It has been widely recognized that the combination of carbon nanotube (CNT) and liquid crystals (LCs) not only provides a useful way to align CNTs, but also dramatically enhances the order in the LC phases, which is especially useful in liquid crystal display (LCD) technology. As the measure of this phase behavior, the complex specific heat is presented over a wide temperature range for a negative dielectric anisotropy alkoxyphenylbenzoate liquid crystal (9OO4) and CNT composites as a function of CNT concentration. The calorimetric scans were performed under near-equilibrium conditions between 25 and 95 °C, first cooling and then followed by heating for CNT weight percent ranging from ϕw = 0 to 0.2. All 9OO4/CNT mesophases have transition temperatures ∼1 K higher and a crystallization temperature 4 K higher than that of the pure 9OO4. The crystal phase superheats until a strongly first-order specific heat feature is observed, 0.5 K higher than in the pure 9OO4. The transition enthalpy for the nanocomposite mesophases is 10% lower than that observed in the pure 9OO4. The strongly first-order crystallization and melting transition enthalpies are essentially constant over this range of ϕw. Complementary electroclinic measurement on a 0.05 wt. % sample, cooling towards the smectic-C phase from the smectic-A, indicates that the SmA-SmC transition remains mean-field-like in the presence of the CNTs. Given the homogeneous and random distribution of CNTs in these nanocomposites, we interpret these results as arising from the LC-CNT surface interaction pinning the orientational order uniformly along the CNT, without pinning the position of the 9OO4 molecule, leading to a net ordering effect for all phases. These effects of incorporating CNTs into LCs are likely due to “anisotropic orientational” coupling between CNT and LC, the change in the elastic properties of composites and thermal anisotropic properties of the CNTs.
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14 March 2014
Research Article|
March 13 2014
Studies of nanocomposites of carbon nanotubes and a negative dielectric anisotropy liquid crystal
P. Kalakonda;
P. Kalakonda
1Department of Physics,
Worcester Polytechnic Institute
, Worcester, Massachusetts 01609, USA
2Department of Materials Science and Engineering,
Carnegie Mellon University
, Pittsburgh, Pennsylvania 15213, USA
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R. Basu;
R. Basu
3Department of Physics,
The United States Naval Academy
, Annapolis, Maryland 21402, USA
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I. R. Nemitz;
I. R. Nemitz
4Department of Physics,
Case Western Reserve University
, Cleveland, Ohio 44106, USA
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C. Rosenblatt;
C. Rosenblatt
4Department of Physics,
Case Western Reserve University
, Cleveland, Ohio 44106, USA
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G. S. Iannacchione
G. S. Iannacchione
a)
1Department of Physics,
Worcester Polytechnic Institute
, Worcester, Massachusetts 01609, USA
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a)
Electronic mail: gsiannac@wpi.edu
J. Chem. Phys. 140, 104908 (2014)
Article history
Received:
November 23 2013
Accepted:
February 25 2014
Citation
P. Kalakonda, R. Basu, I. R. Nemitz, C. Rosenblatt, G. S. Iannacchione; Studies of nanocomposites of carbon nanotubes and a negative dielectric anisotropy liquid crystal. J. Chem. Phys. 14 March 2014; 140 (10): 104908. https://doi.org/10.1063/1.4867791
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