
Web Release Date: November 28,
Natural Organic Matter Stabilizes Carbon Nanotubes in the Aqueous Phase

and

School of Civil and Environmental Engineering, Georgia Institute of Technology, 200 Bobby Dodd Way, Atlanta, Georgia 30332, and Department of Civil and Environmental Engineering, Rice University, 6100 Main Street, Houston, Texas 77005
Received for review July 31, 2006
Revised manuscript received October 13, 2006
Accepted October 16, 2006
Abstract:
This study investigates the aqueous stability of multi-walled carbon nanotubes (MWNTs) in the presence of natural organic matter (NOM). MWNTs were readily dispersed as an aqueous suspension in both model NOM (Suwannee River NOM (SR-NOM)) solutions and natural surface water (actual Suwannee River water with unaltered NOM background), which remained stable for over 1 month. Microscopic analyses suggested that the suspension consisted primarily of individually dispersed MWNTs. Concentrations of MWNTs suspended in the aqueous phase, quantified using thermal optical transmittance analysis (TOT), ranged from 0.6 to 6.9 mg/L as initial concentrations of MWNT and SR-NOM were varied from 50 to 500 mg/L and 10 to 100 mg/L, respectively. Suwannee River water showed a similar MWNT stabilizing capacity as compared to the model SR-NOM solutions. For the same initial MWNT concentrations, the concentrations of suspended MWNT in SR-NOM solutions and Suwannee River water were considerably higher than that in a solution of 1% sodium dodecyl sulfate, a commonly used surfactant to stabilize CNTs in the aqueous phase. These findings suggest that dispersal of carbon-based nanomaterials in the natural, aqueous environment might occur to an unexpected extent following a mechanism that has not been previously considered in environmental fate and transport studies.
Carbon nanotubes (CNTs) are pure carbon macromolecules consisting of sheets of carbon atoms covalently bonded in hexagonal arrays that are seamlessly rolled into a hollow, cylindrical shape with both ends rounded through pentagon ring inclusions. Variable CNT architectures with diameters in the nanometer range (ca. 1-100 nm) and lengths up to several tens of micrometers give rise to high length to diameter aspect ratios as compared to other carbon fullerenes such as C60 (1). On the basis of their structure, CNTs are categorized into two main species; single-walled nanotubes (SWNTs) and multi-walled nanotubes (MWNTs). The latter results from a coaxial assembly of the multiple SWNTs (2).
CNTs are being considered for a range of applications
due to their exceptional mechanical, electro-optical, and
thermal properties (3, 4)
Unfortunately, a limited amount of information is cur
rently available regarding the fate and transport of CNTs in
the natural and engineering environment and the ultimate
human health effects (14). To date, studies have shown that
CNTs are biologically active as demonstrated by a pulmonary
response via induction of pulmonary granulomas (17, 18)
m crystalline silica),
which is a recognized chronic occupational health hazard
(via inhalation routes). Both SWNT and MWNT were also
attributed to cause loss of phagocytic ability and ultrastructure damage to alveola macrophages (19). Furthermore, CNT
have induced observable toxic responses in other cell cultures
(20, 21)
When considering industrial scale production and use,
observed biological activities, and the fact that CNT and other
fullerene structures have been identified in soot from
common hydrocarbon combustion processes (22, 23)
Given the previous observations that CNTs are stabilized in the aqueous phase by well-characterized surfactants and polymers, it is possible that similar interactions between CNTs and organic molecules present in natural systems will occur. This may result in aqueous dispersion and stabilization of CNTs following a demonstrated mechanism of hydrophobic surface shielding that has not been widely considered in environmental fate and transport studies to date. The objectives of this study were to verify MWNT stabilization, as an aqueous suspension, in both synthetic solutions containing model natural organic matter (NOM) and natural surface water with a high NOM background (Suwannee River) and to develop a method to quantify MWNTs suspended in NOM solutions based on thermal optical transmittance analysis.
MWNTs, produced by a chemical vapor deposition (CVD)
method with purity greater than 90%, were obtained from
the MER Corporation (Tucson, AZ). The average diameter
and average length were reported by the manufacturer to be
140 ± 30 nm (approximately 100 graphene layers per each
molecules on average) and 7 ± 2
m, respectively. Standard
Suwannee River NOM (SR-NOM) obtained from the International Humic Substances Society (IHSS) (St. Paul, MN)
was used as a model NOM. Number average and weight
average molecular weights of SR-NOM determined by gel
permeation chromatography were reported as 1718 and 2703
Da, respectively (40). On the basis of the analytical informa
tion provided by IHSS, SR-NOM is composed of 52.47 wt %
carbon, 4.19 wt % hydrogen, 42.69 wt % oxygen, 1.10 wt %
nitrogen, 0.65 wt % sulfur, and 0.02 wt % phosphate, and the
ash content is 7.0 wt %. A significant amount of carbon in
the SR-NOM is distributed at the carboxylic group (20%),
which provides an acidic moiety to the SR-NOM, as well as
aromatic (23%), aliphatic (27%), and heteroaliphatic (15%)
groups. A 100 mg C/L stock solution was prepared by
dissolving SR-NOM for 24 h and filtering the solution through
a 0.2
m nylon membrane filter (Cole Parmer, Chicago, IL).
For comparison with model SR-NOM, a grab sample of actual
Suwannee River water was obtained from the official sampling
site of the IHSS, located in the Okefenokee National Wildlife
Refugee in Georgia (41). The water sample was transported
in a cooler packed with ice from the sampling location and
preserved in a 4
C temperature room after being filtered
with a 0.2
m nylon membrane filter (Cole Parmer, Chicago,
IL). ACS reagent grade (>99%) sodium dodecyl sulfate (SDS,
CH3(CH2)11OSO3Na, FW = 288.38) (Aldrich Chemical Co.,
Milwaukee, WI), which has a critical micelle concentration
of 0.24% at 25
C, was used as a representative surfactant to
stabilize MWNTs in water. Ultrapure water (>18 M
)
produced by the Milli-Q water purification system (Millipore,
Billerica, MA) was used for the preparation of all solutions.
MWNT suspensions were prepared by adding varying
amounts of MWNT into 100 mL of a Milli-Q water, 1% SDS
solution, a well-known surfactant to stabilize CNTs, as a
positive control, solutions containing varying concentrations
SR-NOM, and Suwannee River water in Erlenmeyer flasks
and vigorously agitating the solutions for 1 h. After settling
for 4 days, the unsettled supernatant (ca. 60% of total volume)
was carefully removed by a syringe from the top of the flask.
The solution was then filtered using a Whatman Model 541
filter paper (20-25
m, Florham Park, NJ) to remove any
undispersed MWNT agglomerates, and the filtrate was
collected for further analyses.
In situ images (i.e., suspended in the water phase) of
MWNTs in suspension were obtained using a Leica DM IRM
Differential Interference Contrast (DIC) Microscope (Wetzlar,
Germany) operated in a reflective index mode and recorded
with a Hamamatsu EM-CCD C9100 Camera (Hamamatsu
City, Japan). The point-to-point resolution of the resulting
image was 0.053
m. Suspended MWNTs were particularly
easy to identify and record due to the contrasting reflective
indexes of MWNT as compared to the aqueous background.
Electron microscopic images were analyzed by a JEM 100C
transmission electron microscope (TEM) (Jeol, Peabody, MA)
using 100 kV electron beam at magnifications of 7200 and
100 000. TEM samples were prepared by placing a droplet
of MWNT aqueous suspension on the 300 mesh copper
carbon grid (Electron Microscopy Science, Hatfield, PA) and
dried overnight at room temperature.
Concentrations of suspended MWNTs were determined
by a Thermal Optical Transmittance (TOT) Analyzer (Sunset
Laboratory, Tigard, OR), UV-vis absorbance, and turbidity
measurements. TOT analysis was performed following the
method described by NIOSH (National Institute for Oc
cupational Safety and Health) (42). Samples for the TOT were
prepared by filtering a known volume of MWNT suspension
through a 25 mm diameter disc type Pallflex 2500 quartz
filter (Pall Corporation, Ann Arbor, MI) with a nominal pore
size of 0.3
m, which has good durability at high-temperature
conditions of TOT, and drying the filter for 24 h at 90
C. An
independent control test confirmed that virtually all MWNTs
stabilized in the aqueous suspension were retained by this
filter (i.e., the concentration of MWNT in the filtrate was less
than the detection limit of the analytical methods used in
this study). NOM and SDS that were not associated with
MWNTs were also removed as filtrates during this step. After
drying, each TOT specimen was prepared by cutting a 1.5
cm2 rectangular area from the center of the glass filter and
loading it on a glass sampling boat of the TOT. Before each
set of measurements, the equipment was calibrated using a
10
L of a 5.0 mg/L sucrose solution. For each measurement,
the flame ionization detector (FID) was calibrated using a
known volume of CH4. UV-vis absorbance and turbidity of
MWNT suspensions were measured by an Agilent 8453 UV-vis spectroscopy system (Palo Alto, CA) and a Hach 2100N
turbidimeter (Loveland, CO), respectively. Concentrations
of NOM remaining in the solution phase, which did not
adsorb onto MWNT, were quantified by UV-vis absorbances
at 254 nm (UV254) after removing the suspended MWNT and
associated NOM with a GHP Acrodisc 0.2
m syringe filter
(Pall Corporation, Ann Arbor, MI). UV254 measurements were
calibrated with DOC analysis (TOC-Vw analyzer, Shimadzu,
Columbia, MD).
The stability of MWNTs in the aqueous phase was largely dependent on the presence of SDS or NOM (Figure 1). The MWNTs added to organic-free Milli-Q water at 500 mg/L (50 mg of MWNTs added to 100 mL of Milli-Q water) settled quickly, and the water became completely transparent in less than an hour (Figure 1a). Upon the addition of the MWNT at the same (equivalent) concentration, a 1% SDS solution immediately became dark and turbid. The solution gradually changed to a light gray suspension after 1 day of settling, and the color of the solution did not noticeably change for over a month (Figure 1b). The solution of 100 mg C/L SR-NOM originally appeared dark and turbid upon equivalent MWNT addition and gradually lightened with a corresponding loss of turbidity during the first 4 days of settling. However, after 4 days, the dark solution, which appeared to be due to the presence of MWNTs, with a yellowish background remained stable for over a month (Figure 1c).
In situ microscopic images of MWNTs suspended in the SDS and SR-NOM solutions are presented in Figure 2. Negligible morphological differences were observed between the MWNTs stabilized by SDS (Figure 2a) and those by SR-NOM (Figure 2b). Both samples contained relatively well-dispersed rod-shaped MWNTs as well as larger size flocs, albeit in much less frequency. A closer examination of MWNTs in a SR-NOM solution by TEM suggested that the majority of MWNTs was suspended as a single tube (a representative image shown in Figure 2c), as evidenced by the presence of a single hollow core (approximately 2 nm in diameter according to the manufacturer) in a single fibrous structure in these images. Bundles of MWNTs (i.e., pairing of several MWNTs along the length axis) were seldom observed. Bubble-like artifacts adjacent to MWNT surfaces might have originated from the sublimation of organic matter due to high-energy electron beam irradiation during TEM analysis. The agglomerates of MWNTs in which a single MWNT appeared to be connected to another MWNT, potentially by bridging through NOM, were also observed during TEM examination. While it is possible that some of these bridged structures might have been additionally generated during a drying process for TEM sample prepara tion, the similar structures were also observed in the in situ images.
In the presence of complex and undefined NOM, analytical
approaches utilizing elemental and molecular characteristics
may prove challenging to quantify the amount of CNT
suspended in the aqueous phase. It should also be noted
that the CNT sample used in this study consists of a mixture
of molecules with different sizes. A method of using TOT
relies on the fact that thermal stabilities of organic carbon
(NOM) and elemental carbon (CNT) are different such that
they can be differentially quantified (43-46)
The TOT analysis typically proceeds in two distinct stages
(52). In the first stage, the temperature increases stepwise up
to 820
C in a He atmosphere to volatilize organic carbon
(OC), which is then oxidized to CO2 via granular MnO2 at 900
C. CO2 is subsequently reduced to CH4 by a Ni/firebrick
methanator at 450
C and quantified by a flame ionization
detector (FID). However, not all of OC is volatilized, as some
becomes pyrolized in the O2 deficient atmosphere. Elemental
carbon (EC) measurements along with pyrolized organic
carbon (PC) correction are performed in the next stage. The
temperature is again raised stepwise in an O2 (10%) and He
(90%) mixed atmosphere. The total amount of thermally
oxidized EC and PC is measured by the FID after reduction
to CH4. Utilizing He-Ne laser transmittance through the
sample, EC from the original sample is differentiated from
PC. In the first stage, as PC is generated and absorbs the
light, the laser transmittance is decreased. However, as both
EC and PC are volatilized, the laser transmittance increases
in the second stage. The point at which the laser transmittance
reaches the initial value (time = 0) is the separation point
between PC and EC. CH4 detected before this point is
attributed to carbon originating from OC, and that detected
after this point is from EC.
Profiles of temperature, laser transmittance, and FID
signals for an entire cycle of a TOT measurement are
presented in Figure 3 along with the split point between OC
and EC. Control experiments were first performed with only
SR-NOM (Figure 3a) and only MWNT (Figure 3b) samples.
The sample containing only SR-NOM was prepared by placing
1 mL of 500 mg/L SR-NOM stock solution on top of the quartz
filter without suction and drying at 90
C. The sample with
only MWNT was prepared by adding MWNT to Milli-Q water,
retrieving an arbitrary fraction onto the quartz filter, and
drying it overnight at 90
C. Therefore, the exact concentra
tions of MWNT were unknown, and quantitative comparison
was not made for these samples. Nevertheless, these experi
ments confirmed that signals from these different carbon
classes do not overlap, allowing for quantitative differentia
tion between MWNT and SR-NOM. During the analysis of
the SR-NOM-only control (Figure 3a), peaks were generated
in both the first and the second stages of analysis, and the
second stage peak appeared to be due to the generation of
PC, as the concentration estimated from the sum of two
peaks agreed with a concentration measured as DOC. For
the MWNT-only sample (Figure 3b), peaks were observed
only in the second stage as EC (with O2 present). When the
sample specimen after one cycle was subject to another entire
TOT cycle, no further change in laser transmittance was
observed, and no more CH4 was produced, confirming that
MWNT conversion to CH4 was complete, consistent with
observations reported in the literature under similar combustion conditions (53, 54)
| Figure 3 Representative TOT thermograms for (a) SR-NOM-only, (b) MWNT-only, and (c) MWNT associated with SR-NOM. |
A representative TOT thermogram for the MWNT and
SR-NOM adduct is shown in Figure 3c. Following this direct
quantification method, concentrations of suspended MWNTs
in synthetic solutions, prepared according to an orthogonal
matrix of varying initial SR-NOM concentrations (10, 25, 50,
and 100 mg C/L) and varying MWNT mass initially added
(50, 100, 250, and 500 mg/L), were analyzed. Results
summarized in Table 1
demonstrate that approximately 0.25-1.4% MWNTs initially added to the SR-NOM solution became
suspended for the range of solution compositions investigated. The fraction of suspended MWNT to the initial mass
increased as more NOM was available. However, NOM
availability was certainly not a limiting factor since the
concentration of suspended MWNT also increased as the
initial MWNT dose increased for the same NOM concentra
tion. This observation suggests that NOM association with
MWNT is a result of a dynamic equilibrium process, similar
to typical adsorbate-adsorbent interactions.
For the same set of samples, the concentration of SR-NOM that was not associated with MWNT was directly measured using absorbance of the filtrate (i.e., after removing MWNT and associated SR-NOM) at 254 nm. Because of the competitive adsorption of different fractions of SR-NOM onto MWNT, some bias can be involved in the quantification of residual SR-NOM with UV254 absorbance. The mass of SR-NOM associated with MWNT (per unit mass) was further calculated by subtracting the SR-NOM concentration in the filtrate from the initial SR-NOM concentration and dividing the value by the initial MWNT concentration. For the calculation, homogeneous adsorption of SR-NOM onto the MWNT was assumed. The mass of SR-NOM associated with MWNT (Table 1) was observed to increase as the relative abundance of SR-NOM increased (i.e., SR-NOM association increased as the initial concentration of SR-NOM increased and/or the initial mass of MWNT added decreased). These results, taken with the TOT results, suggest that the MWNT-NOM suspension formation has two aspects of consideration: (i) the physical dispersion of the MWNT added to solution and (ii) the association/equilibrium processes of NOM to the surface of MWNTs rendering them stable in the aqueous phase.
A spectral analysis of MWNT in the SR-NOM solution showed a distinct, broad increase in the baseline of absorbance spectrum in the visible range (over 500 nm), which was not observed in the solution containing only SR-NOM. Since the increase in baselines appears to be a function of light scattering by MWNT suspension and no specific absorption peak was identified, the absorbance at 800 nm was arbitrarily selected and plotted against the suspended MWNT concentrations determined from TOT analyses, which resulted in a linear correlation (r2 = 0.987) (Figure 4). Similarly, simple turbidity measurements resulted in a reasonable correlation (r2 = 0.952) with the suspended MWNT concentration (results not shown).
| Figure 4 Comparison of light absorbance of MWNTs dispersed in SR-NOM solution at 800 nm and concentration of suspended MWNTs measured by TOT. |
The stability of MWNT was further investigated using an
actual Suwannee River water sample (collected in situ as
described previously) to exclude any potential artifacts that
might have originated from the use of a model compound.
The pH, conductivity, and DOC of the 0.2
m filtered sample
were 3.42, 69.4
S, and 59.1 mg C/L, respectively. Figure 1e
shows 500 mg/L MWNT added to Suwannee River water as
compared to filtered Suwannee River water (Figure 1f). This
picture was taken after agitation for 1 h and quiescent settling
for 4 days. Similar to the model SR-NOM, the Suwannee
River water quickly dispersed MWNT, and the resulting
suspension was stable for over 1 month. When the initial
amount of MWNT added to the Suwannee River water was
varied at 500, 250, 100, and 50 mg/L, the concentration of
suspended MWNT was determined at 6.9, 5.45, 2.27, and
1.76 mg/ L, respectively, which was consistent with observa
tions made with model SR-NOM in that the suspended
MWNT increased as the initial MWNT dose increased. The
amount of NOM adsorbed per unit mass of MWNT was 0.033,
0.042, 0.060, and 0.104 mg C/mg for initial MWNT concentrations of 500, 250, 100, and 50 mg/L, which were also in
reasonable agreement with the results obtained with the
model NOM (Table 1).
The observed similarity in the dispersion nature of the
MWNT in solutions containing NOM and SDS suggests that
MWNT stabilization in the presence of NOM might follow
a similar stabilization mechanism of MWNT surface shielding
by these molecules, which not only leads to more thermodynamically favorable surfaces but also induces electrostatic
and steric stabilization (27, 30, 35, 36)
The enhanced stabilizing propensity might be attributed
to the presence of aromatic fractions of NOM, as compared
to SDS which is aliphatic, as aromaticity and resulting
-
interactions have been identified as an important parameter
in MWNT stabilization by various surfactant molecules (34,
39)
This research was supported by the United States Environmental Protection Agency (U.S. EPA) STAR Grant D832526. The authors acknowledge Jaekyu Cho at the School of Chemical and Biomolecular Engineering at the Georgia Institute of Technology and Sangil Lee and Evan Cobb at the School of Civil and Environmental Engineering at the Georgia Institute of Technology for their assistance during some of the instrumental analyses.
* Corresponding author phone: (404) 894-2216; fax: (404) 385-7087; e-mail: jaehong.kim@ce.gatech.edu.
Georgia Institute of Technology.
Rice University.
1. Iijima, S. Helical microtubules of graphitic carbon. Nature 1991,
354, 56-58.
2. Cowley, J. M.; Liu, M. Q. The structure of carbon nanotubes
impregnated with yttrium. Micron 1994, 25, 53-61.
3. Dreher, K. L. Health and environmental impact of nanotechnology: Toxicological assessment of manufactured nanoparticles. Toxicol. Sci. 2004, 77, 3-5.
4. Ajayan, P. M.; Charlier, J. C.; Rinzler, A. G. Carbon nanotubes:
From macromolecules to nanotechnology. Proc. Natl. Acad. Sci.
U.S.A. 1999, 96, 14199-14200.
5. Ajayan, P. M.; Zhou, O. Z. Applications of carbon nanotubes.
Carbon Nanotubes 2001, 80, 391-425.
6. Dai, H.; Wong, E. W.; Liebert, C. M. Probing electrical transport
in nanomaterials: conductivity of individual carbon nanotubes.
Science 1996, 272, 523-526.
7. Rueckes, T.; Kim, K.; Joselevich, E.; Tseng, G. Y.; Cheung, C.-L.;
Lieber, C. Carbon nanotube-based nonvolatile randon access
memory for molecular computing. Science 2000, 289, 94-97.
8. Dillon, A. C.; Jones, K. M.; Bekkedahl, T. A.; Kiang, C. H.; Bethune,
D. S.; Heben, M. J. Storage of hydrogen in single-walled carbon
nanotubes. Nature 1997, 386, 377-379.
9. Cheng, H. M.; Yang, Q. H.; Liu, C. Hydrogen storage in carbon
nanotubes. Carbon 2001, 39, 1447-1454.
10. Kong, J.; Franklin, N. R.; Zhou, C.; Chapline, M. G.; Peng, S.;
Cho, K.; Dai, H. Nanotube molecular wires as chemical sensors.
Science 2000, 287, 622-625.
11. Collins, P. G.; Bradley, K.; Ishigami, M.; Zettl, A. Extreme oxygen
sensitivity of electronic properties of carbon nanotubes. Science
2000, 287, 1801-1804.
12. Chopra, S.; McGuire, K.; Gothard, N.; Rao, A. M.; Pham, A.
Selective gas detection using a carbon nanotube sensor. Appl.
Phys. Lett. 2003, 83, 2280-2282.
13. Chopra, S.; Pham, A.; Gaillard, J.; Parker, A.; Rao, A. M. Carbon
nanotube-based resonant-circuit sensor for ammonia. Appl.
Phys. Lett. 2002, 80, 4632-4634.
14. Colvin, V. L. The potential environmental impact of engineered
nanomaterials. Nat. Biotechnol. 2004, 22, 760-760.
15. Lee, B. I.; Qi, L.; Copeland, T. Nanoparticles for materials
design: present and future. J. Ceram. Process. Res. 2005, 6, 31-40.
16. Ball, P. Roll up for the revolution. Nature 2001, 414, 142-144.
17. Warheit, D. B.; Laurence, B. R.; Reed, K. L.; Roach, D. H.;
Reynolds, G. A.; Webb, T. R. Comparative pulmonary toxicity
assessment of single-walled carbon nanotubes in rats. Toxicol.
Sci. 2004, 77, 117-125.
18. Lam, C. W.; James, J. T.; McCluskey, R.; Hunter, R. L. Pulmonary
toxicity of single-walled carbon nanotubes in mice 7 and 90
days after intratracheal instillation. Toxicol. Sci. 2004, 77, 126-134.
19. Jia, G.; Wang, H. F.; Yan, L.; Wang, X.; Pei, R. J.; Yan, T.; Zhao,
Y. L.; Guo, X. B. Cytotoxicity of carbon nanomaterials: Single-walled nanotubes, multi-walled nanotubes, and fullerene.
Environ. Sci. Technol. 2005, 39, 1378-1383.
20. Magrez, A.; Kasas, S.; Salicio, V.; Pasquier, N.; Seo, J. W.; Celio,
M.; Catsicas, S.; Schwaller, B.; Forro, L. Cellular toxicity of carbon-based nanomaterials. Nano Lett. 2006, 6, 1121-1125.
21. Chen, X.; Tam, U. C.; Czlapinski, J. L.; Lee, G. S.; Rabuka, D.;
Zettl, A.; Bertozzi, C. R. Interfacing carbon nanotubes with living
cells. J. Am. Chem. Soc. 2006, 128, 6292-6293.
22. Murr, L. E.; Soto, K. F.; Esquivel, E. V.; Bang, J. J.; Guerrero, P.
A.; Lopez, D. A.; Ramirez, D. A. Carbon nanotubes and other
fullerene-related nanocrystals in the environment: A TEM study.
JOM 2004, 56, 28-31.
23. Utsunomiya, S.; Jensen, K. A.; Keeler, G. J.; Ewing, R. C. Uraninite
and fullerene in atmospheric particles. Environ. Sci. Technol.
2002, 36, 4943-4947.
24. Wang, H.; Hobbie, E. K. Amphiphobic carbon nanotubes as
macroemulsion surfactants. Langmuir 2003, 19, 3091-3093.
25. Girifalco, L. A.; Hodak, M.; Lee, R. S. Carbon nanotubes,
buckyballs, ropes, and a universal graphitic potential. Phys. Rev.
B 2000, 62, 13104-13110.
26. Fu, K. F.; Sun, Y. P. Dispersion and solubilization of carbon
nanotubes. J. Nanosci. Nanotechnol. 2003, 3, 351-364.
27. Jiang, L. Q.; Gao, L.; Sun, J. Production of aqueous colloidal
dispersions of carbon nanotubes. J. Colloid Interface Sci. 2003,
260, 89-94.
28. Huang, L. M.; Cui, X. D.; Dukovic, G.; O'Brien, S. P. Self-organizing high-density single-walled carbon nanotube arrays
from surfactant suspensions. Nanotechnology 2004, 15, 1450-1454.
29. Shen, K.; Curran, S.; Xu, H. F.; Rogelj, S.; Jiang, Y. B.; Dewald,
J.; Pietrass, T. Single-walled carbon nanotube purification,
pelletization, and surfactant-assisted dispersion: A combined
TEM and resonant micro-Raman spectroscopy study. J. Phys.
Chem. B 2005, 109, 4455-4463.
30. O'Connell, M. J.; Bachilo, S. M.; Huffman, C. B.; Moore, V. C.;
Strano, M. S.; Haroz, E. H.; Rialon, K. L.; Boul, P. J.; Noon, W.
H.; Kittrell, C.; Ma, J. P.; Hauge, R. H.; Weisman, R. B.; Smalley,
R. E. Band gap fluorescence from individual single-walled carbon
nanotubes. Science 2002, 297, 593-596.
31. Lecoanet, H. F.; Bottero, J. Y.; Wiesner, M. R. Laboratory
assessment of the mobility of nanomaterials in porous media.
Environ. Sci. Technol. 2004, 38, 5164-5169.
32. Lecoanet, H. F.; Wiesner, M. R. Velocity effects on fullerene and
oxide nanoparticle deposition in porous media. Environ. Sci.
Technol. 2004, 38, 4377-4382.
33. Weisman, R. B.; Bachilo, S. M.; Tsyboulski, D. Fluorescence
spectroscopy of single-walled carbon nanotubes in aqueous
suspension. Appl. Phys. A 2004, 78, 1111-1116.
34. Islam, M. F.; Rojas, E.; Bergey, D. M.; Johnson, A. T.; Yodh, A.
G. High weight fraction surfactant solubilization of single-walled
carbon nanotubes in water. Nano. Lett. 2003, 3, 269-273.
35. Matarredona, O.; Rhoads, H.; Li, Z. R.; Harwell, J. H.; Balzano,
L.; Resasco, D. E. Dispersion of single-walled carbon nanotubes
in aqueous solutions of the anionic surfactant NaDDBS. J. Phys.
Chem. B 2003, 107, 13357-13367.
36. Chen, Q.; Saltiel, C.; Manickavasagam, S.; Schadler, L. S.; Siegel,
R. W.; Yang, H. C. Aggregation behavior of single-walled carbon
nanotubes in dilute aqueous suspension. J. Colloid Interface
Sci. 2004, 280, 91-97.
37. Wang, H.; Zhou, W.; Ho, D. L.; Winey, K. I.; Fischer, J. E.; Glinka,
C. J.; Hobbie, E. K. Dispersing single-walled carbon nanotubes
with surfactants: A small angle neutron scattering study. Nano.
Lett. 2004, 4, 1789-1793.
38. O'Connell, M. J.; Boul, P.; Ericson, L. M.; Huffman, C.; Wang,
Y. H.; Haroz, E.; Kuper, C.; Tour, J.; Ausman, K. D.; Smalley, R.
E. Reversible water-solubilization of single-walled carbon
nanotubes by polymer wrapping. Chem. Phys. Lett. 2001, 342,
265-271.
39. Tan, Y.; Resasco, D. E. Dispersion of single-walled carbon
nanotubes of narrow diameter distribution. J. Phys. Chem. B
2005, 109, 14454-14460.
40. Thapa, P. B.; Nakajima, F.; Furumai, H. Characterization of
natural organic matter in a shallow eutrophic lake. Water Sci.
Technol. 2002, 46, 465-471.
41. Perdue, M., personal communication.
42. NIOSH, Manual of Analytical Methods (NIOSH publication 94-113), Atlanta, GA, 1994.
43. Itkis, M. E.; Perea, D. E.; Jung, R.; Niyogi, S.; Haddon, R. C.
Comparison of analytical techniques for purity evaluation of
single-walled carbon nanotubes. J. Am. Chem. Soc. 2005, 127,
3439-3448.
44. Landi, B. J.; Cress, C. D.; Evans, C. M.; Raffaelle, R. P. Thermal
oxidation profiling of single-walled carbon nanotubes. Chem.
Mater. 2005, 17, 6819-6834.
45. Pang, L. S.; Saxby, J. D.; Chatfield, S. P. Thermogravimetric
analysis of carbon nanotubes and nanoparticles. J. Phys. Chem.
A 1993, 97, 6941-6942.
46. Young, K. D.; Leboeuf, E. J. Glass transition behavior in a peat
humic acid and an aquatic fulvic acid. Environ. Sci. Technol.
2000, 34, 4549-4553.
47. Chow, J. C.; Watson, J. G.; Chen, L. W. A.; Arnott, W. P.;
Moosmuller, H. Equivalence of elemental carbon by thermal/optical reflectance and transmittance with different temperature
protocols. Environ. Sci. Technol. 2004, 38, 4414-4422.
48. Bae, M. S.; Schauer, J. J.; DeMinter, J. T.; Turner, J. R.; Smith,
D.; Cary, R. A. Validation of a semi-continuous instrument for
elemental carbon and organic carbon using a thermal-optical
method. Atmos. Environ. 2004, 38, 2885-2893.
49. Viidanoja, J.; Sillanpaa, M.; Laakia, J.; Kerminen, V. M.; Hillamo,
R.; Aarnio, P.; Koskentalo, T. Organic and black carbon in PM2.5
and PM10: 1 year of data from an urban site in Helsinki, Finland.
Atmos. Environ. 2002, 36, 3183-3193.
50. Wierzbicka, A.; Lillieblad, L.; Pagels, J.; Strand, M.; Gudmunds
son, A.; Gharibi, A.; Swietlicki, E.; Sanati, M.; Bohgard, M. Particle
emissions from district heating units operating on three
commonly used biofuels. Atmos. Environ. 2005, 39, 139-150.
51. Conny, J. M.; Klinedinst, D. B.; Wight, S. A.; Paulsen, J. L.
Optimizing thermal-optical methods for measuring atmospheric
elemental (black) carbon: A response surface study. Aerosol
Sci. Technol. 2003, 37, 703-723.
52. Birch, M. E.; Cary, R. A. Elemental carbon-based method for
monitoring occupational exposures to particulate diesel exhaust.
Aerosol Sci. Technol. 1996, 25, 221-241.
53. Catalado, F. A study on the thermal stability to 1000
C of various
carbon allotopes and carbonaceous matter both under nitrogen
and in air. Fullerene Sci. Technol. 2002, 10, 293-311.
54. Illekova, E.; Csomorova, K. Kinetics of oxidation in various forms
of carbon. J. Therm. Anal. 2005, 80, 103-108.
55. Thorn, K. A.; Folan, D. W.; MacCarthy, P. Characterization of the International Humic Substances Society Standard and Reference Fulvic and Humic Acids by Solution State Carbon-13 (13C) and Hydrogen-1 (1H) Nuclear Magnetic Resonance Spectrometry; U.S. Geological Survey, U.S. Department of Interior: Denver, CO, 1989.
|
MWNT initially added (mg/L) |
|||||
|
|
initial SR-NOM concentration (mg/L) |
500 |
250 |
100 |
50 |
|
suspended MWNT (mg/L) |
100 |
6.92 |
6.95 |
3.75 |
1.42 |
|
|
50 |
5.47 |
3.6 |
2.15 |
1.34 |
|
|
25 |
2.31 |
1.88 |
1.02 |
1.15 |
|
|
10 |
1.26 |
1.06 |
1.17 |
0.68 |
|
NOM mass per unit MWNT mass (mg/mg) |
100 |
0.039 |
0.053 |
0.114 |
0.338 |
|
|
50 |
0.029 |
0.031 |
0.048 |
0.072 |
|
|
25 |
0.02 |
0.024 |
0.027 |
0.036 |
|
|
10 |
0.012 |
0.014 |
0.013 |
0.011 |