Faculty Directory
Contact Information Biographical Information Research Interests Publications Group Information Current Classes
 


1. Nanotube-Based New Materials: Filling

(a) Objectives
  • To determine if filled carbon nanotubes are more stiff than empty carbon nanotubes
  • To study any differences in mechanical behavior based on the molecules or atoms with which the nanotube is filled
  • To investigate how the mechanism by which the nanotube compresses is affected by the presence of the filling molecules or atoms
(b) System Setup
i) Empty Nanotube
  • 100 Å (10,10) single-walled nanotube
ii) Methane Filled Nanotube
  • 100 Å (10,10) single-walled nanotube
  • Methane density is 0.431 g/cm3.
iii) Fullerene Filled Nanotube
  • 100 Å (10,10) single-walled nanotube
  • 8 C60 molecules (density is is 0.752 g/cm3).
(c) Force Curves
  • 100 Å nanotube
  • Data averaged over 5 runs
  • 300 K
  • Ne density is 0.862 g/cm3
  • C60 density is 0.752 g/cm3
  • CH4 density is 0.431 g/cm3
(d) Conclusions
  • The simulations predict that filled nanotubes have a higher buckling force than empty nanotubes but have the same stiffness (Young¡¯s modulus).
  • The buckling force depends on the identity of the filling atoms and molecules and their density.

2. Deflection of Carbon Nanotubes

(a) Setup of System
      Single-walled nanotubes (SWNTs), double-walled nanotubes (DWNTs), and triple-walled nanotube (TWNT) are considered. In particular, the SWNT is either a (28,0) or (16,16) nanotube, the DWNT consists of a (19,0)@(28,0) or (11,11)@(16,16) configuration, and the TWNT consists of a (10,0)@(19,0)@(28,0) or (6,6)@(11,11)@(16,16). The nanotubes are open at one end and capped at the other. The open ends are firmly fixed on space to mimic the attachment of the nanotubes to a rigid surface. Thermostats are applied to the atoms that are within 20 Å of the open end to control the system temperature and maintain a temperature of 300 K. This mimics the transfer of thermal energy from the nanotube to the rigid surface to which it is attached. The length of nanotubes is about 215 Å excluding the hemi-spherical caps. All the bonds that connect the nanotubes and caps are sp2-hybridized, and all defects at the cap-nanotube interface consist of pentagon and heptagon rings.
      Nine Ar atoms are located in an 8 Å × 8 Å plane 200 Å from the fixed points at the end of the nanotube, and 20 Å above from the most upper atoms of the outer nanotube wall. The Ar atoms are propelled once every 2 ps multiple times (5 or 10) into the nanotubes. The kinetic energy of each Ar atom is 10 eV, which corresponds to a velocity of 0.0694 Å/fs (= 6.94 × 103 m/s). After each collision event, the nanotubes are relaxed 100 ps - 140 ps prior to the deposition of the next group of Ar atoms.
If you cannot watch this, launch in
 or  Download QuickTime.
(b) Deformation of Nanotubes
      As the Ar atoms collide with the nanotube 10 times, the nanotube bends and "rumples" form in the wall structure. After the Ar collision events have occurred for 20 ps, the nanotubes are more deformed and remain so for a while. The SWNT, which is more flexible than the DWNTs and TWNTs, even folds over during the subsequent relaxation stage.

(c) Displacement of Nanotubes
      They indicate that the SWNTs displace more easily than the DWNTs and TWNTs after repeated collision events. This is not surprising because of the larger number of nanotube walls, which raise the mass and overall stiffness of the nanotube as a whole. Most nanotube tips continue to move in the direction of Ar flow for 10-30 ps after the last collision event. When the nanotubes are folded, it takes longer for them to reach minimum structures. Displacement after the collisions increases as the number of collisions increase.
      Since the nanotubes flex in an oscillatory manner, the motion of the nanotubes during the relaxation period can be described in terms of amplitude and frequency as follows:

where A0 is the estimated amplitude at the initial state of the relaxation process, f is frequency, t is time in ps, φ is angular phase shift, and τ is relaxation time. A0 is greater than the initial downward-displacement if the oscillation of a nanotube is delayed by φ. As the length of CNTs increases, A0 increases, φ increases, τ increases, while f decreases. As the number of CNT walls increases, A0 increases, φ and decreases.

We provide open source codes for MD simulations: C-H REBO MD code, C-F-H REBO MD code, and C-O-H REBO MD code.



Please send your comments, suggestions, or corrections to webmaster@www.mse.ufl.edu
Last Update: Wednesday, May 27, 2005



Copyright © 2005     Department of Materials Science and Engineering, University of Florida