nanoparticle size measurements
Transcript of nanoparticle size measurements
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Our innovative solutions for
nanoparticle size measurements
Enlight the Nanoworld
Opaque & concentrated media “bring the measurement to your sample”
VASCO™ γ series VASCOTM FLEX
Batch In-situ
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Nano-Materials & Nanoparticles : a new era in science and industry
Promise of major technologic, economic and societal impacts
NPs and NMs already in the field : cosmetics, batteries, paints, inks, food, medicines,
advanced coatings, aerospace, etc….. And it is just the beginning!
Booming demand for advanced materials and application requires to scale up
production installation (incoming material control, process control, quality control)
New monitoring tools required to migrate NPs from R&D labs to
pilot plant and mass production!
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Sometimes size matters… In particular for NPs!
Many mature characterization techniques for particle size:
• Electronic Microscopy: TEM,
• Electrozone Coulter counter
• Mass sensing: Differential Centrifugal Sedimentation, resonant mass
detection
• Optical : Particle tracking, Laser Diffraction, Dynamic Light Scattering
(DLS)
• Related to the specific surface of the particles
• Ability to penetrate membranes or interact with surface
• Aggregation and stability of suspensions
• Functionalization and self assembly capabilities
• Optical, mechanical and electrical properties
• Etc.
d?
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0 1 µm 1 mm100 nm1 nm
Classical Optical microscopy
DLS vs. other techniques
DLS : 4 decades of size range!!!
Laser Diffraction
(Static light scattering)
SAXS, TEM
DLS: 1 nm to 10 µm
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DLS uses Brownian motion as a signature of particle size
Brownian motion= Random “walk”
NPs:
hard spheres without
interactions
Viscosity TemperatureBoltzmann
EINSTEIN (1905)
𝐷 =𝐾𝑇
3𝜋h ∅𝐻∅𝐻 =
𝐾𝑇
3𝜋hD
t
c
t
0
Diffusion coefficient time
L. BACHELIER (1901)
< 𝑋2 𝑡 > ~2 𝐷 𝑡
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Diffusion layerParticle
Stern Layer
Solution
+
+ +
+
+
+
++
+
-
-
-
--
-
--
Hydrodynamic
diameterHydrodynamic
diameter
Core diameter
+
+
+ - --
-
-
+ ++
+
++
+++
+++
+
+++
-
-
-
--
-
-
-
-
-
-
--
++
++
+
+ --
--
--
-
Meaning of hydrodynamic diameter ∅𝐇
Hydrodynamic diameter is usually > Core diameter
(TEM/SAXS) Value by several nm!
Hydrodynamic diameter = diameter of the particle + double layer
thickness
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DLS measurement principle:
Measure light scattering fluctuation to probe the Brownian motion
polarized
1
23
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Intensity measurement and correlogram
Considering coherent electromagnetic waves scattered
and measured at a specific angle (scattering vector q=ki-ks) :
This leads : G(2) (t) = A + β exp (-2q2Dt)
with 𝒒=
𝐬𝐢𝐧(𝜽/𝟐)
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Detected field and Intensity :
EM field: Etot_detect(ωt)=ΣEiexp(i(q.r-ωt))
Intensity: I(t)= Etot(t) x Etot*(t)
Autocorrelation :
Field : g(1) (t) = <E∗(t)E(t+t)><E2(t)>
Intensity : G(2) (t) = <𝐼 𝑡 . 𝐼 𝑡+t >
<𝐼2 𝑡 >
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Correlogram representation: Linear vs Logarithmic
Linear time scale
Logarithmic time scale
No
rma
lize
dA
mp
litu
de
Lin
ear
No
rma
lize
dA
mp
litu
de
Lin
ear
Competitors: Multi-tau correlator
Cordouan: linear correlator
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Correlogram treatment
Inversion problem : How to find the best exponential curve fitting the
experimental curve?
G(2)(t) = A + β exp (-2q2Dt)
t
D?
D ∅𝐻 =𝐾𝑇
3𝜋hD
Fit leads to D, and D to the diameter of NPs ∅𝐻.
G(2) (t)
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Algorithm Number of
populations
Distribution Model
Cumulants1
continuousYes
Assuming a Gaussian
distribution around a
specific size (Zaverage)
Pade
Laplace
Multi (up to 3)
discreteNo
Using Laplace transform of
the decay
SBLMulti
continuousYes
Using a computing method
based of Probabilities
Inversion algorithms for monomodal and polymodal analysis
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The key point of the results : the FIT and the Residues
FIT= mathematical solution given by the algorithms (red curve)
A good fit = Low amplitude (<0,01) and statistically distributed residues
Residues = difference between Fit and measured correlogram
amplitude
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Monomodal sample (one population) 100 nm Latex NPs
Algorithm Size Residus
Cumulants
Pade
Laplace
SBL
Good
Good
Good
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Bi-modal sample (two populations) 30 nm +100 nm Latex NPs mixture
Algorithm Size Residus
Cumulants
Pade
Laplace
SBLGood
Good
Bad fit
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SBL: What is the meaning of the L Curve?
The L curve is a graphic representation of SBL successive iterrations according
to two figures of Merit: Residues index (X axis) and Sparsity index (Y axis)
SBL Initial iterration state
Intermediate iterration state
Most probable solution
Final iterration state
Residues Index«S
pars
ity» index
1
23
4
1
4
3
Iterration cursor
The most probable size distribution= lowest Sparsity and Residues indexes
1
2
3
4
SBL is based on a iterrative algorithm for particle size distribution calculation
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Initial stage1
Intermediate stage
SBL: how to read and tune the L Curve?
Too sparse4
Most probable3
Good Fit
Good Fit
Bad fit
Bad fit2
Size distribution Residues
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Light Scattering: some useful rules of thumb (1):
MIE/ Rayleigh Theory
𝐈 𝐒𝐜𝐚𝐭𝐭 ~ ۹ . 𝐼0(𝐧𝟐−)(𝐧𝟐+𝟐)
2
.
∅𝐻6
4Particle refractive index
Laser Wavelength
Rule of thumb #1: light intensity scattered by 1nm spherical particles is 106 (one
million!) times lower than for 10 nm particles, and 1012 time lower than for 100 nm
ones respectively
=
Intensity Number1/10
100 000/1
Rule of thumb #2: the scattering efficiency (cross section) of the particles is 2.3
times higher for a laser wavelength @532 nm than that of a laser @656 nm
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Light Scattering: some useful rules of thumb (2):
Volume=π
6∅𝐻
3
1/10
Intensity Volume 100/1
Rule of thumb #3: the volume occupied by one 1μm – sphere is the same as one
occupied by 106 spheres with a 10nm diameter
=
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Particle Size and size distribution: some definitions
Distribution 𝒘𝒊𝒅𝒕𝒉 = 𝒁𝒂𝒗𝒈 ∗ 𝑷𝑫𝑰
𝒁𝒂𝒗𝒈 =𝒌𝑩𝑻𝒒²
3𝝅 𝜞:
𝛤 is the average decay rate according to relations:
𝜞 = 𝟎
∞
𝑮(𝚪)𝚪𝒅𝚪
Cumulants analysis
Z-average can be expressed as the intensity weighted based harmonic
mean size
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Particle Size and size distribution: some definitions
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DLS measurement principle: 3 steps process
2autocorrelation function
3Size distribution
Size
Am
plit
ud
e
Intensity fluctuations1
time
Inte
nsity
Measure light scattering fluctuation to probe the Brownian motion
polarized
1
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Our Solutions for Nano-particles size characterization
Opaque & concentrated media “bring the measurement to your sample”
VASCO™ γ series VASCOTM FLEX
Based on Dynamic Light Scattering (DLS)
Measurement in dark and/or concentrated suspension
Size range : from 1nm up to 10µm
Proprietary inversion algorithm for efficient size distribution analysis
Technology transfer from French Petroleum Institute
Batch In-situ
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VASCO™ γ 2 and 3 serie
Opaque & concentrated media
Batch Measurements
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• Innovation in the sample cell configuration: Dual Thickness Control (DTC- patented)
• Thin layer analysis: prevents the sample from local heating and multiple-scattering.
• Backscattering detection (135°): low multiple scattering, better contrast for small
particles
• Higher detection efficiency in opaque media.
• Solvent-proof cell measurement without consumables
• Proprietary inversion algorithm allowing efficient size distribution analysis
• Technology transfer from the French Institute of Petroleum
Vasco particle size analyzer: a unique sample Cell design
Sample
Photon trap
Mobile glass rod
And Beam Dump
Photon counting
DetectorPrism
Laser
Back scattered light
The thin layer analysis mode24
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Measurement of dark /opaque
media
Common DLS artefacts and DTC benefits:
A standard polystyrene latex (Ø=30nm by
TEM) is mixed with black soluble ink (10wt%).
With DTC
32nm
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115nm
With DTC
A standard polystyrene latex (Ø=100nm by TEM)
measured at 0.1 wt%
Measurement of concentrated
samples
85 nm
Photo-detector1
2
3
115nm
Without DTC
DTC reduces impact of
multiple scattering and
light absorption
24nm 32nm
Without DTC
25% error caused by
the laser absorption!! Decrease of the measured
hydrodynamic radius
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Flux
Dual Thickness Controller
Sample Volume
trapped in the cell
VASCO coupled on line with a
peristaltic pump
Unique Online measurement capabilities
ON line size kinetics measurement achieved without stop flow thanks to DTC
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DLS equipments until today
Mature and standardized method (ISO 13321 (1996) & ISO 22412 (2008)
Bench top configuration: solutions dedicated to laboratory analysis
Requires batch sampling: bring the sample to the measurement!
Need sample preparation: filtering, diluting,
Time consuming
Risk of contamination or sample degradation
Need for a new approach for process monitoring!
Disposable cellEmbedded cell
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A change of paradigm:“bring your measurement to your process!”
Features:
Non invasive
Small footprint
Adjustable working distance /scattering angle
Alignment laser for easy installation
High accuracy remote temperature sensor
Easy maintenance
Ideal for measurements in glass capillaries, or
in situ
Combination of the power of DLS, the flexibility of Optical fiber design
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VASCO FLEX: The power of DLS, the flexibility of Optical fiber design
Unique concept: “bring your measurement to your process!”
The idea: fit the solution to each application specs
The idea: fit the solution to each
application specs
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Fiber Remote cell option
Features:
Easy to install, easy maintenance
On-demand fiber length from 1 up to 10 m
The capabilities of a VASCO with the versatility of a remote cell
Compact :ability to work in confined environment (glove box)
Flexibility and upgradability : can easily be detached and replaced by another option
Dual thin film Thickness Control (patented) for concentrated and or opaque sample.
No sample heating, no multiple-scattering
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Features:
Non invasive
Small footprint
Adjustable working distance /scattering angle
Alignment laser for easy installation
High accuracy remote temperature sensor
Flexibility and upgradability : easy switch between options
Easy maintenance
Ideal for measurements in glass capillaries, or in situ
In Situ fibre remote head option
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Thermalized head option
Features:
Broad temperature range : 5° to 80°C ; +/- 0.005° ;
Compact : ability to work in confined environment
(glove box) ;
Compatible with standard 10x10 mm² cuvette
(disposable or QS)
No cross contamination, easy sampling ;
Fluorescence filter option ;
Cuvettes options : disposable cell, glass cell, micro-
cell, flow cell …
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Custom setup head option
Features:
Lab set up for dedicated application
Compatible with standard 10x10 mm2 cuvette (disposable or QS)
No cross contamination, easy sampling,
Fluorescence filter option
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Examples of use of In situ remote head
and applications
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Example 1
Combined Remote DLS & High flux SAXS
for NPs synthesis monitoring
SNOW CONTROL FP7 Project
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Combined Remote DLS & High flux SAXS for NPs synthesis monitoring
F1F2
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On line SiO2 NPs synthesis monitoring
Impact on precursors mixing ratio (F1/F2) Impact of flow rate (F1+F2)
Flow rate = 120µL /min
Hydrolysis –condensation method : TEOS in Ethanol (F1) + NH3 in H2O (F2)
• Consistent results between SAXS and DLS measurements
• Allow to track and tune synthesis process in an accurate way
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Example 2
In situ kinetics monitoring
of Microwave assisted NPs synthesis
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In situ kinetics monitoring of Microwave assisted NPs synthesis
• In situ DLS successfully integrated into a commercial microwave reactor
• Under test and qualification at the College de France-Paris
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Real-time & In situ monitoring of Microwave assisted NPs synthesis
Particle sizeCorrelograms
• Very consistent an d reproducible results
• 1st demonstration ever done opening up new possibility on NP synthesis monitoring
True temperatureCorresponding
Viscosity (cP)
Corrected
Averaged size
(nm)
50°C 0.55 76
90°C 0.3 72
140°C 0.196* 68
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Te
mp
°C
Time (sec)
50°C
140°C
90°C
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Example 3
Particle Size Measurement inside supercritical CO2
synthesis reactor
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Particle Size Measurement inside supercritical CO2 synthesis reactor
Reactor (100 bars, 40°C)
DLS probe
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Particle Size Measurement in supercritical CO2 synthesis reactor
10 wt% styrene rel. to system, 10 wt% Dowfax 8390 (surfactant) rel. to
monomer, 8 wt% Hexa Decane rel. to styrene
Sonicated for 10 min, 65% input intensity
CO2 is used to control the size of nano-emulsion droplets
Use DLS measurements to correlate turbidity variation with particle size
Implement accurate control of the size of monomer droplets/NP
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Example 4
Environmental application: Nano Plastic detection in
Ocean water
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Environmental study : Evidence of Plastic Nps in Ocean
Floating particles
Lab study of Plastic NPs formation under oceanic like UV insolation conditions
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Other examples…
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Magnetic Hyperthermia experiment on NPs for Bio-med applications
Magnetic coil
Remote DLS probe
DLS probe
Remote DLS probe
Magnetic coil
Polymer-grafted iron oxide nanoparticles as thermosensitive MRI contrast agents and magnetic nano-heaters, Gauvin Hemery & al, ,
Journal of Physics D: Applied Physics
Other examples of coupling
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Bibliography
Generality and theory about DLS and light scattering :
• Dynamic Light Scattering, John Wiley & Sons, Inc. New York by Berne, B.J. and Pecora, R.
(1975)
• Laser Light Scattering: Basic Principles and Practice. Second Edition (Dover Books on Physics)
by Benjamin Chu (2007-05-11)
• Particle Characterization: Light Scattering Methods, Kluwer Academic Piblisher; ISBN: 978-0-
7923-6300-2, by Xu, Renliang ,
Some publications with VASCO Flex system:
• Polymer-grafted iron oxide nanoparticles as thermosensitive MRI contrast agents and magnetic
nano-heaters, Gauvin Hemery & al, , Journal of Physics D: Applied Physics
• Combining SAXS and DLS for simultaneous measurements and time-resolved monitoring of
nanoparticle synthesis; A. Schwamberger & al, Nuclear Instruments and Methods in Physics
Research B 343 (2015) 116–122
• Structure and Dynamic Properties of Colloidal Asphaltene Aggregates; Joelle Eyssautier & al;
Langmuir, 2012, 28 (33), pp 11997–12004 - American Chemical Society
• Investigation on Physical Properties and Morphologies of Microemulsions formed with Sodium
Dodecyl Benzenesulfonate, Isobutanol, Brine, and Decane, Using Several Experimental
Techniques, Ayako Fukumoto & al, Energy Fuels 2016 to be published- American Chemical
Society
• Marine plastic litters: the unanalyzed nano-fraction, Julien Gigault & al; The Royal Society of
Chemistry, Env. Sci. Nano, 2016, 00, 1-3
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VASCO FLEX specifications
DTC head « In situ » head Thermalized Head Custom head
Measurement principle Optical Fiber Dynamic Light Scattering (DLS)
OPTICAL HEADS’ SPECIFICATIONS
Temperature Monitoring YesYes +
Customer sensor interfacingYes
Yes +
Customer sensor interfacing
Temperature Range (°C) 15°C - 70°C (option 90°C) Customer range 5°C - 80°C Customer range
Min. Sample Volume (µL) <50µL (cell dependant)
Sample Cells Built-in (patented) In situ Standard cell* Custom
Solvent compatibility Aqueous & Organic solvents All solvents
Scattering Angle (°) 135° 170° 170° Custom
Particle size range 0.5 nm – 10 µm (sample dependant)
Sample concentration range 10-4 % to 40% volume 10-5 % to 5~10% volume (sample dependant)
Head’s weight 3.5 kg < 0.5 kg 0.5 kg Custom
Head’s dimensions 110 x 185 x 250 mm (HWD) 50 x 25 x 120 mm (HWD) 100 x 90 x 235 mm (HWD) Custom
Options & accessories Online measurement Thermalized cell (10-70°C) - -
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Cordouan Technologies proprietary
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ZETA POTENTIAL ANALYZER
• The best resolution thanks to
modern data acquisition &
computing
• Unique carbon electrodes
WALLIS™
NP TRACES (size & cc.)
• Unique LIBD technology
• Size range: 15 to 1000nm
• Cc ranges :
103 – 1011 part/ml (det. only)
106 – 1011 part/ml (det. + size)
MAGELLAN™
ELECTRON MICROSCOPY
• Unique TEM/SEM/STEM
benchtop microscope
• Glow discharge for EM grids
functionalization
ELMO™
PARTICLE SIZE ANALYZER by DLS
• Patented DTC technology for concentrated / absorbent samples
• Unique algorithms (Pade Laplace & SBL) for a better distribution analysis
• Flex: In–situ measurement / easy coupling to reactors
• Patent pending on new applications
• Synthesis kinetics monitoringVASCO VASCO flex™
Our product portfolio
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For more information:
www.cordouan-tech.com
Tel : +33 (0)5 56 15 75 39
Thank you for your attention
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Cordouan Technologies proprietary