Developing Reference Methods for Nanomaterials
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Date
Event title
www.nanovalid.eu
Title of Event: NanoValid Summer School, Tallinn/ Estonia
Date: June 16th, 2014
Dispersion and characterisation of nanoparticles
Partner representative name: Annegret Potthoff, Tobias Meißner
Partner organisation name: Fraunhofer-Gesellschaft (Germany)
Developing Reference Methods for Nanomaterials
© Fraunhofer
Wertheim/BronnbachMannheim
Karlsruhe
Pfinztal
Ettlingen Stuttgart
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Kandern
Efringen-Kirchen
AlzenauWürzburg Bayreuth
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Halle
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Itzehoe
Lübeck
ErfurtJena
HermsdorfIlmenau
Berlin
Sulzbach-Rosenberg
Remagen
66 institutes and independent research units
More than 22,000 staff Headquarter in München
Fraunhofer-Gesellschaft, the largest organisation for applied research in Europe
Fraunhofer Institute for Ceramic Technologies and Systems (IKTS) in Dresden
Delevopment of state-of-the-art advanced ceramic materials
Characterisation of materials Powder and suspension
characterisation
Developing Reference Methods for Nanomaterials
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Topics Physico-chemical characterisation for toxicologic assessment
Relevance of nanomaterial definitions for particle characterisation
Dispersion decides
Colloid chemical stability of nanoparticles/ analysis of zeta potential
Particle size analysis Dynamic Light Scattering (DLS) Comparison to Nanoparticle Tracking (NTA)
Applications and examples Powder characterization Dispersion of nanoparticles prior to toxicological tests Proteins – natural dispersant aids How to analyze a nanostructured powder?
Conclusions
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Physico-chemical characterisation for toxicological assessment
ISO/TR 13014:2012
Physical description
Chemical composition
Extrinsic properties
Time
Batch
Which parameters?
How often?
When?
From what?
Nanomaterial
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What does it mean – nanomaterial?
Definition according to ISO/TS 80004-4:2011
Nanostructuredmaterial
Nanostructuredpowder
Agglomerates, aggregates,
nanoparticles
Nanocomposite Solid nanofoam
Nanoporousmaterial
Fluid nanodispersion
Material with an nanoscaled (1 nm – 100 nm) internal or external structure
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COMMISSION RECOMMENDATION on the definition of nanomaterial
2011/696/EU, recommendation of 18 October 2011
`Nanomaterial` means a natural, incidental or manufactured material containing particles, in an unbound state or as an aggregate or as an agglomerate and where, for 50 % or more of the particles in the number size distribution, one or more external dimensions is in the size range 1 nm – 100 nm.
“Nanomaterials” by EU definition are among “nanostructured materials” according to ISO norm.
EU commission recommends, that about 50 % of particles – calculatedfrom a number weighted distribution – have to comply with this condition, while there is no similar definition in ISO norm.
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Materials considered in this presentation
Nanostructuredmaterial
Nanostructuredpowder
Agglomerates, aggregates,nanoobjects
Nanocomposite Solid nanofoam
Nanoporousmaterial
Fluid nanodispersion
Nanostructuredmaterial
Nanostructuredpowder
Agglomerates, aggregates,
nanoparticles
Nanocomposite Solid nanofoam
Nanoporousmaterial
Fluid nanodispersion
Independent on amount of nanoscaled material.
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Which pc parameters are the most relevant for toxicological assessment
ISO/TR 13014:2012
Physical descriptionParticle size/ particle size distributionState of agglomeration and aggregationParticle shapeSpecific surface area
Chemical compositionCompositionPurity/ impuritiesSurface chemistry
Extrinsic propertiesSurface chargeSolubilityDispersability
Nanoparticle
Suspending media
Solid-liquid interface
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How do they look like
Example: TiO2 P25 (Evonik)Nanoparticles form aggregates and agglomerates
Wikipedia/Nanogold
Nanostructured powders and nanocomposites Fluid nanodispersions
Example: Au dispersionNanoparticles are separated
Particle? Particle size? Particle size analysis?
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How do they occur
Surface chemistry? Surface charge? Interactions at the interface?
Nel et al., 2009
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Dispersion decides
Prior to any analysis we have to check, what we would like to know!
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Characterisation of nanomaterials requires information about dispersability
Natural nanoparticledispersed in air
Eyjafjallajokull 2010
Oberdörster 2005
Inhalation studies fortoxicological testing
Dispersion in air Analysis after dry dispersion
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Characterisation of nanomaterials requires information about dispersability
Technical nanoparticledispersed in fluid
www.brand.de
Preparation prior to toxicologicalor ecotoxicological testing
Dispersion in liquid Analysis after wet dispersion
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Dispersion decides
(1) Particle´s behaviour
Powders in liquids
Agglomerates or aggregates and primary particles?
Influencing factors
Kind of particle stress
Specific energy input (time, intensity)
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Dispersion decides
(2) Particle´s behaviour in fluids
Charges at particle surfaces
Electrosteric effects
Influencing factors
pH value
Natural or artificial dispersantaids
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Analysis of zeta potential
Colloid chemical stabilized?
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Surface charges and zeta potential
Strongly bounded ions are fixed at particle surfaces (= inner and outer Helmholtz layer)
Loosely associated ions for charge compensation (= diffuse double layer)
Stern model describes conditions insystems with moderate ionic strength (10-4 … 10-2 mol/l).
Thickness of diffuse double layer depends on concentration and chargeof ions
Zeta potential: Difference between potential on shear plane and potentialwithin the fluid (example: negative)
diffuse Schicht
star
re S
chic
htFi
xed
laye
r
Diffuse double layer
She
ar p
lane
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Colloid chemical stable?
Stable suspensions:suspendedor with sedimentation
Instable suspensions:flocculation orcoagulation (agglomeration)
Colloid chemical stable suspensions might be stable against sedimentation,but they do not necessarily have to!
Value of zeta potential Repulsive forces between particles Electrostatic stability Agglomeration of particles
Value of zeta potential 0 Repulsive forces between particles Electrostatic stability Agglomeration of particles
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Analysis of zeta potential
Measurement principle ConcentrationElectrophoretic light scattering * Up to 5 vol%Streaming potential Up to 5 vol%Electroosmosis Below 0,5 wt%Sedimentation potential Below 0,5 wt%Electro sonic amplitude * 1 to 40 vol%
ISO norms are available for
- sampling and sample splitting and- *-marked measurement principles.
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Electrophoretic light scattering (ELS) – measurement principle
E
FE = E . qFR = -6r v
Moving particle(negative charge)
- -- --- - - -
--
-
++
++
+
- - FEFR --
-
Shifted counter ion cloud
+
Acceleration of particles in an electric field FE – Accelerating force Stokes friction acts against particle movement FR – Retarting force
v / E = q / 6 r When FE = FR constant particle movement
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Zeta potential – calculation from electrophoresis
r < 0.1 r > 100
Large Particle with a thin Double Layer Small Particle with thick Double Layer
v / E = µe = 2 or f[r] / 3 HENRY Equation
µe = 2 r / 3 µe = r) / SMOLUCHOWSKI Equation
HUECKEL Equation
v / E = q / 6 r
Correction for surface conductivity Correction function for changes of dielectricity and viscosity Correction for particle shape Corrections for high ion and particle concentrations
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Analysis of particle sizes
Sample preparation finalized successfully
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Analysis of particle size distributions of dispersed nanomaterials in liquids
Measurement principle Measurement range ConcentrationDynamic light scattering */ Photon cross correlationspectroscopy *
1 nm – 5 µm Up to 5 vol%
Nanoparticle tracking 10 nm – 1 µm Up to 108 particle/mLUltrasound attenuation * 4 nm – 40 µm 1 to 40 vol%Laserlight diffraction * 20 nm – 3000 µm Below 0,5 wt%Centrifugal sedimentation * 10 nm – 100 µm Below 0,5 wt%
ISO norms are available for
- sampling and sample splitting- dispersing and- *-marked measurement principles.
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Dynamic light scattering (DLS) – measurement principle
Is 2
Is2
t
Autocorrelation function(depends on diffusion coefficient D)
Is
t
Fluctuation of scattered light intensity at detector
Laserlight
Input
Detector
Beam stopLaserlight
Output
Medium intensity
Correlator
Analyzation ofscattered light
Malvern
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Dynamic light scattering (DLS) – measurement principle
Small particles:G1 vs time
500 1000 1500 2000Time(us)
0.2
0.4
0.6
0.8
G1
G1 vs time
500 1000 1500 2000Time(us)
0.2
0.4
0.6
0.8
G1
Large particles:
time t
time tI
I
Malvern
Diffusion velocity – highScattered light intensity – low
Diffusion velocity – lowScattered light intensity – high
Correlogram
Correlation function
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Dynamic light scattering (DLS) – result
Depending on sample preparation hydrodynamic diameter xDLS maydescribe diameter of primary particles, aggregates or agglomerates
Calculation of intensity-weighted particle size distribution,conversion into volume-weighted particle size distribution possible
DTkx B
3 Calculation of particle size from diffusion coefficient: xDLS
Polydispersity index PI (between 0 and 1)
Developing Reference Methods for Nanomaterials
Intensity-weighted distribution Volume-weighted distribution
Exam
ple
1Ex
ampl
e 2
Dynamic light scattering (DLS) – Comparison of different approachesPresence of nanoparticles and serum proteins in cell culture medium Analysis using mean particle size and PI (cumulant method) difficult
Usage of complex algorithm calculating size distributions
Developing Reference Methods for Nanomaterials
Intensity-weighted distribution Volume-weighted distribution
Exam
ple
1Ex
ampl
e 2
Dynamic light scattering (DLS) – Comparison of different approachesPresence of nanoparticles and serum proteins in cell culture medium Analysis using mean particle size and PDI (cumulant method) difficult
Usage of complex algorithm calculating size distributions
Simultaneous detection of proteins and particles not always possible usingDLS scattered light intensity r6-dependency
Simple cumulant method “detects” proteins via increased PI, but mean sizeis error-prone SiO2 particles appear smaller than they are
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Volume-weighted or number-weigthed concentration?
Vtennis balls!=
Vmedicine ball
xtb xmb xtb xmb
Number-weighted distribution Volume-weighted distribution
Nano?40 % below 100 nm
95 % below 100 nm
10 100 1000 10000Particle size [nm]
Developing Reference Methods for Nanomaterials
Dynamic Light Scattering vs. Nanoparticle Tracking Analysis
DLS NTAAnalysed particleproperty
Brownian motion Brownian motion
Analysis of particlevelocity
Time dependent lightscattering
Video analysis of particletracking
Calculated result Diffusion coefficient fromEinstein equation Hydrodynamic diameter
Diffusion coefficient fromEinstein equation Hydrodynamic diameter
Particle size range 1 nm – 5 µm 10 nm – 1 µmResults xDLS, PI;
intensity or volume weighteddistribution
Number weighted particlesize distribution,concentration
Concentration Up to 5 vol% Up to 108 particle/mLCompatibility ISO/TS 80004-4:2011 EU commission
Developing Reference Methods for Nanomaterials
Advantages and limitations
DLS NTALimitation due to sedimentation of large (or high-aggregated!) particles,
especially for high-density materialsGood for fluid nanodispersions and for well-dispersable nanostructured
powders and nanocomposites (narrow PSD)Few small particles very difficult todetect in presence of large particles
Small particles detectable in presenceof large particles
Detection of time stability of PSD possible (including agglomerationprocesses)
Detection of time stability of PSD should be possible
Analysis in physiological and in ecotoxicological relevant media possibleParticle concentrations as often testedin in-vitro tests
Particle concentrations as often testedecotoxicological tests
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Applications and examples
Tools for sample preparation and particle size analysis available
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Example 1: Powder characterisation
500 nm
Particle size= size of aggregates and primary particles= „smallest dispersable unit“
Requirements for dispersionColloid chemical stability high= high value of zeta potential dosage of dispersant necessary
Complete deagglomeration= high specific energy input dispersion by ultrasound (sonotrode)
Dispersion strategy prior topowder characterisation isdescribed in ISO 14887:2000
TiO2 P25
Comparison toBET ~ 45 m²/gxBET ~ 21 nm
Size from SEM or TEM image
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Example 1: Comparison of results for particle size analysis
Analysis in water containing polyphosphate |ZPSmoluchowski| > 60 mV DLS measurement
Well dispersable powder, which consists of small aggregates (xDLS > xBET) Complementary results from different measurement methods
500 nm
TiO2 P25
BET ~ 45 m²/g (xBET ~ 21 nm)
Size from SEM or TEM image
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Example 2: Dispersion – the main challenge
Dispersion of nanomaterials for toxicological testing
No standardized procedure for dispersion available!!!
Results strongly depend on sample preparation.
Recommendation for “Dispersion SOP” will be developed within NanoValid project.
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No
Yes Disperse directly in
media
Under relevant/ possible
conditions
Worst-casescenario
Acceptagglomeration
Yes
No
Smallestdispersable
unit
Disperse directly in
media
Characterisation, i. e. by DLS
Specify energyinput
Specifydispersant aid
Yes
NoPredispersion
in water
Predispersionin water
Decision of principle considerations
Origin: D4.32 (NanoValid project)
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Comparison of results
Time-dependent analysis Specify concentration of BSA, which acts as a dispersant aid
Example: TiO2 NP in PBS
Smallestdispersable unitxDLS remains constantduring testing
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Comparison of results
Example: TiO2 NP in DMEM + FBS
Increase
Smallestdispersable unit
Reducedagglomeration
Energy-input-dependent analysis Specify specific energy input
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First results of a round-robin test
500 nm
Silica OX50
BET: 50 m²/gxBET ~ 40 nm
SOP with detailed specification of concentration, dispersion, energy input etc. 4 out of 7 partners receive similar results
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Example 3: Zeta potential analysis in toxicological tests
Due to adsorptionof proteins nanoparticles changetheir behaviour in presence, i. e. of LSZ.
Proteins may act as dispersant aids xDLS remains constant.
-20
-15
-10
-5
0
5
10
15
20
2 3 4 5 6 7 8 9 10 11 12 13
pH
zeta
pot
entia
l [m
V]
tungsten carbide (WC)lysozyme (LSZ)WC + LSZ
Challenge: Analysis of zeta potentials in physiological mediaConductivity compression of electric double layer low values of zeta potential
Analysis of solid-liquid interface
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Example 4: How to analyze a nanomaterial?
1 µm 200 µm
Nanostructured powder according to ISO/TS 80004-4:2011
Bad dispersability aggregates are micron-scaled and settle down very fast
DLS does not meet all requirements!
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Example 4: How to analyze a nanomaterial?
Use same dispersion procedure as for nanoparticlesAnalysis by laserlight diffraction aggregates of up to 100 µm in size!
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Conclusions
Dispersion decides, but is not yet standardized for nanotoxicological testing
“Nanomaterial” or not – sometimes a question of definition
Zeta potential - a tool for stability analysis
DLS or NTA? DLS + NTA + BET + SEM/TEM + … = results are complementary
DLS – a tool for analysis in physiological and in ecotoxicological relevant media
Particle size analysis of nanostructured materials sometimes requires devices other then DLS
As particle properties change depending on time, batch or surrounding behaviour, they always need to be investigated prior, while and after toxicological testing.
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Thank you for your attention!
Contact: [email protected]