericity: How spherical is the particle? Roundness: How round is the particle?
  • 57. © 2018 HORIBA, Ltd. All rights reserved. Poll! What are the shapes of your particles?
  • 58. © 2018 HORIBA, Ltd. All rights reserved. Hegman Gauge • Used in paint and coatings industry – Device has tapered center channel – Slurry is placed in channel, then straight edge is drawn across it – “Hegman Number” is where particles disturb smooth surface of slurry – Information from largest particles only – no distribution
  • 59. © 2018 HORIBA, Ltd. All rights reserved. Sieves • Weigh % sample caught on known screen sizes • Solid particles 30 m – 30 mm (and larger) Advantages: Low equipment cost Direct measurement method No practical upper limit Disadvantages: Limited lower range Time Consuming High Labor Cost Need Large Sample Available through www.retsch.com
  • 60. © 2018 HORIBA, Ltd. All rights reserved. Electrical Sensing Zone • Coulter Principle – Based on change in conductivity of aperture as particle traverses. – Requires conducting liquid. – Directly measures particle volume and counts. – High resolution – Used for blood cell counting more than industrial applications
  • 61. © 2018 HORIBA, Ltd. All rights reserved. Light Obscuration • Light Obscuration: Advantages: • Particle count available • USP<788> testing • High resolution histogram Disadvantages: • Dilution required for particle size analysis • Prone to cell clogging Light Source Liquid Flow Sensing Zone DetectorLight is blocked by single particles as they traverse the light beam
  • 62. © 2018 HORIBA, Ltd. All rights reserved. Sedimentation • Stokes Law Time Sedimentation of same density material in a viscous medium Vp = Settling velocity of discrete particle g = Gravity constant ρp = Density of Particle ρl = Density of Carrier Fluid µ = Viscosity of Carrier Fluid Note: assumes settling of spherical particle Under-sizes compared to other techniques if non-spherical  g V D lp p     18
  • 63. © 2018 HORIBA, Ltd. All rights reserved. Sedimentation Issues • Comparison of Brownian Motion and Gravitational Settling • Below 1 micrometer, Brownian motion becomes an appreciable factor in particle dynamics. Gravity sedimentation may not be an appropriate measurement technique for very small particles. Particle Diameter (In micrometers) Movement due to Brownian Motion Movement due to Gravitational Settling 0.01 2.36 >> 0.005 0.25 1.49 > 0.0346 0.50 1.052 > 0.1384 1.0 0.745 ~ 0.554 2.5 0.334 < 13.84 10.0 0.236 << 55.4 (Movement in 1 second; Particle density of 2.0 grams/cc)
  • 64. © 2018 HORIBA, Ltd. All rights reserved. Particles in suspension undergo Brownian motion due to bombardment by solvent molecules in random thermal motion. Most common technique for sub-micron sizing Range: 1 nm – 1 m* * Density dependent, when does settling become prominent motion? D6 kT RH   Autocorrelation Function Signal Stokes-Einstein Dynamic Light Scattering
  • 65. © 2018 HORIBA, Ltd. All rights reserved. Manual Microscopy • Count particles in a given field of view • Use graticule to obtain size • Repeat this process for a number of fields • At least hundreds of particles must be sized Advantages: Simple Inexpensive Can see shape Disadvantages: Slow Measures very few particles Very tedious
  • 66. © 2018 HORIBA, Ltd. All rights reserved. Dynamic: Particles flow past camera(s) Static: Particles fixed on slide, stage moves slide Automated Microscopy
  • 67. © 2018 HORIBA, Ltd. All rights reserved. Image Acquisition and enhancement Thresholding Image Processing Measurements Objective & camera Subjective or automatic Decisions or black box Advantages: Quick size + shape info Statistically valid High resolution Particle images Disadvantages: Expense Knowing which numbers are important Automated Microscopy
  • 68. © 2018 HORIBA, Ltd. All rights reserved. Acoustic Spectroscopy • Acoustic signal sent into concentrated sample • Detector measure attenuation f (frequency, distance from source) Advantages: • Can accommodate high sample concentrations (no dilution) • Rheological properties • Also measure zeta potential Disadvantages: • Need at least 1 wt% particles • Need to know wt% • Minimum sample = 15 ml Detector Signal source Signal output
  • 69. © 2018 HORIBA, Ltd. All rights reserved. Laser Diffraction •Converts scattered light to particle size distribution •Quick, repeatable •Powders, suspensions •Most common technique
  • 70. © 2018 HORIBA, Ltd. All rights reserved. Key Points • Particle Analysis is about distributions • Define terms (results) exactly – Volume vs. Number • Different techniques give different answers since they measure different things – All are correct… • Discuss results in terms of technique.
  • 71. © 2018 HORIBA, Ltd. All rights reserved. © 2018 HORIBA, Ltd. All rights reserved. 71
  • 72. © 2018 HORIBA, Ltd. All rights reserved. Danke Большое спасибо Grazie Σας ευχαριστούμε 감사합니다 Obrigado 谢谢 ขอบคุณครับ ありがとうございました धन्यवाद நன்ற Cảm ơn Dziękuję Tack ska ni ha Thank you Merci Gracias