Microsecond spICP-MS for dual-element detection ... · Microsecond spICP-MS for dual-element...
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Manuel David MontañoColorado School of MinesJuly 10th, 2014
Microsecond spICP-MS for dual-element detection: Environmental and Analytical Applications
Manuel David Montaño
ERC Teleconference SeminarColorado School of Mines
July 10th, 2014
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Manuel David MontañoColorado School of MinesJuly 10th, 2014
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spICP-MS dual-element detection
Benn, T.; Westerhoff, P. Environmental Science and Technology, 2008
• Entry of ENMs into the environment
• Principles and operation of spICP-MS
• Particle-by-particle dual-element analysis Isotopic ratio determination (Ag NPs) Core-shell nanomaterials
o Sed-FFF fraction collection
o Particle size and number
determination
Natural vs. engineered NPs
o Bulk elemental ratios
o Cerium dioxide ENPs in
stream water
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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ENM Environmental Release
Nowack, B. et al. Environment International, 2013.
• Increasing production of ENPs will lead to inevitable environmental release and exposure
• Release of nanomaterials can come at any point during fabrication and use
• Little information regarding quantity, fate, and behavior of ENPs in environment
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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ENM Environmental Release
Aqueous environment will contain varied assortment of nanomaterials
Important properties to characterizeo Particle sizeo Aggregation stateo Particle number concentrationo Surface groups / chemistry
Challenges for environmental analysiso Low expected release
concentrations (ng L-1)o Changes to surface chemistry /
dispersity by environmental molecules (i.e. humic acid)
o High background of naturally occurring nanomaterials
Montaño, M. et al. Environmental Chemistry, Accepted
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Environmental Transformation of ENMs
Alvarez, ACS Nano, 2009
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Need for Advanced Nanometrology
National Nanotechnology Initiative Workshop, Arlington VA, 2009
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Need for Advanced Nanometrology
National Nanotechnology Initiative Workshop, Arlington VA, 2009
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Single Particle ICP-MS
Montaño, M. et al. Environmental Chemistry, 2014
• Utilizes short dwell times (ms) to detect discrete particle events
• Environmentally relevant detection limit (ng/L)
• Need particles of sufficient mass to be detected
• Can distinguish particle and dissolved
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Principles of spICP-MS Operation
Montaño, M. Unpublished Data
0 50 100 150 200
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Co
unts
Time (sec)
2% HCl
500ppt Au
1000ppt Au
1500ppt Au
2000ppt Au
0 1 2
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600 Au signal
Au
sig
na
l (S
ign
al In
tensity)
Conc. (ppb)
Equation y = a + b*x
Weight No Weighting
Residual Sum
of Squares
465.89825
Pearson's r 0.99893
Adj. R-Square 0.99714
Value Standard Error
Au signal Intercept -4.39476 9.65296
Au signal Slope 294.23719 7.88161
0.00 1.00x10-8
2.00x10-8
0
100
200
300
400
500
600
Avg. counts
/dw
ell tim
e
mass/dwell time
Equation y = a + b*x
Weight No Weighting
Residual Sum
of Squares
465.89825
Pearson's r 0.99893
Adj. R-Square 0.99714
Value Standard Error
Avg.
counts/dwell
time
Intercept -4.39476 9.65296
Slope 3.12509E10 8.37104E8
Dissolved standards Calibration curve Mass flux curve
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Principles of spICP-MS Operation
Montaño, M. Unpublished Data
0 50 100 150 200
0
100
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800
Co
unts
Time (sec)
2% HCl
500ppt Au
1000ppt Au
1500ppt Au
2000ppt Au
0 1 2
0
100
200
300
400
500
600 Au signal
Au
sig
na
l (S
ign
al In
tensity)
Conc. (ppb)
Equation y = a + b*x
Weight No Weighting
Residual Sum
of Squares
465.89825
Pearson's r 0.99893
Adj. R-Square 0.99714
Value Standard Error
Au signal Intercept -4.39476 9.65296
Au signal Slope 294.23719 7.88161
0.00 1.00x10-8
2.00x10-8
0
100
200
300
400
500
600
Avg. counts
/dw
ell tim
e
mass/dwell time
Equation y = a + b*x
Weight No Weighting
Residual Sum
of Squares
465.89825
Pearson's r 0.99893
Adj. R-Square 0.99714
Value Standard Error
Avg.
counts/dwell
time
Intercept -4.39476 9.65296
Slope 3.12509E10 8.37104E8
Dissolved standards Calibration curve Mass flux curve
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Au N
P #
3 (
cts
)
Time (sec)
Au NP #3
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unt
Au NP #3 (cts)
Au NP #3
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10
20
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Count
Size (D.nm)
Au NP #1
Raw particle counts Frequency of particle counts Particle size / number
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Analytical Challenges – High particle no. conc.
Montaño, M. et al. Environmental Chemistry, In Press
500μs
• Nanoparticle events occur over a few hundred microseconds
• Millisecond dwell times may be too large, resulting in coincidence
• This can lead to:o Underestimation of particle
numbero Inaccurate sizing of particles
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Analytical Challenges – High particle no. conc.
Montaño, M. et al. Environmental Chemistry, In Press
10ms dwell time
• Nanoparticle events occur over a few hundred microseconds
• Millisecond dwell times may be too large, resulting in coincidence
• This can lead to:o Underestimation of particle
numbero Inaccurate sizing of particles
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Analytical Challenges – High particle no. conc.
Montaño, M. et al. Environmental Chemistry, In Press
500μs10ms dwell time10ms dwell time
• Nanoparticle events occur over a few hundred microseconds
• Millisecond dwell times may be too large, resulting in coincidence
• This can lead to:o Underestimation of particle
numbero Inaccurate sizing of particles
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Analytical Challenges – High dissolved background
Montaño, M. et al. Environmental Chemistry, In Press
NP event• Nanoparticles entering the
plasma are ionized and detected
• The occurrence of background ions is shown as an elevated background
• If the concentration is high enough, it can mask the presence of a nanoparticle event
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Analytical Challenges – High dissolved background
Montaño, M. et al. Environmental Chemistry, In Press
Dwell time
• Nanoparticles entering the plasma are ionized and detected
• The occurrence of background ions is shown as an elevated background
• If the concentration is high enough, it can mask the presence of a nanoparticle event
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Analytical Challenges – High dissolved background
Montaño, M. et al. Environmental Chemistry, In Press
NP eventDwell time
Dwell time• Nanoparticles entering the
plasma are ionized and detected
• The occurrence of background ions is shown as an elevated background
• If the concentration is high enough, it can mask the presence of a nanoparticle event
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Microsecond-single particle ICP-MS
Montaño, M. et al. Environmental Chemistry, In Press
Conventional single particle ICP-MS analyzes dilute concentration of nanoparticles at short dwell times (~10ms)
Nanoparticles events occur over span of hundreds of microseconds (10ms too long)
Microsecond dwell times parse nanoparticle events into a distribution of intensity
Improves ability to analyze high particle number concentrations and high dissolved backgrounds
Opens the door for multi-element analysis on a particle-by-particle basis
30.2 30.3 30.4 30.5 30.6
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ICP
-MS
Res
pons
e (c
ount
s)
Time (sec)
31.10
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-MS
Res
pons
e (c
ount
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10
ms)
10
0μ
s d
well
tim
es
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Improving Particle Resolution: Overcoming coincidence
Montaño, M. et al. Environmental Science: Nano, 2014
11.110 11.115 11.120 11.125 11.130
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140C
ounts
Time (sec)
392 counts
287 counts
352 counts
2ppb 100nm Au NPs (0.1ms)
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Improving Particle Resolution: Overcoming coincidence
Montaño, M. et al. Environmental Science: Nano, 2014
11.110 11.115 11.120 11.125 11.130
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140C
ounts
Time (sec)
392 counts
287 counts
352 counts10ms10ms
2ppb 100nm Au NPs (0.1ms)
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Improving Particle Resolution: Overcoming coincidence
Montaño, M. et al. Environmental Science: Nano, 2014
11.110 11.115 11.120 11.125 11.130
0
20
40
60
80
100
120
140C
ounts
Time (sec)
392 counts
287 counts
352 counts
3ms 3ms 3ms 3ms 3ms 3ms 3ms
2ppb 100nm Au NPs (0.1ms)
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Improving Particle Resolution: Overcoming coincidence
Montaño, M. et al. Environmental Science: Nano, 2014
• Microsecond spICP-MS vastly improves particle resolution
• Particle number concentrations and sizing can be better determined
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Reducing Background Interference
Montaño, M. et al. Environmental Science: Nano, 2014
20 22 24 26 28 30 32 34 36 38 400
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ICP
-MS
response (
counts
)
Time (sec)
0.1ms dwell time
3ms dwell time
10ms dwell time30.845 30.846 30.847 30.848 30.849 30.8500
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ICP
-MS
re
sp
on
se
(co
un
ts)
Time (sec)
• Reducing dwell time results in a reduction of counts from dissolved analyte
• Lower dwell times allow for better resolution between background and analyte signals
500ppt Ag+ + 50ppt Ag NPs
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Reducing Background Interference
Montaño, M. et al. Environmental Science: Nano, 2014
Increasing Dissolved Ag+ Concentration
Decreasin
g dw
ell time
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Dual-element Detection in spICP-MS
Montaño, M. et al. Environmental Science: Nano, 2014
• New microsecond dwell times allow for the analysis of two elements within a single particle
• Applied to the analysis of complex (core-shell) nanomaterials
• Possible method for differentiating between naturally occurring and engineered nanomaterials
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Principles of Dual-element Analysis
Montaño, M. et al. Environmental Chemistry, In Press
Time required for the quadrupole to switch between the two masses
Dwell time of a given mass analyte
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Limitations of dual-element ICP-MS
NP events (500μs)
• The length of the settling time results in “lost” analyte signal
• Analysis is not simultaneous, and will result in variable signal of the two analytes
• Currently qualitative on a particle by particle basis, but can be quantitative with the overall average of signal intensity
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Limitations of dual-element ICP-MS
Settling Time
• The length of the settling time results in “lost” analyte signal
• Analysis is not simultaneous, and will result in variable signal of the two analytes
• Currently qualitative on a particle by particle basis, but can be quantitative with the overall average of signal intensity
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Limitations of dual-element ICP-MS
Settling Time Ag detection
• The length of the settling time results in “lost” analyte signal
• Analysis is not simultaneous, and will result in variable signal of the two analytes
• Currently qualitative on a particle by particle basis, but can be quantitative with the overall average of signal intensity
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Limitations of dual-element ICP-MS
Settling Time Ag detection Au detection
• The length of the settling time results in “lost” analyte signal
• Analysis is not simultaneous, and will result in variable signal of the two analytes
• Currently qualitative on a particle by particle basis, but can be quantitative with the overall average of signal intensity
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Proof of Concept – Isotopic Ratios
Montaño, M. et al. Environmental Science: Nano, 2014
• 60nm silver nanoparticles were analyzed for isotopes 107Ag and 109Ag
• These two isotopes occur in early equal ratios naturally
(107Ag: 51.35% and 109Ag: 48.65%)
• Some individual peaks show ratios similar to natural isotopic abundance
• Average of overall intensities match closely with natural abundance:
(107Ag: 50.7% and 109Ag: 49.2%)(n= 125000)
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Core-shell Nanomaterials
30 nm 15 nm15 nm
• Some nanomaterials have complex morphologies such as a core-shell structure
• Examples of core-shell nanomaterials includeo Carbon-coated metal oxides for catalysis o Metal sulfide capped semiconducting
quantum dots
• Both the core and shell must contain an detectable amount of mass to be analyzed by dual-element spICP-MS
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Experimental Set-up
Suwanpetch, R.; Montaño, M.; Tadjiki, S.; Ranville, J. In preparation, 2014
• Gold core (30nm) – Silver shell (15nm) nanoparticles were analyzed by single particle ICP-MS
• Fractions were collected from both Flow field flow fractionation (AF4) and Centrifugal-FFF (Sed-FFF)
• AF4 is a separation technique based off of hydrodynamic diameter
• Centrifugal-FFF separates according to a particles buoyant mass
Asymmetrical Flow Field Flow Fractionation (AF4)
Centrifugal Field Flow Fractionation (Sed-FFF)
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Flow Field Flow Fractionation Chromatograms
Suwanpetch, R.; Montaño, M.; Tadjiki, S.; Ranville, J. In preparation, 2014
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Inte
nsity (
cp
s)
Retention time (min)
Ag-107
Au-197
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ICP
-MS
Response (
counts
)
Time (sec)
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Ag Response
197
Au Response
AF4 coupled to ICP-MS Sed-FFF coupled to ICP-MS
• Both fractograms show co-eluting of gold and silver peaks
• Evidence for one single particles, instead of individual gold and silver particles in solution
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Flow Field Flow Fractionation Chromatograms - Mixtures
Suwanpetch, R.; Montaño, M.; Tadjiki, S.; Ranville, J. In preparation, 2014
• Separation of a mixture by AF4 would show just one particle type at 60nm
• Separation of particles by Sed-FFF would show particle of similar mass
• Analysis by spICP-MS can differentiate between core-shell (bi-metallic) and single metal nanomaterials
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Particle size of Core-shell NMs by spICP-MS
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Dia
mete
r (n
m)
Time (min)
Au-ST
Au-JR
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mete
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m)
Time (min)
Ag-ST
Ag-JR
Gold Core Diameter ComparisonTotal Diameter Comparison
(Based on silver mass)
• Particle sizes are consistent with distribution of intensity by FFF-ICP-MS
• Gold core at peak maxima (30min) is 30nm
• Total diameter at peak maxima (assuming 30nm core) is ~45nm
Suwanpetch, R.; Montaño, M.; Tadjiki, S.; Ranville, J. In preparation, 2014
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Particle Number Concentration Comparison
15 20 25 30 35 40 45 50
0
1x108
2x108
3x108
4x108
5x108
6x108
7x108
8x108
9x108
Part
icle
num
ber
conc. (P
art
icle
s/L
)
Time (min)
107Ag nanoparticles
197Au nanoparticles
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rtic
le n
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be
r co
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rtic
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Time (min)
107Ag Nanoparticles
197Au Nanoparticles
Replicate 1 Replicate 2
• Discrepancy in particle number concentration (# of events detected)
• Possible loss of gold analyte signal to background due to small size
Suwanpetch, R.; Montaño, M.; Tadjiki, S.; Ranville, J. In preparation, 2014
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Particle Number Concentration Comparison
15 20 25 30 35 40 45 50
0
1x108
2x108
3x108
4x108
5x108
6x108
7x108
8x108
9x108
Part
icle
num
ber
conc. (P
art
icle
s/L
)
Time (min)
107Ag nanoparticles
197Au nanoparticles
20 30 40 50
0.0
5.0x107
1.0x108
1.5x108
2.0x108
2.5x108
Pa
rtic
le n
um
be
r co
nc.
(Pa
rtic
les/L
)
Time (min)
107Ag Nanoparticles
197Au Nanoparticles
Replicate 1 Replicate 2
• Discrepancy in particle number concentration (# of events detected)
• Possible loss of gold analyte signal to background due to small size
Suwanpetch, R.; Montaño, M.; Tadjiki, S.; Ranville, J. In preparation, 2014
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Dual-element Analysis of Core-shell NPs
• Dual-element analysis of NPs show presence of both gold and silver
• Some gold signal may be lost to the background
• Dual element analysis and individual particle analysis shows consistent elemental intensity ratios:Dual element analysis
107Ag: 77.7% /197Au: 22.3%Individual particle analysis 107Ag: 71.2%/ 197Au: 28.8%
Montaño, M. et al. Environmental Science: Nano, 2014
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Environmental Analytical Challenges – Natural Nanomaterials
Kiser, M. et al. Environmental Science and Technology, 2008
Ti-containing mineral in biosolid (Kiser)
TiO2 nanoparticles in toothpaste
• ENPs will be released into an environment containing several naturally occurring nanomaterials
• Natural nanomaterials are present in concentrations much higher than expected release concentrations
• Many of these nanomaterials will be of similar chemical composition to their engineered analogues
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Environmental Analytical Challenges – Natural Nanomaterials
Kiser, M. et al. Environmental Science and Technology, 2008
Ag nanoparticles prepared by silver ammonia reduction (Panacek)
Ag nanoparticles found in sock fabric (Benn)
Ag nanoparticles synthesized by Aspergillus flavus (Vigneshwaran)
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ENM vs. NNP Properties
Most engineered nanomaterials have naturally occurring analogues
Some key differences can be used to differentiate natural and engineering NMs
Environmental processes may drastically affect some of these properties (i.e. surface coatings, aggregation state, size distribution)
Elemental composition may remain the most unchanged property in the environment
Montaño, M. et al. Environmental Chemistry, In Press
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Elemental Ratio Analysis
1) Montaño, M. et al. Environmental Chemistry, In Press2) O’Loughling, E. et al. Environ Sci. and Tech. 20033) Burgos, W. et al. Geochimica et Cosmochimica Acta. 2008
• Elemental ratios may be used to differentiate engineered and naturally occurring nanomaterials
• Natural nanomaterials may have broader size distribution than more tightly controlled ENMs
• Particle-by-particle analysis of elemental ratios (μsec-spICP-MS) can be used to differentiate between naturally occurring and engineered nanomaterials
Uraninite nanoparticles precipitated on mixed Fe(II)/Fe(III) hydroxides
Uraninite nanoparticles precipitated from soluble U(VI) by Shewanella oneidensisMR-1 strain
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Elemental Ratio Analysis
Montaño, M. et al. Environmental Chemistry, In Press
Natural elemental ratios show a trend with a natural variation
Statistically significant deviations outside confidence interval of trend may be presence of engineered nanomaterials
May require significant amounts of engineered nanomaterial
Limited information about physical/chemical state of nanomaterials (i.e. aggregation)
Ce 𝑐𝑜𝑛𝑐𝑒𝑛𝑡𝑟𝑎𝑡𝑖𝑜𝑛𝜇𝑔𝐿
La 𝑐𝑜𝑛𝑐𝑒𝑛𝑡𝑟𝑎𝑡𝑖𝑜𝑛𝜇𝑔𝐿
=
1.7𝜇𝑔𝐿 𝐶𝑒
1𝜇𝑔𝐿
𝐿𝑎= 1.7
1.7𝜇𝑔𝐿 Ce +
170𝑛𝑔𝐿 𝐶𝑒𝑂2 𝑁𝑃𝑠
1𝜇𝑔𝐿 𝐿𝑎
= 1.87
Manuel David MontañoColorado School of MinesJuly 10th, 2014
Analysis of a natural nanoparticle will show presence of many elements
Summation of elemental signal can be used to give elemental ratio on a particle basis
Engineered nanomaterial will show the presence of only one element, or have a different elemental ratio
Requires sufficient mass to produce an appreciable, detectable signal
44
Particle-by-particle Elemental Analysis
Montaño, M. et al. Environmental Chemistry, In Press
Manuel David MontañoColorado School of MinesJuly 10th, 2014
Analysis of a natural nanoparticle will show presence of many elements
Summation of elemental signal can be used to give elemental ratio on a particle basis
Engineered nanomaterial will show the presence of only one element, or have a different elemental ratio
Requires sufficient mass to produce an appreciable, detectable signal
45
Particle-by-particle Elemental Analysis
Montaño, M. et al. Environmental Chemistry, In Press
Manuel David MontañoColorado School of MinesJuly 10th, 2014
Analysis of a natural nanoparticle will show presence of many elements
Summation of elemental signal can be used to give elemental ratio on a particle basis
Engineered nanomaterial will show the presence of only one element, or have a different elemental ratio
Requires sufficient mass to produce an appreciable, detectable signal
46
Particle-by-particle Elemental Analysis
Montaño, M. et al. Environmental Chemistry, In Press
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Analysis of an Impacted Natural System
• Analysis of a nearby natural stream (Clear Creek, Golden, CO, USA) showed presence of particles containing Ce and La (fig. A and C)
• Ratio was consistent with literature values
• 80-100nm engineered cerium dioxide was spiked into natural water
• Elemental ratio shifted toward cerium. Presence of cerium-only particles persisted (fig. B and D)
Montaño, M. et al. Environmental Science: Nano, 2014
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Conclusions and Future Outlook
Conclusions
Future Research
Conventional single particle ICP-MS uses dwell times too large for accurate particle sizing and counting
The presence of natural nanomaterials will impede the detection and characterization of engineered nanomaterials
Microsecond dwell times off the ability to improve particle resolution, reduce background signal and introduce particle-by-particle elemental ratios
More work is required to improve sensitivity of single particle ICP-MS to detect smaller particle sizes
New TOF-ICP-MS may be used to detect several elements within a single particle*
Develop methods to identify aggregation state of nanomaterials in the environment
Borovinskaya, O. et al. JAAS, 2013.
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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Acknowledgements
Ranville Research Group
Collaborators:o Hamid Badiei, Samad
Bazargan, Pritesh Patel, Dylan McNair, Kenneth Neubauer(Perkin Elmer)
o Christopher Higgins (CSM)o Soheyl Tadjiki (PostNova
Analytics)o Rabiab Suwanpetch
Fundingo Semiconductor Research
Corporationo EPA Contract No. EP-C-11-039
Pictured from left to right: Jacob Williamson, Rabiab Suwanpetch, Jingjing Wang,Dr. James Ranville, Angela Barber, Evan Gray, Manuel Montaño, Elizabeth Traudt
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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References
1. Nowack, B.; David, R.; Fissan, H.; Morris, H.; Shatkin, J.; Stintz, M.; Zepp, R.; Brouwer, D. Potential release sceanrios for carbon nanotubes used in composites. Environment International, 2013, 59, pp. 1-11.
2. Montano, M.; Ranville, J.; Lowry, G.; von der Kammer, F.; Blue, J. Current status and future direction for examining engineered nanomaterials in natural systems. Environmental Chemistry. Accepted April 2014.
3. Kiser, M.; Westerhoff, P.; Benn, T.; Wang, Y.; Pêrez-Rivera, J.; Hristovski, K. Titanium Nanomaterial Removal and Release from Wastewater Treatment . Environmental Science and Technology. 2008, 43, pp. 6757-6763.
4. Montaño, M.; Ranville, J.; Badiei, H.; Bazargan, S. Improvement in the detection and characterization of engineered nanomaterials using spICP-MS with microsecond dwell times. Environmental Science: Nano. Submitted 2014.
5. Borovinskaya, O.; Hattendorf, B.; Tanner, M.; Gschwind, S.; Günther, D. A prototype of a new inductively coupled plasma time-of-flight mass spectrometer providing temporally resolved, multi-element detection of short signals generated by single particles and droplets. Journal of Analytical Atomic Spectrometry, 2013, 28, pp. 226-233.
6. Panáček, A.; Kvitek, L.; Prucek, R.; Kolář, M.; Večeřová, R.; Pizúrová, N.; Sharma, V.; Nevěčná, T.; Zbořil, R. Silver Colloid Nanoparticles: Synthesis, Characterization, and Their Antibacterial Activity. Journal of Physical Chemistry B, 2006, 110, pp. 16248-16253.
7. Benn, T.; Westerhoff, P. Nanoparticle Silver Released into Water from Commercially Available Sock Fabrics. Environmental Science and Technology, 2008, 42, pp. 4133-4139.
8. Vigneshwaran, N.; Ashtaputre, N.; Varadarajan, P.; Nachane, R.; Paralikar, K.; Balasubramanya, R. Biological synthesis of silver nanoparticles using the fungus Aspergillus flavus. Materials Letters, 2007, 61, pp. 1413-1418.
Manuel David MontañoColorado School of MinesJuly 10th, 2014
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QUESTIONS?