C O M M U N I C A T I O N S
Table 1. Electrical Conductivity of p-PNCPA/SWNT Composite
wt %
SWNT
drying temp
(°C)
electrical conductivity
(S/m)
10
20
20
50
20
50
0.04
0.26
0.91
2.29
control the microstructure and behavior in the solid state will have
potential applications in polymer nanocomposite preparation.
To conclude, we have synthesized a novel thermo-responsive
polymer with 5 mol % pyrene side groups (p-PNCPA) to disperse
SWNTs in water. Cryo-TEM micrographs obtained at temperatures
above and below the LCST of this thermo-responsive polymer
revealed the bundled and exfoliated microstructure of SWNTs,
respectively. Viscosity measurements show shear-thinning and
nearly Newtonian behavior of the suspensions above and below
LCST. Turbidity measurements suggest that p-PNCPA retains its
intrinsic thermo-responsive properties in the presence of SWNTs,
with no significant change in the transition temperature. Evaluation
of dried composite films suggests that the microstructure in the
liquid state is preserved in the solid state to a large extent.
Temperature controlled dispersion of SWNTs in water provides a
new technique for controlling properties in the liquid and solid states
that could impact nanotube-based sensing and composites respectively.
Figure 2. Viscosity of p-PNCPA/SWNT suspensions as a function of shear
rate at 10 and 50 °C.
ments are complementary to cryo-TEM, and thus it is reasonable
to deduce that p-PNCPA/SWNT suspensions are well dispersed at
10 °C and relatively bundled at 50 °C.
To understand the temperature response of p-PNCPA in the
presence of SWNTs, turbidity (actually decadic absorbance) at 400
nm was examined in the absence and presence of SWNTs, as shown
in Figure 3. It can be seen that there is a significant increase in
turbidity of the p-PNCPA solution at 30 °C, and this is because of
the coil-globule transition of p-PNCPA. The p-PNCPA/SWNT
suspensions also show a small but significant increase at ∼30 °C,
which corresponds to the transition temperature of p-PNCPA. Thus,
the thermo-responsive characteristics of p-PNCPA are retained in
the presence of SWNTs.
Acknowledgment. The authors would like to acknowledge
financial support for this work from the Texas Engineering
Experiment Station (TEES) and the National Science Foundation
(CMMI 0644055). Dr. Christos Savva is thanked for his assistance
with cryo-TEM (part of the Microscopy and Imaging Center [MIC]
at Texas A&M). The acquisition of the FEI Quanta 600 FE-SEM
was supported by the National Science Foundation (DBI 0116835),
the VP for Research Office, and TEES. The University of Mainz
is gratefully acknowledged for financial support.
Supporting Information Available: Synthesis scheme of p-PNCPA,
experimental details, 1H NMR spectra of p-PNCPA, UV/vis absorption
and fluorescence emission spectra of p-PNCPA, SEM of dried
composite films, and hydrodynamic radius of p-PNCPA as a function
of temperature. This material is available free of charge via the Internet
References
Figure 3. Turbidity as a function of temperature for aqueous p-PNCPA/
(1) Kam, N. W. S.; Liu, Z. A.; Dai, H. J. Angew. Chem., Int. Ed. 2006, 45,
577–581.
SWNT neat suspension and p-PNCPA solution in water.
(2) Bianco, A.; Kostarelos, K.; Partidos, C. D.; Prato, M. Chem. Commun.
2005, 57, 1–577.
To investigate the solid-state microstructure, suspensions of
p-PNCPA/SWNT were dried at temperatures below and above
LCST (i.e., 20 and 50 °C, respectively) to form thin composite
films. Scanning electron microscopy was performed on the dried
composite films. Results (see Supporting Information) show a high
degree of aggregation in the films dried at 50 °C. Electrical
conductivity measurements made on these composites (see Table
1) showed significantly higher conductivity for films dried at 50
°C at all the concentrations studied (i.e., 10 and 20 wt % SWNT).
This improved electrical conductivity for the film dried at 50 °C is
due to better nanotube-nanotube contacts resulting from weaker
polymer-nanotube interaction. This leads to a more aggregated,
more heavily networked microstructure, much like the case in the
liquid suspension. In the film dried at 20 °C, the closer association
between polymer and nanotube restricts the electron flow by
creating an insulating layer and reducing the contact points between
tubes. This method of tailoring microstructure in the liquid state to
(3) Barone, P. W.; Baik, S.; Heller, D. A.; Strano, M. S. Nat. Mater. 2005, 4,
86–U16.
(4) Bandyopadhyaya, R.; Nativ-Roth, E.; Regev, O.; Yerushalmi-Rozen, R.
Nano Lett. 2002, 2, 25–28.
(5) Islam, M. F.; Rojas, E.; Bergey, D. M.; Johnson, A. T.; Yodh, A. G. Nano
Lett. 2003, 3, 269–273.
(6) Wang, Y. B.; Iqbal, Z.; Mitra, S. J. Am. Chem. Soc. 2006, 128, 95–99.
(7) Star, A.; Steuerman, D. W.; Heath, J. R.; Stoddart, J. F. Angew. Chem.,
Int. Ed. 2002, 41, 2508.
(8) Grunlan, J. C.; Liu, L.; Kim, Y. S. Nano Lett. 2006, 6, 911–915.
(9) Grunlan, J. C.; Liu, L.; Regev, O. J. Colloid Interface Sci. 2008, 317, 346–
349.
(10) Fujishige, S.; Kubota, K.; Ando, I. J. Phys. Chem. 1989, 93, 3311–3313.
(11) Wang, D.; Chen, L. W. Nano Lett. 2007, 7, 1480–1484.
(12) Kuramoto, N.; Shishido, Y. Polymer 1998, 39, 669–673.
(13) Maeda, Y.; Nakamura, T.; Ikeda, I. Macromolecules 2001, 34, 1391–1399.
(14) Chen, R. J.; Zhang, Y. G.; Wang, D. W.; Dai, H. J. J. Am. Chem. Soc.
2001, 123, 3838–3839.
(15) Inomata, H.; Goto, S.; Saito, S. Macromolecules 1990, 23, 4887–4888.
(16) Yokoyama, A.; Srinivasan, K. R.; Fogler, H. S. Langmuir 1989, 5, 534–
538.
(17) Shaffer, M. S. P.; Windle, A. H. Macromolecules 1999, 32, 6864–6866.
JA905803F
9
J. AM. CHEM. SOC. VOL. 131, NO. 38, 2009 13599