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© 2019 HORIBA, Ltd. All rights reserved. 1
© 2019 HORIBA, Ltd. All rights reserved. 2© 2019 HORIBA, Ltd. All rights reserved. 2
Sampling and Dispersion
HORIBA Instruments Inc.
Particle Characterization
Jeff Bodycomb, Ph.D.
October 29, 2019
© 2019 HORIBA, Ltd. All rights reserved. 3
From: NIST Recommended Practice Guide
Special Publication 960-1
Particle Size Characterization
Ajit Jillavenkatesa
Stanley J. Dapkunas
Lin-Sien H. Lum
Materials Science and
Engineering Laboratory
January 2001
Particle Analysis Workflow
© 2019 HORIBA, Ltd. All rights reserved. 4
Outline
• Sampling from bulk
• Sub-sample for measurement
• Disperse sample
– Wet powders, apply air pressure or
ultrasound
• Sometimes second sub-sampling
– From beaker to instrument
• Perform measurement
© 2019 HORIBA, Ltd. All rights reserved. 5
Measurement Error Sources
• SMALL PARTICLES
– POTENTIALLY SMALL
EXTRACTION ERRORS
(A)
– POTENTIALLY LARGE
SAMPLE PREP ERRORS
(C)
• LARGE PARTICLES
– POTENTIALLY LARGE
EXTRACTION ERRORS
(B)
– POTENTIALLY SMALL
SAMPLE PREP ERRORS
(D)
• INSTRUMENT ERROR IS SMALL AND
RELATIVELY CONSTANT
PARTICLE SIZE
SAMPLE PREPARATION SAMPLE EXTRACTION
INSTRUMENT ERROR
%
E
R
R
O
R A
B
C
D
© 2019 HORIBA, Ltd. All rights reserved. 6
Sample Extraction:
Good Sampling Practices
Learn to Love Your Riffler!
© 2019 HORIBA, Ltd. All rights reserved. 7
Sampling from Flowing Powder
© 2019 HORIBA, Ltd. All rights reserved. 8
Powder Thief
www.samplingsystems.com
Sampling from Drums
© 2019 HORIBA, Ltd. All rights reserved. 9
www.samplingsystems.com
Sampling from Drums
© 2019 HORIBA, Ltd. All rights reserved. 10
Sub-sampling for Measurement
• Not all of sample brought to lab is
analyzed
• Must sub-divide sample
• How to introduce representative
sample into instrument?
© 2019 HORIBA, Ltd. All rights reserved. 11
Technique: Grab Sampling
• PLACE SPATULA INTO POWDER
• EXTRACT SMALL AMOUNT FOR ANALYSIS
• ACCEPTABLE FOR NARROW DISTRIBUTIONS
• SEGREGATE LARGE AND SMALL WHEN POLYDISPERSE
– LARGE PARTICLES PERCOLATE UPWARD
– SMALL PARTICLES GRAVITATE DOWNWARD
• EASY METHOD
• MOST USED METHOD
© 2019 HORIBA, Ltd. All rights reserved. 12
Grab Sampling from Bottle
• When a powder is stored in
a container, it can be mixed
by rolling and tumbling the
container. The container
should not be more than
half to two-thirds full. It is
important to perform this
action before “grabbing” a
sample with a spatula.
• Then pull sample with a spatula…..
© 2019 HORIBA, Ltd. All rights reserved. 13
Technique: Coning & Quartering
•Pile of powder is divided into 4
sections.
•Two diagonal sections are
discarded, and two are retained and
mixed together.
•Mixture is again divided into 4
sections, and two diagonal sections
are mixed.
•Process is repeated until remaining
sample is correct amount for
analysis.
•Can be carried out with very small
sample amount or very large
samples.
© 2019 HORIBA, Ltd. All rights reserved. 14
Technique: Chute Riffling
•Chute splitting allows
sample to vibrate down a
chute to vanes which
separate the mass into two
portions. Each portion
moves further where they
each are divided into two
parts, now giving four parts.
This may be continued until
usually 8 or 16 portions are
obtained.
© 2019 HORIBA, Ltd. All rights reserved. 15
Technique: Rotary Riffling
• The best method of representative splitting
of powders is the ROTARY RIFFLER. The
complete sample to be split is directed
down a chute into open containers. Each
container will receive a sample which is
representative of the original bulk material
because the distribution of material is
averaged over time. The complete amount
of the original bulk sample must be
consumed.
• These splitters are commercially available from
companies that market various types of sample
splitters.
• See: www.retsch.com
• www.quantachrome.com
• www.microscal.com
© 2019 HORIBA, Ltd. All rights reserved. 16
Sample Dividers
© 2019 HORIBA, Ltd. All rights reserved. 17
Sampling Technique Error Levels
• Standard Deviation (σ) in % Sugar-Sand Mixture
• SCOOP SAMPLING 6.31
• TABLE SAMPLING 2.11
• CHUTE RIFFLER 1.10
• SPINNING RIFFLER 0.27
• Density of sand and sugar respectively 2.65 and 1.64 g/ml
• Reference: Allen, T. and Khan, A.A. (1934), Chem Eng, 238, CE 108-112
© 2019 HORIBA, Ltd. All rights reserved. 18
Technique: Sampling from Beaker
• Liquid should be in motion
vertically and horizontally to
insure good mixing.
• Pipette should be about one-
third of the way from the
bottom when extracting
sample.
• Alternative: When mixing
powders into a slurry: make
paste, pipette from paste
IMPELLER PIPETTE
© 2019 HORIBA, Ltd. All rights reserved. 19
Measurement Error Sources
• SMALL PARTICLES
– POTENTIALLY SMALL
EXTRACTION ERRORS
(A)
– POTENTIALLY LARGE
SAMPLE PREP ERRORS
(C)
• LARGE PARTICLES
– POTENTIALLY LARGE
EXTRACTION ERRORS
(B)
– POTENTIALLY SMALL
SAMPLE PREP ERRORS
(D)
• INSTRUMENT ERROR IS SMALL AND RELATIVELY
CONSTANT
PARTICLE SIZE
SAMPLE PREPARATION SAMPLE EXTRACTION
INSTRUMENT ERROR
%
E
R
R
O
R A
B
C
D
© 2019 HORIBA, Ltd. All rights reserved. 20
Sample Preparation:
Dispersions
© 2019 HORIBA, Ltd. All rights reserved. 21
Dispersion Strategies
Powders
When measuring powder as suspension
Choose solvent (avoid dissolution)
Wet powder (surfactant)
Dispersing aid to avoid re-agglomeration
Energy to break agglomerates into primary particles
Pump & stirrer or ultrasound
Suspensions
Dilute
Energy
© 2019 HORIBA, Ltd. All rights reserved. 22
Dispersion Definitions
• WELL DISPERSED particles can be easily detected under
an optical microscope. They are separated from one
another and show no tendency to cling together.
• AGGLOMERATED particles appear in clumps that can be
separated easily by the application of moderate
amounts of energy, such as ultrasonic baths.
• AGGREGATED particles are tightly bound and must be
treated with higher levels of energy. Usually an
ultrasonic probe applied directly to the sample slurry
will disperse the particles. If they are very tightly
bound, they may fracture before they can be separated.
WELL DISPERSED AGGLOMERATED AGGREGATED
© 2019 HORIBA, Ltd. All rights reserved. 23
θ
θ
θ
DROP OF LIQUID ON A SOLID
SMALL (Phylic)
LARGE
(Phobic)
Particle Wetting
• CONTACT ANGLE ( θ )
• The contact angle is a measure of how
well the liquid drop adheres to the
surface of a solid
• Large angles indicate poor wetting
ability.
• Small angles indicate good wetting
ability.
• Surfactants reduce surface tension and
thereby are conducive to good wetting.
• (Instruments are available for
measuring contact angle)
© 2019 HORIBA, Ltd. All rights reserved. 24
Particle Wetting
• Surface tension must be
lowered so liquid will
adhere to particles.
+
+
++
+
+
+
+
+
PARTICLE
LIQUID
GOAL IS TO COMPLETELY COAT
PARTICLE WITH LIQUID
qq
Small Contact
Angle
Good Wetting
Large
Contact
Angle
Bad Wetting
© 2019 HORIBA, Ltd. All rights reserved. 25
Screening for wetting agent
Set up vials or beakers with each candidate dispersant.
Gently put a little bit of fine particle on the top of each.
© 2019 HORIBA, Ltd. All rights reserved. 26
Evaluate Wetting
Poor wetting: particles don’t
break surface tension
Good wetting: particles separate
and stream through surface
© 2019 HORIBA, Ltd. All rights reserved. 27
MEAN
PARTICLE
SIZE
SURFACTANT CONCENTRATION
Effect of Surfactant Addition
• Addition of surfactant to a
sample will disperse the
particles so a proper
measurement may be made.
However, addition of too
much surfactant will cause
agglomeration.
• The graph illustrates that there is an optimum amount of
surfactant to effect optimum dispersion. The Particle Size
Analyzer can determine when the amount of surfactant exceeds
the proper concentration.
• As initial surfactant is added, the mean particle size will
decrease. It will reach a minimum as the proper surfactant
concentration is reached.
• As additional surfactant is added, the apparent mean particle
size will increase, indicating agglomeration of particles.
• Common concentration: 0.01-0.1%
© 2019 HORIBA, Ltd. All rights reserved. 28
NON-POLAR HYDROCARBON
POLAR IONIC DIPOLE
Surfactant Mechanism
•EQUILIBRIUM
established
between
SURFACTANT ON
PARTICLES and
SURFACTANT IN
SOLUTION.
© 2019 HORIBA, Ltd. All rights reserved. 29
Critical Micelle Concentration
• As more surfactant is added, equilibrium shifts.
Surfactant leaves surfaces to start formation of
MICELLES. This is called CRITICAL MICELLE
CONCENTRATION (CMC).
• Particle surfaces are no longer repulsed, and energy of
the system favors REAGGLOMORATION.
-
-
-
-
-
-
-
--
-
-
+++
+
+ +
+
+
+
++
-
MICELLES
+ Cationic Surface
- Anionic Surfactant
+
© 2019 HORIBA, Ltd. All rights reserved. 30
NO SURFACTANT -
AGGLOMERATED PARTICLES
EXCESS SURFACTANT -
REAGGLOMERATION
OF PARTICLES
OPTIMUM CONCENTRATION –
PROPER PARTICLE DISPERSION
Effect of Surfactant Addition
© 2019 HORIBA, Ltd. All rights reserved. 31
Common Surfactants
Nonionic surfactants adsorb to charged and neutral surfaces, create steric
barrier
• Igepal CA630 Ethoxylated octyl phenol Nonionic
• Triton X100 Octylphenoxypolyethoxy ethanol Nonionic
• Tween 20 Polyoxyethylene sorbitan Nonionic
• Aerosol-OT Dioctyl ester Na Sulfo succinic acid Anionic
Cationic surfactants often used for biological samples, strongly bonds to
negatively charged surfaces
Hyrdophobic surface
Polar groups orient to aqueous phase
Anionic surfactant
polar head
non-polar chain
© 2019 HORIBA, Ltd. All rights reserved. 32
Sodium Hexametaphosphate
• Most common stabilizer
• Abbreviated NaHMP
• Keeps particles from re-
agglomerating
• Disperse sample in 0.01 –
1.0% (NaPO3)6 rather than
DI water
• Tetrasodium
pyrophosphate also used
(sodium pyrophosphate,
Na4P2O7)
© 2019 HORIBA, Ltd. All rights reserved. 33
Particle Interactions
• Particles are constantly moving with
respect to one another. When they
approach close enough to cross the
potential barrier (when attractive
forces exceed repulsive forces), they
come together (agglomerate).
• The object is to provide repulsive forces
strong enough to keep particles apart,
even during close approach. This can be
accomplished by surfactant coating of
particle surfaces.
ATTRACTIVE FORCES
(VAN DER WAALS)
REPULSIVE FORCES
(CHARGE)
REPULSIVE FORCES
(CHARGE)
CHARGE CHARGE
+
+
+
+
+
+
+
+
+
+
+
+
© 2019 HORIBA, Ltd. All rights reserved. 34
Inter-particle distance is LARGE.
Van der Waals forces WEAK
Decreasing particle distance
Increasing Van der Waals forces
Particle distance very small
Van der Waals forces strong
+
+
++ ++
+
+
If surfactant charge is
sufficiently high, it will
overcome Van der Waals forces
before the particles approach
closely.
Particle Interactions
© 2019 HORIBA, Ltd. All rights reserved. 35
Vmax
Total Potential Energy
VT
Distance Between Surfaces
0
VT = VA + VR
VA
Attraction
Repulsion
VR
PotentialEnergy
Energy of Interaction
INTERACTION OF
TWO CHARGED
SURFACES
Stability of a system depends on
forces between particles. Random
motion brings them into close
proximity. Whether two particles
will combine depends on potential
barrier between them. Potential
energy consists of two forces, the
ATTRACTIVE one due to Van der
Waals, and the REPULSIVE one due
to electrical double layers around
particles.
If height of the barrier, VT, is lower
than average thermal energy, KT,
then probability is high that two
adjacent particles will eventually
collide. They will probably remain
attached to each other due to
strong Van der Waals forces at very
close distances.
Electrical forces
cause particles
to remain apart.
Van der Waals
forces cause
particles to
come together.
© 2019 HORIBA, Ltd. All rights reserved. 36
Dispersion Stability
steric stabilization
electrostatic stabilization
© 2019 HORIBA, Ltd. All rights reserved. 37
Zeta Potential
•A double layer exists around each
particle. If a particle is negatively
charged, a thin layer of positive
charge forms around the particle
(the Stern Layer). Beyond the
Stern Layer, there is a wider layer
of mostly opposite charge known
as the DIFFUSE Layer.
•The potential at the surface of the
particle is designated the NERNST
Potential, and the potential at the
outside of the Stern layer is
designated the ZETA Potential.
•ZETA Potential is a useful
measurement quantity because it
is a measure of surface activity in
colloidal particles.
Nernst
Potential
Zeta
Potential
Distance (Angstroms)
Diffuse Layer Stern Layer
Particle
electric
potential
(millivolts)
+
+
+
+
+
+
+ +
+
+
+
+
+
+
-
-
-
-
-
--
-
--
-
-
-
-
-
+
+
REPRESENTATION
OF ATTRACTED
LAYERS AND ZETA
POTENTIAL
© 2019 HORIBA, Ltd. All rights reserved. 38
Dispersion: Mechanical Energy
• The purpose of applying energy is to separate
particles for a sufficient period to allow
surfactants to develop a coating.
• TYPES OF ENERGY DEVICES
– Blenders
– Stirrers
– Ultrasonic Devices
• Ultrasonic Bath
• Ultrasonic Probe
• Dilute surfactant is mixed with suspending liquid before
particulate sample is added. As energy is applied, the
surfactant is able to attach to the particles, providing sufficient
charge to keep individual particles apart.
ENERGY
Surfactant
© 2019 HORIBA, Ltd. All rights reserved. 39
Dispersion: Ultrasonic Energy
• Ultrasonic waves generate
microscopic bubbles or
cavities (cavitation) which
produce shearing action
causing the liquid and
suspended particles to
become intensely agitated.
• Agglomerates are broken apart.
• In some cases fragile particles are
shattered.
• The selection of appropriate type and
level of ultrasonic energy must be
made carefully.
Ultrasonic Bath
Ultrasonic Probe
© 2019 HORIBA, Ltd. All rights reserved. 40
Effect of Applied Energy
• The effect of applied
energy is to break up
agglomerates into
individual particles for size
measurement. However, if
too much energy is applied,
particles may by broken
into fragments. The
desired result is to apply
just enough energy to
disperse material into basic
particles for measurement
without damaging friable
materials.
• The graph illustrates how this can be accomplished. Effects of applied
energy on particulate samples can be tested by using results from
measurements made on the instrument. By treating the sample with
varying levels of ultrasonic power, performing analyses, and noting the
average particle size (mean, median) as a function of power level, one
can choose a range of applied energy that is optimum for that material.
INCREASING ENERGY
AVERAGESIZE
Optimum Range
© 2019 HORIBA, Ltd. All rights reserved. 41
Dispersion vs. Breakage
• Dispersion and breakage can both
occur
Ideal World
Real World
© 2019 HORIBA, Ltd. All rights reserved. 42
Summary
• Surfactants wet powders
• Use admixture to alter
surface chemistry
– Sodium hexametaphosphate
– Sodium pyrophosphate
• Ultrasound reduces size
– De-agglomeration and/or
breakage
© 2019 HORIBA, Ltd. All rights reserved. 43© 2019 HORIBA, Ltd. All rights reserved. 43
© 2019 HORIBA, Ltd. All rights reserved. 44
Danke
Большое спасибо
Grazie
Σας ευχαριστούμε
감사합니다
Obrigado
谢谢
ć ŹńčτĹ čŚΓń
ありがとうございました
ध�वाद
நன் ற
Cảm ơn
Dziękuję
Tack ska ni ha
Thank you
Merci
Gracias

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Particle Classroom Series V: Sampling and Dispersion

  • 1. © 2019 HORIBA, Ltd. All rights reserved. 1
  • 2. © 2019 HORIBA, Ltd. All rights reserved. 2© 2019 HORIBA, Ltd. All rights reserved. 2 Sampling and Dispersion HORIBA Instruments Inc. Particle Characterization Jeff Bodycomb, Ph.D. October 29, 2019
  • 3. © 2019 HORIBA, Ltd. All rights reserved. 3 From: NIST Recommended Practice Guide Special Publication 960-1 Particle Size Characterization Ajit Jillavenkatesa Stanley J. Dapkunas Lin-Sien H. Lum Materials Science and Engineering Laboratory January 2001 Particle Analysis Workflow
  • 4. © 2019 HORIBA, Ltd. All rights reserved. 4 Outline • Sampling from bulk • Sub-sample for measurement • Disperse sample – Wet powders, apply air pressure or ultrasound • Sometimes second sub-sampling – From beaker to instrument • Perform measurement
  • 5. © 2019 HORIBA, Ltd. All rights reserved. 5 Measurement Error Sources • SMALL PARTICLES – POTENTIALLY SMALL EXTRACTION ERRORS (A) – POTENTIALLY LARGE SAMPLE PREP ERRORS (C) • LARGE PARTICLES – POTENTIALLY LARGE EXTRACTION ERRORS (B) – POTENTIALLY SMALL SAMPLE PREP ERRORS (D) • INSTRUMENT ERROR IS SMALL AND RELATIVELY CONSTANT PARTICLE SIZE SAMPLE PREPARATION SAMPLE EXTRACTION INSTRUMENT ERROR % E R R O R A B C D
  • 6. © 2019 HORIBA, Ltd. All rights reserved. 6 Sample Extraction: Good Sampling Practices Learn to Love Your Riffler!
  • 7. © 2019 HORIBA, Ltd. All rights reserved. 7 Sampling from Flowing Powder
  • 8. © 2019 HORIBA, Ltd. All rights reserved. 8 Powder Thief www.samplingsystems.com Sampling from Drums
  • 9. © 2019 HORIBA, Ltd. All rights reserved. 9 www.samplingsystems.com Sampling from Drums
  • 10. © 2019 HORIBA, Ltd. All rights reserved. 10 Sub-sampling for Measurement • Not all of sample brought to lab is analyzed • Must sub-divide sample • How to introduce representative sample into instrument?
  • 11. © 2019 HORIBA, Ltd. All rights reserved. 11 Technique: Grab Sampling • PLACE SPATULA INTO POWDER • EXTRACT SMALL AMOUNT FOR ANALYSIS • ACCEPTABLE FOR NARROW DISTRIBUTIONS • SEGREGATE LARGE AND SMALL WHEN POLYDISPERSE – LARGE PARTICLES PERCOLATE UPWARD – SMALL PARTICLES GRAVITATE DOWNWARD • EASY METHOD • MOST USED METHOD
  • 12. © 2019 HORIBA, Ltd. All rights reserved. 12 Grab Sampling from Bottle • When a powder is stored in a container, it can be mixed by rolling and tumbling the container. The container should not be more than half to two-thirds full. It is important to perform this action before “grabbing” a sample with a spatula. • Then pull sample with a spatula…..
  • 13. © 2019 HORIBA, Ltd. All rights reserved. 13 Technique: Coning & Quartering •Pile of powder is divided into 4 sections. •Two diagonal sections are discarded, and two are retained and mixed together. •Mixture is again divided into 4 sections, and two diagonal sections are mixed. •Process is repeated until remaining sample is correct amount for analysis. •Can be carried out with very small sample amount or very large samples.
  • 14. © 2019 HORIBA, Ltd. All rights reserved. 14 Technique: Chute Riffling •Chute splitting allows sample to vibrate down a chute to vanes which separate the mass into two portions. Each portion moves further where they each are divided into two parts, now giving four parts. This may be continued until usually 8 or 16 portions are obtained.
  • 15. © 2019 HORIBA, Ltd. All rights reserved. 15 Technique: Rotary Riffling • The best method of representative splitting of powders is the ROTARY RIFFLER. The complete sample to be split is directed down a chute into open containers. Each container will receive a sample which is representative of the original bulk material because the distribution of material is averaged over time. The complete amount of the original bulk sample must be consumed. • These splitters are commercially available from companies that market various types of sample splitters. • See: www.retsch.com • www.quantachrome.com • www.microscal.com
  • 16. © 2019 HORIBA, Ltd. All rights reserved. 16 Sample Dividers
  • 17. © 2019 HORIBA, Ltd. All rights reserved. 17 Sampling Technique Error Levels • Standard Deviation (σ) in % Sugar-Sand Mixture • SCOOP SAMPLING 6.31 • TABLE SAMPLING 2.11 • CHUTE RIFFLER 1.10 • SPINNING RIFFLER 0.27 • Density of sand and sugar respectively 2.65 and 1.64 g/ml • Reference: Allen, T. and Khan, A.A. (1934), Chem Eng, 238, CE 108-112
  • 18. © 2019 HORIBA, Ltd. All rights reserved. 18 Technique: Sampling from Beaker • Liquid should be in motion vertically and horizontally to insure good mixing. • Pipette should be about one- third of the way from the bottom when extracting sample. • Alternative: When mixing powders into a slurry: make paste, pipette from paste IMPELLER PIPETTE
  • 19. © 2019 HORIBA, Ltd. All rights reserved. 19 Measurement Error Sources • SMALL PARTICLES – POTENTIALLY SMALL EXTRACTION ERRORS (A) – POTENTIALLY LARGE SAMPLE PREP ERRORS (C) • LARGE PARTICLES – POTENTIALLY LARGE EXTRACTION ERRORS (B) – POTENTIALLY SMALL SAMPLE PREP ERRORS (D) • INSTRUMENT ERROR IS SMALL AND RELATIVELY CONSTANT PARTICLE SIZE SAMPLE PREPARATION SAMPLE EXTRACTION INSTRUMENT ERROR % E R R O R A B C D
  • 20. © 2019 HORIBA, Ltd. All rights reserved. 20 Sample Preparation: Dispersions
  • 21. © 2019 HORIBA, Ltd. All rights reserved. 21 Dispersion Strategies Powders When measuring powder as suspension Choose solvent (avoid dissolution) Wet powder (surfactant) Dispersing aid to avoid re-agglomeration Energy to break agglomerates into primary particles Pump & stirrer or ultrasound Suspensions Dilute Energy
  • 22. © 2019 HORIBA, Ltd. All rights reserved. 22 Dispersion Definitions • WELL DISPERSED particles can be easily detected under an optical microscope. They are separated from one another and show no tendency to cling together. • AGGLOMERATED particles appear in clumps that can be separated easily by the application of moderate amounts of energy, such as ultrasonic baths. • AGGREGATED particles are tightly bound and must be treated with higher levels of energy. Usually an ultrasonic probe applied directly to the sample slurry will disperse the particles. If they are very tightly bound, they may fracture before they can be separated. WELL DISPERSED AGGLOMERATED AGGREGATED
  • 23. © 2019 HORIBA, Ltd. All rights reserved. 23 θ θ θ DROP OF LIQUID ON A SOLID SMALL (Phylic) LARGE (Phobic) Particle Wetting • CONTACT ANGLE ( θ ) • The contact angle is a measure of how well the liquid drop adheres to the surface of a solid • Large angles indicate poor wetting ability. • Small angles indicate good wetting ability. • Surfactants reduce surface tension and thereby are conducive to good wetting. • (Instruments are available for measuring contact angle)
  • 24. © 2019 HORIBA, Ltd. All rights reserved. 24 Particle Wetting • Surface tension must be lowered so liquid will adhere to particles. + + ++ + + + + + PARTICLE LIQUID GOAL IS TO COMPLETELY COAT PARTICLE WITH LIQUID qq Small Contact Angle Good Wetting Large Contact Angle Bad Wetting
  • 25. © 2019 HORIBA, Ltd. All rights reserved. 25 Screening for wetting agent Set up vials or beakers with each candidate dispersant. Gently put a little bit of fine particle on the top of each.
  • 26. © 2019 HORIBA, Ltd. All rights reserved. 26 Evaluate Wetting Poor wetting: particles don’t break surface tension Good wetting: particles separate and stream through surface
  • 27. © 2019 HORIBA, Ltd. All rights reserved. 27 MEAN PARTICLE SIZE SURFACTANT CONCENTRATION Effect of Surfactant Addition • Addition of surfactant to a sample will disperse the particles so a proper measurement may be made. However, addition of too much surfactant will cause agglomeration. • The graph illustrates that there is an optimum amount of surfactant to effect optimum dispersion. The Particle Size Analyzer can determine when the amount of surfactant exceeds the proper concentration. • As initial surfactant is added, the mean particle size will decrease. It will reach a minimum as the proper surfactant concentration is reached. • As additional surfactant is added, the apparent mean particle size will increase, indicating agglomeration of particles. • Common concentration: 0.01-0.1%
  • 28. © 2019 HORIBA, Ltd. All rights reserved. 28 NON-POLAR HYDROCARBON POLAR IONIC DIPOLE Surfactant Mechanism •EQUILIBRIUM established between SURFACTANT ON PARTICLES and SURFACTANT IN SOLUTION.
  • 29. © 2019 HORIBA, Ltd. All rights reserved. 29 Critical Micelle Concentration • As more surfactant is added, equilibrium shifts. Surfactant leaves surfaces to start formation of MICELLES. This is called CRITICAL MICELLE CONCENTRATION (CMC). • Particle surfaces are no longer repulsed, and energy of the system favors REAGGLOMORATION. - - - - - - - -- - - +++ + + + + + + ++ - MICELLES + Cationic Surface - Anionic Surfactant +
  • 30. © 2019 HORIBA, Ltd. All rights reserved. 30 NO SURFACTANT - AGGLOMERATED PARTICLES EXCESS SURFACTANT - REAGGLOMERATION OF PARTICLES OPTIMUM CONCENTRATION – PROPER PARTICLE DISPERSION Effect of Surfactant Addition
  • 31. © 2019 HORIBA, Ltd. All rights reserved. 31 Common Surfactants Nonionic surfactants adsorb to charged and neutral surfaces, create steric barrier • Igepal CA630 Ethoxylated octyl phenol Nonionic • Triton X100 Octylphenoxypolyethoxy ethanol Nonionic • Tween 20 Polyoxyethylene sorbitan Nonionic • Aerosol-OT Dioctyl ester Na Sulfo succinic acid Anionic Cationic surfactants often used for biological samples, strongly bonds to negatively charged surfaces Hyrdophobic surface Polar groups orient to aqueous phase Anionic surfactant polar head non-polar chain
  • 32. © 2019 HORIBA, Ltd. All rights reserved. 32 Sodium Hexametaphosphate • Most common stabilizer • Abbreviated NaHMP • Keeps particles from re- agglomerating • Disperse sample in 0.01 – 1.0% (NaPO3)6 rather than DI water • Tetrasodium pyrophosphate also used (sodium pyrophosphate, Na4P2O7)
  • 33. © 2019 HORIBA, Ltd. All rights reserved. 33 Particle Interactions • Particles are constantly moving with respect to one another. When they approach close enough to cross the potential barrier (when attractive forces exceed repulsive forces), they come together (agglomerate). • The object is to provide repulsive forces strong enough to keep particles apart, even during close approach. This can be accomplished by surfactant coating of particle surfaces. ATTRACTIVE FORCES (VAN DER WAALS) REPULSIVE FORCES (CHARGE) REPULSIVE FORCES (CHARGE) CHARGE CHARGE + + + + + + + + + + + +
  • 34. © 2019 HORIBA, Ltd. All rights reserved. 34 Inter-particle distance is LARGE. Van der Waals forces WEAK Decreasing particle distance Increasing Van der Waals forces Particle distance very small Van der Waals forces strong + + ++ ++ + + If surfactant charge is sufficiently high, it will overcome Van der Waals forces before the particles approach closely. Particle Interactions
  • 35. © 2019 HORIBA, Ltd. All rights reserved. 35 Vmax Total Potential Energy VT Distance Between Surfaces 0 VT = VA + VR VA Attraction Repulsion VR PotentialEnergy Energy of Interaction INTERACTION OF TWO CHARGED SURFACES Stability of a system depends on forces between particles. Random motion brings them into close proximity. Whether two particles will combine depends on potential barrier between them. Potential energy consists of two forces, the ATTRACTIVE one due to Van der Waals, and the REPULSIVE one due to electrical double layers around particles. If height of the barrier, VT, is lower than average thermal energy, KT, then probability is high that two adjacent particles will eventually collide. They will probably remain attached to each other due to strong Van der Waals forces at very close distances. Electrical forces cause particles to remain apart. Van der Waals forces cause particles to come together.
  • 36. © 2019 HORIBA, Ltd. All rights reserved. 36 Dispersion Stability steric stabilization electrostatic stabilization
  • 37. © 2019 HORIBA, Ltd. All rights reserved. 37 Zeta Potential •A double layer exists around each particle. If a particle is negatively charged, a thin layer of positive charge forms around the particle (the Stern Layer). Beyond the Stern Layer, there is a wider layer of mostly opposite charge known as the DIFFUSE Layer. •The potential at the surface of the particle is designated the NERNST Potential, and the potential at the outside of the Stern layer is designated the ZETA Potential. •ZETA Potential is a useful measurement quantity because it is a measure of surface activity in colloidal particles. Nernst Potential Zeta Potential Distance (Angstroms) Diffuse Layer Stern Layer Particle electric potential (millivolts) + + + + + + + + + + + + + + - - - - - -- - -- - - - - - + + REPRESENTATION OF ATTRACTED LAYERS AND ZETA POTENTIAL
  • 38. © 2019 HORIBA, Ltd. All rights reserved. 38 Dispersion: Mechanical Energy • The purpose of applying energy is to separate particles for a sufficient period to allow surfactants to develop a coating. • TYPES OF ENERGY DEVICES – Blenders – Stirrers – Ultrasonic Devices • Ultrasonic Bath • Ultrasonic Probe • Dilute surfactant is mixed with suspending liquid before particulate sample is added. As energy is applied, the surfactant is able to attach to the particles, providing sufficient charge to keep individual particles apart. ENERGY Surfactant
  • 39. © 2019 HORIBA, Ltd. All rights reserved. 39 Dispersion: Ultrasonic Energy • Ultrasonic waves generate microscopic bubbles or cavities (cavitation) which produce shearing action causing the liquid and suspended particles to become intensely agitated. • Agglomerates are broken apart. • In some cases fragile particles are shattered. • The selection of appropriate type and level of ultrasonic energy must be made carefully. Ultrasonic Bath Ultrasonic Probe
  • 40. © 2019 HORIBA, Ltd. All rights reserved. 40 Effect of Applied Energy • The effect of applied energy is to break up agglomerates into individual particles for size measurement. However, if too much energy is applied, particles may by broken into fragments. The desired result is to apply just enough energy to disperse material into basic particles for measurement without damaging friable materials. • The graph illustrates how this can be accomplished. Effects of applied energy on particulate samples can be tested by using results from measurements made on the instrument. By treating the sample with varying levels of ultrasonic power, performing analyses, and noting the average particle size (mean, median) as a function of power level, one can choose a range of applied energy that is optimum for that material. INCREASING ENERGY AVERAGESIZE Optimum Range
  • 41. © 2019 HORIBA, Ltd. All rights reserved. 41 Dispersion vs. Breakage • Dispersion and breakage can both occur Ideal World Real World
  • 42. © 2019 HORIBA, Ltd. All rights reserved. 42 Summary • Surfactants wet powders • Use admixture to alter surface chemistry – Sodium hexametaphosphate – Sodium pyrophosphate • Ultrasound reduces size – De-agglomeration and/or breakage
  • 43. © 2019 HORIBA, Ltd. All rights reserved. 43© 2019 HORIBA, Ltd. All rights reserved. 43
  • 44. © 2019 HORIBA, Ltd. All rights reserved. 44 Danke Большое спасибо Grazie Σας ευχαριστούμε 감사합니다 Obrigado 谢谢 ć ŹńčτĹ čŚΓń ありがとうございました ध�वाद நன் ற Cảm ơn Dziękuję Tack ska ni ha Thank you Merci Gracias